TEM Investigation and FBB Model Explanation to the Phase Relationships between(1)
课堂版How to write a body part
Key
7 This method obtains a precipitate through the addition of BaCl2.2H2O; the resulting precipitate can be washed and stored easily.
6 Samples 10–18 were prepared in our laboratory using a revised version of the precipitation method established by the ISF Institute in Germany.6 7 This method obtains a precipitate through the addition of BaCl2.2H2O; the resulting precipitate can be washed and stored easily. 8 The samples were subsequently shipped to ISF for analysis by accelerator mass spectrometry (AMS). 9 All tubing used was stainless steel, and although two samples were at risk of CFC contamination as a result of brief contact with plastic, variation among samples was negligible.
Your Task: Building a Model
Bosch Access Professional Edition 2.0说明书
The introduction of access control in a company is often done in several small steps. At first only a few central areas are monitored. As system needs expands, access control may become part of an integrated security system. Access Professional Edition 2.0 (Access PE) allows you to start small. Your investment is always safeguarded, because it supports the same controllers as Bosch’s large scale project based systems. If you need to expand your system at a later date, the door leading to an integrated management system including AMC access control is wide open.System OverviewAccess PE provides self contained access control for small and medium-sized companies. Its installation is extremely simple and fast. There is no need to install and administer a database system. The system is easy to use and enables a person with minimal training to create badges and administer access rights in a very short time. Specific event logging and reporting allows you to trace who was when and where on your company’s grounds.You can choose your readers and cards from the same bundle of devices, which are supported by Bosch’s medium to large scale BIS/ACE Access Engine systems, thereby safeguarding your investment for future extensions. Card personalization is included in Access PE, providing you with the means to design your badges, to perform image acquisition with USB-cameras and to use most commercially available Card Printers.In addition to given standardized door models it is possible to use extended I/O functionality to exert influence on diverse conditions while monitoring inputs or setting outputs.The Access PE can be extended with two modules. A Video System on the one side and an Offline Locking System [selected markets, only] on the other side.The Offline Locking System (OLS) is integrated into the Access PE – so a person can use the same card for both systems.Through integrated video functionality and using the wide range of Bosch IP devices an operator for example can do a video verification by comparing live streams with the database image of the person requesting for access. Additional surveillance of the back and front of the person saves your company for unauthorized access.Access Professional Edition 2.0▶Compact access control based on Bosch’s innovativeAMC controller family▶Integrated Video Verification▶Multi-user system with definable user profiles▶Attendance tableau▶Online swipe▶Easy upgrade to BIS/ACE through import of existingcardholder and device data▶Includes Badge Designer for Photo ID Badge Printing▶Integrated Offline Locking System (OLS) [selectedmarkets, only]2Access PE runs on a standard PC with a Windows operating system (2003, XP, or Vista). This can be a single workstation computer or a client-server system with a central server and remote workstations.NoteMicrosoft Windows XP Professional is required for any video integration.FunctionsPos.Description1Server with Access PE 2.0 software 2Workstations 3Printer4AMC2 – access controller 5Reader 6Door strikesThe Access PE system, along with AMC access controllers,offers the following features:•A wide range of pre-defined and self-explaining door models allow fast and easy hardware configuration through one-click selection of the door type, such as standard door, turnstile, elevator, with entrance / exit reader, and so on.•Real-time activation of reader and cardholder configurations in the access controllers.•Time zone support for AMC - allows installations across different time zones.•Time schedules for time-based access permission defined per weekday including the definition of extra days, holidays, etc..•Time schedules for automatic activation/deactivation of cardholder settings, such as access rules, pin codes and so on.•Time schedules for automatic activation/deactivation of system settings, such as setting door status to permanent open from 9 a.m. to 5 p.m.•Online swipe – verification via database image automatically provided through access request.•Three PIN code types can be used for persons:-Verification PIN with alarm code feature -Identification PIN – substitudes a card -IDS-PIN to arm special areas•Choose between the following access modes -Card only -PIN only -PIN or card•Temporary activation/blocking of cardholders, either manually or time controlled.•Definable input fields for cardholder information.•Anti-Passback•Card personalization for importing cardholder images and creating your individual corporate badge designs printable on standard card printers.•Up to three cards can be assigned to a person.•Creation of an acknowledgment of receipt together with the print of the picture and the badge design.•Creation of logical areas, which could be single rooms,groups of rooms, whole floors or parking lots, where access control points could be assigned to.•Full archival and restoral of system data.•Using the Bosch controller family AMC digital and monitored I/Os for additional control and monitoring functions or easy intrusion features.•Supported languages:-English -German -Dutch -Polish-Simplified Chinese -Russian -Spanish-Portuguese (Brazil)•Detailed event log for recording access events.•Integrated filter- and reporting features.•Export into standard CSV-format for further processing.•Comprehensive online help3VideoPos.DescriptionAdditional t o t he p ositions i n t he f irst s ystem o verview t he v ideo c omponents are included now.7Cameras 8DVR or encoderEntrances from special interest can be equipped with additional video devices providing different options. The integrated video functionality in Access PE allows to assign up to five cameras to a door, each to be used as an ID or surveillance camera. With video verification the security level is raised by comparing the person's database image with a live stream while the environment can be observed for tail-gating or possible threats.Any violation, such as door open time exceeds, will provide alarm images for further investigation. Storage of those alarm images and retrieval of alarm archives using Boschvideo storage systems are supported as well.Additional functionalities are:•Alarm verification – providing live images caused through typical alarms around a door.•Video playback from archives reporting on accessrequests or alarm situation with minimum search time.•Live video can be selected from single camera or 2x2matrix (quad mode).Offline Locking System (OLS) [selected markets, only]The OLS uses some components of the Online System. In the picture above the part with the grey background shows the devices which are used for both systems. On the left hand side there are devices of the Online-System and on the right devices of the OLS.Pos.Description 1Workstation2Server with configuration applications and the database 3Access control reader with write module 4Card – can be used for both systems 5AMC2 4R4 – access controller 6Access control reader7Dialog reader to read and write cards 8OLS terminalWith the OLS it is possible to integrate a large quantity of rooms which are far away or not so security relevant in the access control system. All data are stored in the samedatabase and the persons need only one card for both – the Online- and the Offline-System.4Special reader with write-module (3), which are usually used for access control in the Online System, renew data and validity dates on the cards.Note Writing OLS data onto cards can only be used with an AMC2 4R4. Systems with Wiegand-interface-controller (AMC 4W) have to beexpanded with at least one AMC2 4R4 and thecorresponded reader.Parts Included•Access Professional Edition Software•Card Personalization Software•Quick start guide•Documentation CDTechnical SpecificationsMax. number of active cardholders10,000Cards/person up to 3PIN codes 4 to 8 digitsPIN code types Verification PINIdentification PINArming PINDoor PINAccess modes Card onlyPIN onlyPIN or cardMax. number of time profiles255Max. number of access authorizations255Max. number of area/time authorizations255Max. number of access authorizations groups255Max. number of readers128Max. number of remote workstations16Max. number of I/O extension boards per AMC1VideoMax. number of cameras128 Identification camera1/entrance Surveillance cameras up to 4/entranceBack surveillance2/entranceFront surveillance2/entranceAlarm and logbook camera1/entranceOffline Locking System (OLS) [selected markets, only]Max. number of entrances1,000Time models15Periods/ time model4Special days10Ordering InformationAccess PE - Basic License1 Client, 16 Readers, 2,000 CardsASL-APE2P-BASEAccess PE - Extended License2 Clients, 64 Readers, 10,000 CardsASL-APE2P-BEXTAccess PE - Reader Expansion LicenseAdditional 16 readers – highest limit per sys-tem: 128 readersASL-APE2P-RDRAccess PE - Client Expansion LicenseOne additional client – highest limit per sys-tem: 16 clientsASL-APE2P-CLIAccess PE - Video Activation LicenseEnables video with 16 channelsASL-APE2P-VIDBAccess PE - Video Expansion LicenseAdditional 16 channels – highest limit per sys-tem: 128 channelsASL-APE2P-VIDEAccess PE - OLS Activation LicenseEnables Offline Locking System (OLS) with 16doorsASL-APE2P-OLSBAccess PE - OLS Expansion LicenseOne additional door for the Offline LockingSystem (OLS) – highest limit per system:1,000 doorsASL-APE2P-OLSEAmericas:Bosch Security Systems, Inc. 130 Perinton Parkway Fairport, New York, 14450, USA Phone: +1 800 289 0096 Fax: +1 585 223 9180***********************.com Europe, Middle East, Africa:Bosch Security Systems B.V.P.O. Box 800025600 JB Eindhoven, The NetherlandsPhone: + 31 40 2577 284Fax: +31 40 2577 330******************************Asia-Pacific:Robert Bosch (SEA) Pte Ltd, Security Systems11 Bishan Street 21Singapore 573943Phone: +65 6258 5511Fax: +65 6571 2698*****************************Represented by© Bosch Security Systems Inc. 2010 | Data subject to change without notice T6197545611 | Cur: en-US, V9, 4 Jul 2010。
TEM+investigations+on+layered+ternary+ceramics
•ReviewTEM Investigations on Layered Ternary CeramicsZhijun LIN1,2),Meishuan LI1)and Yanchun ZHOU1)†1)Shenyang National Laboratory for Materials Science,Institute of Metal Research,Chinese Academy of Sciences,Shenyang110016,China2)Graduate School of Chinese Academy of Sciences,Beijing100039,China[Manuscript received October23,2006]Layered ternary ceramics represent a new class of solids that combine the merits of both metals and ceramics.These unique properties are strongly related to their layered crystal structures and microstructures.The com-bination of atomic-resolution Z-contrast scanning transmission electron microscopy(STEM)and transmission electron microscopy(TEM),selected area electron diffraction(SAED),convergent beam electron diffraction (CBED)represents a powerful method to link microstructures of materials to macroscopic properties,al-lowing layered ternary ceramics to be investigated in an unprecedented detail.Microstructural information obtained using TEM is useful in understanding the formation mechanism,layered stacking characteristics,and defect structures for layered ternary ceramics down to atomic-scale level;and thus provides insight into under-standing the“Processing-Structure-Property”relationship of layered ternary ceramics.Transmission electron microscopic characterizations of layered ternary ceramics in Ti-Si-C,Ti-Al-C,Cr-Al-C,Zr-Al-C,Ta-Al-C and Ti-Al-N systems are reviewed.KEY WORDS:Layered ternary ceramics;MAX phase;TEM;STEM;Interfacial structure1.IntroductionIn1960s,Nowotny and co-workers[1–4]madefirst attempts on the exploration of a large group of car-bides and nitrides.They embarked on the investiga-tions of ternary carbides and nitrides including the H¨a gg or H–phases.A large number of ternary com-pounds were identified during that decade.Thirty years later,Barsoum[5]published a detailed review on a new class of solids called M n+1AX n phases(M is an early transition metal;A is an A-group element (mostly IIIA and IVA)and X is either C and/or N, n=1,2,or3).The MAX phases are described as thermodynamically stable nanolaminates,which are elastically stiff,electrically and thermally conductive, readily machinable,relatively soft,damage tolerant and thermal-shock resistant.Over the past decade, exciting progresses have been made in the synthesis, microstructure,property,and design of M n+1AX n phases.In the present review,we extend the do-main of M n+1AX n phases to layered ternary ceramics and highlight the microstructural characterizations of layered ternary ceramics using various transmission electron microscopy(TEM)techniques.Concrete ex-amples rather than generalized descriptions will be given in this paper.We hope that this approach will help the readers understand both the basic TEM con-cepts and ideas on investigations of layered ternary ceramics.This paper is structured as follows:the first section contains a brief introduction of layered ternary ceramics,together with a concise description of several TEM techniques including selected area electron diffraction(SAED),convergent beam elec-tron diffraction(CBED),high-resolution transmis-sion electron microscopy(HRTEM),scanning trans-mission electron microscopy(STEM),and electron energy loss spectroscopy(EELS).Section two deals with atomic-scale characterizations of layered ternary †Prof.,Ph.D.,to whom correspondence should be addressed, E-mail:yczhou@.ceramics using SAED,CBED,HRTEM,and STEM. The third section summarizes investigations on the formation mechanism of layered ternary ceramics mainly by SAED,HRTEM,and Z-contrast STEM. Finally,conclusions on microstructural characteriza-tions of layered ternary ceramics using TEM tech-niques are drawn and some future trends in thisfield are highlighted in the last section.1.1Introduction of layered ternary ceramicsLayered ternary ceramics represent an unusual family of compounds that combine both the mer-its of metals and ceramics.These ceramics cover M n+1AX n phases[5],layered ternary carbides in the T(T=Sc,Zr,Hf,U)-Al-C[6–20],and A(A=Al,Sc, Lu,Gd)-B-C[21–28]systems.The crystal structures of the M n+1AX n phases(M2AX,M3AX2,M4AX3), T2Al3C4,and A3BC3are displayed in Fig.1[1–5,7,10,25]. The crystal structures of M n+1AX n phases consist of two fundamental units,i.e.,the nonstoichiometric MX x unit and A atomic plane.The most pronounced difference between the crystal structures shown in Figs.1(a–c)is the number of M-layers within every two A-layers,i.e.,there are two,three,and four M-layers within every two A-layers in M2AX,M3AX2, M4AX3,respectively.Ternary T-Al-C compounds can be viewed as the intergrown structures consisting of two kinds of layers.One is the(T-C)m(m=1,2or 3)slab in the NaCl-type structure and the other con-sists of Al3C2unit in an arrangement similar to that of the binary aluminum carbide Al4C3[6,8].A-B-C com-pounds,on the other hand,generally contain a linear C-B-C unit,which plays an important role in deter-mining their mechanical performance[21–25].Owing to the unique crystal structures,layered ternary ceram-ics display advantageous attributes such as high mod-ulus,excellent thermal-shock and high-temperature oxidation resistance,and damage tolerance.Ti3SiC2[29–69],Ti3AlC2[67–82],and Ti2AlC[80–100] are representative layered ternary ceramics,which have been extensively investigated.To conserve space,Fig.1Crystal structures for:(a)M2AX,(b)M3AX2,(c)M4AX3,(d)T2Al3C4,(e)A3BC3[1–5,7,10,25]Table1Typical physical,mechanical,and chemical properties for Ti3AlC2,Ti2AlC,and TiC Compound Crystal Lattice Density Vickers Coefficient ofstructure parameters/nm/(g/cm3)hardness/GPa thermal expansion/K−1Ti3AlC2[5,71–73]Hexagonal a=0.3075, 4.25∼3.59.0×10−6(P63/mmc)c=1.8578Ti2AlC[5,83–86]Hexagonal a=0.3040, 4.11 2.8–48.2×10−6(P63/mmc)c=1.3600TiC[101]Cubic(F m¯3m)a=0.4332 4.9428.5–33.57.9×10−6 Compound Electrical Young s Shear Compressive Bending Oxidation Machinability conductivity modulus modulus strength strength resistance in air/Ω−1·m−1/GPa/GPa/MPa/MPaTi3AlC2[5,71–73]2.9×106,3.5×106297124764375Excellent up to1300◦C Excellent Ti2AlC[5,83–86] 4.4×106270116540275Excellent TiC[101] 1.4×106310–439751–1309220–690Severe(T≥1100◦C)PoorFig.2(a)Brightfield TEM image of the oxide scales formed on a Ti3AlC2substrate.The inner oxide scale is an Al2O3scale while the outer scale is a discontinuous TiO2layer,(b)and(c)composite SAED patterns taken at the Ti3AlC2/Al2O3interfaces.“α”and“H”denoteα-Al2O3and hexagonal Ti3AlC2[77],respectivelyonly a brief description of the research work on the Ti-Al-C system will be introduced here.Jeitschko et al.[2]identified Ti2AlC in the1960s while Pietzka and Schuster[70]first reported Ti3AlC2in1994.By incorporating Al into TiC,layered ternary Ti3AlC2 and Ti2AlC ceramics can be prepared.Table1 summarizes some fundamental properties of Ti3AlC2, Ti2AlC,and TiC[5,71–73,83–86,101].The most salient features for layered ternary Ti-Al-C compounds over binary TiC compound are the machinability,damage tolerance,and high-temperature oxidation resistance. Difficult machinability hinders the extensive applica-tions of traditional ceramics such as SiC and Al2O3. Ternary Ti-Al-C ceramics,on the other hand,can be easily machined using high-speed tool bits with-out lubrication or cooling.The easy machinability and damage tolerance originate from their low shear strength[91].The oxidation resistance of TiAl is not satisfying because no protective Al2O3scale forms during high-temperature oxidation process[102–105].However,it is interesting and surprising that,with much lower Al content,protectively continuous Al2O3scales form on Ti3AlC2and Ti2AlC surfaces during high tem-perature oxidation in air,which were identified us-ing scanning electron microscopes[73,86,90].A typical cross-sectional TEM image of a Ti3AlC2specimen ox-idized at1200◦C for2h is shown in Fig.2(a)[77].The scale is approximately3µm in thickness.The com-pacted scales are well bonded to the substrate.SAED analyses(not shown)indicate that the outermost ox-ide layer is discontinuous TiO2while the inner ox-ide layer is an intact Al2O3layer,which is in good agreement with previous SEM results[73,86,90].More-over,Ti3AlC2substrate and the Al2O3oxide scale satisfy the following two sets of orientation relation-ships(ORs)[77]:(0001)Ti3AlC2//(0001)Al2O3and[11¯20]Ti3AlC2//[¯12¯10]Al2O3(OR−1)(1)(0001)Ti3AlC2//(0001)Al2O3and[11¯20]Ti3AlC2//[1¯100]Al2O3(OR−2)(2) In addition,the measured adhesive strength of Ti3AlC2/Al2O3interface exceeds85MPa[82],which is generally higher than those between other ox-ide scales and corresponding underlying alloys substrates[106–108].The strong adhesion contributes to the good thermal cyclic stability of the oxide scales.It is reasonable that the compacted Al2O3 scale can efficiently protect the Ti3AlC2substrate and accounts for the excellent high-temperature oxidation resistance[73].Conversely,Barsoum et al.[80]claimed that the oxidation resistance of Ti3AlC2and Ti2AlC was not good because a mixed and non-protective ox-ide scale formed during the oxidation process.Their results should be interpreted with care.In the later work,Sundberg et al.[90]reported that the oxida-tion resistance of Ti2AlC was excellent and claimed that the results were consistent with those reported by Zhou and Wang[86].Wefind that the presence of impurities,such as TiC and TiAl,greatly dete-riorates the oxidation resistance of ternary Ti-Al-C ceramics.So microstructure,especially phase compo-sitions should be examined prior to oxidation tests. The exceptional properties of bulk Ti-Al-C ceramics stimulated and promoted the research work on thin films[81].Moreover,inspired by the success in Ti-Al-C system,attempts have been made to explore new material systems with desired properties in the Ti-Si(Al)-C[67–69],Ti-Al-N[109–114],Cr-Al-C[115–120],Ta-Al-C[121–125],Zr-Al-C[10–12,18–20],and Al-B-C[25–26] systems.1.2Brief introduction of several TEM techniquesBefore delving in the details of microstructural characterizations of layered ternary ceramics,it is instructive to have a basic understanding of several TEM techniques.TEM is one of the most power-ful and widely used analytical tools for characteriz-ing microstructures of materials.TEM greatly puts forward our understanding of materials by complet-ing the processing-structure-property links down to atomistic levels.It is now even possible to tailor the microstructure(and mesostructure)of materials to achieve specific sets of properties;the extraordi-nary abilities of modern TEM instruments provid-ing almost all of the structural,phase,and crystallo-graphic information allow us to accomplish this feat.A very complete and easily understanding textbook on TEM,written by Williams and Carter[126],cov-ersfields ranging from specimen preparation,imaging, and diffraction to spectroscopy.Spence[127]reviewed thefield of atomic-resolution transmission electron microscopy and its application to materials science.A recent sensible and tasteful review on STEM is avail-able in the publication by Varela et al.