Performance models for large scale multi-agent systems Using distributed pomdp building blo

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PACSnumbers1215Ff,1130Hv,1210Dm,1125Mj…

PACSnumbers1215Ff,1130Hv,1210Dm,1125Mj…

a r X i v :0803.2889v 2 [h e p -p h ] 14 J u l 2008Mapping Out SU (5)GUTs with Non-Abelian Discrete Flavor SymmetriesFlorian Plentinger ∗and Gerhart Seidl †Institut f¨u r Physik und Astrophysik,Universit¨a t W¨u rzburg,Am Hubland,D 97074W¨u rzburg,Germany(Dated:December 25,2013)We construct a class of supersymmetric SU (5)GUT models that produce nearly tribimaximal lepton mixing,the observed quark mixing matrix,and the quark and lepton masses,from discrete non-Abelian flavor symmetries.The SU (5)GUTs are formulated on five-dimensional throats in the flat limit and the neutrino masses become small due to the type-I seesaw mechanism.The discrete non-Abelian flavor symmetries are given by semi-direct products of cyclic groups that are broken at the infrared branes at the tip of the throats.As a result,we obtain SU (5)GUTs that provide a combined description of non-Abelian flavor symmetries and quark-lepton complementarity.PACS numbers:12.15.Ff,11.30.Hv,12.10.Dm,One possibility to explore the physics of grand unified theories (GUTs)[1,2]at low energies is to analyze the neutrino sector.This is due to the explanation of small neutrino masses via the seesaw mechanism [3,4],which is naturally incorporated in GUTs.In fact,from the perspective of quark-lepton unification,it is interesting to study in GUTs the drastic differences between the masses and mixings of quarks and leptons as revealed by current neutrino oscillation data.In recent years,there have been many attempts to re-produce a tribimaximal mixing form [5]for the leptonic Pontecorvo-Maki-Nakagawa-Sakata (PMNS)[6]mixing matrix U PMNS using non-Abelian discrete flavor symme-tries such as the tetrahedral [7]and double (or binary)tetrahedral [8]groupA 4≃Z 3⋉(Z 2×Z 2)and T ′≃Z 2⋉Q,(1)where Q is the quaternion group of order eight,or [9]∆(27)≃Z 3⋉(Z 3×Z 3),(2)which is a subgroup of SU (3)(for reviews see, e.g.,Ref.[10]).Existing models,however,have generally dif-ficulties to predict also the observed fermion mass hierar-chies as well as the Cabibbo-Kobayashi-Maskawa (CKM)quark mixing matrix V CKM [11],which applies especially to GUTs (for very recent examples,see Ref.[12]).An-other approach,on the other hand,is offered by the idea of quark-lepton complementarity (QLC),where the so-lar neutrino angle is a combination of maximal mixing and the Cabibbo angle θC [13].Subsequently,this has,in an interpretation of QLC [14,15],led to a machine-aided survey of several thousand lepton flavor models for nearly tribimaximal lepton mixing [16].Here,we investigate the embedding of the models found in Ref.[16]into five-dimensional (5D)supersym-metric (SUSY)SU (5)GUTs.The hierarchical pattern of quark and lepton masses,V CKM ,and nearly tribi-maximal lepton mixing,arise from the local breaking of non-Abelian discrete flavor symmetries in the extra-dimensional geometry.This has the advantage that theFIG.1:SUSY SU (5)GUT on two 5D intervals or throats.The zero modes of the matter fields 10i ,5H,24H ,and the gauge supermul-tiplet,propagate freely in the two throats.scalar sector of these models is extremely simple without the need for a vacuum alignment mechanism,while of-fering an intuitive geometrical interpretation of the non-Abelian flavor symmetries.As a consequence,we obtain,for the first time,a realization of non-Abelian flavor sym-metries and QLC in SU (5)GUTs.We will describe our models by considering a specific minimal realization as an example.The main features of this example model,however,should be viewed as generic and representative for a large class of possible realiza-tions.Our model is given by a SUSY SU (5)GUT in 5D flat space,which is defined on two 5D intervals that have been glued together at a common endpoint.The geom-etry and the location of the 5D hypermultiplets in the model is depicted in FIG.1.The two intervals consti-tute a simple example for a two-throat setup in the flat limit (see,e.g.,Refs.[17,18]),where the two 5D inter-vals,or throats,have the lengths πR 1and πR 2,and the coordinates y 1∈[0,πR 1]and y 2∈[0,πR 2].The point at y 1=y 2=0is called ultraviolet (UV)brane,whereas the two endpoints at y 1=πR 1and y 2=πR 2will be referred to as infrared (IR)branes.The throats are supposed to be GUT-scale sized,i.e.1/R 1,2 M GUT ≃1016GeV,and the SU (5)gauge supermultiplet and the Higgs hy-permultiplets 5H and2neously broken to G SM by a 24H bulk Higgs hypermulti-plet propagating in the two throats that acquires a vac-uum expectation value pointing in the hypercharge direc-tion 24H ∝diag(−12,13,15i ,where i =1,2,3is the generation index.Toobtainsmall neutrino masses via the type-I seesaw mechanism [3],we introduce three right-handed SU (5)singlet neutrino superfields 1i .The 5D Lagrangian for the Yukawa couplings of the zero mode fermions then readsL 5D =d 2θ δ(y 1−πR 1) ˜Y uij,R 110i 10j 5H +˜Y d ij,R 110i 5H +˜Y νij,R 15j5i 1j 5H +M R ˜Y R ij,R 21i 1j+h.c. ,(3)where ˜Y x ij,R 1and ˜Y x ij,R 2(x =u,d,ν,R )are Yukawa cou-pling matrices (with mass dimension −1/2)and M R ≃1014GeV is the B −L breaking scale.In the four-dimensional (4D)low energy effective theory,L 5D gives rise to the 4D Yukawa couplingsL 4D =d 2θ Y u ij 10i 10j 5H +Y dij10i 5H +Y νij5i ∼(q i 1,q i 2,...,q i m ),(5)1i ∼(r i 1,r i 2,...,r im ),where the j th entry in each row vector denotes the Z n jcharge of the representation.In the 5D theory,we sup-pose that the group G A is spontaneously broken by singly charged flavon fields located at the IR branes.The Yukawa coupling matrices of quarks and leptons are then generated by the Froggatt-Nielsen mechanism [21].Applying a straightforward generalization of the flavor group space scan in Ref.[16]to the SU (5)×G A represen-tations in Eq.(5),we find a large number of about 4×102flavor models that produce the hierarchies of quark and lepton masses and yield the CKM and PMNS mixing angles in perfect agreement with current data.A distri-bution of these models as a function of the group G A for increasing group order is shown in FIG.2.The selection criteria for the flavor models are as follows:First,all models have to be consistent with the quark and charged3 lepton mass ratiosm u:m c:m t=ǫ6:ǫ4:1,m d:m s:m b=ǫ4:ǫ2:1,(6)m e:mµ:mτ=ǫ4:ǫ2:1,and a normal hierarchical neutrino mass spectrumm1:m2:m3=ǫ2:ǫ:1,(7)whereǫ≃θC≃0.2is of the order of the Cabibbo angle.Second,each model has to reproduce the CKM anglesV us∼ǫ,V cb∼ǫ2,V ub∼ǫ3,(8)as well as nearly tribimaximal lepton mixing at3σCLwith an extremely small reactor angle 1◦.In perform-ing the group space scan,we have restricted ourselves togroups G A with orders roughly up to 102and FIG.2shows only groups admitting more than three valid mod-els.In FIG.2,we can observe the general trend thatwith increasing group order the number of valid modelsper group generally increases too.This rough observa-tion,however,is modified by a large“periodic”fluctu-ation of the number of models,which possibly singlesout certain groups G A as particularly interesting.Thehighly populated groups would deserve further system-atic investigation,which is,however,beyond the scopeof this paper.From this large set of models,let us choose the groupG A=Z3×Z8×Z9and,in the notation of Eq.(5),thecharge assignment101∼(1,1,6),102∼(0,3,1),103∼(0,0,0),52∼(0,7,0),52↔4FIG.3:Effect of the non-Abelian flavor symmetry on θ23for a 10%variation of all Yukawa couplings.Shown is θ23as a function of ǫfor the flavor group G A (left)and G A ⋉G B (right).The right plot illustrates the exact prediction of the zeroth order term π/4in the expansion θ23=π/4+ǫ/√2and the relation θ13≃ǫ2.The important point is that in the expression for θ23,the leading order term π/4is exactly predicted by thenon-Abelian flavor symmetry G F =G A ⋉G B (see FIG.3),while θ13≃θ2C is extremely small due to a suppression by the square of the Cabibbo angle.We thus predict a devi-ation ∼ǫ/√2,which is the well-known QLC relation for the solar angle.There have been attempts in the literature to reproduce QLC in quark-lepton unified models [26],however,the model presented here is the first realization of QLC in an SU (5)GUT.Although our analysis has been carried out for the CP conserving case,a simple numerical study shows that CP violating phases (cf.Ref.[27])relevant for neutri-noless double beta decay and leptogenesis can be easily included as well.Concerning proton decay,note that since SU (5)is bro-ken by a bulk Higgs field,the broken gauge boson masses are ≃M GUT .Therefore,all fermion zero modes can be localized at the IR branes of the throats without intro-ducing rapid proton decay through d =6operators.To achieve doublet-triplet splitting and suppress d =5pro-ton decay,we may then,e.g.,resort to suitable extensions of the Higgs sector [28].Moreover,although the flavor symmetry G F is global,quantum gravity effects might require G F to be gauged [29].Anomalies can then be canceled by Chern-Simons terms in the 5D bulk.We emphasize that the above discussion is focussed on a specific minimal example realization of the model.Many SU (5)GUTs with non-Abelian flavor symmetries,however,can be constructed along the same lines by varying the flavor charge assignment,choosing different groups G F ,or by modifying the throat geometry.A de-tailed analysis of these models and variations thereof will be presented in a future publication [30].To summarize,we have discussed the construction of 5D SUSY SU (5)GUTs that yield nearly tribimaximal lepton mixing,as well as the observed CKM mixing matrix,together with the hierarchy of quark and lepton masses.Small neutrino masses are generated only by the type-I seesaw mechanism.The fermion masses and mixings arise from the local breaking of non-Abelian flavor symmetries at the IR branes of a flat multi-throat geometry.For an example realization,we have shown that the non-Abelian flavor symmetries can exactly predict the leading order term π/4in the sum rule for the atmospheric mixing angle,while strongly suppress-ing the reactor angle.This makes this class of models testable in future neutrino oscillation experiments.In addition,we arrive,for the first time,at a combined description of QLC and non-Abelian flavor symmetries in SU (5)GUTs.One main advantage of our setup with throats is that the necessary symmetry breaking can be realized with a very simple Higgs sector and that it can be applied to and generalized for a large class of unified models.We would like to thank T.Ohl for useful comments.The research of F.P.is supported by Research Train-ing Group 1147“Theoretical Astrophysics and Particle Physics ”of Deutsche Forschungsgemeinschaft.G.S.is supported by the Federal Ministry of Education and Re-search (BMBF)under contract number 05HT6WWA.∗********************************.de †**************************.de[1]H.Georgi and S.L.Glashow,Phys.Rev.Lett.32,438(1974);H.Georgi,in Proceedings of Coral Gables 1975,Theories and Experiments in High Energy Physics ,New York,1975.[2]J.C.Pati and A.Salam,Phys.Rev.D 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D.Carone and R.F.Lebed,Phys.Rev.D62,016009(2000);P.D.Carr and P.H.Frampton,arXiv:hep-ph/0701034;A.Aranda, Phys.Rev.D76,111301(2007).[9]I.de Medeiros Varzielas,S.F.King and G.G.Ross,Phys.Lett.B648,201(2007);C.Luhn,S.Nasri and P.Ramond,J.Math.Phys.48,073501(2007);Phys.Lett.B652,27(2007).[10]E.Ma,arXiv:0705.0327[hep-ph];G.Altarelli,arXiv:0705.0860[hep-ph].[11]N.Cabibbo,Phys.Rev.Lett.10,531(1963);M.Kobayashi and T.Maskawa,Prog.Theor.Phys.49, 652(1973).[12]M.-C.Chen and K.T.Mahanthappa,Phys.Lett.B652,34(2007);W.Grimus and H.Kuhbock,Phys.Rev.D77, 055008(2008);F.Bazzocchi et al.,arXiv:0802.1693[hep-ph];G.Altarelli,F.Feruglio and C.Hagedorn,J.High Energy Phys.0803,052(2008).[13]A.Y.Smirnov,arXiv:hep-ph/0402264;M.Raidal,Phys.Rev.Lett.93,161801(2004);H.Minakata andA.Y.Smirnov,Phys.Rev.D70,073009(2004).[14]F.Plentinger,G.Seidl and W.Winter,Nucl.Phys.B791,60(2008).[15]F.Plentinger,G.Seidl and W.Winter,Phys.Rev.D76,113003(2007).[16]F.Plentinger,G.Seidl and W.Winter,J.High EnergyPhys.0804,077(2008).[17]G.Cacciapaglia,C.Csaki,C.Grojean and J.Terning,Phys.Rev.D74,045019(2006).[18]K.Agashe,A.Falkowski,I.Low and G.Servant,J.HighEnergy Phys.0804,027(2008);C.D.Carone,J.Erlich and M.Sher,arXiv:0802.3702[hep-ph].[19]Y.Kawamura,Prog.Theor.Phys.105,999(2001);G.Altarelli and F.Feruglio,Phys.Lett.B511,257(2001);A.B.Kobakhidze,Phys.Lett.B514,131(2001);A.Hebecker and J.March-Russell,Nucl.Phys.B613,3(2001);L.J.Hall and Y.Nomura,Phys.Rev.D66, 075004(2002).[20]D.E.Kaplan and T.M.P.Tait,J.High Energy Phys.0111,051(2001).[21]C.D.Froggatt and H.B.Nielsen,Nucl.Phys.B147,277(1979).[22]Y.Nomura,Phys.Rev.D65,085036(2002).[23]H.Georgi and C.Jarlskog,Phys.Lett.B86,297(1979).[24]H.Arason et al.,Phys.Rev.Lett.67,2933(1991);H.Arason et al.,Phys.Rev.D47,232(1993).[25]D.S.Ayres et al.[NOνA Collaboration],arXiv:hep-ex/0503053;Y.Hayato et al.,Letter of Intent.[26]S.Antusch,S.F.King and R.N.Mohapatra,Phys.Lett.B618,150(2005).[27]W.Winter,Phys.Lett.B659,275(2008).[28]K.S.Babu and S.M.Barr,Phys.Rev.D48,5354(1993);K.Kurosawa,N.Maru and T.Yanagida,Phys.Lett.B 512,203(2001).[29]L.M.Krauss and F.Wilczek,Phys.Rev.Lett.62,1221(1989).[30]F.Plentinger and G.Seidl,in preparation.。