[128].1.2.1Selected-area electron diffraction and convergent-beam electron diffraction Diffraction patterns are the basis of all image formation in TEM, as well as all crystallographic analyses and defect characterizations.The SAED method for selecting an area is to place an aperture in thefirst image plane below the objective lens and then a pattern of sharp spots(or rings)is observed in the back fo-cal plane of the objective lens.In contrast,in the CBED technique,an incident convergent beam(in the range of0.1-0.5◦)is focused on the specimen and gives rise to a pattern with disks of intensity.The CBED pattern of disk contains a wealth of contrast detail,which is not presented in the sharp spots of SAED pattern.Besides the capability of more pre-cisely determining the lattice parameters of materials than the SAED method,CBED is a powerful tool to determine the point group,space group,and crys-tal system of various materials because the presence of inversion center,glide plane and screw axis can be experimentally distinguished[129].Literature[126] gave an overview of these two diffraction techniques. In the second section,a case on the determination of space group of ternary Zr-Al-C carbides by using SAED and CBED techniques will be presented.1.2.2High-resolution transmission electron mi-croscopy HRTEM is thefirst TEM technique, which is capable of atomic resolution observations. This method has been proved to be indispensable in determining microstructures of materials.Phase-contrast HRTEM uses a coherent imaging technique, and suffers from the fact that data cannot be directlyinverted to retrieve structural information.HRTEMimages are generally not directly interpretable due to the complex nature of the coherent imaging process. In addition,the ability to extract compositional infor-mation from HRTEM images is limited.That is,the major disadvantage of HRTEM is that the obtained image does not necessarily relate to the structure in a simple manner.Image contrast is a complicated function of focus and specimen thickness,even in an aberration-corrected TEM,which means that there is no unique image that gives the best view of the structure.Thus,it is particularly difficult to inves-tigate samples or defects with an unknown structure or composition,which are of course the most interest-ing.One of the most notable advancements over the past decade is the development of quantitative meth-ods to interpret phase-contrast HRTEM images such that atomic coordinates at defects can be quantita-tively determined[130,131].The most widely used indi-rect method for correlating the image intensity in an HRTEM image with the projected crystal structure (especially for defect structures such as interfaces) is the multislice image simulation procedure,which takes into account dynamical scattering effects.De-spite recent advances in quantitative HRTEM utiliz-ing large series of defocused images and/or extensive computation(e.g.see literature[126]),any composi-tional information obtained using HRTEM will always be indirect.However,HRTEM remains a valuable complement to the associated TEM-based analytical techniques.The second major electron imaging ad-vancement is high-angle annular darkfield(HAADF) STEM,in which incoherent atomic-scale images can be formed with a chemical sensitivity.1.2.3High angle annular darkfield or Z-contrast imaging There has been considerable interest in atomic resolution Z-contrast imaging(or HAADF imaging)over the last few years,particularly in its applications to interfaces[132]and other extended defects[133–135].Z-contrast imaging uses a small,con-vergent probe(<0.2nm in diameter)of afield emis-sion gun(FEG)in an STEM system and an annu-lar detector with a large inner radius,as shown in Fig.3.Z-contrast imaging removes coherent effects, and thus the imaging is incoherent.Consequently,the images are directly interpretable and are not subject to contrast reversals due to focus and/or thickness changes as that in HRTEM.This technique is there-fore gaining increasing popularity.Figure3presents another important aspect of the STEM-based tech-nique,EELS,which can be performed simultaneously at a high spatial resolution,thus allowing direct cor-relation between structure and chemistry at the sub-nanometer or even atomic length scale,as discussed further in detail.Because the detected signal is in-coherent using this technique,the intensity in a Z-contrast image,I(R),is given by the convolution of the incident probe intensity function,|P(R)|2,with the crystal object function,O(R):I(R)=|P(R)|2⊗O(R)(3) Even under dynamical diffraction conditions,it has been shown that s-type Bloch states,which are tightly bound to individual atomic columns,are pre-dominantly responsible for the image intensityunder Fig.3Schematic illustration of simultaneous Z-contrast and EELS in an STEM system[135]zone-axis imaging conditions[136].Consequently,the object function is localized on atomic columns.It should also be noted that the Rutherford scattering cross-sections to high angles are much greater for ele-ments with higher atomic number(Z),so that the intensity of a Z-contrast image scales with atomic number,produces peaks of intensity at the cation sites while yields almost no intensity at low-Z col-umn positions[137].Moreover,in the limit of Ruther-ford scattering,this goes as Z2,so the contrast in a Z-contrast image will also vary approximately as Z2. The exact contrast details depend on the experimen-tal set up and are affected by factors such as electron channeling or detector size.But over a fairly large ranges of defocus or sample thicknesses,the image will nonetheless represent the sample structure in a straightforward way.1.2.4X-ray energy dispersive spectroscopy (XEDS)XEDS is one of the most convenient and effective microscopically analytical techniques. Acquisition of the characteristic X-rays emitted by materials when illuminated by the electron beam provides a direct,quantitative measure of chemical compositions.XEDS has been the most extensively used technique for measuring segregation,starting with the pioneering studies of Doig and Flewitt[138], who demonstrated that monolayer-level segregation was detectable in thin foils.Today,with an FEG-STEM,the spatial resolution can be less than2nm and segregation can be quantified with a sensitiv-ity approaching0.01monolayer[139].A common ap-proach is to acquire a segregation profile by stepping the electron probe along a line perpendicular to theFig.4XEDS line-scanning plot of Ti across two Al2O3 grains with corresponding HAADF image shownin the inset[82]segregation area.Figure4shows an example of a plot of Ti segregation to the grain boundary within an Al2O3oxide scale,where the enhanced Ti level (about3-5nm in thickness)at the grain boundary is clearly observed with increasing signals across the boundary[82].Recent optimization of instruments has allowed the acquisition of compositional maps at a high spatial resolution(<2nm)and high sensitivity (<0.1monolayer)[140].Due to the fact that XEDS only detects∼1%X-ray,the signal is quite weak,es-pecially for the light elements.Secondly,the energy resolution of XEDS is about130eV,which is rela-tively high,and the light elements have serious over-lapping spectra.The XEDS detector is located as close as possi-ble to specimen.Regular holders have the additional disadvantage that the holder area around the speci-men is“deep”,which hinders the acquisition of signal. Thus,it is very difficult to exclude spurious X-rays, which are generated outside the area of interest,be-cause of the proximity of the detector.In order to reduce these X-rays,a proper low-background speci-men holder is strongly recommended.The situation is essential especially when quantitative analyses are carried out.1.2.5Electron energy loss spectroscopy (EELS)EELS is another TEM technique for microanalysis of materials.This method is signifi-cantly more appropriate for analyses of light elements (Z<11),as well as many transition metal and rare earth elements.A larger proportion of the inner-shell excitations can be recorded by an EELS spec-trometer than an XEDS detector.Most often the core-loss region of the EEL spectrum,corresponding to inner shell ionizations,is analyzed to obtain an insight into the chemical composition and electronic structure of materials[141–143].Compositional pro-files across the planar boundary can be performed to identify the presence of reaction phases and to determine the chemical width of an interface.Typ-ically,the compositional accuracy is in the order of5-10wt pct.The spatial resolution can be sub-nanometer when performed with a focused electron probe in an FEG-TEM.In fact,in an STEM system under channeling conditions,spectra can be obtained at an atomic resolution directly from the interface plane and specific atomic columns[144,145].Thus,it is particularly useful because EELS can provide ele-mental and electronic structure information down to the atomic length scale within an STEM.The ioniza-tion edge onsets and EELS near-edgefine structures (ELNES),which include information about the un-occupied density of states,are sensitive to the local coordination and electronic structure.The ELNES for many elements exhibits a shape characteristic of the valence and bond strength of atom.Detailed descriptions on this technique can be referenced to literature[128,146,147].2.Atomic Scale Microstructures of LayeredTernary CeramicsAll the specimens for TEM investigations in this paper were prepared using conventional methods,i.e., by slicing,gluing the specimen face to face(for cross-sectional specimens only),grinding,dimpling,andfi-nally ion milling to electron transparent.TEM ob-servations were performed using a200kV JEM-2010 TEM(JEOL,Japan)and a300kV Tecnai G2F30 TEM(FEI company,Netherland),which is equipped with an energy dispersive spectroscopic system,a high angle annular darkfield detector in an STEM system, and a post column EELS system.2.1Determination of space group using SAED andCBEDElectron diffraction is the basis of all TEM ing SAED analysis,Arunajatesan and Carim[32]firstly investigated the symmetry of Ti3SiC2.Morgiel et al.[35]investigated the mi-crostructures of Ti3SiC2-based ceramics.Rounded TiC and angular SiC inclusions,as well as TiSi2phase were identified.Farber et al.[51]determined the Burg-ers vector of dislocations in Ti3SiC2in tilting exper-iments.Thereafter,SAED plays an increasing role in determining the crystal structure,lattice param-eters,defect structure,and crystallographic orien-tations of layered ternary compounds.The CBED method,however,is less employed due to the difficul-ties in analyzing the experimental results.All crystal structures can be specified by a set of Bravais lattice vector( R)and a set of vectors describ-ing the positions of the basis atoms( r j)[148].In prac-tice,however,the number of basis atoms can be quite large and simply listing them is cumbersome.Space group is a simple and efficient way to overcome these difficulties.By acknowledging the symmetry of the atomic configuration,it is usually possible to distill the description of the basis down to a small number of parameters.Consequently,crystal structure data are always presented with reference to the space group or underlying symmetry of the structure.It is,there-fore,important to understand the space group of a crystal.X-ray diffraction(XRD)is usually used to deter-mine the space group of materials.However,XRD results may be misinterpreted when dealing with ma-terials containing impurities or defects because the spot size of an X-ray diffractometer is relatively large (typically at micrometer scale).At this point,TEM displays its advantage on microstructual domain anal-ysis since the spot size of a convergent electron beam can easily reach nanometer scale.Thefirst attemptFig.5SAED patterns of hexagonal ZrAl 3C 5with the electron beam parallel to the directions of [0001](a),[1¯210](b)and [1¯100](c),respectively,an SAED pattern with the orientation being positioned between [1¯210]and [1¯100](d),a CBED pattern showing the symmetry of a 6-fold rotation about the [0001]axis and also the symmetry of the mirror reflection across two independent planes (e),a CBED pattern showing the existence of a mirror plane on (0001)(f)[10]to investigate the space group of layered ternary ce-ramics using TEM was made by Arunajatesan and Carim [32].They reported the point group of Ti 3SiC 2as 6/mmm .Ma et al.[76]systematically investigated microstructures of Ti 3AlC 2and determined the space group of this compound as P63/mmc by combining SAED and CBED.They also illustrated the determi-nation of an impurity,TiAl 3,using SAED and CBED.Following the scheme of Ma et al.[76],the present authors clarified the space group of Zr 2Al 3C 4and Zr 3Al 3C 5.Using XRD analysis,the space group of Zr 2Al 3C 4was reported to be P 31c (C 43v )by Schuster andNowotny [7],P 63/mmc by Parth´e and Chabot [13],and P 63mc by Fukuda et al.[8].Similarly,Zr 3Al 3C 5was determined to have P 63/mmc [7,14]and P 63mc symmetry [6].Therefore,it is necessary to clarify the symmetry of both carbides.Figure 5(a–c)are SAED patterns which were indexed as [0001],[1¯210],and [1¯100]zone axes,respectively,of the hexagonal Zr 3Al 3C 5[10].From these patterns of low-indices ba-sic zone axes,the lattice parameters are derived as a =0.33nm and c =2.76nm,which are consistent with those determined from powder X-ray analyses [6,7,14].These SAED patterns are also informative for learn-ing extinction rules.It is noted that all reflections in the [1¯210]pattern appear,but the (000l )(l =odd)reflections in the [1¯100]pattern are absent,imply-ing the existence of a c glide plane.The appearance of the {000l }(l =odd)reflections in the [1¯210]pat-tern can be attributed to double diffraction [76,96,149].Figure 5(d)is an SAED pattern whose orientation ispositioned between [1¯210]and [1¯100].As shown in Fig.5(d),the (000l )reflections with l =odd are also absent,which indicates that there is a 63screw axis along the [0001]axis [76,96].Figure 5(e)is a CBED pattern,which was acquired from a Zr 3Al 3C 5grain along the [0001]zone axis.A 6-fold axis of rotational symmetry as well as two independent and mutually perpendicular mirror planes (each of them is repro-duced every 60◦by the action of the 6-fold axis)is observed.These two types of mirror planes are par-allel to the 6-fold axis.The symmetry is determined to be 6mm .In addition,the symmetry shown in the SAED [1¯210]pattern (Fig.5(b))is 2mm .A 6mm symmetry and a 2mm symmetry indicate a unique 6/mmm point group for Zr 3Al 3C 5.Figure 5(f)is a CBED pattern showing the existence of a mirror plane on (0001).A 6mm symmetry and a mirror plane on (0001)further confirm the 6/mmm point group for Zr 3Al 3C 5.A combination of the information derived from these SAED and CBED patterns indicats that Zr 3Al 3C 5has a space group P 63/mmc ,which is in good correspondence with the results of Parth´e andChabot [13].The symmetry of Zr 2Al 3C 4was also in-vestigated using SAED and CBED.The lattice pa-rameters obtained are a =0.33nm and c =2.24nm,which agree well with previously reported data [7,14].Zr 2Al 3C 4was also determined to have a point group 6/mmm and a space group P 63/mmc ,which is in consistent with that reported by Mikhalenko et al.[14].The SAED and CBED patterns of Zr 2Al 3C 4areFig.6HRTEM image of Ti2AlC with the electron beam parallel to the[1¯210]direction[96]similar to those of Zr3Al3C5,and therefore,are not shown for brevity.More recently,wefind that the reason for the dis-crepancy in the space group determined using XRD might originate from the impurities and defects es-pecially stacking faults in the as-prepared layered ternary ceramics.In other words,XRD analyses col-lect the reflections from a relatively large area;both the impurities and defects in the specimens contribute to the XRD profile.Consequently,the results may be misinterpreted because some reflections are overlap-ping.On the other hand,TEM analysis can concen-trate on an individual grain without defects(single-crystal).Thus,the TEM results are more accu-rate at this point.The presently determined space group for Zr3Al3C5is also supported byfirst princi-ples calculations[12].2.2HRTEM investigations of layered ternary ceramicsHRTEM is a conventional and useful method in exploring the microstructural features of materials. This technique enables the investigations of ceram-ics with an atomic scale resolution.The most recent major discovery was the observation and synthesis of bucky-tubes,which resulted entirely from HRTEM observation[150].As far as layered ternary ceramics are concerned,HRTEM is a useful tool to character-ize both layered stacking characteristics and interfa-cial microstructures.The layered stacking characteristics of most lay-ered ternary ceramics(hexagonal structure)can be observed in an HRTEM image when viewed along the[1¯210]direction.Experimental HRTEM image of Ti2AlC,with the electron beam parallel to this zone axis,is displayed in Fig.6[96].As mentioned above, HRTEM imaging is sensitive to experimental param-eters.So,image simulations of the Ti2AlC crystal structure were performed using the Cerius2software (Molecular Simulation Inc.,USA)in a wide range of defocus and thickness permutations.Simulations show that there is one-to-one correspondence between the Ti and Al atomic columns and the bright spots in the image.This allows the interpretation of stacking sequence through image contrast.The image fringes with a periodicity of1.36nm along[0001]direction can be seen.The C atoms cannot be resolved in our microscopes.Taking Ti and Al into account,the im-ages can be described as a layered stacking with the sequence of ABABAB(the underlined letters denote the Al layers and the remained letters represent Ti layers)along[0001]direction.This type of stacking sequence for Ti and Al atoms is consistent with pre-vious results,which were derived from powder XRD analyses[1].There are cases that bright spots in HRTEM im-ages do not correspond to atomic columns.For ex-ample,Farber et al.[52]observed different stacking characteristics for Ti3SiC2in an HRTEM image and concluded that polymorphic transformation occurred during the ion-milling process.On the other hand, Yu et al.[42]reported that bright spots in HRTEM images did not correspond to the atomic columns. By combining image simulations and HRTEM imag-ing,they also identified two polymorphs,i.e.,α-and β-Ti3SiC2and claimed that theα-phase was more stable.The subsequent theoretical investigations us-ingfirst principles calculations are noteworthy[41]. The phase transition path fromα-toβ-Ti3SiC2was clearly illustrated,and the lattice dynamic of these two polymorphs was investigated.Theoretical calcu-lations revealed thatα-Ti3SiC2is more stable than theβ-phase.HRTEM imaging is also effective in under-standing the interfacial structure of layered ternary ing this method,the interfacial structures of Ti3SiC2/TiC[39,44–46,58],Ti5Si3/TiC[44], Ti3AlC2/Al2O3[77],Ti3AlC2/TiC[76,81], Ti2AlC/TiAl[96],and Ti2AlC/TiC[81,96]were investi-gated.The following shows an example of character-izing the Ta2AlC/TaC interface[124].XEDS anal-ysis shows that minor amount of cubic TaC was occasionally observed in Ta2AlC.In order to de-termine the crystallographic relationship between these two carbides,high-resolution imaging was conducted.Figure7(a)shows an HRTEM im-age of the interfacial structure between Ta2AlC and TaC[124].It is seen that TaC forms a coher-ent interface with Ta2AlC and the crystallographic orientation relationship between TaC and Ta2AlC can be described as:(111)TaC//(0001)Ta2AlC and [1¯10]TaC//[1¯210]Ta2AlC.In order to better un-derstand the structural relationship between TaC and Ta2AlC,an interfacial structural model based on the observed orientation relationship is pro-posed and shown in Fig.7(b).The Ta-C units of Ta2AlC are locally the same as those of TaC, which ensures a coherent interfacial structure be-tween TaC and bining the orien-tation relationships between binary cubic car-bides and layered ternary carbides identified in the Ti-Si-C and Ti-Al-C systems[44–46,76,81,89,96], a generalized orientation relationship between binary cubic MX carbides/nitrides and lay-ered ternary M x A y X z-phases carbides/nitrides is proposed as:[1¯10]MX//[1¯210]M x A y X z and (111)MX//(0001)M x A y X z(where M is an early transition metal element;A is a IIIA and IV group element;X is carbon or nitrogen,and x,y,z are。
市场调查方法(英文版)第十五章
15–14
EXHIBIT 15.2 Independent Samples t-Test Results
© 2007 Thomson/South-Western. All rights reserved.
15–15
What Is ANOVA?
• Analysis of Variance (ANOVA)
➢ An analysis involving the investigation of the effects of one treatment variable on an interval-scaled dependent variable
➢ A hypothesis-testing technique to determine whether statistically significant differences in means occur between two or more groups.
❖ Behavior, characteristics, beliefs, opinions, emotions, or attitudes
• Bivariate Tests of Differences
➢ Involve only two variables: a variable that acts like a dependent variable and a variable that acts as a classification variable.
❖ Differences in mean scores between groups or in comparing how two groups’ scores are distributed across possible response categories.
单壁碳纳米管储氢的统计理论模型
单壁碳纳米管储氢的统计理论模型张帆【摘要】Hydrogen energy is an environmentally friendly and renewable energy source. The development and application of hydrogen energy will bring great changes for the structure of energy sources from the long view. Carbon nanotubes were reported to be very promising materials for storing hydrogen form some research finding, which has been a hot spot in the applied research field of studying nano materials. Although many experimental results for hydrogen storage in carbon nanotubes were reported, corresponding theoretical investigation of adsorption mechanisms have almost not developed and it is difficult to find the theoretical equation of hydrogen storage quantity in particular. In this paper, statistical theory model on the basis of interaction between hydrogen molecules and carbon atoms was presented, and the formula of hydrogen storage quantity was obtained, which is almost in agree with the experiment value. The conclusion can provide theoretical reference for studying hydrogen storage in carbon nanotubes.%氢能是一种洁净的可再生的能源,从长远的观点看,氢能的发展与利用能够使能源结构发生重大变化。
Understanding individual human mobility patterns
a r X i v :0806.1256v 1 [p h y s i c s .s o c -p h ] 7 J u n 2008Understanding individual human mobility patternsMarta C.Gonz´a lez,1,2C´e sar A.Hidalgo,1and Albert-L´a szl´o Barab´a si 1,2,31Center for Complex Network Research and Department of Physics and Computer Science,University of Notre Dame,Notre Dame IN 46556.2Center for Complex Network Research and Department of Physics,Biology and Computer Science,Northeastern University,Boston MA 02115.3Center for Cancer Systems Biology,Dana Farber Cancer Institute,Boston,MA 02115.(Dated:June 7,2008)Despite their importance for urban planning [1],traffic forecasting [2],and the spread of biological [3,4,5]and mobile viruses [6],our understanding of the basic laws govern-ing human motion remains limited thanks to the lack of tools to monitor the time resolved location of individuals.Here we study the trajectory of 100,000anonymized mobile phone users whose position is tracked for a six month period.We find that in contrast with the random trajectories predicted by the prevailing L´e vy flight and random walk models [7],human trajectories show a high degree of temporal and spatial regularity,each individual being characterized by a time independent characteristic length scale and a significant prob-ability to return to a few highly frequented locations.After correcting for differences in travel distances and the inherent anisotropy of each trajectory,the individual travel patterns collapse into a single spatial probability distribution,indicating that despite the diversity of their travel history,humans follow simple reproducible patterns.This inherent similarity in travel patterns could impact all phenomena driven by human mobility,from epidemic prevention to emergency response,urban planning and agent based modeling.Given the many unknown factors that influence a population’s mobility patterns,ranging from means of transportation to job and family imposed restrictions and priorities,human trajectories are often approximated with various random walk or diffusion models [7,8].Indeed,early mea-surements on albatrosses,bumblebees,deer and monkeys [9,10]and more recent ones on marine predators [11]suggested that animal trajectory is approximated by a L´e vy flight [12,13],a random walk whose step size ∆r follows a power-law distribution P (∆r )∼∆r −(1+β)with β<2.While the L´e vy statistics for some animals require further study [14],Brockmann et al.[7]generalized this finding to humans,documenting that the distribution of distances between consecutive sight-ings of nearly half-million bank notes is fat tailed.Given that money is carried by individuals, bank note dispersal is a proxy for human movement,suggesting that human trajectories are best modeled as a continuous time random walk with fat tailed displacements and waiting time dis-tributions[7].A particle following a L´e vyflight has a significant probability to travel very long distances in a single step[12,13],which appears to be consistent with human travel patterns:most of the time we travel only over short distances,between home and work,while occasionally we take longer trips.Each consecutive sightings of a bank note reflects the composite motion of two or more indi-viduals,who owned the bill between two reported sightings.Thus it is not clear if the observed distribution reflects the motion of individual users,or some hitero unknown convolution between population based heterogeneities and individual human trajectories.Contrary to bank notes,mo-bile phones are carried by the same individual during his/her daily routine,offering the best proxy to capture individual human trajectories[15,16,17,18,19].We used two data sets to explore the mobility pattern of individuals.Thefirst(D1)consists of the mobility patterns recorded over a six month period for100,000individuals selected randomly from a sample of over6million anonymized mobile phone users.Each time a user initiates or receives a call or SMS,the location of the tower routing the communication is recorded,allowing us to reconstruct the user’s time resolved trajectory(Figs.1a and b).The time between consecutive calls follows a bursty pattern[20](see Fig.S1in the SM),indicating that while most consecutive calls are placed soon after a previous call,occasionally there are long periods without any call activity.To make sure that the obtained results are not affected by the irregular call pattern,we also study a data set(D2)that captures the location of206mobile phone users,recorded every two hours for an entire week.In both datasets the spatial resolution is determined by the local density of the more than104mobile towers,registering movement only when the user moves between areas serviced by different towers.The average service area of each tower is approximately3km2 and over30%of the towers cover an area of1km2or less.To explore the statistical properties of the population’s mobility patterns we measured the dis-tance between user’s positions at consecutive calls,capturing16,264,308displacements for the D1and10,407displacements for the D2datasets.Wefind that the distribution of displacements over all users is well approximated by a truncated power-lawP(∆r)=(∆r+∆r0)−βexp(−∆r/κ),(1)withβ=1.75±0.15,∆r0=1.5km and cutoff valuesκ|D1=400km,andκ|D2=80km(Fig.1c,see the SM for statistical validation).Note that the observed scaling exponent is not far fromβB=1.59observed in Ref.[7]for bank note dispersal,suggesting that the two distributions may capture the same fundamental mechanism driving human mobility patterns.Equation(1)suggests that human motion follows a truncated L´e vyflight[7].Yet,the observed shape of P(∆r)could be explained by three distinct hypotheses:A.Each individual follows a L´e vy trajectory with jump size distribution given by(1).B.The observed distribution captures a population based heterogeneity,corresponding to the inherent differences between individuals.C.A population based heterogeneity coexists with individual L´e vy trajectories,hence(1)represents a convolution of hypothesis A and B.To distinguish between hypotheses A,B and C we calculated the radius of gyration for each user(see Methods),interpreted as the typical distance traveled by user a when observed up to time t(Fig.1b).Next,we determined the radius of gyration distribution P(r g)by calculating r g for all users in samples D1and D2,finding that they also can be approximated with a truncated power-lawP(r g)=(r g+r0g)−βr exp(−r g/κ),(2) with r0g=5.8km,βr=1.65±0.15andκ=350km(Fig.1d,see SM for statistical validation). L´e vyflights are characterized by a high degree of intrinsic heterogeneity,raising the possibility that(2)could emerge from an ensemble of identical agents,each following a L´e vy trajectory. Therefore,we determined P(r g)for an ensemble of agents following a Random Walk(RW), L´e vy-Flight(LF)or Truncated L´e vy-Flight(T LF)(Figure1d)[8,12,13].Wefind that an en-semble of L´e vy agents display a significant degree of heterogeneity in r g,yet is not sufficient to explain the truncated power law distribution P(r g)exhibited by the mobile phone users.Taken together,Figs.1c and d suggest that the difference in the range of typical mobility patterns of indi-viduals(r g)has a strong impact on the truncated L´e vy behavior seen in(1),ruling out hypothesis A.If individual trajectories are described by a LF or T LF,then the radius of gyration should increase in time as r g(t)∼t3/(2+β)[21,22]while for a RW r g(t)∼t1/2.That is,the longer we observe a user,the higher the chances that she/he will travel to areas not visited before.To check the validity of these predictions we measured the time dependence of the radius of gyration for users whose gyration radius would be considered small(r g(T)≤3km),medium(20<r g(T)≤30km)or large(r g(T)>100km)at the end of our observation period(T=6months).Theresults indicate that the time dependence of the average radius of gyration of mobile phone users is better approximated by a logarithmic increase,not only a manifestly slower dependence than the one predicted by a power law,but one that may appear similar to a saturation process(Fig.2a and Fig.S4).In Fig.2b,we have chosen users with similar asymptotic r g(T)after T=6months,and measured the jump size distribution P(∆r|r g)for each group.As the inset of Fig.2b shows,users with small r g travel mostly over small distances,whereas those with large r g tend to display a combination of many small and a few larger jump sizes.Once we rescale the distributions with r g(Fig.2b),wefind that the data collapses into a single curve,suggesting that a single jump size distribution characterizes all users,independent of their r g.This indicates that P(∆r|r g)∼r−αg F(∆r/r g),whereα≈1.2±0.1and F(x)is an r g independent function with asymptotic behavior F(x<1)∼x−αand rapidly decreasing for x≫1.Therefore the travel patterns of individual users may be approximated by a L´e vyflight up to a distance characterized by r g. Most important,however,is the fact that the individual trajectories are bounded beyond r g,thus large displacements which are the source of the distinct and anomalous nature of L´e vyflights, are statistically absent.To understand the relationship between the different exponents,we note that the measured probability distributions are related by P(∆r)= ∞0P(∆r|r g)P(r g)dr g,whichsuggests(see SM)that up to the leading order we haveβ=βr+α−1,consistent,within error bars, with the measured exponents.This indicates that the observed jump size distribution P(∆r)is in fact the convolution between the statistics of individual trajectories P(∆r g|r g)and the population heterogeneity P(r g),consistent with hypothesis C.To uncover the mechanism stabilizing r g we measured the return probability for each indi-vidual F pt(t)[22],defined as the probability that a user returns to the position where it was first observed after t hours(Fig.2c).For a two dimensional random walk F pt(t)should follow ∼1/(t ln(t)2)[22].In contrast,wefind that the return probability is characterized by several peaks at24h,48h,and72h,capturing a strong tendency of humans to return to locations they visited before,describing the recurrence and temporal periodicity inherent to human mobility[23,24].To explore if individuals return to the same location over and over,we ranked each location based on the number of times an individual was recorded in its vicinity,such that a location with L=3represents the third most visited location for the selected individual.Wefind that the probability offinding a user at a location with a given rank L is well approximated by P(L)∼1/L, independent of the number of locations visited by the user(Fig.2d).Therefore people devote mostof their time to a few locations,while spending their remaining time in5to50places,visited with diminished regularity.Therefore,the observed logarithmic saturation of r g(t)is rooted in the high degree of regularity in their daily travel patterns,captured by the high return probabilities(Fig.2b) to a few highly frequented locations(Fig.2d).An important quantity for modeling human mobility patterns is the probabilityΦa(x,y)tofind an individual a in a given position(x,y).As it is evident from Fig.1b,individuals live and travel in different regions,yet each user can be assigned to a well defined area,defined by home and workplace,where she or he can be found most of the time.We can compare the trajectories of different users by diagonalizing each trajectory’s inertia tensor,providing the probability offinding a user in a given position(see Fig.3a)in the user’s intrinsic reference frame(see SM for the details).A striking feature ofΦ(x,y)is its prominent spatial anisotropy in this intrinsic reference frame(note the different scales in Fig3a),and wefind that the larger an individual’s r g the more pronounced is this anisotropy.To quantify this effect we defined the anisotropy ratio S≡σy/σx, whereσx andσy represent the standard deviation of the trajectory measured in the user’s intrinsic reference frame(see SM).Wefind that S decreases monotonically with r g(Fig.3c),being well approximated with S∼r−ηg,forη≈0.12.Given the small value of the scaling exponent,other functional forms may offer an equally goodfit,thus mechanistic models are required to identify if this represents a true scaling law,or only a reasonable approximation to the data.To compare the trajectories of different users we remove the individual anisotropies,rescal-ing each user trajectory with its respectiveσx andσy.The rescaled˜Φ(x/σx,y/σy)distribution (Fig.3b)is similar for groups of users with considerably different r g,i.e.,after the anisotropy and the r g dependence is removed all individuals appear to follow the same universal˜Φ(˜x,˜y)prob-ability distribution.This is particularly evident in Fig.3d,where we show the cross section of ˜Φ(x/σ,0)for the three groups of users,finding that apart from the noise in the data the curves xare indistinguishable.Taken together,our results suggest that the L´e vy statistics observed in bank note measurements capture a convolution of the population heterogeneity(2)and the motion of individual users.Indi-viduals display significant regularity,as they return to a few highly frequented locations,like home or work.This regularity does not apply to the bank notes:a bill always follows the trajectory of its current owner,i.e.dollar bills diffuse,but humans do not.The fact that individual trajectories are characterized by the same r g-independent two dimen-sional probability distribution˜Φ(x/σx,y/σy)suggests that key statistical characteristics of indi-vidual trajectories are largely indistinguishable after rescaling.Therefore,our results establish the basic ingredients of realistic agent based models,requiring us to place users in number propor-tional with the population density of a given region and assign each user an r g taken from the observed P(r g)ing the predicted anisotropic rescaling,combined with the density function˜Φ(x,y),whose shape is provided as Table1in the SM,we can obtain the likelihood offinding a user in any location.Given the known correlations between spatial proximity and social links,our results could help quantify the role of space in network development and evolu-tion[25,26,27,28,29]and improve our understanding of diffusion processes[8,30].We thank D.Brockmann,T.Geisel,J.Park,S.Redner,Z.Toroczkai and P.Wang for discus-sions and comments on the manuscript.This work was supported by the James S.McDonnell Foundation21st Century Initiative in Studying Complex Systems,the National Science Founda-tion within the DDDAS(CNS-0540348),ITR(DMR-0426737)and IIS-0513650programs,and the U.S.Office of Naval Research Award N00014-07-C.Data analysis was performed on the Notre Dame Biocomplexity Cluster supported in part by NSF MRI Grant No.DBI-0420980.C.A.Hi-dalgo acknowledges support from the Kellogg Institute at Notre Dame.Supplementary Information is linked to the online version of the paper at /nature.Author Information Correspondence and requests for materials should be addressed to A.-L.B.(e-mail:alb@)[1]Horner,M.W.&O’Kelly,M.E.S Embedding economies of scale concepts for hub networks design.Journal of Transportation Geography9,255-265(2001).[2]Kitamura,R.,Chen,C.,Pendyala,R.M.&Narayaran,R.Micro-simulation of daily activity-travelpatterns for travel demand forecasting.Transportation27,25-51(2000).[3]Colizza,V.,Barrat,A.,Barth´e l´e my,M.,Valleron,A.-J.&Vespignani,A.Modeling the WorldwideSpread of Pandemic Influenza:Baseline Case and Containment Interventions.PLoS Medicine4,095-0110(2007).[4]Eubank,S.,Guclu,H.,Kumar,V.S.A.,Marathe,M.V.,Srinivasan,A.,Toroczkai,Z.&Wang,N.Controlling Epidemics in Realistic Urban Social Networks.Nature429,180(2004).[5]Hufnagel,L.,Brockmann,D.&Geisel,T.Forecast and control of epidemics in a globalized world.Proceedings of the National Academy of Sciences of the United States of America101,15124-15129 (2004).[6]Kleinberg,J.The wireless epidemic.Nature449,287-288(2007).[7] D.Brockmann,D.,Hufnagel,L.&Geisel,T.The scaling laws of human travel.Nature439,462-465(2006).[8]Havlin,S.&ben-Avraham,D.Diffusion in Disordered Media.Advances in Physics51,187-292(2002).[9]Viswanathan,G.M.,Afanasyev,V.,Buldyrev,S.V.,Murphy,E.J.,Prince,P.A.&Stanley,H.E.L´e vyFlight Search Patterns of Wandering Albatrosses.Nature381,413-415(1996).[10]Ramos-Fernandez,G.,Mateos,J.L.,Miramontes,O.,Cocho,G.,Larralde,H.&Ayala-Orozco,B.,L´e vy walk patterns in the foraging movements of spider monkeys(Ateles geoffroyi).Behavioral ecol-ogy and Sociobiology55,223-230(2004).[11]Sims D.W.et al.Scaling laws of marine predator search behaviour.Nature451,1098-1102(2008).[12]Klafter,J.,Shlesinger,M.F.&Zumofen,G.Beyond Brownian Motion.Physics Today49,33-39(1996).[13]Mantegna,R.N.&Stanley,H.E.Stochastic Process with Ultraslow Convergence to a Gaussian:TheTruncated L´e vy Flight.Physical Review Letters73,2946-2949(1994).[14]Edwards,A.M.,Phillips,R.A.,Watkins,N.W.,Freeman,M.P.,Murphy,E.J.,Afanasyev,V.,Buldyrev,S.V.,da Luz,M.G.E.,Raposo,E.P.,Stanley,H.E.&Viswanathan,G.M.Revisiting L´e vyflightsearch patterns of wandering albatrosses,bumblebees and deer.Nature449,1044-1049(2007). [15]Sohn,T.,Varshavsky,A.,LaMarca,A.,Chen,M.Y.,Choudhury,T.,Smith,I.,Consolvo,S.,High-tower,J.,Griswold,W.G.&de Lara,E.Lecture Notes in Computer Sciences:Proc.8th International Conference UbiComp2006.(Springer,Berlin,2006).[16]Onnela,J.-P.,Saram¨a ki,J.,Hyv¨o nen,J.,Szab´o,G.,Lazer,D.,Kaski,K.,Kert´e sz,K.&Barab´a si A.L.Structure and tie strengths in mobile communication networks.Proceedings of the National Academy of Sciences of the United States of America104,7332-7336(2007).[17]Gonz´a lez,M.C.&Barab´a si,plex networks:From data to models.Nature Physics3,224-225(2007).[18]Palla,G.,Barab´a si,A.-L.&Vicsek,T.Quantifying social group evolution.Nature446,664-667(2007).[19]Hidalgo C.A.&Rodriguez-Sickert C.The dynamics of a mobile phone network.Physica A387,3017-30224.[20]Barab´a si,A.-L.The origin of bursts and heavy tails in human dynamics.Nature435,207-211(2005).[21]Hughes,B.D.Random Walks and Random Environments.(Oxford University Press,USA,1995).[22]Redner,S.A Guide to First-Passage Processes.(Cambridge University Press,UK,2001).[23]Schlich,R.&Axhausen,K.W.Habitual travel behaviour:Evidence from a six-week travel diary.Transportation30,13-36(2003).[24]Eagle,N.&Pentland,A.Eigenbehaviours:Identifying Structure in Routine.submitted to BehavioralEcology and Sociobiology(2007).[25]Yook,S.-H.,Jeong,H.&Barab´a si A.L.Modeling the Internet’s large-scale topology.Proceedings ofthe Nat’l Academy of Sciences99,13382-13386(2002).[26]Caldarelli,G.Scale-Free Networks:Complex Webs in Nature and Technology.(Oxford UniversityPress,USA,2007).[27]Dorogovtsev,S.N.&Mendes,J.F.F.Evolution of Networks:From Biological Nets to the Internet andWWW.(Oxford University Press,USA,2003).[28]Song C.M.,Havlin S.&Makse H.A.Self-similarity of complex networks.Nature433,392-395(2005).[29]Gonz´a lez,M.C.,Lind,P.G.&Herrmann,H.J.A system of mobile agents to model social networks.Physical Review Letters96,088702(2006).[30]Cecconi,F.,Marsili,M.,Banavar,J.R.&Maritan,A.Diffusion,peer pressure,and tailed distributions.Physical Review Letters89,088102(2002).FIG.1:Basic human mobility patterns.a,Week-long trajectory of40mobile phone users indicate that most individuals travel only over short distances,but a few regularly move over hundreds of kilometers. Panel b,displays the detailed trajectory of a single user.The different phone towers are shown as green dots,and the V oronoi lattice in grey marks the approximate reception area of each tower.The dataset studied by us records only the identity of the closest tower to a mobile user,thus we can not identify the position of a user within a V oronoi cell.The trajectory of the user shown in b is constructed from186 two hourly reports,during which the user visited a total of12different locations(tower vicinities).Among these,the user is found96and67occasions in the two most preferred locations,the frequency of visits for each location being shown as a vertical bar.The circle represents the radius of gyration centered in the trajectory’s center of mass.c,Probability density function P(∆r)of travel distances obtained for the two studied datasets D1and D2.The solid line indicates a truncated power law whose parameters are provided in the text(see Eq.1).d,The distribution P(r g)of the radius of gyration measured for the users, where r g(T)was measured after T=6months of observation.The solid line represent a similar truncated power lawfit(see Eq.2).The dotted,dashed and dot-dashed curves show P(r g)obtained from the standard null models(RW,LF and T LF),where for the T LF we used the same step size distribution as the onemeasured for the mobile phone users.FIG.2:The bounded nature of human trajectories.a,Radius of gyration, r g(t) vs time for mobile phone users separated in three groups according to theirfinal r g(T),where T=6months.The black curves correspond to the analytical predictions for the random walk models,increasing in time as r g(t) |LF,T LF∼t3/2+β(solid),and r g(t) |RW∼t0.5(dotted).The dashed curves corresponding to a logarithmicfit of the form A+B ln(t),where A and B depend on r g.b,Probability density function of individual travel distances P(∆r|r g)for users with r g=4,10,40,100and200km.As the inset shows,each group displays a quite different P(∆r|r g)distribution.After rescaling the distance and the distribution with r g(main panel),the different curves collapse.The solid line(power law)is shown as a guide to the eye.c,Return probability distribution,F pt(t).The prominent peaks capture the tendency of humans to regularly return to the locations they visited before,in contrast with the smooth asymptotic behavior∼1/(t ln(t)2)(solid line)predicted for random walks.d,A Zipf plot showing the frequency of visiting different locations.The symbols correspond to users that have been observed to visit n L=5,10,30,and50different locations.Denoting with(L)the rank of the location listed in the order of the visit frequency,the data is well approximated by R(L)∼L−1. The inset is the same plot in linear scale,illustrating that40%of the time individuals are found at theirfirsttwo preferred locations.FIG.3:The shape of human trajectories.a,The probability density functionΦ(x,y)offinding a mobile phone user in a location(x,y)in the user’s intrinsic reference frame(see SM for details).The three plots, from left to right,were generated for10,000users with:r g≤3,20<r g≤30and r g>100km.The trajectories become more anisotropic as r g increases.b,After scaling each position withσx andσy theresulting˜Φ(x/σx,y/σy)has approximately the same shape for each group.c,The change in the shape of Φ(x,y)can be quantified calculating the isotropy ratio S≡σy/σx as a function of r g,which decreases as S∼r−0.12(solid line).Error bars represent the standard error.d,˜Φ(x/σx,0)representing the x-axis cross gsection of the rescaled distribution˜Φ(x/σx,y/σy)shown in b.。
EFECTIS发布新版建筑构件检测标准
为0.995,其中:Ts 为60 m in 后电热膜与棉被接触处的温 度,7\为环境温度。
可以认为,在汗蒸房、足浴房等环境温 度较高的场所,电热膜具有的引燃能力也较强。
进行火灾 原因调查时,可以利用该模型计算方法,模拟火场条件,初 步计算并判断电热膜引燃其周围可燃物的可能性。
4总结(1) 电热膜的引燃能力随着功率的增加而变强,当覆盖 物为棉被,试样功率为160 W 时,电热膜与棉被接触处最高 温度高于一般的可燃物的燃点;小于100 W 时,引燃能力较 差。
毛巾作为覆盖物时,所能达到的最高温度比棉被低 201左右。
(2)电热膜表面覆盖物的厚度越大,电热膜与覆盖物接触处温度越高,可燃物越容易被引燃。
毛巾作为覆盖物时, 若其厚度较低,其危险性比棉被低,而厚度较高时,与棉被 相当。
(3) 覆盖物所含水分会降低电热膜的引燃能力,含水率越高,电热膜的引燃能力越差。
(4)建立了模拟电热膜、覆盖物传热的物理模型,通过 与实验结果对比,验证了该模型的准确性。