程式性直流电压负载 Chroma 63200系列说明书

程式性直流电压负载 Chroma 63200系列说明书

ProgrammableChroma's 63200 series of programmable electronicloads are designed for a wide variety of dc powerconversion products including; DC power sources,battery chargers, server power supplies, dc-dcconverters, batteries and many others. Thehigh power rating, parallel and synchronizationcapabilities, and the ability to provide up to 2.7times of rated power for short duty cycle loadingmake 63200 series especially well-suited for highpower applications such as switch-mode rectifiersand for discharging batteries packs and fuel cells.The 63200 series offers 12 different models withpower ranges from 2600 watts to 15600 watts,currents from 50A to 1000A and operatingvoltages from 0 to 1000V. By paralleling modulesvery large systems can be assembled existing93.6kW. Four operating modes provide differentload simulation methods designed for variousapplications. The CC/CR modes are designedto test constant voltage power supplies andconverters. CV mode simulates the battery fortesting battery chargers and current sources, andCP mode is ideal for battery testing by simulatingreal discharge profiles.The 63200 series can sink rated current downto 1VDC even under the highest specified risetime. This unique feature guarantees the bestloading performance for low voltage/high currentapplications. With it's unique external waveformsimulation and Master / Slave control capability,the 63200 series electronic loads allow users toparallel and synchronize more than one loadtogether using an internal or external loadingcontrol signal. This feature provides unlimited loadsimulation and increased power.The 63200 series also provides necessar ymeasurement func tions and shor t circuitsimulations that extend the test capability for themost demanding engineering and automated testapplications.With front LCD displays and rotary knob, the 63200loads offer versatile bench top operation. Users arealso able to control the loads remotely via GPIB orRS-232 interface or with a USB adapter. Complexwaveforms can also be created by driving theloads from an analog programming source (i.e.function generator).Chroma 63200 loads incorporate built-in fanspeed controls to minimize audio noise. The self-diagnosis routines, built-in protection against OC,OP, OT, and an alarm indicating OV reverse polarityto ensure safe operation and reliability. PROGRAMMABLE DC ELECTRONIC LOADMODEL 63200 SERIESRS-232GPIBChroma's 63200 series electronic loads provide constant current, constant resistance, constant voltage and constant power modes.The CC and CR mode load simulation is helpful to test whether the output voltage of the UUT remains stable, or regulated under different load conditions. For battery chargers, CV mode can change the output voltage to test if the battery charger is providing the correct charging current corresponding to the battery voltage. If the UUT is a battery, the electronic load is able to simulate the behavior of the device that uses the battery. For many battery discharge applications, power consumption patterns need to be analyzed. The constant power, or CP mode, is ideal for these applications.For low voltage/high current applications, the 63200 series is available with a low voltage mode, which provides ultra-low voltage operation and in many cases can compensate for large voltage loss in the input wiring.The 63200 series loads use a current closed loop design connecting all power MOSFET devices in parallel, to insure high accuracy load control with minimal drift (less than 0.15% of the current setting). The MOSFET technology keeps the input impedance to a minimum and enables the load to draw very high current even at very low voltages. For example, the model 63209 is capable of drawing 1,000A at only 1V input.Model 63209(15600W) Input CharacteristicsThe Chroma 63200 series loads have a built-in 15-bit precision A/D converter that can achieve 0.05%+0.05% F.S., 0.1%+0.1% F.S. and 0.3%+0.3% F.S. accuracy for voltage, current, and power measurements respectively. These measurements can be displayed simultaneously on three big LED readouts for convenience. In addition to standard measurements, the 63200 series also provides voltage and current monitor outputs, which are useful when the user needs to monitor the voltage and current waveform via a scope.Arbitrary Waveform Generatorexternal loadinG waveform SimulationmaSter / Slave parallel controlThe 63200 series electronic loads can be controlled by an external analog control signal, which is generated by any kind of signal or an arbitrary waveform generator. This makes it capable of simulating any loading waveform observed in the field within the load specifications.When higher power is required, it is common to parallel two electronic loads together to draw higher current. The 63200 series high power loads have a smart Master/Slave control mode. When the loads are set to Master/Slave mode, users can program the loading (CC mode only) on the master unit. The loading current values of the slave unit(s) will be calculated and downloaded by the master unit automatically. In short, unlike traditional designs, users now have the option of operating several loads in Master/Slave mode as a single load unit.Modern electronic devices operate at very high speeds; therefore, it is important for an electronic load to perform well during the transient and dynamic testing. To satisfy these testing applications, the 63200 loads offer outstanding high speed, programmable dynamic load simulation and control capabilities. The figure below shows the programmable parameters of the 63200 load modules. The programmable slew rate makes the simulation of transient load changes demanded by the requirement of real life application possible. The internal waveform generator of the 63200 is capable of producing a maximum slew rate of 25A/µs (63208), and dynamic cycling up to 20kHz. Its dedicated remote load sense and control circuitry guarantee theminimum waveform distortion during continuous load changes.Chroma's 63200 Series DC Loads provide a unique surge load simulation capability which allows users to overdrive the loads up to 2.7 times their rated power for short periods. This feature is ideal when the average power required by the UUT is low compared to short-term peak power demands. Plasma Display Panel (PDP) testing is one typical applications, others include battery 3C discharge, breaker & fuse over rating (300% to 1000%) tests, car engine startup simulation and DC motor startup simulation.The amount of surge loading available using the 63200 loads is related to initial loading conditions. Figures 1 and 2 show the relationship of the initial state (Load_Low under Dynamic mode) and the maximum acceptable overdrive power. Under this operation, the load will display an Over Power Protection Alarm (OPP) and will disable the load current if the user violates the maximum surge load capability showed in the figures.Note 1 :The Initial state under Static Mode should last at least 1 second.Note 2 :This surge load capability will be regulated by the temperature de-rating characteristics. (Refer to Note 1 in Specifications)Note 3 :Examples below assume the use of the Model 63201 load with a continuous rating of 2600W/300A/1-80VDC Note 4 :Model 63211/63212 does not support this feature.Example 1: STATIC LOADINGThe Model 63201 can be overdriven to approximately 5200W (200% of its rated continuous power rating) for 6.0 ms when the starting power is 650W (25% of its rated power). This is represented by DOT on the blue curve in Figure 1.Example 2: DYNAMIC LOADINGThe Model 63201 is capable of a zero - to- 6500W (250%) pulse at a duty cycle of 5%. This is represented by the DOT on the purple curve in Figure 2.Chroma's 63200 series electronic loads can also simulate a short circuit condition. The load can short a DC power source or any power supply that has abuilt in current limit function and measure its short circuit current so that users can verify if the UUT current limit is functional.The 63200 loads include a unique timing and measurement function. This allows for precision time settings and measurements in the range of 1s to 99,999s. This feature also allows users to set a final cutoff voltage and timeout value for battery discharge testing and similar applications. For example, the figure to the right shows that the 63200's internal timer can be initiated automatically when starting load on. The timer will stop counting until the cutoff voltage value is reached, or timeout occurs.Electronic & Electrical Devices TestingAlmost all modern electronic equipment have a built in power supply. Therefore, a DC electronic load is an important instrument for these devices during the R/D and Q/A phases. For example, A/D, D/D and D/A stages are normally integrated within a UPS. The Chroma 63200 electronic loads are helpful in testing the internal A/D and D/D boards of UPS devices.Battery TestingFor most applications, power consumption patterns are based on constant power. Therefore, the CP mode of the 63200 series electronic load is ideal to use as a discharge load for battery testing.System integrationChroma 63200 series electronic loads provide GPIB, RS-232 and RS-485 PC controllable interfaces. These features combined with the external waveformsimulation and voltage / current monitoring capability make Chroma 63200 series ideal for automatic system integration.Power Supply TestingPower supplies play a critical role in electrical and electronic devices. They have diversified into several different configurations for various applications. For example, AC/AC power supplies are used for UPS and AVR, AC/DC power supplies are used for server power supplies, and DC/AC power supplies areused for inverters that transfer battery power to AC for home appliances. Lastly, DC/DC converters are widely used in battery powered devices such ascellular phones and laptop computers. With four different load modes, Chroma 63200 series electronic loads are capable of testing many different DC output power supplies either directly or via a rectifier. They can also be used to test AC output power supplies.Server Power SupplyUPS/AVRRectifier1. Power Switch2. LED Display: Voltage read back3. LED Display: Current/ ohm read back4. LED Display: Power read back5. LCD Display: For setting and editing6. Rotary knob: To adjust the loading and parameter setting7. Numeric key: For data setting8. Function key: To select load mode, control mode, and define the reading specification9. System key:For system config and data store, recall 10. Load terminal11. Voltage sense terminal 12. RS-485 connector 13. GPIB connector 14. RS-232C connector15. Voltage monitor output:Analog output which indicates the voltage waveform 16. Current monitor output: Analog output which indicates the current waveform 17. External V reference:External programming voltage inputModel: 63203, 63204panel deScriptionThe 63200 series can be operated from the front panel or controlled by softpanel software. The user friendly software includes all the functions of 63200 series, and is easy to understand and operate. The 63200 series can be configured with either GPIB or RS-232 interfaces as an option for remote control and automated testing applications.Sequence TestBattery Discharge Test Dynamic Test Main Operation Menu OCP Test1002003004005006007008009001000110010020030040050060070080090010001020304050607080901001101201301401501600123456789101100.10.20.30.40.50.60.70.80.9 1.0 1.1102030405060708090100V-I Curve :Model 63201/ 63203/ 63205/ 63206/ 63207/ 63208/ 63209Low Voltage Operating :Model 63201/ 63203/ 63205/ 63206/ 63207/ 63208/ 63209Low Voltage Operating :Model 63202/ 63204/ 63210/ 63211/ 63212V-I Curve :Model 63202/ 63204/ 63210/ 63211/ 63212 Voltage(V)Voltage(V)Current(A)Current(A)Current (A)Current (A)Voltage (V)Voltage (V) Note: All specifications are measured at load input terminals. (Ambient temperature of +25)Model 63208 / 63209 / 63210Model 63211 / 63212Model 63203 / 63204Model 63201 / 63202Model 63205Model 63206 / 63207NOTE*1 : The power rating specifications at ambient temperature=25˚C and see the diagram below for power derating. NOTE*2 : If the operating voltage exceeds the rated voltage for 1.1 times, it would cause permanent damage to the device. NOTE*3 : S (siemens) is the SI unit of conductance, equal to one reciprocal ohm.NOTE*4 : The Vin must be greater than min. operating voltage of each model.NOTE*5 : Setting error will be 1% for R<0.005 at CRL range.NOTE*6 : The Vin must be greater than 7V of each model.NOTE*7 : Power F.S. = Vrange x Irange F.S.63200-E-201408-1000Worldwide Distribution andService NetworkJAPANCHROMA JAPAN CORP .472 Nippa-cho, Kouhoku-ku, Yokohama-shi, Kanagawa,223-0057 JapanTel: +81-45-542-1118Fax: +81-45-542-1080http://www.chroma.co.jp E-mail:******************U.S.A.CHROMA SYSTEMS SOLUTIONS, INC.19772 Pauling, Foothill Ranch, CA 92610Tel: +1-949-600-6400Fax: +1-949-600-6401 E-mail:*******************Developed and Manufactured by :HEADQUARTERS CHROMA ATE INC.66 Hwaya 1st Rd., KueishanHwaya Technology Park,Taoyuan County 33383,Taiwan Tel: +886-3-327-9999Fax: +886-3-327-8898 E-mail:******************EUROPECHROMA ATE EUROPE B.V.Morsestraat 32, 6716 AH Ede,The Netherlands Tel: +31-318-648282Fax: +31-318-648288 E-mail:******************CHINA CHROMA ELECTRONICS(SHENZHEN) CO., LTD.8F, No.4, Nanyou Tian An Industrial Estate, Shenzhen, China PC: 518052Tel: +86-755-2664-4598Fax: +86-755-2641-9620A632001A632004A63200663201 : DC Electronic Load 80V/300A/2.6kW 63202 : DC Electronic Load 600V/50A/2.6kW 63203 : DC Electronic Load 80V/600A/5.2kW 63204 : DC Electronic Load 600V/100A/5.2kW 63205 : DC Electronic Load 80V/180A/6.5kW 63206 : DC Electronic Load 80V/600A/10.4kW 63207 : DC Electronic Load 80V/300A/10.4kW 63208 : DC Electronic Load 80V/600A/15.6kW 63209 : DC Electronic Load 80V/1000A/15.6kW 63210 : DC Electronic Load 600V/150A/14.5kW 63211 : DC Electronic Load 1000V/150A/15.6kW 63212 : DC Electronic Load 1000V/150A/10kW A632001 : Remote ControllerA632002 : Load Cable 38mm/242A/200cmx2A632003 : Load Cable 80mm/390A/200cmx2A632004 : Sync. Link Box for 6330A & 63200 series A632005 : Softpanel for 63200 seriesA632006 :NI USB-6211 Bus-Powered Multifunction DAQnumber of parallel load unitS and ratinGorderinG information。

cgg模块RAMUR参数

cgg模块RAMUR参数

GeneralThe module removes multiples (characterized as events with a slower velocity) or linear events from a trace gather. The Y-flag must be set at the end of every elementarygather. Input traces must be ordered according to the spatial co-ordinate usedfor the Radon transform. Traces are output in the order of the input elementary gathers.Anti-multiple filtering (first option MA)The module computes a model of primary and multiple events. This computation is based on data decomposition into user-defined parabolas and performed using a high-resolution, de-aliased least-squares method in the frequency-space (f-x) domain for each frequency of the pass-band defined by FMIN and FMAX. Events corresponding to parabolas with a greater curvature are considered to be multiples. Events corresponding to parabolas smaller than this threshold are considered to be primary events. The zone limits between primaries and multiples is user defined (DTCUT). The difference between data and the sum of primary and multiple events is considered as linear noise. By default, the module subtracts the model of multiples or the model of multiples plus the linear noise from the input gather (see the LAMBDA parameter).Anti-noise filtering (first option NA)The module builds signal and (linear) noise events. This building is based on a userdefinedlinear model.On input, a gather is modelled as a superimposition of a number of linear events plus the random noise.The computation is performed using a high-resolution, de-aliased least-squares method in the frequency- space (f-x) domain for each frequency of the pass-band defined by FMIN and FMAX.CGG2 RAMUR User’s Manual GeoclusterBy default, the module subtracts the model with organized noise or the model with organized noise plus the random noise from each gather (see LAMBDA parameter). Equalization options (second option PA)Input traces are equalized before filtering. This equalization is similar to that applied by the DYNQU module (blank option) with a sliding operator. The PA option (Preserved Amplitude) reverses equalization after Radon filtering.Geocluster User’s Manual RAMUR 3CGGFUNCTION CALLDescriptionColumn contents1 *3-7 RAMUR9-10 First option:MA: Multiple attenuation using modelling of parabolas.NA: Linear noise attenuation.12-13 Second option:Blank: No equalisation/un-equalisation of input traces.PA: Traces are equalised before processing and un-equalised after processing.15-16 Input buffer: contains the trace to be processed.23-24 Output buffer: contains the processed trace.31-80 ParametersParameters common to all optionsMandatory parametersXRM i i = Far trace offset (in meters or feet). This offset is used as a reference when computing the Radon model. Integer.YMX j j =Maximum coverage of a unit gather (CDP, shotpoint,…). Integer.FMIN f f = Minimum frequency (in Hz) of the spectrum used in the computation of the models. Integer.0 f < F Nyquist.FMAX g g = Maximum frequency (in Hz) of the spectrum used in the computation of the models. Integer.Maximum (0,FMIN) < g < F Nyquist.YB k k = Number of the secondary loop to which output traces are transmitted. Integer.1< k <99The selection of the FMIN and FMAX frequencies is essential in the processing cost. The computation of models is only performed on the user-defined frequency band.CGG4 RAMUR User’s Manual GeoclusterParameters describing the area to scanDTMIN v v = Lower limit (in milliseconds) for scanning parabolas or straight lines relative to the horizontal. Integer.In option MA, it is the minimum residual NMO at offset XRM. Inoption NA, it is the minimum shift at offset XRM with respect tozero.In general, v is negative or null, and always smaller than DTMAX.When v is positive, flat events cannot be modelled.DTMAX w w = Upper limit (in milliseconds) for scanning parabolas or straight lines relative to the horizontal. Integer.In option MA, it is the maximum residual NMO at offset XRM. Inoption NA, it is the maximum shift at offset XRM with respect tozero.DTMIN < w.DDT z z = Increment (in milliseconds) between parabolas or straight linesat offset XRM. Integer.0 < z < (DTMAX-DTMIN)DTCUT eor DTCUT e, DTCUT fe (,f) = Separating threshold(s) in milliseconds used to define thezone of multiples and linear noises. Integer.If DTCUT is coded once only, the lines or parabolas includedbetween DTCUT and DTMAX are not used to build the signalmodel.If DTCUT is coded twice, the lines or parabolas included betweenthe two DTCUTs are not used to build the signal model.Parts which are not used for the signal model are used to model multiplesor linear noises.The values given to e and f must lie within the [DTMIN,DTMAX]interval. If two thresholds are defined e must be smaller than f.orDTKEEP e,or DTKEEP e, DTKEEP fe(,f) = Separating thresholds in milliseconds used to define the zoneof primaries or the signal zone to be preserved. Integer.If DTKEEP is coded only once, only the lines or parabolas included between DTKEEP and DTMAX are used to build the signal model.If DTKEEP is coded twice, only the lines and parabolas includedbetween the two DTKEEPs are used to build the signal model.Parts which are not used for the signal model are used to model theGeocluster User’s Manual RAMUR 5CGGmultiples or linear noises.The values given to e and f must lie within the [DTMIN,DTMAX]interval. If two thresholds are defined, e must be smaller than f.Parameters for windowing managementNCX m, TAPX nThe Radon filtering is performed on spatial sliding windows made ofm traces with an overlap of n traces. Integer.0 < m, 0 n.The size of the sliding spatial window is essential in the quality ofthe results.NCT o, TAPT pThe Radon filtering is performed on o milliseconds time sliding windowswith an overlap of p milliseconds. Integer.0 < o, 0 δ p.Optional parametersProcessing window parametersTIi or KTIr i = Initial time in milliseconds of the processing window after NMO. Integer. By default, i = 0r = Multiplier coefficient of the water bottom values read from theLFD (which must then be defined). Real.LFDd d = Number of the water bottom library. Integer.TAPIi i = Length of the tapering zone in milliseconds between the processed trace and the original data at the beginning of the processingwindow. Real. By default i = 100 msec.TFf f = Final time in milliseconds, after NMO, of the processing window. Integer. By default f = trace length in milliseconds.0 δ TI < TFTAPFg g = Length of the tapering zone in milliseconds between the processed trace and the original data at the end of the processing window.Real. By default g = 100 msec.Parameters for windowing managementXCXh h = Length, in meters, of the spatial sliding windows. If XCX is coded, the spatial sliding windows have a variable number of traces,and NCX is the minimum number of traces in a window.In the MA option, h is indeed the length of the first sliding window(starting at offset zero). The other windows have a constant squaredoffset length (of h2).0 < hCGG6 RAMUR User’s Manual GeoclusterModel and processing parametersPp p = Factor controlling the focusing of the Radon decomposition. Forlarge P values, the Radon spectra will be better focused, sometimesat the expense of the accuracy of the data modelling. The value 0.0results in identical results to MULTP (no weight).By default, p = 1.0.0.0 δ p δ 2.0Fb b = Factor controlling the sparseness of the Radon decomposition.For large b values, the Radon spectra will be sparser, sometimes atthe expense of the accuracy of the data modelling.Real. By default, b = 0.1.0 < bSc c =Whitening factor applied to the weight. The value 0.0 can lead tounstable behavior. The value 1.0 results in identical results toMULTP (no weight). Real.0.0 δ b δ 1.0By default, b = 0.001FWAd d = Between FMIN and FWA, a same weight is applied, which is averaged from a preliminary pass on this frequency band.FMIN δ d < FWBBy default, d = FMIN+(FMAX-FMIN)/10FWBe e = Last frequency where the