参考文献:[1] 张洪识,治俭.低温辐射电热膜行业及市场发展研究概况[c ]//全国红外加热发展研讨会论文集,2015.[2] 周晓佳.汗蒸类场所电气火灾特点及预防对策分析[J].建筑安全,2017,32(6):61-63.[3] 赵荣华.低温辐射电热膜供暖系统作:住宅建筑中的利用[J ].科技与企业,2014,(14):191.[4] 胡明葸.碘钨灯引燃能力的实验研究与ANSYS 软件分析[J ].消防技术与产品信息,2017,(10):23_27.[5] 金静,张金专.碘钨灯引燃能力实验研究[J].消防科学与技术,2016,35(4):587-590.[6] 马迪,张金专.电暖器对毛毯和报纸的引燃能力研究[J ].武膂学院学报,2016,35(5):717—720.[7] 任松发,姜英.红外线式电暖器热辐射引起火灾的研究[J ].武膂学院学报,2000,16(1):40-43.[8] 杜宝相.一起电热膜汗蒸房火灾的认定[J].消防科学与技术,2014,33(1):114-116.[9] 马瑛.汗蒸养生房的电气防火[J].消防技术与产品信息,2013,(3):12-13.[10] 孙宁•.汗蒸房电热膜及电气线路故障起火原W 认定[J ].消防科学与技术,2014,33(8):975-977.[11] 张斌,鲁志宝,陈克,等.电热膜火灾危险性分析[.I].消防科学》彳技术,2018,37(6):851-854.[12] LU P B,CHENG F ,()U Y Y\,et al.A flexible and transparentthin film heater based on a carbon fiber/heat-resistant cellulose composite[J].Composites Science and Tecnology ,2017,153:1—6.[13] BORISOVA N V ,SLADKC)V () M ,ARTEMI*:NK() A A.Developingan electric heater design based on carbon fibres[J].Fibre Chemistry , 2007,39( 1 ):45-48.[14] CH1EN T H.TZO U I) Y, HU 八NG Z S ,e V u/.lligh performance326infrared heatersusing carbon fiber filamentsdecorated with alumina layer by microwave-assisted methodJJ].Journal of the Taiwan Institute of Chemical Engineers, 2016,59:521—525.[15]徐凯.基于Matlab 导热问题的数值模拟[J].上海丁.程大学学报,2016,30(4):354-358.Study on the ignition ability of metal-basedelectrothermal filmWANG Ji1, YANG Zan2, RAN Xue-qing3(1. China People's Police University, Hebei Langfang065000, China; 2. Harbin Fire and Rescue D ivision, H eilongjiang Harbin 150000, China; 3. Zhangjiakou Fire Rescue Division, Hebei Zhangjiakou 075000, China)Abstract: In order to study the ignition ability o f m etal-based electrotherm al film , cotton quilt and towel are selected as combustible cover m aterials. The tem perature changes o f various positions o f the cover material w ere studied experim entally, under the conditions o f different film power, covering thickness andm oisture content. A model was established. The tem perature of the place electrotherm al film connecting the cover at different am bient tem peratures w ere calculated by the m odel.The results o f this paper can provide som e reference data for fire prevention and fire investigation o f electrotherm al film fire.Key words: m etal- based electrotherm al film; ignition ability; flam m able cover; model calculation作者简介:王霁(1980—),女,河北石家庄人,中国 人民警察大学讲师,博士,主要从事消防材料学方面的研 究,河北省廊坊市安次区西昌路220号,065000。
外文翻译注塑模的单浇口优化
Single gate optimization for plastic injection moldAbstract:Abstract: This paper deals with a methodology for single gate location optimization for plastic injection mold. The objective of the gate optimization is to minimize the warpage of injection molded parts, because warpage is a crucial quality issue for most injection molded parts while it is influenced greatly by the gate location. Feature warpage is defined as the ratio of maximum displacement on the feature surface to the projected length of the feature surface to describe part warpage. The optimization is combined with the numerical simulation technology to find the optimal gate location, in which the simulated annealing algorithm is used to search for the optimum. Finally, an example is discussed in the paper and it can be concluded that the proposed method is effective.Key words: Injection mold, Gate location, Optimization, Feature warpage.INTRODUCTIONPlastic injection molding is a widely used, com- plex but highly efficient technique for producing a large variety of plastic products, particularly those with high production requirement, tight tolerance, and complex shapes. The quality of injection molded parts is a function of plastic material, part geometry, mold structure and process conditions. The most important part of an injection mold basically is the following three sets of components: cavities, gates and runners, and cooling system.Lam and Seow (2000) and Jin and Lam (2002) achieved cavity balancing by varying the wall thick- ness of the part. A balance filling process within the cavity gives an evenly distributed pressure and tem- perature which can drastically reduce the warpage of the part. But the cavity balancing is only one of the important influencing factors of part qualities. Espe- cially, the part has its functional requirements, and its thicknesses should not be varied usually.From the pointview of the injection mold design, a gate is characterized by its size and location, and the runner system by the size and layout. The gate size and runner layout are usually determined as constants. Relatively, gate locations and runner sizes are more flexible, which can be varied to influence the quality of the part. As a result, they are often the design pa- rameters for optimization.Lee and Kim (1996a) optimized the sizes of runners and gates to balance runner system for mul- tiple injection cavities. The runner balancing was described as the differences of entrance pressures for a multi-cavity mold with identical cavities, and as differences of pressures at theend of the melt flow path in each cavity for a family mold with different cavity volumes and geometries. The methodology has shown uniform pressure distributions among the cavities during the entire molding cycle of multiple cavities mold.Zhai et al.(2005a) presented the two gate loca- tion optimization of one molding cavity by an effi- cient search method based on pressure gradient (PGSS), and subsequently positioned weld lines to the desired locations by varying runner sizes for multi-gate parts (Zhai et al., 2006). As large-volume part, multiple gates are needed to shorten the maxi- mum flow path, with a corresponding decrease in injection pressure. The method is promising for de- sign of gates and runners for a single cavity with multiple gates.Many of injection molded parts are produced with one gate, whether in single cavity mold or in multiple cavities mold. Therefore, the gate location of a single gate is the most common design parameter for optimization. A shape analysis approach was pre- sented by Courbebaisse and Garcia (2002), by which the best gate location of injection molding was esti- mated. Subsequently, they developed this methodol- ogy further and applied it to single gate location op- timization of an L shape example (Courbebaisse,2005). It is easy to use and not time-consuming, while it only serves the turning of simple flat parts with uniform thickness.Pandelidis and Zou (1990) presented the opti- mization of gate location, by indirect quality measures relevant to warpage and material degradation, which is represented as weighted sum of a temperature dif- ferential term, an over-pack term, and a frictional overheating term. Warpage is influenced by the above factors, but the relationship between them is not clear. Therefore, the optimization effect is restricted by the determination of the weighting factors.Lee and Kim (1996b) developed an automated selection method of gate location, in which a set of initial gate locations were proposed by a designer and then the optimal gate was located by the adjacent node evaluation method. The conclusion to a great extent depends much on the human design er’s in tuition, because the first step of the method is based on the desi gner’s proposition. So the result is to a large ex- tent limited to the designer’s experience.Lam and Jin (2001) developed a gate location optimization method based on the minimization of the Standard Deviation of Flow Path Length (SD[L]) and Standard Deviation of Filling Time (SD[T]) during the molding filling process. Subsequently, Shen et al.(2004a; 2004b) optimized the gate location design by minimizing the weighted sum of filling pressure, filling time difference between different flow paths, temperature difference, and over-pack percentage. Zhai et al.(2005b) investigated optimal gate location with evaluation criteria of injection pressure at the end of filling. These researchers presented the objec- tive functions asperformances of injection molding filling operation, which are correlated with product qualities. But the correlation between the perform- ances and qualities is very complicated and no clear relationship has been observed between them yet. It is also difficult to select appropriate weighting factors for each term.A new objective function is presented here to evaluate the warpage of injection molded parts to optimize gate location. To measure part quality di- rectly, this investigation defines feature warpage to evaluate part warpage, which is evaluated from the “flow plus warpage” simulation outputs of Moldflow Plastics Insight (MPI) software. The objective func- tion is minimized to achieve minimum deformation in gate location optimization. Simulated annealing al- gorithm is employed to search for the optimal gate location. An example is given to illustrate the effec- tivity of the proposed optimization procedure.QUALITY MEASURES: FEATURE WARPGEDefinition of feature warp ageTo apply optimization theory to the gate design, quality measures of the part must be specified in the first instance. The term “quality” may be referred to many product properties, such as mechanical, thermal, electrical, optical, ergonomical or geometrical prop- erties. There are two types of part quality measures: direct and indirect. A model that predicts the proper- ties from numerical simulation results would be characterized as a direct quality measure. In contrast, an indirect measure of part quality is correlated with target quality, but it cannot provide a direct estimate of that quality.For warpage, the indirect quality measures in related works are one of performances of injection molding flowing behavior or weighted sum of those. The performances are presented as filling time dif- ferential along different flow paths, temperature dif- ferential, over-pack percentage, and so on. It is ob- vious that warpage is influenced by these perform- ances, but the relationship between warpage and these performances is not clear and the determination of these weighting factors is rather difficult. Therefore, the optimization with the above objective function probably will not minimize part warpage even with perfect optimization technique. Sometimes, improper weighting factors will result in absolutely wrong re- sults.Some statistical quantities calculated from the nodal displacements were characterized as direct quality measures to achieve minimum deformation in related optimization studies. The statistical quantities are usually a maximum nodal displacement, an av- erage of top 10 percentile nodal displacements, and an overall average nodal displacement (Lee and Kim,1995; 1996b). These nodal displacements are easy to obtain from the simulation results, the statistical val- ues, to some extents, representing the deformation. But the statistical displacement cannot effectively describe the deformation of the injection molded parts.In industry, designers and manufacturers usually pay more attention to the degree of part warpage on some specific features than the whole deformation of the injection molded parts. In this study, feature warpage is defined to describe the deformation of the injection parts. The feature warpage is the ratio of the maximum displacement of the feature surface to the projected length of the feature surface (Fig.1):where γ is the feature warpage, h is the maximum displacement on the feature surface deviating from the reference platform, and L is the projected length of the feature surface on a reference direction paralleling the reference platform.For complicated features (only plane feature discussed here), the feature warpage is usually sepa- rated into two constituents on the reference plane, which are represented on a 2D coordinate system:where γx, γy are the constituent feature warpages in the X, Y direction, and L x, L y are the projected lengths of the feature surface on X, Y component.Evaluation of feature wa rpageAfter the determination of target feature com- bined with corresponding reference plane and pro- jection direction, the value of L can be calculated immediately from the part with the calculating method of analytic geometry (Fig.2). L is a constant for any part on the specified feature surface and pro- jected direction. But the evaluation of h is more com- plicated than that of L.Simulation of injection molding process is a common technique to forecast the quality of part de- sign, mold design and process settings. The results of warpage simulation are expressed as the nodal de- flections on X, Y, Z component (W x, W y, W z), and the nodal displacement W. W is the vector length of vector sum of W x·i, W y·j, and W z·k, where i, j, k are the unit vectors on X, Y, Z component. The h is the maximum displacement of the nodes on the feature surface, which is correlated with the normal orientation of the reference plane, and can be derived from the results of warpage simulation.To calculate h, the deflection of ith node is evaluated firstly as follows:where W i is the deflection in the normal direction of the reference plane of ith node; W ix, W iy, W iz are the deflections on X, Y, Z component of ith node; α,β,γ are the angles of normal vector of the reference; A and B are the terminal nodes of the feature to projectingdirection (Fig.2); WA and WB are the deflections of nodes A and B:where W Ax, W Ay, W Az are the deflections on X, Y, Zcomponent of node A; W Bx, W By and W Bz are the de- flections on X, Y, Z component of node B; ωiA and ωiB are the weighting factors of the terminal node deflections calculated as follows:where L iA is the projector distance between ith node and node A. Ultimately, h is the maximum of the absolute value of W i:In industry, the inspection of the warpage is carried out with the help of a feeler gauge, while the measured part should be placed on a reference plat- form. The value of h is the maximum numerical reading of the space between the measured part sur- face and the reference platform.GATE LOCATION OPTIMIZATION PROBLEM FORMATIONThe quality term “warpag e”means the perma- nent deformation of the part, which is not caused by an applied load. It is caused by differential shrinkage throughout the part, due to the imbalance of polymer flow, packing, cooling, and crystallization.The placement of a gate in an injection mold is one of the most important variables of the total mold design. The quality of the molded part is greatly af- fected by the gate location, because it influences the manner that the plastic flows into the mold cavity. Therefore, different gate locations introduce inho- mogeneity in orientation, density, pressure, and temperature distribution, accordingly introducing different value and distribution of warpage. Therefore, gate location is a valuable design variable to minimize the injection molded part warpage. Because the cor- relation between gate location and warpage distribu- tion is to a large extent independent of the melt and mold temperature, it is assumed that the moldingconditions are kept constant in this investigation. The injection molded part warpage is quantified by the feature warpage which was discussed in the previous section.The single gate location optimization can thus be formulated as follows:Minimize:Subject to:where γ is the feature warpage; p is the injection pressure at the gate position; p0 is the allowable in- jection pressure of injection molding machine or the allowable injection pressure specified by the designer or manufacturer; X is the coordinate vector of the candidate gate locations; X i is the node on the finite element mesh model of the part for injection molding process simulation; N is the total number of nodes.In the finite element mesh model of the part, every node is a possible candidate for a gate. There- fore, the total number of the possible gate location N p is a function of the total number of nodes N and the total number of gate locations to be optimized n:In this study, only the single-gate location problem is investigated.SIMULATED ANNEALING ALGORITHMThe simulated annealing algorithm is one of the most powerful and popular meta-heuristics to solve optimization problems because of the provision of good global solutions to real-world problems. The algorithm is based upon that of Metropolis et al. (1953), which was originally proposed as a means to find an equilibrium configuration of a collection of atoms at a given temperature. The connection be- tween this algorithm and mathematical minimization was first noted by Pincus (1970), but it was Kirkpatrick et al.(1983) who proposed that it formed the basis of an optimization technique for combina- tional (and other) problems.To apply the simulated annealing method to op timization problems, the objective function f is used as an energy function E. Instead of finding a low energy configuration, the problem becomes to seek an approximate global optimal solution. The configura- tions of the values of design variables are substituted for the energy configurations of the body, and the control parameter for the process is substituted for temperature. A random number generator is used as a way of generating new values for the design variables. It is obvious that this algorithm just takes the mini- mization problems into account. Hence, while per- forming a maximization problem the objective func- tion is multiplied by (−1) to obtain a capable form.The major advantage of simulated annealing algorithm over other methods is the ability to avoid being trapped at local minima. This algorithm em- ploys a random search, which not only accepts changes that decrease objective function f, but also accepts some changes that increase it. The latter are accepted with a probability pwhere ∆f is the increase of f, k is Boltzm an’s constant, and T is a control parameter which by analogy with the original application is known as the system “tem perature”irrespective of the objective function involved.In the case of gate location optimization, the implementation of this algorithm is illustrated in Fig.3, and this algorithm is detailed as follows:(1) SA algorithm starts from an initial gate loca- tion X old with an assigned value T k of the “tempera- ture”parameter T (the “temperature” counter k is initially set to zero). Proper control parameter c (0<c<1) in annealing process and Markov chain N generateare given.(2) SA algorithm generates a new gate location X new in the neighborhood of X old and the value of the objective function f(X) is calculated.(3) The new gate location will be accepted with probability determined by the acceptance functionFig.3 The flow chart of the simulated annealing algorithmAPPLICATION AND DISCUSSIONThe application to a complex industrial part is presented in this section to illustrate the proposed quality measure and optimization methodology. The part is provided by a manufacturer, as shown in Fig.4. In this part, the flatness of basal surface is the most important profileprecision requirement. Therefore, the feature warpage is discussed on basal surface, in which reference platform is specified as a horizontal plane attached to the basal surface, and the longitu- dinal direction is specified as projected reference direction. The parameter h is the maximum basal surface deflection on the normal direction, namely the vertical direction, and the parameter L is the projected length of the basal surface to the longitudinal direc- tion.Fig.4 Industrial part provided by the manufac tur e rThe material of the part is Nylon Zytel 101L (30% EGF, DuPont Engineering Polymer). The molding conditions in the simulation are listed in T able 1. Fig.5 shows the finite element mesh model ofthe part employed in the numerical simulation. It has1469 nodes and 2492 elements. The objective func- tion, namely feature warpage, is evaluated by Eqs.(1), (3)~(6). The h is evaluated from the results of “Flow+Warp” Analysis Sequence in MPI by Eq.(1), and the L is measured on the industrial part immediately, L=20.50 mm.MPI is the most extensive software for the in- jection molding simulation, which can recommend the best gate location based on balanced flow. Gate location analysis is an effective tool for gate location design besides empirical method. For this part, the gate location analysis of MPI recommends that the best gate location is near node N7459, as shown in Fig.5. The part warpage is simulated based on this recommended gate and thus the feature warpage is evaluated: γ=5.15%, which is a great value. In trial manufacturing, part warpage is visible on the sample work piece. This is unacceptable for the manufacturer.The great warpage on basal surface is caused bythe uneven orientation distribution of the glass fiber, as shown in Fig.6a. Fig.6a shows that the glass fiber orientation changes from negative direction to posi- tive direction because of the location of the gate, par- ticularly thegreatest change of the fiber orientation appears near the gate. The great diversification of fiber orientation caused by gate location introduces serious differential shrinkage. Accordingly, the fea- ture warpage is notable and the gate location must be optimized to reduce part warpageT o optimize the gate location, the simulated an- nealing searching discussed in the section “Simulated annealing algorithm” is applied to this part. The maximum number of iterations is chosen as 30 to ensure the precision of the optimization, and the maximum number of random trials allowed for each iteration is chosen as 10 to decrease the probability of null iteration without an iterative solution. Node N7379 (Fig.5) is found to be the optimum gate loca- tion.The feature warpage is evaluated from the war- page simulation results f(X)=γ=0.97%, which is less than that of the recommended gate by MPI. And the part warpage meets the manufacturer’s requirements in trial manufacturing. Fig.6b shows the fiber orien- tation in the simulation. It is seen that the optimal gate location results in the even glass fiber orientation, and thus introduces great reduction of shrinkage differ- ence on the vertical direction along the longitudinal direction. Accordingly, the feature warpage is re- duced.CONCLUSIONFeature warpage is defined to describe the war- page of injection molded parts and is evaluated based on the numerical simulation software MPI in this investigation. The feature warpage evaluation based on numerical simulation is combined with simulated annealing algorithm to optimize the single gate loca- tion for plastic injection mold. An industrial part is taken as an example to illustrate the proposed method. The method results in an optimal gate location, by which the part is satisfactory for the manufacturer. This method is also suitable to other optimization problems for warpage minimization, such as location optimization for multiple gates, runner system bal- ancing, and option of anisotropic materials.注塑模的单浇口优化摘要:本文论述了一种单浇口位置优化注塑模具的方法。
【免费下载】XRD在固溶体中的应用
XRD在固溶体中的应用固溶体是指溶质原子进入溶剂晶格中而保持溶剂类型的多元素物相。
通常以一种化学物质为基体溶有其他物质的原子或分子所组成的晶体,在合金和硅酸盐系统中较多见,在其他多原子物质中亦存在。
固溶体分为间隙型固溶体和置换型固溶体,间隙型固溶体是由溶质原子溶于溶剂晶格中原子之间的而形成的间隙(四面体间隙或八面体间隙)中构成,置换型固溶体是由溶质原子代替溶剂晶格中的原子构成。
掺杂原子的进入,在一定程度上,影响原来物质的晶体结构,发生晶格畸变。
通过阅读文献,发现国内外学者主要研究置换型固溶体,而对间隙型固溶体的研究很少。
点阵参数是晶体结构最基本的参数,任何一种晶体物质在一定状态下都有一定的点阵参数,但当温度、受力状态、化学成分等任一条件发生变化时,都会引起点阵参数的相应变化。
利用精确的XRD数据,辅助精修软件,可以准确计算出晶体物质的点阵参数,得到空间群类型,进而确定晶体物质的晶体结构。
测定点阵参数的目的是为了求得物质的物理参量以及研究溶入外来元素后引起的性质变化和参数的关系等。
为获得精确的XRD数据,需要稳定高能的XRD光源,现在使用较多的是同步辐射光源的XRD线站。
1921年,Vegard[1]在Phs.上发表了《the constitution of mixed crystals and the space occupied by atoms》,指出具有相同晶体结构两组元(1,2)所形成的的固溶体,其晶格常数(a)是掺入原子浓度(c1)的线性函数:a=ca1+(1-c1)a2,后人称之为Vegard定律。
但是,Vegard定律经常与实际固溶体的a—c1曲线发生偏离,随着固态物理学的发展进步,后来有学者指出Vegard定律与实际情况不相符的根本原因在于它没有考虑到溶质和溶剂原子在固溶体中由于近邻原子的不同而引起原子电子结构状态的变化[2],提出了广义Vegard定律。
广义Vegard 定律是指单固溶体合金的晶格参量为该合金系统中所含原子的价电子状态的特征晶格参量按其相应的状态原子浓度线性叠加,即如果知道某合金各状态的价电子结构以及状态浓度便可计算出该合金的晶格参量。
纳米压痕 纯铁 氢 硬度 位错