weight is updated. Between FWB andFMAX the weight is kept constant.FWA < e δ FMAXBy default, e = FMAXLTAPt t = Length, in milliseconds, of the taper centered on the separating threshold curves. This parameter is referenced to XRM. By default,t = 40 ms. Integer.0 < tLTAPMDx x = Length, in milliseconds, of the taper applied to parabolas (Option MA) or straight lines (option NA) from (DTMIN-x) to DTMIN andfrom DTMAX to (DTMAX+x). Integer.By default, x = 100 ms.0 < xComputation of the residual noise modelBy default, the residual noise is assumed to belong to the same frequency range as the multiples. It is then removed simultaneously with the multiples:Output = Input – Multiples – LAMBDA(Input-(Multiples+Primaries))LAMBDAc c = Coefficient between 0 and 1 giving the ratio of the residual noiseto remove. Real.0 = no noise removal.1 = full noise removal.0 δ c δ 1. By default, c = 0Geocluster User’s Manual RAMUR 7CGGInternal selection of algorithmsThe module has several algorithms that perform the same computations. Their relative CPU efficiency depend mainly on the number of traces in the spatial windows (NCX) and the number of p-traces (NP). Most of the so-called ’fast’ algorithms are fast for large enough NCX and/or NP values. By default, the module tries to guess the likely faster algorithm, but with rough criteria: if the CPU is a critical factor, the user should test by himself the relative speeds.Some of the algorithms give approximate results, but with a high enough precision for usual cases. However, in the case of unacceptable results, one should make a test with the exact algorithms, or increase the accuracy of the approximate algorithms. LSId d = Choice of undetermined or overdetermined least-squares inverse.1 = underdetermined case: should be prefered for NP>NCX2 = overdetermined case: should be prefered for NP<NCXSelecting 1 or 2 may slightly change the results. In contrast with theother optimisation parameters, it is adviced to not play with this one,unless you know what you’re doing.Integer. By default, d=1 if NCX NP, d=2 if NCX > NPOPTIMAa a = Tau-p modelling.1 = classical exact2 = fast approximate3 = fast approximate (faster than 2 for very large NCX)Integer. By default, a is set according to LSI, NCX and NPOPTIMBb b = Tau-p stack.1 = classical exact2 = fast approximateInteger. By default, b is set according to NCX and NPOPTIMCc c = System solver choice.1 = direct exact solver2 = fast iterative approximate solverInteger. By default, c is set according to LSI, NCX and NPACCAd d = Accuracy (number of digits) of the approximate algorithm selected by OPTIMA2Integer. By default, d=3ACCCe e = Accuracy (number of digits) of the approximate algorithm selected by OPTIMC2Integer. By default, e=3Parameters specific to the PA optionOptional parametersAVCj j = Length, in milliseconds, of the equalisation operator.Integer. By default, j = 200 ms (equalisation level set to 5000).0 < j.CGG8 RAMUR User’s Manual GeoclusterTRACE HEADERStatus of the output trace headerX = updated word 0 = zeroed word blank = directly transcribed1 2 3 4 5 6 7 8 9 0WORDS 1 to 10WORDS 11 to 20WORDS 21 to 30WORDS 31 to 40WORDS 41 to 50WORDS 51 to 60WORDS 61 to 64Geocluster User’s Manual RAMUR 9CGGRECOMMENDATIONSRemarks• Input traces in RAMUR (MA/NA) must have been NMO-corrected by FANMO. • As the running time is proportional to the FMIN to FMAX range, special atte ntion should be given to these parameters. They should be selected by looking atthe frequency spectrum of the data within the processing window.• The DDT parameter controls the number of functions that are built and the computationtime. An increment of 20 to 32 ms is often sufficient. Tests should bemade to determine the most suitable value for DDT and the DTMIN to DTMAX range.• The F and S parameters control the focalization of the seismic events into the Radon spectra. Large values of F and small values of S lead to sparse spectra atthe expense of the data modelling accuracy.• The use of sliding temporal and spatial windows enables you to simplify the number of seismic events to handle. With a smaller number of events, the high resolution, de-aliased Radon transform is better focused and avoids the artefacts commonly related to aperture and spatial sampling limitations.• RAMUR always outputs the same number of traces with the same offset as input. Invalid traces on input will be invalid traces on output.• Too small spatial windows may lead to poor separation between signal and noise. Typical values are:• NCX: 20,TAPX: 5,NCT: 400, TAPT: 100.• Smaller spatial windows may be used with the NA option• To correctly model the primaries, the DTMIN parame ter should always be negative .• If some algorithmic optimizations are enabled, S0 (the default) can some times lead to instabilities. To avoid this problem, set the S slightly positive value(0.01). However, it has been observed that strongly aliased multiples are better attenuated with S0.• NCT is automatically raised to the nearest power of 2 (in number of samples) of the FFT length.• Decreasing the accuracy of the approximate algorithms (ACCA & ACCC)speeds them up.• Invalid traces are considered as valid traces containing null values. They should therefore be removed before using RAMUR.CGGLimits• The size of the spatial windows (NCX) must be less than 512 traces• The number of parabolas must be less than 1024• The length of temporal windows NCT must be less than 16384*SIGeocluster User’s Manual RAMUR 11CGGEXAMPLESExample 1Tableau 1:Anti-multiple processing(MA option )Anti-noise processing(NA option )Principle: Create a multiple model to besubtracted to the data to be processed.Principle: Create a model of linear noisesto be subtracted to the data to be processedMultiples are assumed to be parabolas. Multiples are assumed to be lines.Step 1: RAMUR works on NMOcorrectedCDP gathers. It is advisable tofirst playback some gathers which areNMO corrected in order to distinguish theresidual curvatures of the multiples.Step 1: RAMUR works on shotpoint orCDP gathers. It is advisable to firstplayback some gathers which are NMOcorrected.Step 2: The previous step enables you to define essential RAMUR parameters (DTMIN, DTMAX, DDT). The values of DTMIN and DTMAX are given at the far-trace offset XRM defined by the user. The DDT parameter is given according to the number of traces. DTMIN and DTMAX must be selected in such a way that they include the totality of the events present. In particular, they must contain the steepest events.Traces to be processed are ordered inWORD4, WORD20.Traces to be processed are ordered inWORD4 or WORD2, WORD20 withreverse and direct traces possiblyseparated (by concatenation WORD2,WORD3 for example).CGG* LIBRI HB 01 1 CGG2 RAMUR3 CALLAS4 RAMURDG48 OPTION MA* LIBRI FD 1 WORD19=LINE2742,WORD4,( 1)= 1680,( 192)= 1680( 516)= 1733,( 764)= 1772,( 844)= 1788,( 904)= 1802,( 964)= 1821,( 976)= 1823,( 1076)= 1867,( 1088)= 1869,( 1364)= 2020,( 1516)= 2103, ( 1600)= 2141,( 1668)= 2165,( 1748)= 2182,( 1860)= 2199,( 1964)= 2207, ( 2104)= 2213,( 2264)= 2213,( 2340)= 2215,( 2352)= 2221,( 2364)= 2235, ( 2372)= 2236,( 2384)= 2224,( 2404)= 2222,( 2428)= 2221,( 2444)= 2225, ( 2456)= 2230,( 2468)= 2234,( 2480)= 2233,( 2500)= 2239,( 2528)= 2248, ( 2552)= 2260,( 2568)= 2263,( 2600)= 2277,( 2712)= 2326,( 2728)= 2330, ( 2752)= 2340,( 2768)= 2351,( 2780)= 2350,( 2824)= 2365,( 2936)= 2394, ( 3004)= 2407,( 3060)= 2415,( 3112)= 2421,( 3192)= 2423,( 3392)= 2428, * BOUCL 1* RUNET 01FILE=local:/discar/proj/1006400/DATA/RAMURDG4.cst* PLOTX 01 ECH70,PAS8,AG,LS0,DG,G30,PLOTTER=BW24,W1900-W9000,NOSIMP,NOCRD,MOT4,MOT20,TOP,(RAMUR INPUT),LHB1,* RAMUR MA 01 02 YB2,XRM4880,YMX192,FMIN5,FMAX80,DTMIN-300,DTMAX1200,DDT12,DTCUT300,NCX192,TAPX5,NCT500,TAPT50,F0.1,KTI1.8,LFD1,TAPI100.,TAPF100.,TF9000.,LSI2,* FINBO* DLOOP 2* PLOTX 02 ECH70,PAS8,AG,LS0,DG,G30,PLOTTER=BW24,W1900-W9000,NOSIMP,NOCRD,MOT4,MOT20,TOP,(RAMUR OUTPUT),LHB1,HISTORY* FINBO* PROCS X(YB1)。

REGATRON产品说明书

REGATRON产品说明书

Product DescriptionREGATRONPerformance. Precision. Quality. 05/2020 © Regatron AG. All Rights Reserved.DC and AC Power Sources Modular – Programmable – EfficientVERSATILEDC Applications Testing / Simulation / Cycling / Charging /Discharging of: Batteries ∙ Supercaps ∙ Fuel Cells ∙ ElectricalEnergy Storage Devices ∙ On-board Electrical Systems andComponents ∙ E-Drive Trains ∙ Photovoltaic and otherInverters ∙ Plasma Surface Technology.AC Applications Grid Simulation ∙ Simulation of GridImpedance e.g. for Anti-Islanding Tests ∙ RLC Load Mode∙Power Amplifier ∙ High Bandwidth Hardware in the Loop (P-HIL) with External Real-tim e Processor ∙ R+D on Smart GridConfigurations.AC and DC General Test Lab Applications ∙ Standard Tests ∙Programmable Tests ∙ Versatile Educational Laboratory Applications.OUR PRODUCT RANGETC.ACS Regenerative 4-Quadrant AC Power Sources0 – 305 Vrms (L-N), 0 – 528 Vrms (L-L)30 kVA up to 1000 kVA/acsTC.GSS Regenerative 2-Quadrant DC Power Supplies0 – 1500 VDC*, 20 kW up to 2000+ kW/gssTopCon Quadro DC Power Supplies0 – 1500 VDC*, 10 kW up to 2000+ kW/tcpTC.GXS Regenerative DC Electronic Loads0 – 1500 VDC*, 20 kW up to 2000+ kW/gxsTC.DSS Bidirectional DC/DC ConvertersDC line side: 800 – 830 VDC load side ratings: 0 – 1500 V*, 20 kW up to 2000+ kW /dssCustom Designed Programmable PowerFew 100 W up to few 1000 kW/customNEW! G5 Series DC Power Supplies/g5OUR TEST SOLUTIONSBattery Simulators /batsimGrid Simulators /gridsimPV Simulators /pvsim* Voltages up to 2000 VDC available on requestRegatron AG Regatron Inc. Feldmuehlestrasse 50 100 Overlook Center, 2nd Floor 9400 Rorschach Princeton, NJ 08540 SWITZERLAND USA OUR BASIC COMMITMENTMeeting ever Changing Application RequirementsFinely graduated voltage- / power levelsModular design allows for parallel- or series configuration Even mixed parallel- / series operation is availableEasily scalable and configurable by user in the field Designed for Various Application ConditionsAir- or liquid cooling2-channel safety interface and user safety options Rugged models for harsh environmental conditions Cabinet turn-key solutionsUnrivaled Programming FunctionalityApplication software packages for automated tests and efficient data logging / reporting:▪Battery Simulation (BatSim)▪Battery Testing (BatControl)▪Capacitance Simulation (CapSim)▪PV Simulation (SASControl)▪Grid Simulation (GridSim)Programming interfaces and APIsOperating software for configuration, settings, diagnostics Integrated 8-channel scope for analysisMade in SwitzerlandDeveloped and manufactured by REGATRON Performance – Precision – Quality3 years warranty, extended warranty availableWidely recognized qualified and timely customer support。

博斯DesignMax DM3SE表面安装扬声器技术参数说明书

博斯DesignMax DM3SE表面安装扬声器技术参数说明书

TECHNICAL DATADesignMax DM3SEsurface-mounted loudspeakerTechnical SpecificationsProduct OverviewWith coaxial two-way drivers, the 30-watt DesignMax DM3SE loudspeaker offers clear, intelligible highs and surprising low end for its size — along with premium aesthetics that complement any commercial sound installation. The DM3SE features a two-way 3.5-inch woofer and .75-inch coaxial tweeter mounted within the Dispersion Alignment system, delivering a frequency range of 75 Hz – 20 kHz. The DM3SE is surface-mounted, IP55 outdoor-rated, and locks onto a hidden QuickHold U-bracket for fast, secure installation.Key FeaturesCombine DesignMax models to complete any design, big or small — 12 loudspeakers to mix and match, from 2-inch, low-profile models to 8-inch, high-SPL compression-driver loudspeakers and outdoor-rated options.Deliver clear highs and surprising low-end for their size with coaxial two-way drivers — no DSP or EQ required. For evenbetter sound, combine with select Bose DSPs and amplifiers to enable Bose loudspeaker EQ and SmartBass processing, which expands performance and response at any listening level.Ensure a consistent listening experience throughout the room with the Dispersion Alignment system, which matches the coverage of the woofer to the pattern of the tweeter.Blend with any room design with elegant form factors, minimum-bezel grilles available in black or white, and removable logos.Reduce installation time with the patented QuickHold mounting system, which also reduces strain, hassle, and the chance of product damage.Install easily with industry-standard accessories — all models include Euroblock connectors; in-ceiling models include plenum-rated backcans, tile bridges, and front-access audio wiring that makes installation and troubleshooting easier.Install DM3SE outside — IP55 rating with standard aluminum grille for outdoor use.DesignMax DM3SEsurface-mounted loudspeakerFootnotes(1) Frequency response and range measured on-axis in half-space environment with Bose EQ voicing(2) Sensitivity measured on-axis in half-space environment averaged 100 Hz – 10 kHz using recommended High-Pass protection(3) Maximum SPL calculated from sensitivity and power handling specifications, exclusive of power compression.(4) AES standard 2-hour duration with IEC system noise(5) Bose extended-lifecycle test using pink noise filtered to meet IEC268-5, 6-dB crest factor, 500-hour duration.(6) Measured in whole-space environment6。