Recent developments in the study of hydrogen embrittlement:Hydrogeneffect on dislocation nucleationAfrooz Barnoush *,Horst VehoffSaarland University,Department of Materials Science,Bldg.D22,P.O.Box 151150,D-66041Saarbruecken,GermanyReceived 11March 2010;received in revised form 30May 2010;accepted 30May 2010Available online 2July 2010AbstractIn this paper,the intrinsic complexities of the experimental examination of hydrogen embrittlement are discussed.On the basis of these complexities,an experimental approach,in situ electrochemical nanoindentation,is proposed and performed on different materials.This technique is capable of registering the onset of plasticity in extremely small volumes,namely perfect crystals in hydrogen-free and charged conditions.It is shown that hydrogen reduces the required stress for the onset of plasticity,i.e.homogeneous dislocation nucle-ation by reduction in the shear modulus,dislocation line energy and stacking fault energy.The change in the shear modulus can be related to reduction in crystal cohesion whereas the reduction in dislocation line energy and stacking fault energy are explained by the defactant concept,i.e.reduction in the defect formation energy in the presence of hydrogen.Thus,neither hydrogen-enhanced dec-ohesion nor hydrogen-enhanced plasticity,but the reduction in the cohesion and defect formation energy are responsible for hydrogen embrittlement.Ó2010Acta Materialia Inc.Published by Elsevier Ltd.All rights reserved.Keywords:Hydrogen embrittlement;Nanoindentation;Yield phenomena;Electrochemistry;Dislocation nucleation1.IntroductionHydrogen embrittlement is a severe environmental type of failure that affects almost all metals and alloys.With advancing technology,the use of high-strength structural materials for lightweight construction and energy conser-vation becomes a necessity.In spite of the success of mate-rials scientists in developing alloys with outstanding combinations of high tensile strength and high fracture toughness,hydrogen embrittlement still has a widespread effect that severely degrades the fracture resistance of these alloys.On the other hand,with the depletion of fossil fuels,mankind is searching for other sources of energy.Hydro-gen is believed to be a possible future energy source and it is very possible that a “hydrogen economy ”will be real-ized within the next 50years.In such a scenario,large-scale production,storage,transportation and use of hydrogenwill become necessary.However,the problems in materials caused by hydrogen embrittlement,reported as early as 1875by Johnson [1],could limit the progress of such an economy.Since Johnson first reported on hydrogen embrittlement,various strong views on the mechanisms of hydrogen embrittlement have been vigorously discussed and thoroughly reviewed in the literature [2–4].Because of the technological importance of hydrogen embrittlement,many people have explored the nature,causes and control of hydrogen-related degradation of metals [5–7].This has resulted in an enormous number of sometimes controver-sial findings and/or interpretations.Moreover,frequently an ad hoc approach,focusing on urgent technical problems at hand,is adopted which raises the question of how this isolated case or interpretation really reflects on any basic,general concepts.It thus seems apparent that the findings gathered so far cannot be accounted for by a single domi-nant mechanism.As an example,Fig.1shows the results of conventional hydrogen embrittlement testing of 34different grades of1359-6454/$36.00Ó2010Acta Materialia Inc.Published by Elsevier Ltd.All rights reserved.doi:10.1016/j.actamat.2010.05.057*Corresponding author.E-mail address:a.barnoush@matsci.uni-sb.de (A.Barnoush)./locate/actamatActa Materialia 58(2010)5274–5285steel within465test runs[8].The embrittlement index shown in Fig.1is the reduction in the fracture area in hydrogen-charged vs.hydrogen-free conditions during uni-axial tensile tests.The scatter observed within the results shown in Fig.1demonstrates the need for a new experi-mental approach to the investigation of hydrogen embrit-tlement.It is necessary tofind the source of this scatter in conventional hydrogen embrittlement testing methods. In this paper we will briefly review the different experimen-tal approaches used to study hydrogen embrittlement with a special focus on in situ local examination methods of hydrogen–dislocation interactions due to the conclusive role of dislocations in fracture and hydrogen embrittlement aspect is the wide range of intrinsic/extrinsic variables con-cerning the material itself.The experimental approach for examination of hydrogen embrittlement is based on the elimination of diverse factors within these three aspects. For example,let us consider uniaxial straining of a single crystal sample combined with controlled hydrogen charg-ing on the surface.The uniaxial stressfield simplifies the stress condition,i.e.the mechanical aspect of hydrogen embrittlement,in the e of a single crystal and con-trolled hydrogen charging condition reduces the complexi-ties due to the material and environmental aspects of hydrogen embrittlement in the test.Unfortunately,due to the large difference in the scale of these aspects controlling the process of hydrogen embrittlement,this experimental methodology is not very successful.The uniaxial stressfield of the above-mentioned example is not uniform,unlike the scale of hydrogen interacting with defects like dislocations and vacancies.This problem becomes more complicated as the microstructure becomes more complex with the intro-duction of grain boundaries,pores,second phases,etc. On the other hand,surface hydrogen charging of macro-scopic samples results in a concentration gradient,which again can override the microscopic process of hydrogen embrittlement.Additionally,microstructural features like dislocations,grain boundaries and interfaces can interact with hydrogen diffusion by providing faster diffusion routes or acting as traps for hydrogen.Superimpose upon this theFig. 1.The hydrogen embrittlement index measured by conventionalmechanical testing for34different grades of steel within465test runsFig.2.Global description of hydrogen embrittlement interaction aspects.Materialia58(2010)5274–52855275grain boundary fracture,enhanced shear or enhanced localized microvoid formation,or all of the above.One possible solution to these problems,arising from the experimental methodology used for studying hydrogen embrittlement,is the local examination of the hydrogen effect.This entails reducing the scale of the testing method down to the microstructural level such that all three con-trolling aspects of hydrogen embrittlement(Fig.2)can be defined within the test.Few attempts of this kind of approach have been done previously.Vehoffand Neumann [9]developed a method for studying crack propagation in a controlled environment under controlled plastic strain con-ditions.This method was used to study the hydrogen effect on crack growth mechanisms in Fe–2.6%Si[10]and Ni [11].In their experiments they controlled:(i)environmental aspects by using an ultrahigh-vacuum chamber and con-trolling the partial pressure of hydrogen;(2)mechanical aspects by controlling plastic strain and confining the stress to a smallfield ahead of the crack;and(iii)material aspects by selection of specifically oriented single crystals and focusing on the fracture process zone(Fig.3).Through these perfectly defined experimental conditions they were able to propose a model based on hydrogen-enhanced dec-ohesion(HEDE)and hydrogen trapping in front of a crack tip in the fracture process zone[10,11].Another intelligent experimental approach for small-scale observation of hydrogen effects on mechanical prop-erties was use of in situ straining tests in an environmental transmission electron microscope(TEM)developed by Birnbaum and Sofronis[12].With this technique it was possible for thefirst time to directly observe the effect of hydrogen on dislocations.Unfortunately,there are some uncertainties within the experimental conditions of this technique which must be mentioned here:(i)The electron beam dissociates hydrogen molecules to produce atomic hydrogen.Bond et al.[13]determined that the fugacity of the dissociated hydrogen was between30and750MPa. (ii)Since mode III(shear off)is usually easier in thinfilms, crack growth experiments under a defined mode I loading are very difficult to realize and therefore interpretation of the crack growth results become very difficult.(iii)Field of view is limited to the transparent region of the sample.By the introduction of micro-and nanoscale mechanical testing methods,like instrumented nanoindentation(NI) and nanoindenting atomic force microscopy(NI-AFM),a new era in mechanical testing of extremely small volumes started[14].Gerberich et al.[15]was thefirst one who men-tioned the potential application of micromechanical tests for the examination of hydrogen embrittlement.Since then, several researchers have used the NI technique to probe the effects of hydrogen on mechanical properties[16–20].The main advantage of the NI technique is its capability to resolve the dislocation nucleation in samples with low dis-location density[21,22].Additionally,analytical solutions for stress underneath the tip prior to dislocation nucleation within the elastic deformation are available,so the mechan-ical aspects of the experiments can be defined.The volume probed during the test is extremely small and can be char-acterized by means of different techniques,like electron backscatter diffraction(EBSD)and electron channeling contrast[23],and therefore,material aspects can be resolved.The referenced studies[16–20]used ex situ hydro-gen charging techniques which resulted in uncertaintiesFig.3.Hydrogen effect on the crack tip opening angle in:(a)vacuum and(b)hydrogen atmosphere.Sharpness of the crack tip in stressed Fe–3wt.%single crystal increases progressively with increasing hydrogen pressure[10].Table1Summary of the high-resolution testing methods used for local examination of hydrogen embrittlement. Experimental approach Different aspects of the hydrogen embrittlementMechanical Environmental MaterialIn situ crackpropagation test Defined and analyticallycan be treatedDefined Defined in the case of macroscopic single crystals withspecific orientation,very hard to apply on complexmicrostructuresIn situenvironmentalTEM tests Undefined Undefined due to dissociation of Hmolecules by electron beam(low pressure,very high fugacity)Defined with very high-resolution but only within thefield of viewNanoindentation on ex situ chargedsamples Before pop-in is definedand can analytically betreatedUndefined,due to out gassing andconcentration gradientPerfect defect-free crystalIn situ ECnanoindentation Before pop-in is definedand can analytically betreatedDefined Perfect defect-free crystalMaterialia58(2010)5274–5285within the hydrogen concentration especially near the sur-face of the sample where the mechanical testing was carried out.We solved this problem by performing in situ ECNI tests while the surface hydrogen concentration was kept constant by setting the surface electrochemical potential inside the proper electrolyte[24–26].Table1summarizes the local high-resolution techniques for examination of hydrogen embrittlement.A comparison of these methods shows the advantage of ECNI in provid-ing the required conditions to perform a defined experi-ment in accordance with different aspects of hydrogen embrittlement.In this paper,we report the results of ECNI tests on different metals with different hydrogen embrittle-ment susceptibilities.It will be shown that ECNI is capable of quantitatively resolving the sensitivity to hydrogen embrittlement.3.Experimental3.1.MaterialsThe materials used in this study and the electropolishing parameters and electrochemical hydrogen charging condi-tions for each are summarized in Tables2and3.The sin-gle-crystal specimens were cut by spark erosion from large single crystals with a misalignment of less than2°controlled by EBSD.The polycrystalline specimens were cut from samples with large grains a few millimeters in diameter which act like a single crystal during NI when all tests are performed in the same rge grains or single crystals eliminate the scatter in the data due to orien-tation differences.The samples were mechanically polished down to0.25l m.Afterwards,samples were annealed at 80%of the melting temperature in a vacuum greater than 10À6mbar for24h and cooled in the furnace in order to minimize the lattice defect density.Immediately before indentation the samples were electropolished according to the parameters given in Table2to have a well-defined reproducible surface condition.Special attention was paid to surface preparation since,as mentioned before,a defect-free and low-roughness surface is necessary in order to observe the dislocation nucleation during NI.When examined with an AFM,the sample surface had an root-mean-square roughness of less than1nm,and asperities or steps appeared infrequently on the surface.3.2.InstrumentationThe experiments were performed with a Hysitron Tribo-ScopeÒin conjunction with a Digital Instruments Nano-scope IIÒand a Hysitron TriboIndenterÒ.The indenter, designed especially for tests in liquid,had a Berkovich or conical diamond tip(see Table3).For the NI-AFM system, a three-electrode electrochemical setup with a platinum counter electrode and an Ag/AgCl reference electrode was developed,as shown schematically in Fig.4.Consequently, all the electrochemical potentials in this work are reported against an Ag/AgCl reference electrode.A Bank Elektronik TG97potentiostat was used to control the electrochemical potentials,and the electrochemical data were recorded on a PC using an AD–DA interface.The cell was made from Tef-lon e,and made tofit into the nanoindenter sample holder. Nanoindentation tests were made inside this electrochemi-cal cell while the sample was covered with approximately 2mm of electrolyte.The whole system was put into a cham-ber containing a protective atmosphere of nitrogen and helium in order to eliminate the oxygen effect in the electro-chemical reaction.The solution was injected from outside the chamber through a polyethylene tube connected to a MicroFil e pipette.There are additional concerns that arise when indenting in a liquid environment due to the capillary and buoyancyTable2Summary of the samples studied and their electropolishing conditions.Material Purity Microstructure Electropolishing conditionSolution Potential(V)Temperature(°C)Time(s) Copper Zone refined(111)H3PO4/ethanol202030 Aluminum99.991mm grains HClO4/ethanol40030Fe–3wt.%Si See Table41mm grains H2SO4/CH3OH121060FeAl(40at.%Al)Zone refined(100)H2SO4/CH3OH351090 Nickel Zone refined(111)H2SO4/CH3OH301560 Table3Summary of the electrochemical hydrogen charging and discharging(passivation)conditions.Material Test solution pH H-charging potential Passivation potential Indenter tip Copper Borate buffer9À1000mV250mV Berkovich Aluminum Borate buffer9À1250mV OCP Berkovich Aluminum0.05M Na2SO46OCP250mV Berkovich Fe–3wt.%Si Borate buffer9À1000mV n.a.Berkovich FeAl0.05M Na2SO46À1100mV100mV Conical Nickel0.05M Na2SO46À1000mV500mV BerkovichA.Barnoush,H.Vehoff/Acta Materialia58(2010)5274–52855277forces acting on the tip.To overcome this,the surface is first engaged with a higher set point of contact force.The tip is then moved a few nanometres away from the surface and the forces on the tip balance while it rests above the surface.After this procedure the surface can be easily engaged as usual.Another important concern during the in situ ECNI test is cleanliness.Therefore,all electrolytes were prepared from analytical grade compounds and dou-ble-distilled water.Prior to the tests,the electrochemical cell was cleaned in piranha acid to remove most organic matter and to make it hydrophilic and water compatible.The tip and its shaft were also cleaned carefully before each test in a mixture of ethanol and isopropanol and then in double-distilled water.A clean tip shaft reduces the capil-lary forces acting on it and reduces the probability of dis-engagement of the tip during surface imaging inside the solution.A low impurity content in the electrolyte inhibitsthe deposition of these impurities during electrochemical polarization of the surface.The electrolyte pH and compo-sition should also be selected very carefully to inhibit any possible corrosion and surface roughening.Hence,these parameters are selected for each sample individually.4.Results 4.1.CopperCopper is known for its very low hydrogen solubility and diffusivity.DeWulf and Bard [27]showed that without hydrogen recombination poisons (e.g.As 2O 3)no detectable hydrogen concentration develops in copper.This makes the copper a proper calibration material for in situ ECNI tests,where no effect of cathodic charging should be observed.Typical load–displacement (L –D )curves under cathodic and anodic potentials are given in Fig.5.4.2.AluminumAluminum is a reactive metal protected by a thin stable oxide layer with semi-conductive properties.At potentials cathodic to the open circuit potential (OCP)of Al,cathodic hydrogen evolution due to the reduction of hydrogen ions and water occurs simultaneously with anodic oxidation and dissolution processes [28].This makes the electrochem-ical hydrogen charging of Al without damaging the surface difficult.Therefore,an alternative method controlling the pH of the solution was developed and used for hydrogen charging of Al [29].It is well known that oxide-covered metals immersed in aqueous solutions terminate in an out-ermost layer of hydroxyl groups due to their interaction with water molecules [30].In aqueous solutions,the surface hydroxyl groups will remain undissociated if the pH of theTable 4Analysis of the Fe–3wt.%Si alloy used in this study in.C Si Mn P S Cr Ni Mo Cu Al Ti Nb V B Zr Ce 0.0032.3830.2020.0130.0120.0330.0480.0150.0200.3650.0050.0200.0020.00080.0050.009Fig.4.Schematic drawing of the experimental setup.10020030040050001020304050607080Depth (nm)01002003004005006000102030405060708090Depth (nm)Fig.5.Typical L –D curves of copper under:cathodic and (b)anodic polarization.Materialia 58(2010)5274–5285aqueous solution is the same as the isoelectric point (IEP)of the oxide.If the pH is less than the IEP,the surface will acquire a positive charge.MOH ðsurf ÞþH þðaq Þ!MOH þ2ðsurf Þð1ÞIf the pH is greater than the IEP,the surface will acquire a negative charge MOH ðsurf ÞþOH Àðaq Þ!MO Àðsurf ÞþH 2Oð2ÞThe air-formed oxide film on Al has the IEP value of9.5[31].According to the Eqs.(1)and (2),the pH can greatly affect the hydrogen absorption during immersion of the sample in electrolyte under OCP.Hence,the tests on Al were performed in two different solutions (Table 3).Typical L –D curves of the aluminum sample at different pH levels and electrochemical polarizations are given in Fig.6.4.3.Fe–3wt.%SiThe Fe–3wt.%Si alloy is a single-phase body-centered cubic crystal.The electrochemical behavior of this metal is quite similar to that of pure iron and has a very low aqueous corrosion resistance in solutions with low pH.Therefore,in situ ECNI tests were performed in a pH 9borate buffer solution.This electrolyte is preferred because of the possibility of both controlled cathodic removal of prior oxide films and highly efficient anodic passivation.However,during the in situ ECNI experiments,due to the limited volume of the electrochemical cell and the use of Ag/AgCl reference electrodes,contamination of electro-lyte with Cl Àions resulted in the breakdown of the passive layer.All attempts for producing a stable passive layer failed and resulted in a corroded surface that was not suit-able for NI experiments.Therefore,in the case of the Fe–3wt.%Si sample,the NI results under cathodic potential are compared with the results in air.Fig.7a shows typical load displacement curves during NI of the Fe–3wt.%Si sample in air.The same sample was indented in the same grain under a cathodic potential of À1000mV.This resulted in the load displacement curves shown in Fig.7b.4.4.FeAl intermetallicThe commercial importance of iron aluminides for high temperature structural applications has been well estab-lished [32].Iron aluminides contain two of the most widely available metals,namely Fe and Al.They offer low mate-rial costs,conservation of strategic materials and lower density than stainless steels,with excellent oxidation and sulfidation resistance.In spite of all these inherent advanta-ges,the binary iron aluminides suffer from hydrogen embrittlement.A conical indenter with a cone angle of 90°was used to perform the indentations on FeAl intermetallic alloy with 40at.%Al.The resulting L –D curves in different conditions are given in Fig.8.4.5.NickelThe freshly electropolished nickel has a thin (0.6–0.8nm)film of NiO which can be reduced by cathodic polarization in Na 2SO 4solution with a pH lower than 8[33].Anodic polarization of nickel in the same solution produces a new passive layer,which is a 0.9–1.2nm film of NiO.This film cannot be reduced in a neutral solution.This fact was used during in situ ECNI experiments to exclude surface effects from the effects of hydrogen [34].D curves of aluminum in:(a)pH6solution (OCP light-colored/anodic dark-colored)and (b)pH9solution (cathodic light-colored/OCP 05001000150020002500255075100Depth (nm)o a d (µN )H-chargedH-freeHertzian fitL –D curves of Fe–3wt.%Si in:(a)air and (b)hydrogen-charged condition.Typical load displacement curves obtained in different con-dition are shown in Fig.9.5.DiscussionThe L –D curves of Figs.5–9all show three stages:elastic loading,an excursion in depth (pop-in)at the onset of plas-ticity and continued elastoplastic loading.The initial elastic portion of the loading curves can be fitted with the Hertz-ian elastic responseP ¼43E r ffiffiffiffiffiffiffiffiRh 3p ð3Þwhere P is the applied load,h is the indentation depth,R is the radius of the tip curvature and E r is the reduced mod-ulus,given by 1E r ¼1Àm 21E 1þ1Àm 22E 2ð4ÞHere E is the elastic modulus of the material,m is the Poisson’s ratio,and the subscripts 1and 2refer to the tip and the sample respectively.The initial elastic loading begins as soon as the tip contacts the material surface and continues until dislocation nucleation or motion occurs.Typical dislocation densities in an annealed metal are in the range 106–108cm À2,with dislocations spaced between 1and 10l m apart.A typical indentation test in the elastic regime probes a lateral region of at most a couple of hun-dred nanometers to the point where the pop-in is noted.This suggests the volume of material sampled by the inden-tation test at this depth is smaller than the average disloca-tion spacing,so that an indentation placed randomly on the surface would have a significant probability of sampling a region that contains no pre-existing dislocations.Experi-mental studies [35,36]have been conducted and all lend credibility to the assumption that,for a well-annealed and electropolished sample,the indenter tip can initially contact a volume of material small enough to be dislocation free.The absence of dislocations means the material continues to load elastically until the shear stress under the tip reaches a value near the theoretical shear strength of the material,well above that necessary to activate an existing dislocation source.At this point dislocations are homogeneously nucle-ated,followed by subsequent glide and multiplication events.Homogeneous dislocation nucleation (HDN)should occur when the stress beneath the indenter tip approaches the theoretical shear strength of the material.The term HDN is used here to indicate that dislocations are nucleated from otherwise dislocation-free material.For an indentation test,the applied shear stress that nucle-ates a dislocation can be assumed to be the maximum shear stress beneath the indenter during purely elastic loading.According to continuum mechanics,the maximum shear stress is acting on a point 0.48times the contact radius,a ,below the sample puter simulations have also shown that dislocations nucleate at this point [37].The posi-tion of this maximum shear stress z s (max)and its value s max is givenbyFig.8.Typical L –D curves of FeAl in:(a)hydrogen-free and (b)hydrogen-charged conditions.0501001502002503000102030405060Depth (nm)Depth (nm)a10020030040050001020304050607080ba d (µN )a d (µN )Pop-inFig.9.L –D curves for nickel in:(a)hydrogen-charged and (b)hydrogen-free conditions.z sðmaxÞ¼0:48Áa¼0:483PR4E r13ð5Þs max¼0:316E2rp3RP13ð6ÞTable5summarizes the effect of hydrogen charging on the mean value of pop-in load s max and its position below the surface of all studied samples.For comparison,the the-oretical strength(s th%l/20)according to Frenkel’s model is also given in the Table5.5.1.Hydrogen effect on HDNThe above results clearly indicate that the pop-in load in the hydrogen-charged condition is lower than in the hydrogen-free condition.This change cannot be attributed to the surface topography since it has been imaged and revealed no surface roughening[24,25].Fig.10,as an example,shows the surface topography of the FeAl sam-ple inside the electrolyte.Therefore,the reduction in the pop-in load clearly shows the hydrogen effect on HDN. This is in good agreement with molecular dynamic simu-lations performed by Wen et al.[37].Their results,like other experimental NI results on hydrogen-charged mate-rials[18–20],used hydrogen-enhanced plasticity(HELP) to explain the reduction in the pop-in load.However, the analytical description of the HELP mechanism is based on reduction of elastic interactions by solute hydro-gen between dislocations and elastic centers which act as barriers,such as nearby dislocations and solute pinning points[12].As mentioned before,during NI,the probed volume of the material is so small that it can be assumed to be a perfect crystal without any defects.Therefore,elas-tic shielding of the dislocations by trapped hydrogen atoms is not capable of explaining the observed enhanced plasticity.In adsorption-induced dislocation emission (AIDE)[2,38]the formation energy of dislocations at the crack tip is reduced by hydrogen being absorbed on the crack surfaces.As opposed to HELP,it is the external hydrogen on the crack surface and not the internal hydro-gen in the bulk that enhances the dislocation nucleation in AIDE.Therefore,neither HELP(in the original formula-tion[12])nor AIDE is capable of explaining the hydro-gen-induced reduction in the pop-in load during NI.According to the classic dislocation theory,the free energy required for HDN during NI is determined by the line energy of the newly formed loop c dis and the work for extending the dislocation loop s b per loop area.Here s is the maximum shear stress under the indenter induced by the external load and b is the Burgers vector of the dis-location.If the dislocation forms as a partial,the stacking fault energy(SFE)c also contributes to the required energy for HDN.Then the formation energy of a circular loop of radius r isD G¼2p r cdisþp r2cÀp r2b sð7ÞThe elastic self-energy for a full circular dislocation loop of radius r in an infinite elastic solid is given byc dis¼2Àt1Àtl b2r4ln4rqÀ2ð8ÞFig.11shows the plots of D G as a function of loop radius calculated for the observed mean values of s max in the hydrogen-charged and hydrogen-free conditions.The material constants used are given in Tables5and6.The free-energy curves for HDN pass through a maximumTable5Summary of the mean pop-in load for the H-charged and H-free conditions and comparison between theoretical strength,l/20and measured shear stress at the onset of the pop-in.3topography of FeAl sample under:(a)cathodic and(b)anodic potential where no surface rougheningA.Barnoush,H.Vehoff/Acta Materialia58(2010)5274–52855281。