FISHER防喘振控制

FISHER防喘振控制
1 SEC.
Pd
100%
D
A
Pd
A C B
D 0 100%

Qs
DPo
A C B
D
0 100%源自DPcA C BD
Performance curves are usually very flat near surge操作曲线靠近喘振线 Even small changes in compressor pressure differential cause large flow changes压缩机压差的微小变化也会引起较 大的流量变化 The speed of approaching surge is high; in only 0.4 seconds, DPO dropped by 14%, with a 2% change in DPc 到达喘振线的时 间为0.4秒。
hr DEV < 0
DEV = 0
- Operating Point
DEV > 0 qr
[File Name or Event] Emerson Confidential 27-Jun-01, Slide 7
2
Surge margin Or Surge Control Line SCL
The approach to surge is fast快速到达喘振点
• Flow and Pressure Transmitters流量及压力变送器 • Piping Layout配管布置 • Antisurge Control Valve防喘振控制阀
[File Name or Event] Emerson Confidential 27-Jun-01, Slide 4
[File Name or Event] Emerson Confidential 27-Jun-01, Slide 9

多尺度分解法

多尺度分解法

Multiscale Methods in TurbulenceThomas J.R.Hughes,Victor M.Calo and Guglielmo ScovazziInstitute for Computational and Engineering Sciences,University of Texas at Austin201E.24th StreetACE6.412,1University Station C0200,Austin,Texas78712-0027,U.S.AExtended SummaryVariational multiscale concepts for Large Eddy Simulation(LES)were introduced in Hughes et al.[7]. The basic idea was to use variational projections in place of the traditionalfiltered equations and to focus modeling onfine-scale equations rather than coarse-scale equations.Avoidance offilters eliminates many difficulties associated with the traditional approach,namely,inhomogeneous non-commutativefilters necessary for wall-boundedflows,use of complexfiltered quantities in compressibleflows,the closure problem,etc.In addition,modeling confined to thefine-scale equations retains numerical consistency in the coarse-scale equations and thus permits full rate-of-convergence of the underlying numerical method in contrast with the usual approach which limits convergence rate due to artificial viscosity effects in the fully resolved scales(O(h4/3)in the case of Smagorinsky-type models).Initial versions of the variational mulsticale method focused on dividing resolved scales into coarse andfine designations,and eddy viscosities,inspired by traditional models,were only included in thefine scale equations and acted only on thefine scales.This version was studied in[8,9,16]and found to work very well on homogeneous isotropic flows and fully-developed equilibrium and non-equilibrium turbulent channelflows.Static eddy viscosity models were employed in these studies but superior results were subsequently obtained through the use of dynamic models,as reported in Holmen et al.[4]and Hughes et al.[11].Good numerical results were obtained with the static approach by other of investigators,namely,Collis[2],Jeanmart and Winckelmans [14]and Ramakrishnan and Collis[18,19,20,21].Particular mention should be made of the work of Farhat and Koobus[3],and Koobus and Farhat[15],who have implemented this procedure in an unstructured mesh,finite volume,compressibleflow code,and applied it very successfully to a number of complex test cases and industrialflows.We believe that this initial version of the variational multiscale concept has already demonstrated its viability and practical utility and is,at the very least,competitive with traditional LES turbulence modeling approaches.Nevertheless,there is still significant room for improvement.The use of traditional eddy viscosities to representfine-scale dissipation is an inefficient mechanism.Employing an eddy viscosity in the resolved fine scales to represent turbulent dissipation introduces a consistency error which results in the resolved fine scales being“sacrificed”to retain full consistency in the coarse scales.(In our opinion,this is still better than the traditional approach in which consistency in all resolved scales is sacrificed to represent turbulent dissipation.)This procedure is felt to be“inefficient”because approximately7/8of the resolved scales are typically ascribed to thefine scales.Another shortcoming noted for the initial version of the variational multiscale method is too small an energy transfer to unresolved modes when the discretization is very coarse(see,e.g.,Hughes et al.[11]).This phenomenon is also noted for some traditional models,such as the dynamic Smagorinsky model[11],but seems to be somewhat more pronounced for the multiscale version of the dynamic model.The objectives of recent multiscale work have been to capture all scales consistently and to avoid use of eddy viscosities altogether.This holds the promise of much more accurateand efficient LES procedures.In this work,we describe a new variational multiscale formulation which makes considerable progress toward these goals.In what follows,all resolved scales are viewed as coarse scales,which obviates the issue of inefficiency ab initio.We begin by taking the view that the decomposition into coarse andfine scales is exact.For example, in the spectral case,the coarse-scale space consists of all Fourier modes beneath some cut-off wave number and thefine-scale space consists of all remaining Fourier modes.Consequently,the coarse-scale space has finite dimension whereas thefine-scale space is infinite dimensional.The derivation of the coarse-and fine-scale equations proceeds,first,by substituting the split of the exact solution into coarse andfine scales into the Navier-Stokes equations,then,second,by projecting this equation into the coarse-andfine-scale subspaces.The projection into coarse scales is afinite dimensional system for the coarse-scale component of the solution,which depends parametrically on thefine-scale component.In the spectral case,in addition to the usual terms involving the coarse-scale component,only the cross-stress and Reynolds-stress terms involve thefine-scale component.In the case of non-orthogonal bases,even the linear terms give rise to coupling between coarse andfine scales.The coarse-scale component plays an analogous role to thefiltered field in the classical approach,but has the advantage of avoiding all problems associated with homogeneity, commutativity,walls,compressibility,etc.The projection intofine scales is an infinite-dimensional system for thefine-scale component of the solution which depends parametrically on the coarse-scale component. We also assume the cut-off wave number is sufficiently large that the philosophy of LES is appropriate. For example,if there is a well-defined inertial sub-range,then we assume the cut-off wave number resides somewhere within it.This assumption enables us to further assume that the energy content in thefine scales is small compared with the coarse scales.This turns out to be crucial in our efforts to analytically represent the solution of thefine-scale equations.The strategy is to obtain approximate analytical expressions for thefine scales then substitute them into the coarse-scale equations which are,in turn,solved numerically. If the scale decomposition is performed in space and time,the only approximation in the procedure is the representation of thefine-scale solution.To provide a framework for thefine-scale approximation, we assume an infinite perturbation series expansion to treat thefine-scale nonlinear term in thefine-scale equation.By virtue of the smallness of thefine scales,this expansion is expected to converge rapidly under the circumstances described in many cases of practical interest.The remaining part of thefine-scale Navier-Stokes system is the linearized operator which is formally inverted through the use of a Green’s function.The combination of a perturbation series and Green’s function provides an exact formal solution of thefine-scale Navier-Stokes equations.The driving force in these equations is the Navier-Stokes system residual computed from the coarse scales.This expresses the intuitively obvious fact that if the coarse scales constitute a good approximation to the solution of the problem,the coarse-scale residual will be small and the resultingfine-scale solution will be small as well.This is the case we have in mind and it provides a rational basis for assuming the perturbation series converges rapidly.Note that one cannot use such an argument on the original problem because in this case the perturbation series would almost definitely fail to converge.(If we could have used this argument,we would have solved the Navier-Stokes equations analytically!Unfortunately,it does not work.)The formal solution of thefine-scale equations suggests various approximations may be employed in practical problem solving.We are tempted to use the word“modeling”because approximate analytical representations of thefine scales constitute the only approximation and hence may be thought of as the“modeling”component of the present approach but we want to emphasize that it is very different from classical modeling ideas which are dominated by the addition of ad hoc eddy viscosities.We will present numerical results that demonstrate these eddy-viscosity terms are unnecessary in the present circumstances.There are two aspects to the approximation of thefine scales:1)Approximation of the Green’s function for the linearized Navier-Stokes system;and2) approximation of the nonlinearities represented by the perturbation series.Thefirst and obvious thought for the latter aspect,nonlinearity,is to simply truncate the perturbation series.This idea is investigated,as well as another promising idea,in conjunction with some simple approximations of the Green’s function. It turns out there is considerable experience in local scaling approximations of the Green’s function based on the theory of stabilized methods[5,6,10].The Green’s function is typically approximated by locally defined algebraic operators(i.e.,the“τ’s”of stabilized methods)multiplied by local values of the coarse-scale residual.With this approximation of the solution of the linearized operator,nonlinearities can beeasily accounted for in perturbation series fashion.Another approach that accounts for nonlinearities in thefine-scale equations is to introduce a nonlinear algebraic scaling of the Navier-Stokes equations.The resulting local nonlinear algebraic system can be analytically solved.It possesses the reasonable analytical property that if the coarse-scale residual is small,it converges to the linearized solution.These newer variational multiscale ideas,and the older variants,were implemented in afinite volume code that has enjoyed widespread use in turbulence simulations(see Pierce and Moin[17]).Following along the lines of Jacobs and Durbin[12,13],who performed DNS investigations of bypass transition of a boundary layer,we examine this difficult problem from the point of view of the variational multiscale and classical LES.Our aim was to solve this problem as an LES and demonstrate the efficacy of the new ideas in the process.In our work we endeavor to show the effectiveness,or deficiencies,of LES approaches by studying them over a range of resolutions,from coarse tofine.In our studies of bypass transition we went as far as DNS in thefine-scale end of the spectrum,and1/8DNS resolution in each spatial direction.The coarsest LES mesh then involves about1/512the number of equations as the DNS mesh and approximately1/4,096 of the computational effort.We found,independent of the LES method,that in order to accurately simulate bypass transition,the decay of input homogeneous,isotropic,free-stream turbulence must be the same for all meshes.A procedure was developed in which we were able to simulate consistent energy decay with distance of the free-stream turbulence across the range of meshes considered.We then compared the methods to represent bypass transition.We found that the“1/8DNS mesh”was incapable of representing either the laminar region of the boundary layer or the free-stream turbulence evolution due to too few points in the wall normal direction.We found that all methods gave essentially the same solution at the DNS level, whereas only the new variational multiscale formulation was able to attain relatively mesh independent solutions without parameter adjustment for the1/4,1/2and full DNS mesh cases.The1/4DNS involves 1/64the number of mesh points as the DNS case and1/512the computational parison is made with classical LES procedures,such as the dynamic Smagorinsky model,which tends in this instance to exhibit significant sensitivity to thefilter-width ratio,and previous versions of the variational multiscale method in which afine-scale dynamic Smagorinsky model is parison is also made with some classical stabilized methods,such as SUPG(see Brooks and Hughes[1]).We conclude that the newest method is superior to all previous methods and offers a promising new path for turbulence research in LES.However,it obviously needs testing on a wider variety offlows and implementation in a variety of numerical frameworks,such as,spectral,finite difference andfinite element,before definitive conclusions can be drawn.In our experience,the particular numerical discretization method has an enormous impact on the results,and its influence is often underestimated by practitioners evaluating models. References[1]A.N.Brooks and T.J.R.Hughes.Streamline upwind/Petrov-Galerkin formulations for convectiondominatedflows with particular emphasis on the incompressible Navier-Stokes puter Methods in Applied Mechanics and Engineering,32:199–259,1982.[2]S.S.Collis.Multiscale methods for turbulence simulation and control.Technical Report Version1.1,Mechanical Engineering and Materials Science,Rice University,2002.Available at/∼collis/papers/vki2002_notes.pdf.[3]C.Farhat and B.Koobus.Finite volume discretization on unstructured meshes of the multiscaleformulation of large eddy simulations.In Rammerstorfer F.G.Mang H.A.and Eberhardsteiner J., editors,Proceedings of the Fifth World Congress on Computational Mechanics(WCCM V),Vienna University of Technology,Austria,July7-122002.Fifth World Congress on Computational Mechanics.[4]J.Holmen,T.J.R.Hughes,A.A.Oberai,and G.N.Wells.Sensitivity of the scale partition forvariational multiscale LES of channelflow.Physics of Fluids,16(3):824–827,2004.[5]T.J.R.Hughes.Multiscale phenomena:Green’s functions,the Dirichlet-to-Neumann formulation,subgrid scale models,bubbles,and the origins of stabilized puter Methods in Applied Mechanics and Engineering,127:387–401,1995.[6]T.J.R.Hughes,G.Feijóo.,L.Mazzei,and J.B.Quincy.The variational multiscale method–A paradigmfor computational puter Methods in Applied Mechanics and Engineering,166:3–24,1998.[7]T.J.R.Hughes,L.Mazzei,and rge eddy simulation and the variational multiscaleputing and Visualization in Science,3:47–59,2000.[8]T.J.R.Hughes,L.Mazzei,A.A.Oberai,and A.A.Wray.The multiscale formulation of large eddysimulation:Decay of homogeneous isotropic turbulence.Physics of Fluids,13(2):505–512,2001.[9]T.J.R.Hughes,A.A.Oberai,and rge eddy simulation of turbulent channelflows by thevariational multiscale method.Physics of Fluids,13(6):1784–1799,2001.[10]T.J.R.Hughes,G.Scovazzi,and L.P.Franca.Multiscale and stabilized methods.In E.Stein,R.de Borst,and T.J.R.Hughes,editors,Encyclopedia of Computational Mechanics.John Wiley&Sons, Ltd.,2004.[11]T.J.R.Hughes,G.N.Wells,and A.A.Wray.Energy transfers and spectral eddy viscosity ofhomogeneous isotropic turbulence:Comparison of dynamic Smagorinsky and multiscale models over a range of disretizations.Technical Report04-20,Institute for Computational Engineering and Sciences,University of Texas at Austin,2004.Available at/reports/2004/0420.pdf.[12]R.G.Jacobs and P.A.Durbin.Bypass transition phenomena studied by computer simulation.Technical Report TF-77,Flow Physics and Computation Division,Department of Mechanical Engineering,Stanford University,2000.[13]R.G.Jacobs and P.A.Durbin.Simulations of bypass transition.Journal of Fluid Mechanics,428:185–212,2001.[14]H.Jeanmart and parison of recent dynamic subgrid-scale models in the caseof the turbulent channelflow.In Proceedings Summer Program2002,pages105–116,Stanford,CA,2002.Center for Turbulence Research,Stanford University&NASA Ames.[15]B.Koobus and C.Farhat.A variational multiscale method for the large eddy simulation ofcompressible turbulentflows on unstructured meshes–application to vortex puter Methods in Applied Mechanics and Engineering,193(15–16):1367–1383,2004.[16]A.A.Oberai and T.J.R.Hughes.The variational multiscale formulation of LES:Channelflow atRe=590.In40th AIAA Ann.Mtg.,AIAA2002-1056,Reno,NV,Jan.2002.[17]C.D.Pierce and P.Moin.Progress-variable approach for large eddy simulation of turbulentcombustion.Technical Report TF-80,Flow Physics and Computation Division,Department of Mechanical Engineering,Stanford University,2001.Available at /Pierce/thesis.pdf.[18]S.Ramakrishnan and S.S.Collis.Variational multiscale modeling for turbulence control.In AIAA1stFlow Control Conference,AIAA2002-3280,St.Louis,MO,June2002.[19]S.Ramakrishnan and S.S.Collis.Multiscale modeling for turbulence simulation in complexgeometries.In40th AIAA Aerospace Sciences Meeting and Exhibit,AIAA2004-0241,Reno,NV,Jan.2004.[20]S.Ramakrishnan and S.S.Collis.Partition selection in multiscale turbulence modeling.Preprint,2004.[21]S.Ramakrishnan and S.S.Collis.Turbulence control simulation using the variational multiscalemethod.AIAA Journal,42(4):745–753,2004.。