碳点荧光法测定羟基自由基和葡萄糖
碳点荧光法测定羟基自由基和葡萄糖于海萍;黄述朝;高吉刚;王晓艳【摘要】以柠檬酸和二聚氰胺为原料,水热法制出了发蓝绿色荧光的氮掺杂碳点,这种碳点的粒径小、水溶性好、荧光量子产率高.该碳点的荧光可被芬顿反应产生的羟基自由基猝灭,从而建立了羟基自由基的测定方法,测定的线性范围为9.5×10-7~7.5×10-5 mol·L-1,测定极限为9.5×10-7 mol·L-1.耦合葡萄糖在过氧化酶(GOD)作用下产生H2O2的反应,建立了碳点荧光法测定葡萄糖含量的新方法,该方法应用于人体尿液的葡萄糖含量的测定,取得了满意的结果.【期刊名称】《广州化工》【年(卷),期】2018(046)013【总页数】4页(P70-72,85)【关键词】碳点;二聚氰胺;羟基自由基;葡萄糖【作者】于海萍;黄述朝;高吉刚;王晓艳【作者单位】山东农业大学化学与材料科学学院,山东泰安 271018;山东农业大学化学与材料科学学院,山东泰安 271018;山东农业大学化学与材料科学学院,山东泰安 271018;山东农业大学化学与材料科学学院,山东泰安 271018【正文语种】中文【中图分类】O644.1羟基自由基(·OH)是一种对生物体毒性最强、危害最大的活性氧粒子之一,它可以与生物体内的糖类、氨基酸、蛋白质、核酸和脂类多种分子作用[1],造成细胞和组织的坏死或损伤,引发机体功能的衰退和许多疾病的产生[2],因此,及时准确的检测羟基自由基是非常必要的。
常见的检测羟基自由基的方法有分光光度法、荧光光度法、高效液相色谱和电化学检测等方法,它们各有特点,同时也存在着灵敏度不高、光稳定性差、前处理复杂等缺点[3-4]。
荧光碳点作为一种新型的荧光材料,除了具有高荧光性外,还具有较好的生物相容性、水溶性、光稳定性[5-7],以及原料易得、制备方法灵活多样[8]、易于修饰等特点[9-10],受到人们广泛的关注[11-12]。
案件侦察模型
案件侦察模型As we all know, the investigation of cases is a crucial part of the criminal justice system. 案件侦察是刑事司法体系中至关重要的一部分。
It involves gathering evidence, analyzing information, and connecting the dots to solve crimes. 它涉及收集证据、分析信息,以及连接相关线索来解决犯罪。
A well-designed case investigation model can streamline the process and improve the efficiency of law enforcement agencies. 一个设计良好的案件侦察模型可以简化流程,提高执法机构的效率。
Therefore, it is essential to develop a comprehensive and effective model for case investigations. 因此,开发一种全面有效的案件侦察模型至关重要。
One of the key components of a successful case investigation model is the use of technology. 一个成功的案件侦察模型的关键组成部分之一是利用技术。
Technology can aid in the collection and analysis of data, as well as in the preservation of evidence. 技术可以帮助收集和分析数据,同时也有助于证据的保护。
For example, forensic software can assist in identifying suspects through DNA analysis or fingerprint matching.比如,取证软件可以通过DNA分析或指纹比对帮助识别嫌疑人。
化学research proposal范文
化学research proposal范文化学 Research ProposalIntroduction:Chemistry plays a critical role in various scientific disciplines and societal applications. The development of new materials, drugs, and energy sources heavily relies on advancements in chemical research. This research proposal aims to investigate the synthesis of novel nanomaterials with enhanced catalytic properties for various chemical reactions. The proposed project will explore the fabrication of metal-organic frameworks (MOFs) and investigate their potential applications in heterogeneous catalysis.Objective:The main objective of this research proposal is to synthesize MOFs and evaluate their catalytic efficiency for different reactions. The specific objectives include:1. Synthesis of MOFs with desired structures and properties.2. Characterization of the fabricated MOFs using advanced techniques.3. Evaluation of the catalytic activity of MOFs for specific reactions.4. Understanding the mechanisms behind the catalytic behavior of MOFs.5. Optimization of the synthesis and catalytic conditions for improved performance.Methodology:Synthesis of MOFs:In this study, MOFs will be synthesized using a solvothermal method. The reaction mixture containing metal ions, organic ligands, and solvents will be heated at an elevated temperature under autogenous pressure. The resulting crystalline MOFs will be collected, washed, and dried for further characterization.Characterization:The synthesized MOFs will be characterized using various techniques, including X-ray diffraction (XRD), scanning electron microscopy (SEM), transmission electron microscopy (TEM), and Fourier-transform infrared spectroscopy (FTIR). These techniques will provide important information about the phase purity, morphology, and structural properties of the fabricated MOFs.Catalytic Evaluation:The catalytic activity of the MOFs will be evaluated for several reactions, such as the oxidation of organic compounds and the reduction of nitroaromatics. The reactions will be carried out in a fixed-bed reactor under controlled conditions. The conversion, selectivity, and stability of the catalysts will be monitored to assess their performance.Mechanistic Study:To understand the underlying mechanisms of the catalytic activity, various characterization techniques will be employed. In situ FTIR spectroscopy will be used to monitor the adsorption and desorption of reactants and intermediates on the MOF catalysts. Density functional theory(DFT) calculations will be conducted to provide theoretical insights into the reaction pathways and identify the active sites within the MOF structures.Optimization:Based on the obtained results, optimization of the synthesis and catalytic conditions will be carried out to improve the performance of the MOF catalysts. Factors such as temperature, pressure, and reactant concentration will be systematically varied to identify the optimal conditions for specific reactions.Expected Results:It is anticipated that the synthesis of MOFs with tailored structures and functionalities will lead to the development of efficient catalysts for various chemical transformations. The research outcomes will contribute to the understanding of structure-activity relationships in MOFs and provide insights for the design of advanced catalysts.Conclusion:This research proposal outlines a comprehensive investigation into the synthesis and catalytic evaluation of MOFs for various chemical reactions. The proposed study aims to contribute to the field of heterogeneous catalysis by developing novel nanomaterials with improved performance. The results obtained from this research will have significant implications for the development of sustainable and efficient catalytic processes.。
1月26日雅思机经真题回忆
1月26日雅思机经真题回忆Section 1新题/旧题:旧题场景:教育主题:不同年龄的游泳课程题型及数量:10填空题考试题目+答案:1. introduce breathing techniques in water2. focus on the safety3. improving the diving4. intermediate level course are for adults5. 课程开始时间:13th/30th January (有待确认)6. each learner should bring a towel7. aim to improve speed8. bring change to rent locker9. required to swim with a hat10 improve in confidence考点:基本功及同意替换可参考真题:C6T1S1;C6T2S1Section 2新题/旧题:新题场景:环境主题:如何在家中节约能源题型及数量:6单选+4多选考试题目+答案:11. A (几天后就会开展节约能源的工作)12. C (switch off appliance)13. B (可以网上付款,用户满意度高)14. A (装双层玻璃)15. A (不适合房子)16. 暂缺17-18. C (只烧够用的水) E (换掉漏水的管子)19-20. 暂缺考点:同义替换可参考真题:C10T2S2;C10T3S2Section 3新题/旧题:旧题场景:教育主题:学生和老师讨论关于老房子的研究项目题型及数量:10填空考试题目+答案:21. material background: relevant information about the history of a village.22. history of age23. house’s planner work out ground plan24. go to library to get large-scale maps25. investigation must focus on the: take drawings of staircase and fireplaces26. reasons for choosing this topic27. for example at university: taking piece of wood sample28. essays should describe problems fully and honestly29. pay attention to occupancy30. finally she should mention: unanswered questions考点:同意替换,结构转换可参考真题:C6T2S3;C9T1S3;C11T2S4Section 4新题/旧题:旧题场景:建筑主题:建筑设计题型及数量:3单选+5匹配+2填空考试题目+答案:31-33)multiple choices31. recently, a fast growth of construction of new airportsC. deserves close attention32. one noticeable fact is that construction of new airports isB. more important than other buildings (more significant)33. What are the airport, cities and town in commonA. respond to change34-38)Matching: scenarios(红字为关键字)34. S1-there are more expensive flights because the economic depression causesfuel shortage35. S2-there are emerging new airports36. S3-there are also new transports pattern appeared37. S4-people’s interest in flying is declining in Western countries38. S5-airlines can not hold business because the cost of maintenance39-40)Completion: the disadvantages of travel39. if the environmental problems continue, airport must be imposed on the “green tax”40. flight will close down if a trip does not get an insurance考点:同意替换,结构转换。
商务英语写作chapter6
Chapter 6 Adjustment and RefusalsIn business world it is unavoidable to receive complaints and claims. How to appropriately resolve the matter becomes a tough and challenging task. It is said the most difficult business letter is to respond to complaints and claims. However, there are still some useful tips for writing it without damaging the company's image.AdjustmentWhen you get a complaint or claim, you may either grant an adjustment or reject it depending on the circumstances. When you grant an adjustment, the situation is a happy one for your customer. You are correcting an error. You are doing what you were asked to do. As in other positive situations, a letter written in the direct order is appropriate. The direct-order plan follows these general steps:1.Begin directly---with the good news.2.Incidentally1 identify the correspondence that you are answering.3.Avoid negatives that recall the problem.4.Regain lost confidence through explanation or action.5.End with a friendly, positive comment.RefusalRefusal of a request is definitely a bad news message; therefore, an indirect order is preferred. In the refusal letter, you have two goals. The main one is to say no; the other is to maintain goodwill. You could achieve the first goal by simply saying no ---plainly and directly. Maintaining goodwill, however, requires more. The following general pattern will help you better handle the tasks.1.Begin with words that indicate response to the request and are neutralas to the answer, and set up the strategy.2.Present your justification or explanation, using positive language andyou-viewpoint.3.Refuse positively.4.End with adapted, goodwill comment.The following two letters are written according to thewriting principles mentioned above. Now read the lettersand try to figure out how the writing principles areapplied in them. The questions after the letters might helpyou accomplish the task.Letter A Letter of adjustmentDear Mrs. Williams:Your repaired video game is being returned by UPS, and you should receive it within a week. Skilled engineers made your video game almost as good as new.Recently Pace Electronic has acquired the assets of Four Star Games and has became responsible for repairs under warranties. Now you can be assured of prompt and reliable service. Any future repairs can be made by one of the dealers of our expanded network (see enclosed sheet).Also enclosed is a brochure showing some of our exciting new products, as well as Four Star's old favorites. You can order by mail, using the order form in the brochure, or call 1-800-877-PACE. We look for-ward to helping you enjoy your video game.Letter B Credit refusal letterDear Mr. Sands:We sincerely appreciate your interest in an account with White-Horton & Company. Whenever we can, we are always willing to serve you.In determining what we can do for you regarding your June 8 request for credit, we made the routine checks you authorized. The information we have received permits us to serve you only as a cash customer2. But asyou know, cash buying here at White-Horton's discount prices can make a very real saving for your budget.We hope to see you in the store again very soon, and we look forward to the opportunity of serving you.Questions for Comprehension1.What kind of order does each letter adopt?2.How does the author of adjustment begin his/her letter?3.Do the replies clearly state the problems?4.How does each author arrange the body of his/her letter?5.Is the tone of each letter polite and considerate?6.How does each author end his/her letter?7.What's the purpose of each letter?8.Does each letter state clearly its explanation?9.What's your impression on these letters?10. Sum up the requirements for writing an adjustment and a refusal.Sample Analysis1Sample 6-1 Adjustment for the wrong materialsDear Glenn Presley:The correct consignment of the clothing material will reach you within 20 days.I'm grateful for your letter dated September 1st. We're sorry to learn that the clothing materials don't match the sample. After careful examination, we found that we had misfilled3your order and another order that was different from yours with only one letter. We have arranged for the correct consignment and it would arrive at your place by September 24th.As compensation for the wrong delivery, I would like to provide you a 5% discount on this consignment, and I hope such an arrangement is satisfactory to you.Thank you for your letter of March 3rd and we will take care of your broken-down sewing machines.It is our common practice to carry out a careful screening to ensure our machines functional and reliable before they are finally sent out to customers. We are so confident and proud of our quality that our warran-ties4 run for as long as the customers possess the products.Your letter informing us of the problem has been handed to the Technology Department. The senior engineers will make a careful research to find out the potential problem areas. Simply send us the bill for the repairs and we'll reimburse you the costs.For any problems arising with this or any other machines we produced, simply take it to your nearest Sharp Machine Distributor who will repair it at no expense for you.Sincerely yours,Sample 6-3 Refusal to claim on replacement1Dear Mr. Mitchell:We understand your concern about the software Model 4050 you mentioned in your letter of May 6. We are willing to do as much as we reasonably can to make things right.From your description and our staff's careful research, we found that there was something wrong in the computer networks you adopted.As it is stated in the operating instruction, this software is solely compatible5 with Windows XP, which is different from Windows 98. And before you use this software, you should have to install the starting sys-tem6 at the bottom of the box first. But you haven't installed it. Therefore, please install the starting system first and then try it with Windows XP. For other procedures, please follow the procedures strictly with our instruction brochure.We hope the software will bring much convenience and profit to you.Frankly yours,Sample 6-5 Adjustment of a wrong order •Dear Mr. White:I would be disappointed to lose your cooperation, but even more disappointed to lose your faith and friendship in our firm. So I sincerely thank you for your letter that was written in friendliness to give us an-other opportunity.I am sorry that you had to send the wrong order back, which, I know, is really bothering. Though you didn't send back the leather chairs of which we sent the wrong style and the amount is not that much, we want to made it right. We will immediately send the sandal-wood chairs that you wanted.I must apologize again for the inconvenience has caused you. If you want to change any other items in your order, let me know and we will send them to you. You can return them when you are convenient. A check for postage is also enclosed as we don't expect to have you pay the extra expense because of our mistakes.You have been a customer of long standing. We will try our best to avoid mistakes in serving you.Dear Sirs:We have received your letter of October 15, but we are surprised to know your unreasonable request.Obviously, the rice was wetted by the seawater during the transportation, so you shouldn't claim on us. You have to write to those who are responsible.Sincerely yours,Language for WritingI. Notes1. incidentally: adv.The issue was brought up incidentally at the meeting.2.cash customer:The credit investigation survey permits us only to serve you as a cash customer.3.misfill: v.We misfilled your order owing to the carelessness on the part of our warehouse worker.4.warranty: n.The car enjoys a five-year warranty period.patible: adj.The two systems are not compatible.6.starting system:The new starting system proves much faster than the older ones,7. route: v.We will route the information to the headquarters by tomorrow.II. Useful Sentence Patterns1. BeginningAdjustment1)... should reach you in three days...2) The attached check for... is Newton's way of assuring you that your satisfaction is very important to us.3) By... (time), your three Dove Bicycles should reach you at... shop.Refusal1) We understand your concern about the.... As always, we are willing to do asmuch as we reasonably can to make things right.2) You were right in assuming that.... We are always interested in doingwhatever we can to make our sales satisfactory.3) Your order and request are sincerely appreciated. We are always grateful forthe opportunity of serving you in the best way we can.2. Indirect Refusing1) The best we can do is...2)... permit us to serve you only as a cash customer.3) We feel at this time you will be acting in your own best interest by...4) We must consider the sale final.5)In view of this explanation, you will understand why we must stand by ourguarantee policy in this case.3. Ending1) Thank you for this opportunity to explain. We shall continue to work hard toprovide you with the service you have a right to expect.2) We hope to see you again in the store, and we look forward to theopportunity of serving you..3) We are always pleased to do business with your organization and willcontinue to serve you with quality industrial equipment.4) So, whenever it is convenient, please come by and let us...5) We wish you the best in enjoying from...ExercisesI. Put the following sentences into the right order and make it a completeletter.a..Please accept our apologies for the delay.b. The mistake has been corrected and will never occur again.c. Our internal research has uncovered a bottleneck in our fulfillmentprocedures.d. Thank you for your letter of December 10th regarding your order thechinaware.e. Therefore, we have delayed several shipments, including yours.f.Your order has now been ranged and shipped.g. Please contact me if I can offer any help.II.Fill in the blanks of the following letter with the words given. Change the form where necessary.recover invoice appreciateregarding account inconvenienceDear Sirs:Thank you for your letter dated January 18th __________ the mistaken bill.On January 4th, a virus hit our computer system. When we ________ our collapse system, we discovered the __________ were out of order.We realized that all the _____________ we have sent out were inaccurate, including the one you received on January 8th.We have corrected all the accounts and sent new invoices.We are extremely sorry for the_________brought to our customers; therefore, we enclosed a 15% discount coupon for your next order.W e ___________ your cooperation during this time and look forward to serving you again.Sincerely yours,III. Read the following adjustment and see if you can improve i t.Thank you for your letter of May 3rd concerning the furniture you purchased. I'm sorry that we have sent you the wrong size.The mistake was made by our distribution department and they made a mistake in looking for the right name.Sincerely apologize for the inconvenience it brought you.1) One of your customers, Mrs. Douglas, wrote to claim to you that youhave mixed up the tables she ordered. After examination, you foundthat it was owing to the loss of the sales file of that purchase.You are asked to write a response to her claim and tell her you will offer her a 10% discount on her next purchase as compensation.2)Your customer, Mr. Bidwell wrote to you that you had sent him thewrong bill with $150 overcharged. After calculation, you found that hehad missed to calculate the transportation fees.Now write him a letter to refuse his request.。
TEM法在工程勘察中的研究与应用
T EM 法在工程勘察中的研究与应用郭玉松 (黄委会勘测规划设计研究院 郑州 450003) 【提要】 本文主要介绍了瞬变电磁法在堤防工程及水利水电工程勘察中的研究进展情况及应用效果,通过实际探测资料的分析,介绍了T E M 法探测技术。
【关键词】 瞬变电磁法 工程勘察 隐患探测 【Abstract 】 T he developm ent of research oninstantaneous electrom agnetic m ethod in engineering investiga 2ti on of em bankm ent and hydraulic engineering and the results after use are introduced herein .T he T E M m ethod fo r p ro specting is p resented th rough analyses of p ractical detecti on data .【Key words 】 instantaneous electrom agnetic m ethod engineering investigati on h idden danger detecti on1 前言瞬变电磁法(T E M )近几年来在国内外得到迅速发展,在金属矿勘探、油气田勘探和煤田勘探等矿床勘探中得到广泛应用。
尤其值得注意的是它正开始步入工程勘察、地下水及地热勘察的行列中,成为国内外引人注目的地球物理勘探方法之一。
为了研究T E M 法在堤防及水利水电工程勘察中的有效性,几年来进行了大量的试验研究工作,取得了可喜的地质效果,该方法在探测堤防工程大体积异性材料,划分地层结构中发挥了重要作用。
2 基本原理时间域瞬变电磁法(简称T E M 法)是近几年发展起来的一种地球物理方法。
它是利用不接地回线(或接地线源)向地下发送一次脉冲磁场(或电场),在一次脉冲磁场(或电场)的间歇期间,利用线圈(或接地电极)观测地层响应二次涡流场的方法。
透射电镜半导体样品制备流程英语
透射电镜半导体样品制备流程英语## Transmission Electron Microscopy (TEM) Semiconductor Sample Preparation.Transmission electron microscopy (TEM) is a powerful characterization technique used to study the microstructure of materials at the nanometer scale. It is widely used in the semiconductor industry to analyze the crystal structure, defects, and interfaces of semiconductor devices. Preparing high-quality TEM samples is crucial for obtaining reliable and interpretable results.### Sample Preparation Workflow.The general workflow for TEM sample preparation of semiconductors involves the following steps:1. Sample selection and preparation: The first step isto select a representative sample from the device under investigation. The sample should be thin enough (typicallyless than 100 nm) to allow the electron beam to penetrate and form an image.2. Mechanical thinning: The sample is mechanically thinned using a dimple grinder or ion milling to create a thin region. This process is performed carefully to avoid introducing defects or damaging the sample.3. Chemical etching: Chemical etching is used tofurther thin the sample and remove any surface damage caused by mechanical thinning. The etchant used depends on the semiconductor material and the desired sample thickness.4. Cleaning: The sample is cleaned to remove any contaminants or residues from previous preparation steps. This is typically done using solvents or plasma cleaning.5. Mounting on a TEM grid: The thinned sample is mounted on a TEM grid, which is a thin metal support that holds the sample in place during imaging.### Specific Techniques for Different Semiconductors.The specific sample preparation techniques used mayvary depending on the type of semiconductor material being studied. Here are some common methods for different semiconductors:Silicon: Mechanical thinning using a dimple grinder followed by chemical etching in a solution of hydrofluoric acid (HF) and nitric acid (HNO3).Gallium arsenide (GaAs): Mechanical thinning using anion miller followed by chemical etching in a solution of HF, HNO3, and hydrogen peroxide (H2O2).Indium phosphide (InP): Mechanical thinning using anion miller followed by chemical etching in a solution of HCl, H2O2, and deionized water.### Advanced Techniques.In addition to the basic sample preparation steps,there are several advanced techniques that can be used toimprove the quality of TEM samples:Focused ion beam (FIB) milling: FIB milling uses a focused beam of ions to precisely thin and shape the sample. This technique allows for the preparation of samples with complex geometries or specific cross-sections.Plasma cleaning: Plasma cleaning uses a low-pressure plasma to remove surface contaminants and improve the sample's conductivity. This is particularly useful for samples that are prone to surface oxidation.Cryo-TEM: Cryo-TEM involves preparing and imaging the sample at cryogenic temperatures. This technique preserves the sample's native state and minimizes beam damage.### Quality Control.The quality of the TEM sample is critical for obtaining reliable results. Several quality control measures can be employed to ensure the sample's integrity:Thickness measurement: The thickness of the sample can be measured using a variety of techniques, such as electron energy loss spectroscopy (EELS) or scanning transmission electron microscopy (STEM).Crystallographic orientation: The crystallographic orientation of the sample can be determined using electron diffraction.Defects and imperfections: The presence of defects or imperfections in the sample can be identified by carefully examining the TEM images.By following these sample preparation procedures and implementing appropriate quality control measures, researchers can obtain high-quality TEM samples that provide valuable insights into the microstructure of semiconductor materials.。
地质学报.英文版.
地质学报.英⽂版.2019-06-251.Taxonomy and Stratigraphy of Late Mesozoic Anurans and Urodeles from ChinaWANG Yuan2.Early Permian Conodonts from the Baoshan Block, Western Yunnan, ChinaJI Zhansheng,YAO Jianxin,JIN Xiaochi,YANG Xiangning,WANG Yizhao,Yang Hailin,WU Guichun3.Conodont Biostratigraphy of the Middle Cambrian through Lowermost Ordovician in Hunan, South ChinaDONG Xiping,John E.REPETSKI,Stig M.BERGSTR(O)M4.K-Ar Geochronology of Mesozoic Mafic Dikes in Shandong Province, Eastern China:Implications for Crustal ExtensionLiu Shen,HU Ruizhong,Zhao Junhong,Feng Caixia5.SHRIMP Geochronology of Volcanics of the Zhangjiakou and Yixian Formations, Northern Hebei Province, with a Discussion on the Age of the Xing'anling Group of the Great Hinggan Mountains and Volcanic Strata of the Southeastern Coastal Area of ChinaNIU Baogui,HE Zhengjun,SONG Biao,REN Jishun,Xiao Liwei6.Panorama of the Opening-Closing Tectonics Theory in ChinaYang Weiran,ZHENG Jiandong7.Characteristics and Tectonic Significance of the Gravity Field in South ChinaYAN Yafen,Wang Guangjie,ZHANG Zhongjie8.Surplus Space Method:A New Numerical Model for Prediction of Shallow-seated Magmatic BodiesDENG Jun,Huang Dinghua,Wang Qingfei,WAN Li,YAO Lingqing,GAO Bangfei,Liu Yan9.An Inverse Analysis of the Comprehensive Medium Parameters and a Simulation of the Crustal Deformation of the Qinghai-Tibet PlateauYang Zhiqiang,Chen Jianbing,JU Tianyi,LI Tianwen10.A Simple Monte Carlo Method for Locating the Three-dimensional Critical Slip Surface of a SlopeXIE Mowen11.Geochemistry of Ore Fluids and Rb-Sr Isotopic Dating for the Wulong Gold Deposit in Liaoning, ChinaWEI Junhao,QIU Xiaoping,GUO Dazhao,Tan Wenjuan12.Distribution Characteristics of Effective Source Rocks and Their Control on Hydrocarbon Accumulation:A Case Study from the Dongying Sag, Eastern ChinaZhu Guangyou,JIN Qiang,ZHANG Shuichang,Dai Jinxing,Zhang Linye,LI Jian13.Speleogenesis of Selected Caves beneath the Lunan Shilin and Caves of Fenglin Karst in Qiubei, YunnanStanka (S)EBELA,Tadej SLABE,LIU Hong,Petr PRUNER14.Abstracts of Acta Geologica Sinica (Chinese edition) Vol.78, No.6, 200415.Contents of Acta Geologica Sinica Vol.78, Nos.1-6, 20041.New Data of Phosphatized Acritarchs from the Ediacaran Doushantuo Formation at Weng'an, Guizhou Province, Southwest China2.A New Genus of Fossil Cycads Yixianophyllum gen. nov. from the Late Jurassic Yixian Formation, Western Liaoning, China3.On a New Genus of Basal Neoceratopsian Dinosaur from the Early Cretaceous of Gansu Province, China4.A Preliminary Study on the Red Beds in the Northern Heyuan Basin, Guangdong Province, China5.Field Relationships, Geochemistry, Zircon Ages and Evolution of a Late Archaean to Palaeoproterozoic Lower Crustal Section in the Hengshan Terrain of Northern China6.Relationships between Basic and Silicic Magmatism in Continental Rift Settings: A Petrogeochemical Study of Carboniferous Post-collisional Rift Silicic Volcanics in Tianshan, NW China7.SHRIMP Age of Exotic Zircons in the Mengyin Kimberlite, Shandong, and Their Formation8.Jurassic Intra-plate Basaltic Magmatism in Southeast China: Evidence from Geological and Geochemical Characteristics of the Chebu Gabbroite in Southern Jiangxi Provincete Paleozoic Fluid Systems and Their Ore-forming Effects in the Yuebei Basin, Northern Guangdong, China10.Origin and Distribution of Groundwater Chemical Fields of the Oilfield in the Songliao Basin, NE China11.Origins of High H2S-bearing Natural Gas in China12.Abstracts of Acta Geologica Sinica (Chinese Edition) Vol. 79, No. 5, 200513.GUIDANCE FOR CONTRIBUTORS1.A New Ceratopsian from the Upper Jurassic Houcheng Formation of Hebei, ChinaZHAO Xijin,CHENG Zhengwu,XU Xing,Peter J. MAKOVICKY2.New Fossil Beetles of the Family Ommatidae (Coleoptera: Archostemata) from the Jehol Biota of ChinaTANJingjing,REN Dong,SHIH Chungkun,GE Siqin3.A Basal Titanosauriform from the Early Cretaceous of Guangxi, ChinaMO Jinyou,WANG Wei,HUANG Zhitao,HUANG Xin,XU Xing4.Discovery of Paleogene Sporopollen from the Matrix Strata of the Naij Tal Group-Complex in the Eastern Kunlun Orogenic BeltGUO Xianpu,WANG Naiwen,DING Xiaozhong,ZHAO Min,WANG Daning5.Dinomischus from the Middle Cambrian Kaili Biota, Guizhou, ChinaPENG Jin,ZHAO Yuanlong,LIN Jih-Pai6.The Liaonan Metamorphic Core Complex: Constitution, Structure and EvolutionLIU Junlai,GUAN Huimei,JI Mo,CAO Shuyun,HU Ling7.Eruption of the Continental Flood Basalts at ~259 Ma in the Emeishan Large Igneous Province, SW China: Evidence from Laser Microprobe 40Ar/39Ar DatingHOU Zengqian,CHEN Wen,LU Jiren8.An Important Spreading Event of the Neo-Tethys Ocean during the Late Jurassic and Early Cretaceous: Evidence from Zircon U-Pb SHRIMP Dating on Diabase in Nagarz(e), Southern TibetJIANG Sihong,NIE Fengjun,HU Peng,LIU Yan 9.Lead Isotopic Composition and Lead Source of the Huogeqi Cu-Pb-Zn Deposit, Inner Mongolia, ChinaZHUXiaoqing,ZHANG Qian,HE Yuliang,ZHU Chaohui10.S, C, O, H Isotope Data and Noble Gas Studies of the Maoniuping LREE Deposit, Sichuan Province, China: A Mantle Connection for MineralizationTIAN Shihong,DING Tiping,MAO Jingwen,LI Yanhe,YUAN Zhongxin11.B, Sr, O and H Isotopic Compositions of Formation Waters from the Bachu Bulge in the Tarim BasinCAIChunfang,PENG Licai,MEI Bowen,XIAO Yingkai12.Mechanism of Varve Formation and Paleoenvironmental Research at Lake Bolterskardet, Svalbard, the ArcticCHU Guoqiang,LIU Jiaqi,GAO Denyi,SUN Qing13.Geochemical Indications of Possible Gas Hydrates in the Northeastern South China SeaLU Zhengquan,WUBihao,ZHU Youhai,QIANG Zuji,WANG Zaimin,ZHANG Fuyuan14.Pyrite Formation in Organic-rich Clay, Calcitic and Coal-Forming EnvironmentsGordana DEVI(C),PetarPFENDT,Branimir JOVAN(C)I(C)EVI(C),Zoran POPOVIC15.An In Vitro Investigation of Pulmonary Alveolar Macrophage Cytotoxicity Introduced by Fibrous and Grainy Mineral DustsDONG Faqin,DENG Jianjun,WU Fengchun,PU Xiaoyong,John HUANG,FENG Qiming,HE Xiaochun16.A Study of Chromium Adsorption on Natural Goethite Biomineralized with Iron BacteriaSUN Zhenya,ZHU Chunshui,HUANG Jiangbo,GONG Wenqi,CHEN Hesheng,MU Shanbin17.Ferruginous Microspherules in Bauxite at Maochang, Guizhou Province, China: Products of Microbe-Pyrite Interaction? ZHOU Yuefei,WANG Rucheng,LU Jianjun,LI Yiliang18.Abstracts of Acta Geologica Sinica (Chinese Edition) Vol. 80, No. 7, 200619.Abstracts of Acta Geologica Sinica (Chinese Edition) Vol. 80, No. 8, 200620.GUIDANCE FOR CONTRIBUTORS1.Jinfengopteryx Compared to Archaeopteryx, with Comments on the Mosaic Evolution of Long-tailed Avialan BirdsJIShu'an,JI Qiang2.New Nodosaurid Dinosaur from the Late Cretaceous of Lishui, Zhejiang Province, ChinaL(U) Junchang,JIN Xingsheng,SHENG Yiming,LI Yihong,WANG Guoping,Yoichi AZUMA3.The First Stegosaur (Dinosauria, Ornithischia) from the Upper Jurassic Shishugou Formation of Xinjiang, ChinaJIA Chengkai,Catherine A. FOSTER,XU Xing,James M. CLARK4.Precious Fossil-Bearing Beds of the Lower Cretaceous Jiufotang Formation in Western Liaoning Province, ChinaZHANG Lijun,YANG Yajun,ZHANG Lidong,GUO Shengzhe,WANG Wuli,ZHENG Shaolin5.Miocene Tectonic Evolution from Dextral-Slip Thrusting to Extension in the Nyainqêntanglha Region of the Tibetan PlateauWU Zhenhan,Patrick J. BAROSH,ZHAO Xun,WU Zhonghai,HU Daogong,LIU Qisheng6.Mesoproterozoic Earthquake Events and Breakup of the Sino-Korean PlateQIAO Xiufu,GAO Linzhi,PENG Yang7.Sedimentology and Chronology of Paleogene Coarse Clastic Rocks in East-Central Tibet and Their Relationship to Early Tectonic UpliftZHOU Jiangyu,WANG Jianghai,K. H. BRIAN,A. YIN,M. S. MATTHEW8.Provenance of Precambrian Fe- and Al-rich Metapelites in the Yenisey Ridge and Kuznetsk Alatau, Siberia: Geochemical SignaturesIgor I. LIKHANOV,Vladimir V. REVERDATTO9.Early Indosinian Weiya Gabbro in Eastern Tianshan, China: Elemental and Sr-Nd-O Isotopic Geochemistry, and Its Tectonic ImplicationsZHANG Zunzhong,GU Lianxing,WU Changzhi,ZHAI Jianping,LI Weiqiang,TANG Junhua10.Diagenesis and Fluid Flow History in Sandstones of the Upper Permian Black Jack Formation, Gunnedah Basin, Eastern AustraliaBAI Guoping,John B. KEENE11.REE Geochemistry of Sulfides from the Huize Zn-Pb Ore Field, Yunnan Province: Implication for the Sources of Ore-forming MetalsLI Wenbo,HUANG Zhilong,QI Liang12.In, Sn, Pb and Zn Contents and Their Relationships in Ore-forming Fluids from Some In-rich and In-poor Deposits in ChinaZHANG Qian,ZHU Xiaoqing,HE Yuliang,ZHU Zhaohui13.Burial Records of Reactive Iron in Cretaceous Black Shales and Oceanic Red Beds from Southern TibetHUANG Yongjian,WANG Chengshan,HU Xiumian,CHEN Xi14.Modes of Occurrence and Geological Origin of Beryllium in Coals from the Pu'an Coalfield, Guizhou, Southwest ChinaYANG Jianye15.40Ar/39Ar Dating of the Shaxi Porphyry Cu-Au Deposit in the Southern Tan-Lu Fault Zone, Anhui ProvinceYANG Xiaoyong,ZHENG Yongfei,XIAO Yilin,DU Jianguo,SUN Weidong16.Carbonate Sequence Stratigraphy of a Back-Arc Basin: A Case Study of the Qom Formation in the Kashan Area, Central IranXU Guoqiang,ZHANG Shaonan,LI Zhongdong,SONG Lailiang,LIU Huimin17.Genetic Relationship between Natural Gas Dispersal Zone and Uranium Accumulation in the Northern Ordos Basin, ChinaGAN Huajun,XIAO Xianming,LU Yongchao,JIN Yongbin,TIAN Hui,LIU Dehan18.Occurrences of Excess 40Ar in Hydrothermal Tourmaline:Interpretations from 40Ar-39Ar Dating Results by Stepwise HeatingQIU Huaning,PU Zhiping,DAI Tongmo19.Removal of Cadmium Ions from Aqueous Solution by Silicate-incorporated HydroxyapatiteSHI Hebin,ZHONG Hong,LIU Yu,DENG Jinyang20.GUIDANCE FOR CONTRIBUTORS1.A New Titanosauriform Sauropod from the Early Late Cretaceous of Dongyang, Zhejiang ProvinceL(U) Junchang,Yoichi AZUMA,CHEN Rongjun,ZHENG Wenjie,JIN Xingsheng2.New Fossil Beetles of the Family Elateridae from the Jehol Biota of China (Coleoptera: Polyphaga)CHANG Huali,REN Dong3.New Record of Palaeoscolecids from the Early Cambrian of Yunnan, ChinaHU Shixue,LI Yong,LUO Huilin,FU Xiaoping,YOU Ting,PANG Jiyuan,LIU Qi,Michael STEINER4.Three New Stoneflies (Insecta: Plecoptera) from the Yixian Formation of Liaoning, ChinaLIU Yushuang,RENDong,Nina D. SINITSHENKOVA,SHIH Chungkun5.Annelid from the Neoproterozoic Doushantuo Formation in Northeastern Guizhou, ChinaWANG Yue,WANG Xunlian6.A New Female Cone, Araucaria beipoiaoensis sp. nov. from the Middle Jurassic Tiaojishan Formation, Beipiao, Western Liaoning, China and Its Evolutionary SignificanceZHENG Shaolin,ZHANG Lidong,ZHANG Wu,YANG Yajun7.The Most Complete Pistosauroid Skeleton from the Triassic of Yunnan, ChinaZHAO Lijun,Tamaki SATO,LI Chun8.Chitinozoans from the Fenxiang Formation (Early Ordovician) of Yichang, Hubei Province, ChinaCHENXiaohong,Florentin PARIS,ZHANG Miao9.Sedimentary Features and Implications for the Precambrian Non-stromatolitic Carbonate Succession: A Case Study of the Mesoproterozoic Gaoyuzhuang Formation at the Qiangou Section in Yanqing County of BeijingMEI Mingxiang10.Jurassic Tectonics of North China: A Synthetic ViewZHANG Yueqiao,DONG Shuwen,ZHAO Yue,ZHANG Tian11.Thick-skinned Contractional Salt Structures in the Kuqa Depression, the Northern Tarim Basin: Constraints from Physical ExperimentsYU Yixin,TANG Liangjie,YANG Wenjing,JIN Wenzheng,PENG Gengxin,LEI Ganglin12.Jurassic Tectonic Revolution in China and New Interpretation of the "Yanshan Movement"DONG Shuwen,ZHANG Yueqiao,LONG Changxing,YANG Zhenyu,JI Qiang,WANG Tao,HU Jianming,CHEN Xuanhuate Mesozoic Thermotectonic Evolution of the Jueluotage Range,Eastern Xinjiang, Northwest China: Evidence from Apatite Fission Track DataZHU Wenbin,WAN Jinglin,SHU Liangshu,ZHANG Zhiyong,SU Jinbao,SUN Yan,GUO Jichun,ZHANG Xueyun14.Basin-and Mountain-Building Dynamic Model of "Ramping-Detachment-Compression" in the West Kunlun-Southern Tarim Basin MarginCUI Junwen,LI Pengwu,GUO Xianpu,DING Xiaozhong,TANG Zhemin15.High Pressure Response of Rutile Polymorphs and Its Significance for Indicating the Subduction Depth of Continental CrustMENG Dawei,WU Xiuling,FAN Xiaoyu,ZHANG Zhengjie,CHEN Hong,MENG Xin,ZHENG Jianping HtTp:// 16.Exsolutions of Diopside and Magnetite in Olivine from Mantle Dunite, Luobusa Ophiolite, Tibet, ChinaRENYufeng,CHEN Fangyuan,YANG Jingsui,GAO Yuanhong17.SAED and HRTEM Investigation of PalygorskiteCHEN Tao,WANG Hejing,ZHANG Xiaoping,ZHENG Nan18.Petrologic and REE Geochemical Characters of Burnt RocksHUANG Lei,LIU Chiyang,YANG Lei,ZHAO Junfeng,FANG Jianjun19.Precise Dating and Geological Significance of the Caledonian Shangyou Pluton in South Jiangxi ProvinceMAO Jianren,ZENG Qingtao,LI Zilong,HU Qing,ZHAO Xilin,YE Haimin20.SHRIMP U-Pb Zircon Dating of the Tula Granite Pluton on the South Side of the Altun Fault and Its Geological ImplicationsWU Suoping,WU Cailai,WANG Meiying,CHEN Qilong,Joseph L. WOODEN21.Geochemistry and SHRIMP Zircon U-Pb Age of Post-Collisional Granites in the Southwest Tianshan Orogenic Belt of China: Examples from the Heiyingshan and Laohutai PlutonsLONG Lingli,GAO Jun,WANG Jingbin,QIANQing,XIONG Xianming,WANG Yuwang,WANG Lijuan,GAO Liming22.Zircon LA-ICP MS U-Pb Age, Sr-Nd-Pb Isotopic Compositions and Geochemistry of the Triassic Post-collisional Wulong Adakitic Granodiorite in the South Qinling, Central China, and Its PetrogenesisQIN Jiangfeng,LAI Shaocong,WANG Juan,LI Yongfei23.Estimating Influence of Crystallizing Latent Heat on Cooling-Crystallizing Process of a Granitic Melt and Its Geological ImplicationsZHANG Bangtong,WU Junqi,LING Hongfei,CHEN Peirong24.Archean Mass-independent Fractionation of Sulfur Isotope:New Evidence of Bedded Sulfide Deposits in the Yanlingguan-Shihezhuang area of Xintai, Shandong ProvinceLI Yanhe,HOU Kejun,WAN Defang,YUE Guoliang 25.Geochemical Mapping: With Special Emphasis on Analytical RequirementsXIE Xuejing,CHENG Hangxin,LIU Dawen1.A Baby Pterodactyloid Pterosaur from the Yixian Formation of Ningcheng, Inner Mongolia, ChinaL(U) Junchang2.A New Theropod Dinosaur from the Middle Jurassic of Lufeng, Yunnan, ChinaWU Xiao-chun,Philip J.CURRIE,DONG Zhiming,PAN Shigang,WANG Tao3.Aerodynamic Characteristics of the Crest with Membrane Attachment on Cretaceous Pterodactyloid NyctosaurusXING Lida,WU Jianghao,LU Yi,L(U) Junchang,JI Qiang4.New Fossil Palaeontinids from the Middle Jurassic of Daohugou, Inner Mongolia, China(Insecta, Hemiptera)WANG Ying,REN Dong5.Evolution of Dentary Diastema in Iguanodontian DinosaursKatsuhiro KUBOTA,Yoshitsugu KOBAYASHI6.Revision of the Clam Shrimp Genus Magumbonia from the Upper Jurassic of the Luanping Basin,Hebei,Northern ChinaLI Gang,SHEN Yanbin,LIU Yongqing,Peter BENGTSON,Helmut WILLEMS,Hiramichi HIRAN07.Yarlongite:A New Metallic Carbide MineralSHI Nicheng,BAI Wenji,LI Guowu,XIONG Ming,FANG Qingsong,YANG Jingsui,MA Zhesheng,RONG He8.Phase Equilibria of Hornblende-Bearing Eclogite in the Western Dabie Mountain,Central ChinaZHANG Jingsen,WEI Chunjing,LOU Yuxing,SU Xiangli9.Diagenesis and Evolution of the Holocene Coquinite from the Haishan Island,Eastern Guangdong,ChinaSUNJinlong,XU Huilong,QIU Xuelin,ZHAN Wenhuan,LI Yamin10.Structural Characteristics and Formation Mechanism in the Micangshan Foreland,South ChinaXU Huaming,LIU Shu,QU Guosheng,LI Yanfeng,SUN Gang,LIU Kang11.Tectonic Evolution of the Middle Frontal Area of the Longmen Mountain Thrust Belt, Western Sichuan Basin, ChinaJIN Wenzheng,TANG Liangjie,YANG Keming,WAN Guimei,L(U) ZhiZhou,YU Yixinx12.Oxygen and Hydrogen Isotopes of Waters in the Ordos Basin,China: Implications for Recharge of Groundwater in the North of Cretaceous Groundwater BasinYANG Yuncheng,SHEN Zhaoli,WENG Dongguang,HOU Guangcai,ZHAO Zhenhong,WANG Dong,PANG Zhonghe13.Variations of Microbial Communities and the Contents and Isotopic Compositions of Total Organic Carbon and Total Nitrogen in Soil Samples during Their PreservationTAO Qianye,LI Yumei,WANG Guo'an,QIAO Yuhui,LIU Tung-Sheng14.Tectonic Landform of Quaternary Lakes and Its Implications for Deformation in the Northern Qinghai-Tibet PlateauWANG An,WANG Guocan,LI Dewei,XIE Defan,LIU Demin15.A Climatic Sequence Stratigraphic Model in the Terrestrial Lacustrine Basin:A Case Study of Green River Formation,Uinta Basin,USAWANG Junling,ZHENG Herong,XIAO Huanqin,ZHONG Guohong,Ronald STEEL,YIN Peigui16.Accumulation Mechanisms and Evolution History of the Giant Puguang Gas Field, Sichuan Basin, ChinaHAOFang,GUO Tonglou,DU Chunguo,ZOU Huayao,CAI Xunyu,ZHU Yangming,LI Pingping,WANGChunwu,ZHANG Yuanchun17.Origin and Accumulation of Natural Gases in the Upper Paleozoic Strata of the Ordos Basin in Central ChinaZHU Yangming,WANG Jibao,LIU Xinse,ZHANG Wenzheng18.Differential Tectonic Deformation of the Longmen Mountain Thrust Belt,Western Sichuan Basin,ChinaTANG Liangjie,YANG Keming,JIN Wenzheng,WAN Guime,L(U) Zhizhou,YU Yixin19.Tectonic Framework and Deep Structure of South China and Their Constraint to Oil-Gas Field DistributionWANG Qingchen,LIU Jinsong,DU Zhili,CAI Liguorge-scale Tazhong Ordovician Reef-fiat Oil-Gas Field in the Tarim Basin of ChinaZHOU Xinyuan,WANG Zhaoming,YANG Haijun,ZHANG Lijuan,HAN Jianfa,WANG Zhenyu注:本⽂为⽹友上传,不代表本站观点,与本站⽴场⽆关。
材料表征技术
入射线
X射线
X射线 晶体结构 衍射规律
试样(晶
体)?
衍射线
分析(结构)
XRD谱 I:强度
d(2):位置
XRD分析
结构
尺度:埃量级—核外电子结构;微米级的晶粒度。 尺度更大的孔隙、裂纹等
结构(或组织结构)(广义)包括从原子结构到 肉眼能观察到的宏观结构各个层次的构造状况的 通称。原子结构、分子结构、晶体结构、电畴结 构等。
材料表征技术(一)
金灯仁
参考书:无机非金属材料测试方法 材料现代分析方法
X射线衍射分析原理、方法、应用 (周上祺)等
(英文版)
绪论(一)
现代分析测试技术:是研究物质的微观状 态与宏观性能之间关系的一种手段.
人们能通过改变分子或晶体的结构来达 到控制物质宏观特性的目的,所以科学 技术的发展离不开分析测试.
• 传统的显微组织结构与成分分析测试方法
光学显微镜:100nm, 表面形态,难以实现同位微 区分析 化学分析:平均成分,不能给出元素分布
• X射线衍射与电子显微分析
• XRD:晶体结构、晶胞参数、晶体缺陷、相等。
• 局限性:无法形貌观察与晶体结构分析微观同位结 合;微 米、纳米级选择性分析
• 电子显微镜(EM,Electron Microscope):用高能电子束 作光源,用磁场作透镜,高分辨率和高放大倍数
• 其它
X射线光电子能谱(XPS)、俄歇电子能谱(AES)、 扫描隧道显微镜(STM)、原子力显微镜(AFM)等
• 要求与目标 正确选择方法、制订方案、分析结果 为以后掌握新方法打基础
• 课程安排
第一章 X射线的性质
• •1.1 引言 • •1.2 X射线的本质 • •1.3 X射线的产生及X射线管 • •1.4 X射线谱 • •1.5 X射线与固体物质相互作用
拦截器多模估计制导控制系统综合设计方法
航天控制Jun.2009-76‘Aer。
spaceContr。
1V01.27,N。
.3拦截器多模估计/制导/控制系统综合设计方法唐治理1雷虎民1邵雷1徐剑芸21.空军工程大学导弹学院,陕西三原7138002.中国空空导弹研究院,河南洛阳471009摘要在拦截高速高机动目标时,针对目标作随机机动,估计、制导系统独立设计的前提条件一分离定理和确定性等价原则不再满足,也不存在一个全局的估计/制导算法对所有的目标机动方式均为最优的问题,讨论了它估计/制导系统综合设计的必要性。
并考虑到制导/控制综合设计的系统比独立设计的制导、控制系统有更优越的性能,以及高阶滑模控制有优良的控制性能,给出了一种基于高阶滑模的多模估计/制导/控制综合设计系统的结构。
关键词动能拦截器;随机机动目标;高阶滑模控制;多模控制中图分类号:V448.2文献标识码:A文章编号:1006-3242(2009)03-0076-04Multi-modelEstimate/Guidance/ControlSystemIntegratedDesignforInterceptorTANGZhililLEIHuminlSHAOLeilXUJianyun21.TheMissileInstitute,AirForceEngineeringUniversity,Shanxi713800,China2.TheAir—to—AirMissileInvestigationInstituteofChina,Luoyang471009,ChinaAbstractWheninterceptsthehighvelocityandhighlymaneuverabletarget,forthemaneuverofthetargetisrandom,theprincipleofseparationandcertaintyequivalencearenotvalidityduringthedes喀nestimatorandguidances弘temofinterceptingmissile,thereisnoglobaloptimalestimate/guidancelawforallfeasi-bletargetmaneuver,therefore,thenecessityofintegrateddesignofe5ti,n口te/g“£d口ncesystemarediscussed.Consideringguidance/controlintegrateddesignsystemisadvantagethantheonewhichseparatedesigned,andhigher—orderslidingmodecontrolhasgoodpeoCormance,ahigher—orderslidingmodecontrolbasedmulti—modelesfimn幻r/guido,暑ce/cDntroZintegrateddes喀nsystemstructureforinterceptormissileispresen-ted.KeywordsKinetickillvehicle;Randommaneuverabletarget;Higher-orderslidingmode;Multi—model高速度高机动弹道目标给拦截器设计提出了严峻的挑战,尤其是针对高速高机动的弹道目标,・总装武器装备预研基金项目(9140A04051M07JB3201);航空科学基金资助项目(2006ZCl2004)收稿日期:2008-02-02作者简介:唐治理(1981一),男,湖南益阳人,博士研究生,主要研究方向为非线性变结构控制理论和非线性飞行器控制系统设计;雷虎民(1960.),男,陕西合阳人,教授,博士生导师,主要研究方向为非线性控制理论及其在飞行器导航、精确制导与控制中的应用;邵雷(1982.),男,湖北天门人,博士研究生,主要研究方向为多模型控制理论及在非线性飞行器控制系统设计中的应用;徐剑芸(1971-),女,陕西汉中人,研究员,主要研究方向为导弹高精度制导与控制律设计及其工程实现。
- 1、下载文档前请自行甄别文档内容的完整性,平台不提供额外的编辑、内容补充、找答案等附加服务。
- 2、"仅部分预览"的文档,不可在线预览部分如存在完整性等问题,可反馈申请退款(可完整预览的文档不适用该条件!)。
- 3、如文档侵犯您的权益,请联系客服反馈,我们会尽快为您处理(人工客服工作时间:9:00-18:30)。
TEM Investigation and FBB Model Explanation to the Phase Relationships between Titanates and Titanium DioxidesHongwei Liu,Eric R.Waclawik,Zhanfeng Zheng,Dongjiang Yang,Xuebin Ke,Huaiyong Zhu,and Ray L.Frost*Discipline of Chemistry,Faculty of Science and Technology,Queensland Uni V ersity of Technology,Brisbane QLD 4001,AustraliaRecei V ed:April 23,2010;Re V ised Manuscript Recei V ed:May 31,2010Sodium and hydrogen titanates fibers and three TiO 2polymorphs (TiO 2(B),anatase,and rutile)were prepared from inorganic titanium compounds by hydrothermal reaction and calcination.The nature and morphologies of the nanofibers with layered structure were investigated by means of X-ray diffraction (XRD)and transmission electron microscopy (TEM).It was revealed that the phase transitions between titanates and titania (via proton titanate)could be interpreted systemically by the fundamental building blocks (FBB)model.The reaction also requires interconversion between some corner-linked and edge-linked pairs of TiO 6octahedrons.A generalized relationship of phase transitions between sodium/hydrogen titanates and titania by the wet-chemical process was proposed.A duplex pentagonal prism scheme was implied to summarize all of the phase relationships between titanates and titania.I.IntroductionMuch attention has been put into the design and fabrication of nanostructures based on metal oxides in the past decade because of their peculiar electronic and optic properties and their potential applications in technology.1-5There is great interest in the development of titanates and TiO 2-based solids with nanoscale dimensions and high morphological specificity 6,7such as nanofibers,8nanosheets,9and nanotubes 10because of their de-monstratedpotentialinsolarenergyconversion,11photocatalysis,12,13photovoltaic devices,14,15and as carrier for metallic nanopar-ticles.16Hydrothermal treatment of different TiO 2precursors in a highly alkaline medium is a powerful way to prepare nanotubes and nanowires,but the information about the structure of the synthesized nanostructures is still unclear despite intensive investigations.In contradiction with previous investigations,Sun et al.17report that as-synthesized nanotubes are titanates and can be described as Na x H 2-x Ti 3O 7.Thermal treatment of these materials leads to the formation of different titanates with the general formula Na 2Ti n O 2n +1.Recently,it was also mentioned that as-synthesized nanotubes or nanorods have an even more complex structure,Na x H 2-x Ti n O 2n +1·y H 2O.18-20Treatment of these nanoparticles with a HCl solution produced nanotubes and nanorods of H 2Ti 3O 7.Although the importance of continuing efforts to develop alternate approaches to the synthesis of the nanostructures has been realized,4the potential for controlled reactions of these nanostructures has not drawn significant attention.In fact,phase transitions at moderate temperature are strongly preferred for constructing inorganic structures on nanometer scale (nano-scale)21because the delicate nanostructures can easily be lost at high temperatures due to sintering.The present authors’recent work has described a reversible scheme of transitions between nanoscale titanium dioxides to and from nanoscale titanates.22We found for the first time that phase transitions from the titanate nanostructures to TiO 2polymorphs take place readilyin wet-chemical processes at temperatures close to ambient.Furthermore,the resultant TiO 2nanocrystals can react with concentrated NaOH solution,yielding hollow titanate nanotubes.In the present work,we report phase transitions from titanate fibers to hexatitanate,TiO 2(B),and anatase.The phase transitions are systematically explained by a fundamental building blocks (FBB)model,and a stereoschematic is implied on the basis of the above explanation.II.Experimental Section1.Sample Preparation.NaOH pellets and HNO 3(both are AR grade from Aldrich)and TiOSO 4·x H 2O (98%,from Fluka)were used in the synthesis.Titanate nanofibers in this study were prepared via a hydrothermal reaction between a concen-trated NaOH solution and an inorganic titanium salt.15Specif-ically,10.7g of TiOSO 4·H 2O was dissolved into 80mL of water and stirred until becoming clear.The resultant TiOSO 4solution was mixed with 100mL of 15M NaOH solution while stirring.The mixture (white suspension)was then transferred into a 200mL Teflon-lined stainless steel autoclave and kept at a temperature between ambient and 200°C for 48h to yield titanate precipitates via a hydrothermal reaction.The white precipitate in the autoclaved mixture was recovered by cen-trifugation and washed with deionized water four times by dispersing the wet cake into 100mL of water and recovering the solid by centrifugation.The sodium titanate product was labeled as T3.T3was calcinated at 500°C for 16h under air flow to obtain a new titanate T6.The sodium titanates T3and T6were then neutralized using 0.1M HCl solution and washed with water to remove most of the sodium ions.We dried the resultant hydrogen titanate (H-titanate;denoted as T3-H and T6-H,respectively)at 100°C for 16h and then dispersed this into a dilute (0.05M)HNO 3solution,at temperatures selected to form anatase (TA).On the other hand,the resultant hydrogen titanate (H-titanate)was carried out at 500°C in an atmosphere of air flow (20cm 3/min)to obtain TiO 2(B)(denoted as “TB”).Standard laboratory safety precautions,including the use of appropriate hoods,*Corresponding author.E-mail:r.frost@.au.J.Phys.Chem.C 2010,114,11430–114341143010.1021/jp103644x 2010American Chemical SocietyPublished on Web 06/14/2010vessels,and safety gloves,were required when handling the strong acids and bases.2.Sample Characterization.The microstructures and mor-phologies of products were investigated using transmission electron microscopy (TEM)and X-ray diffraction (XRD)techniques.TEM images were recorded on a Philips CM20TEM,employing an accelerating voltage of 200kV and double-tilt holder.High-resolution transmission electron microscopy (HRTEM)was carried out on a Philips Tecnai F20under an accelerating voltage of 200kV.XRD patterns of the sample powders were recorded using a Shimadzu XRD-6000diffrac-tometer,equipped with a graphite monochromator.Cu K R radiation (λ)0.15418nm)and a fixed power source (40kV and 40mA)were used.The samples were scanned at a rate of 1°(2θ)/min over a range of 2-80°,which covers the main characteristic diffraction peaks of the titanates,anatase,and TiO 2(B).X-ray photoelectron spectroscopy (XPS)spectra were recorded in an ESCALAB 250spectrometer,and Al K R radiation was used as the X-ray source.The C1s peak at 284.5eV was used as a reference for the calibration of the binding energy (BE)scale.III.Results and Discussion3.1.Phase Transformations from Titanate to Titania.The preparation procedure of the samples used here is shown in Scheme 1summarized from the viewpoint of phase transforma-tion.The phase transformations were investigated by X-ray diffraction (Figure 1).The directly obtained product (T3,Figure 1A)from hydro-thermal reaction is consistent mainly with tritanate phase (Na 2Ti 3O 7,monoclinic,S.G.P 21/m ,a )0.8566nm,b )0.3804nm,c )0.9133nm, )101.57°,ICSD #250000),althoughthere are some impurities,which is similar to the result given by Kolen’ko et al.23X-ray photoelectron spectroscopy (XPS)of the surface indicated that this washed product possessed a sodium content of ∼10wt %Na.The T3was converted to T6shown in Figure 1B (Na 2Ti 6O 13,monoclinic,S.G.C 2/m ,a )1.513nm,b )0.3745nm,c )0.9159nm, )99.30°,ICSD #23877)after calcining at 500°C.Proton titanate T6-H (H 2Ti 6O 13,Figure 1C)was obtained by ion-exchange of the Na with H from the respective sodium titanate T6.It is noted that the basal structure of proton titanate was not changed,although the ion-exchange process results in the decrease of the d -spacing in the layered structure.Calcining the proton titanate T6-H yielded TB shown in Figure 1D (TiO 2(B),monoclinic,S.G.C 2/m ,a )0.6524nm,b )0.3740nm,c )01.218nm, )107.05°,ICSD #41056),TA shown in Figure 1E (anatase,tetragonal,S.G.I 41/amd ,a )0.3782nm,c )0.9502nm,ICSD #63711),depending on the calcination temperature.It is noteworthy that the fibril morphology was heritage from T3for all of the above samples.All of the obtained titania phases can react with concentrated NaOH solution and yield trititanate.In addition,the phases involved here exhibit a complicated transition relationship,which has been summarized in Figure 2.All titanates on the green plane in Figure 2can be converted into titania directly by an acid-assisted wet-chemical process as reported earlier.163.2.TEM Observation.The phase transition process was also confirmed by transmission electron microscopy (TEM)and corresponding electron diffraction (ED)patterns,as shown in Figure 3.The lattice parameters for the samples were calculated from ED patterns and listed in Table 1.Figure 3A shows a typical low-magnification TEM image of as-prepared nanofibers of T3sample.The corresponding ED patterns (Figure 3B)indicate that it has a high crystallinity of the nanostructures,which are also confirmed by XRD.The ED patterns can be indexed as the monoclinic C 2/m space group,using the Na 2Ti 3O 7parameters.Figure 3C shows a typical low-magnification TEM image of as-prepared nanofibers of T6sample.The correspond-ing ED patterns (Figure 3D)indicate that this sample has also a high crystallinity of the nanostructures,which are confirmed by XRD.The ED patterns can be indexed as the monoclinic P 21space group,using the Na 2Ti 6O 13parameters.The zone axis is [001].Figure 3E shows a low-magnification image of proton titanate T6-H (H 2Ti 6O 13),a product of ion exchange of T6.The powder X-ray diffraction pattern of the sample reveals that the crystal structure is almost the same as that of T6because the positions of peaks of the sample are almost coincident with those of T6.It could be deduced that the structure of the sample is the sameSCHEME 1:Schematic Showing Phase Transformation Relationships between the Samples Used in This StudyaaT3(6)represents trititanate (hexatitanate).T3(6)-H represents proton trititanate(hexatitanate).Figure 1.Powder X-ray diffraction patterns of the titania-basednanofibers.Figure 2.A generalized phase transition between sodium-and hydrogen-titanates,anatase,TiO 2(B),and rutile by the wet-chemical process.Phase Relationships between Titanates and Titanium Dioxides J.Phys.Chem.C,Vol.114,No.26,201011431as T6based on the relationship of the crystal structure between T3and T3-H.The ED taken down [001]is shown in Figure 2F.The lattice parameters determined by ED are about 1.46nm for a ,0.382nm for b ,and 1.30for c ,which slightly depart from those of T6.Figure 3G and I show the TEM micrograph of TB (TiO 2(B))and TA (anatase)samples.The corresponding ED for TB sample (Figure 3H)down [001]can be indexed as the monoclinic C 2/m space group,using the TiO 2(B)parameters.The correspondingED down [67j 1]for TA is shown in Figure 3J,and can be indexed as the tetragonal I 41/amd space group,using the anatase parameters.3.3.FBB Model Explanation to Phase Transitions be-tween Titanates and Titania.There are many ways developed to describe the structures and the relationships between inorganic crystals.Veblen has discussed the utility of the poly somatic-series approach.24It cannot be simply applied to describe the TiO 2polymorphs,primarily because of the absence of slabs common to all polymorphs.In this work,the titanium oxide structures will be discussed on the approach based on the use of fundamental building blocks (FBB),25emphasized by the similarities between the structures.Banfield 26has used this model to represent the relationships among the TiO 2minerals.All of the structures except rutile related in this study can be constructed from a unit composed of four edge-sharing octa-hedrons,which are shown in Figure4.The difference between the corner-shared octahedrons and edge-shared octahedrons is marked with arrows.Thus,polyhedral representation of the structures of titanate and titania in this work can be described as Figure 5.It is shown in Figure 5the polyhedral representation of the structures of titanate and titania.All of the projections are viewed down [010]except rutile (down [001]).In Figure 5a,every three TiO 6octahedrons form a slab by edge-sharing,and the slabs connect with each other to form a layer of TiO 6octahedrons in corner-linked mode.Thus,upper-layer and lower-layer TiO 6octahedrons form layered-structural trititanate.If atomic sites between TiO 6slab layers are occupied by sodium ions,it is sodium titanate (Figure 5a).If they are taken by hydrogen ions,it is hydrogen trititanate (Figure 5b).If TiO 6layers in trititanate are connected in corner-linked mode,it will change into microporous structure.Thus,sodium hexati-tanate and hydrogen hexatitanate can be obtained as shown in Figure 5c and d.Given the absence of ions,if all TiO 6octahedrons are corner-linked,we can get rutile (Figure 5g).Similarly,if all octahedrons are edge-linked,we can get TiO 2(B)(Figure 5e)or anatase (Figure 5f).By applying the FBB model,the present authors have successfully explained the structural evolution in several transi-tion systems,such as the absorption of ammonium ions,27bivalent Ba and Sr cations 28,29by trititanate,and conversion of trititanate to hexatitanate.30A PBB schematic representing the transition of Na 2Ti 3O 7to TiO 2(B)is implied in Figure 6.There are four steps that are needed for converting this structural transition.Figure 6A shows an undistorted representation of the Na 2Ti 3O 7structure viewed down [010].The conversion from Na 2Ti 3O 7to TiO 2(B)requires replacement of Na cations with hydrogen ions,whichcorre-Figure 3.TEM microstructure of the samples used in this study.PanelsA,C,E,G,and I are T3,T6,T6-H,TB,and TA fibers,respectively.Panels B,D,F,H,and J are the electron diffraction patterns corresponding to the above samples in the same sequence.TABLE 1:Phase Compositions and Crystallographic Parameters for Nanofiberscrystal structureparameters (nm)reference phasecomposition space group a bc(deg)Ti3Na 2Ti n O 2n +1,n )3,4,9C 2/m 1.5130.3750.91699.3T6Na 2Ti 6O 13P21 1.560.378 1.22105Ti6-H a H 2Ti 6O 13P21 1.460.38 1.30105TB TiO 2(B)C 2/m 1.2160.3740.651107.29TAanataseI 41/amd0.37890.9537aCrystalline parameters for Ti6-H are measured in this study.11432J.Phys.Chem.C,Vol.114,No.26,2010Liu et al.sponds to step I.The reaction also requires interconversion between some corner-linked and edge-linked pairs of Ti -O 6octahedra,which have been illustrated in Figure 6b and c.The slab of TiO 6octahedron in trititanate is -3-3-3-;that is,every three edge-shared octahedrons connect mutually by corner-sharing,which will become -2-2-2-after conversion in step II (Figure 6c)and step III (Figure 6d).The structure of TiO 2(B)(Figure 6e)thus becomes reality by relative slipping of upper layer and lower layer (step III)followed by dehydration (step IV),as shown in the enlarged inset of Figure 6.IV.ConclusionThe phase transformations from sodium trititanate to hexati-tanate and from proton titanate to TiO 2(B)and anatase were investigated by XRD and TEM.It was revealed that the phase transitions and morphological derivation between titanates,anatase,and TiO 2(B)(via proton titanate)could be interpreted systemically by the fundamental building blocks model (FBB).A generalized relationship of phase transitions between sodiumand hydrogen titanates,anatase,TiO 2(B),and rutile by the wet-chemical process was then proposed.A duplex pentagonal prism scheme was then implied to summarize all of the relationships between titanates and titania including this work and previous work.It is the first time in which seven compounds of titanium have been made into one stereoscheme,showing the complex connections among them.Acknowledgment.The financial and infra-structure support of the Queensland University of Technology Inorganic Materials Research Program of the School of Physical and Chemical Sciences is gratefully acknowledged.The Australian Research Council (ARC)is thanked for funding the instrumentation.References and Notes(1)Li,D.;Xia,Y.Ad V .Mater.2004,16,1151–1170.(2)Limmer,S.J.;Cao,G.Ad V .Mater.2003,15,427–431.(3)Xia,Y.;Yang,P.;Sun,Y.;Wu,Y.;Mayers,B.;Gates,B.;Yin,Y.;Kim,F.;Yan,H.Ad V .Mater.2003,15,353–389.(4)Rao,C.N.R.;Deepak,F.L.;Gundiah,G.;Govindaraj,A.Prog.Solid State Chem.2003,31,5–147.(5)Patzke,G.R.;Krumeich,F.;Nesper,R.Angew.Chem.,Int.Ed.2002,41,2446–2461.(6)Hennings,D.;Klee,M.;Waser,R.Ad V .Mater.1991,3,334–340.(7)Newnham,R.E.MRS Bull.1997,22,20–33.(8)Gao,X.P.;Zhu,H.Y.;Pan,G.L.;Ye,S.H.;Lan,Y.;Wu,F.;Song,D.Y.J.Phys.Chem.B 2004,108,2886–2872.(9)Sukpirom,N.;Lerner,M.M.Chem.Mater.2001,13,2179–2185.(10)Kasuga,T.;Hiramatsu,M.;Hoson,A.;Sekino,T.;Niihara,ngmuir 1998,14,3160–3163.(11)Gra ¨tzel,M.Nature 2001,414,338–344.(12)Fujishima,A.;Hashimoto,K.;Watanabe,T.TiO 2Photocatalysis Fundamentals and Applications ;BKC,Inc.:Tokyo,1999.Figure 4.A scheme of functional buildingblocks.Figure 5.Polyhedral representation of the structures of titanate and titania.All of the projections are down [010]except rutile (down[001]).Figure 6.Diagram illustrating the stepwise conversion of Na 2Ti 3O 7(a)to TiO 2(B)(d).Parts (b)and (c)are the proposed intermediate.Phase Relationships between Titanates and Titanium Dioxides J.Phys.Chem.C,Vol.114,No.26,201011433(13)Linsebigler,A.L.;Lu,G.;Yates,J.T.Chem.Re V.1995,95,735–758.(14)Sugiura,T.;Yoshida,T.;Minoura,H.Electrochem.Solid-State Lett. 1998,1,175–177.(15)Tokudome,H.;Miyauchi,mun.2004,958–959.(16)Huang,J.G.;Kunitake,T.;Onoue,mun.2004, 1008–1009.(17)Sun,X.;Li,Y.Chem.-Eur.J.2003,9,2229–2238.(18)Armstrong,G.;Armstrong,A.R.;Canales,J.;Bruce,P.G.Chem. Commun.2005,2454–2456.(19)Armstrong,A.R.;Armstrong,G.;Canales,J.;Garsia,R.;Bruce, P.G.Ad V.Mater.2005,17,862–865.(20)Armstrong,A.R.;Armstrong,G.;Canales,J.;Bruce,P.G.Angew. Chem.,Int.Ed.2004,43,2286–2288.(21)Zhu,H.Y.;Gao,X.P.;Lan,Y.;Song,D.Y.;Xi,Y.X.;Zhao, J.C.J.Am.Chem.Soc.2004,126,8380–8381.(22)Zhu,H.Y.;Lan,Y.;Gao,X.P.;Ringer,S.P.;Zheng,Z.F.;Song,D.Y.;Zhao,J.C.J.Am.Chem.Soc.2005,127,6730–6736.(23)Kolen’ko,Y.V.;Kovnir,K.A.;Gavrilov,A.I.;Garshev,A.V.; Frantti,J.;Lebedev,O.I.;Churagulov,B.R.;Gustaaf Van Tendeloo,G.V.; Yoshimura,M.J.Phys.Chem.B2006,110,4030–4038.(24)Veblen,D.R.Am.Mineral.1991,76,801–826.(25)Moor,P.B.Am.Mineral.1986,71,540–546.(26)Banfield,J.F.;Veblen,D.R.Am.Mineral.1992,77,545–557.(27)Yang,D.J.;Zheng,Z.F.;Zhu,H.Y.;Liu,H.W.;Gao,X.P.Ad V. Mater.2008,20,2777–2781.(28)Liu,H.W.;Yang,D.J.;Waclawik,E.R.;Ke,X.B.;Zheng,Z.F.; Zhu,H.Y.;Frost,R.L.J.Raman Spectrosc.,in press.(29)Liu,H.W.;Zheng,Z.F.;Yang,D.J.;Waclawik,E.R.;Ke,X.B.; Zhu,H.Y.;Frost,R.L.J.Raman Spectrosc.,in press.(30)Yang,D.J.;Zheng,Z.F.;Yuan,Y.;Liu,H.W.;Waclawik,E.R.; Ke,X.B.;Xie,M.X.;Zhu,H.Y.Phys.Chem.Chem.Phys.2010,12, 1271–1277.JP103644X11434J.Phys.Chem.C,Vol.114,No.26,2010Liu et al.。