丹麦SMEDEG电子蓬松式多速循环泵说明说明书

丹麦SMEDEG电子蓬松式多速循环泵说明说明书

SMEDEG RDOF DENMARKEV RANGE MUL TI-SPEED GLANDLESS CIRCULATORS■Unique 1-2-3 modular pump construction ■Clearly visible multi-speed electrical regulator ■Most models have built-in thermal overload protection ■Single and three phase motors■Wide range of optional controls available ■Same pump suitable for heating or chilled water ■H.W.S. iron pumps ■H.W.S. bronze pumps ■Boiler shunt pumps ■1400 and 2800 r.p.m. pumps■Flanges, up to 65 mm, double drilled as standard for maximum interchangeability ■Single-case twin pumps■IsoBar TM - circulator range - with integral electronic regulation is also available2SMEDEG RDOF DENMARKEV RANGE MUL TI-SPEEDGLANDLESS CIRCULATORSField of applicationDark blue pumps for heating/chilled water. Yellow pumps for se-condary hot water applications. Temperature range -15°C to +120°C. In secondary hot water applications it is recommended that water temperature does not exeed 65°C, to minimise lime deposit.Maximum content of Glycol 50%. Maximum working pressure 10Bar.“TUT” anti-lime system in HWS pumpsThe life of a secondary hot water circulating pump can be extended if the limescale build-up in its rotor bearing area can be minimised.Normal raw water contains a certain amount of lime which will pre-cipitate out as the temperature increases (max. recommended HWS water temp. 65°C). Smedegaard´s patented answer to this problem is to fit a TUT pressure equalising seal, manufactured in brass and stainless steel, to all HWS ”V” and ”VZ” secondary glandless pumps . This seal reduces the number of water changes in the rotor chamber and hence the amount of lime deposited.Pump mediumClean, nonviscous, nonaggressive and nonexplosive fluids without any solids or fibres. Antifreeze without any mineral oil. If any liquid other than water is being pumped, we recommend that you contact Smedegaard or their representatives as the pump characteristics may change. Special models available upon request.Materials of construction Pump:Cast iron or bronze Impeller:Cast iron/Polysulphone/bronze Shaft:Stainless steel Can:Stainless steel Bearings:Carbon “O” Rings:EPDM rubberModel identification EV Glandless Range 5 Internal port dia. 50mm (2")125 Nominal impeller dia. in mm 4 Motor 4-pole (1400 rpm.)2 Motor 2-pole (2800 rpm.)C Dark blue heating/chilled pump CD Dark blue single-case twin pump V Yellow iron pump for H.W.S. with lime content VZ Yellow bronze pump for H.W.S with lime content Z Yellow bronze pump for H.W.S.See availability of models on the individual curves and in the tables.ImpellerAll impellers are balanced to ensure that bearings are not influenced by any imbalance from within the pump, resulting in quieter operation and longer life.MotorMotors of glandless construction, with class F insulation, designed and produced by Smedegaard, are used with these pumps to ensure quiet operation and long life. Standard voltages are 1x230V ,3x230V , 3x400V , +6%, -10%, 50HZ (IEC 38). IP 42 for 3-speedmotors and IP 44 for 4-speed motors.ConstructionEV circulators are designed with the unique 1-2-3 modular pump construction, i.e. the pump consists of three assemblies, the pump casing, the rotating element and the stator. This together with the high efficiency of the motor and the use of recycleable materials,means that great attention has been paid to the environment. An advanced lubrication system, which gives efficient cooling of the motor, together with a hardened stainless steel shaft, substantial carbon bearings and a one-piece can arrangement, all accurately machined , ensures very quiet operation and longer life.Adjustment of capacity and energy savingsThe motor and pump casing are designed for maximum efficiency.In addition EV circulator can be adjusted to give 3 or 4 positive pump curves, via the clearly visible multi-speed selector switch.This ensures total flexibility and is the only adjustment needed to secure maximum energy saving and minimum noise level. Commercial EV circulators are 4-speed and domestic EV circula-tors are 1- and 3-speed.3EV RANGE MUL TI-SPEEDGLANDLESS CIRCULATORSSMEDEG RDOF DENMARKTwin PumpsMost of the “EV” range can be supplied as single-case twins, model reference letters CD. Two motors and an additional non-return valve are built-in the same casting and in the majority of cases the overall dimensions and connections remain the same as a single pump.“Y” Piece ManifoldsIn addition to the single-case twin pumps, the SMEDEGAARD TAS TWIN “Y” PIECES with built-in isolating and non-return valves can be supplied for use with single pumps up to 125 mm (5").These manifolds are suitable for temperatures up to 110°C with a maximum system pressure of 10 bar and a pump working pressure of 3 bar.InstallationThe pump should always be installed with the pump shaft horizontal and the motor terminal box must not be mounted in a downward position. The motor of the pump must not be insulated and it is very important that the drain holes (mainly for condensate) in the motor flange are unobstructed.Direction of flow through the pump casing is indicated by an arrow.It is recommended that the pump is mounted in vertical pipework,pumping upwards. If flow, in a heating system, has to be downwards, an air vent must be fitted at the highest point before pump suction. HWS secondary pumps should never be fitted pumping downwards. If a single case twin pump is fitted in horizontal pipework an automatic air vent should be fitted in the plug provided on the side of pump casing.For further details see Smedegaard’s installation guide for EV glandless range.Electrical connection and motor protectionPumps should be wired in accordance with existing regulations.Motor protection may not be required on EV2/3-40/65-70-2 pumps. The larger pumps need overload protection.When wired through a Smedegaard 132 starter, overload protection is automatically achieved immaterial of speed selected, using terminals “a” and “b” in the terminal box. For availability, see individual curves. If a standard motor starter is used, amp ratings/speed settings are shown on the individual pump curves and on the pump nameplates.Approvals and standardsThe EV pumps range is CE marked and approved according to EN 60-335-2-51. The hydraulic performance curves are published according to EN 1151/EN 29906 grade 2.EV RANGE MUL TI-SPEEDGLANDLESS CIRCULATORSThe models in this catalogue represent Smedegaard’s complete glandless range, except IsoBar.Details for larger duties using glanded pumps, see leaflets T, HIL, N and NM.(D) = Available as twin pump.SMEDEG RDOF DENMARK4EV RANGE MUL TI-SPEEDGLANDLESS CIRCULATORSSMEDEG RDOF DENMARK5EV 2-65-2 C / EV 3-65-2 C Heating/chilled EV 3-65-2 CD Twin pump (1 1/2" RG.)EV 2-65-2 VZ / EV 3-65-2 VZ HWS bronze EV 2-65-2 V / EV 3-65-2 V HWS ironExternal motor protection is not needed with these pumps.Union⁄"-1"-1⁄"⁄"-1"-1⁄"130/180180⁄"-1"-1⁄"130/18004321m4812 lgpm0lgpm01234m 04812012m ⁄"-1"-1⁄"130/180EV RANGE MUL TI-SPEEDGLANDLESS CIRCULATORSSMEDEG RDOF DENMARK6Union 1⁄"4812m 1208040Union ⁄"-1"-1⁄"1801⁄"21000,51,52,53,51,02,03,0m kPa 302010⁄"-1"-1⁄"1801234m 403020103 x 4000,250,40EV RANGE MUL TI-SPEEDGLANDLESS CIRCULATORSSMEDEG RDOF DENMARK71⁄" - 40 mm.3 x 4000,850,650,530,431⁄" - 40 mm.25000,51,52,53,51,02,03,0mkPa 30201001357246mkPa 604020250246m kPa 6040201⁄" - 40mm.2503 x 4000,550,450,370,300246m kPa 604020EV 4-60-2 C Heating/chilled EV 4-60-2 CD Twin pump EV 4-60-2 VZ HWS bronze EV 4-60-2 V HWS ironNote: Also available as single pump with pump casing port toport dimension 220 mm, model EV 4-67-2C. 1⁄" - 40mm.2" - 50 mm.3402135746m EV RANGE MUL TI-SPEEDGLANDLESS CIRCULATORSSMEDEG RDOF DENMARK81⁄" - 40mm.2" - 50 mm.2" - 50 mm.2503002804812m kPa 120804000,51,52,53,51,02,03,0m kPa 3020102135746m kPa 604020EV 4-95-2 C Heating/chilled EV 4-95-2 CD Twin pump EV 4-95-2 VZ HWS bronze EV 4-95-2 V HWS iron Note: Speed 3 is max duty of single phase pump.EV 5-125-4 CHeating/chilled EV 5-125-4 CD Twin pump EV 5-125-4 VZ HWS bronze EV 5-125-4 V HWS ironEV 5-160-4 CHeating/chilled EV 5-160-4 CD Twin pump2 /" - 65 mm.2803 x 4000,620,420,300,2300,250,751,251,750,501,001,50m EV RANGE MUL TI-SPEEDGLANDLESS CIRCULATORSSMEDEG RDOF DENMARK92" - 50 mm.2" - 50 mm.280280369m4812m kPa 12080402" - 50 mm.28002015105m 4035302520151050246810l/sec.0EV 5-88-2 C Heating/chilled EV 5-88-2 CD Twin pump EV 5-88-2 VZ HWS bronze EV 5-88-2 VHWS ironNote: Speed 3 is max duty of single phase pump.EV RANGE MUL TI-SPEEDGLANDLESS CIRCULATORSSMEDEG RDOF DENMARK102 /" - 65 mm.2 /" - 65 mm.2 /" - 65 mm.3403703401,701,401,201,003 x 4003 x 4002,101,581,351,1502135746m kPa 60402002135746m kPa 60402004812m kPa 12080402 /" - 65 mm.3403 x 4001,201,100,900,7080706050403020100EV 6-125-4 C Heating/chilled EV 6-125-4 CD Twin pump EV 6-125-4 VZ HWS bronze EV 6-125-4 V HWS ironSMEDEG RDOF DENMARK113" - 80 mm.3" - 80 mm.3" - 80 mm.2 /" - 65 mm.3403303603903 x 4001,030,920,830,761,591,231,030,903 x 4003 x 4002,402,001,751,50051015m 00,51,52,53,51,02,03,0mkPa 30201002135746mkPa 60402002135746m EV 6-110-2 C Heating/chilled EV 6-110-2 CDTwin pumpSMEDEG RDOF DENMARK123" - 80 mm.3" - 80 mm.3" - 80 mm.3" - 80 mm.36044036036004812m kPa 120804004261014812mkPa 12080404812m 051015m 0EV 8-95-2 C Heating/chilled EV 8-95-2 CD Twin pump EV 8-95-2 V HWS ironSMEDEG RDOF DENMARK134" - 100 mm.4" - 100 mm.5" - 125 mm.EV 10-130-4 C Heating/chilled4" - 100 mm.38047048545001,00,51,52,53,52,03,0m 02135746m kPa 60402004261014812m01,00,51,52,53,52,03,0m kPa 302010SMEDEG RDOF DENMARK14Wiring details for EV rangeSingle phaseDIAG. ADIAG. BNNPhaseThermal overload protectionDIAG. CDIAG. DN Phase, LPhase, L NThermal overload protectionThree phaseDIAG. EDIAG. FPhase, L1 Phase, L1Phase, L2 Phase, L2Phase, L3Phase, L3Thermal overloadprotectionDIAG. G DIAG. HPhase, L1 Phase, L1Phase, L2 Phase, L2Phase, L3 Phase, L3Note:Above wiring diagrams are cross referenced on the individualpump curves.23DIAG. KCommerciel 4-speed 3-phase.d D2x øL 26SMEDEG RDOF DENMARK15When both PN6 and PN10 are shown, the pump is supplied with flanges double drilled to facilitate interchangeability when used for replacement.Note: 80, 100 and 125 mm pump casings can be supplied drilled PN6 to special order.(D) = Available as twin pump.Note: Model EV 2-50/65/70-2C is available with 120 mm port to port, model CF .Dimensions:Single pumpTwin pumpDimensions in mmModel CFF J26 HJ FØDG EØ D120dC HC H1/4”RG1/4”RGAA B BG EK45°ø d ø D øL40, 50, 65PN 10, DIN 2533K 22.5°ø d ø DøL 80, 100, 125 PN 16, DIN 2533K1/”- 2”EV 5-160-4 (D)340340EV 5-125-4 (D)280280EV 5-100-4300-EV 5-120-2280-EV 4-95-2 (D)250250EV 4-75-2 (D)250250EV 4-60-2 (D)250250EV 4-125-4250-EV 4-100-4 (D)250250EV 3-100-2 (D)180180EV 3-100-4210-EV 2/3-75-2180-EV 2/3-75-4 180-EV 2/3-72-2 (D)180180EV 2/3-70-2 (D)130/180*180EV 2/3-65-2 (D)130/180*180MiniWatt 2/3-50-2130/180*-Type A A1IsoBar TM - circulators with integral regulationIsoBar is a complete range of glandless circulators with integral electronic performance regulation, infinitely adjusting the capacity of the pump to the requirements of the system,without any external sensors.EV 132 StarterThis starter can be used with all EV 4-speed pumps incorpora-ting “a” and “b” motor overload protection with terminal box/wiring diagram 1B, 2C and 2F.The EV 132 starter uses the thermal overload built-in to the motor windings and will switch off the pump in the event of overheating. Overload protec-tion is automatically achieved,immaterial of speed selected on the pump. If thermal overload cuts out the pump, it will not restart until manually reset, us-ing the red on/off switch. After mains failure, the starter will reset automatically.Dimensions in mm: H 170, W 90, D 120.Enclosure: Spec. IP 40.Material: High grade plastic.EV 160 Speed ControlThis control can be used with all 3 phase EV 4-speed pumps, with terminal box/wiring diagram 2E and 2F.The EV 160 speed control can be programmed to change the pump speed between speed 4and off, speed 4 and 1 or speed 1and off. The 7-day clock can be adjusted to change speed when required. The EV 160 can also be controlled by an external signal from a thermostat or pressure switch. The EV 160connects to the pump via a 1.5 m multipin plug cable and no other electrical wiring is necessary.Dimensions in mm: H 170, W 90, D 120.Enclosure : Spec. IP 40.Material: High grade plastic.EV 2140-3 Change-over Panel for twin pumpsThis control for duty/standby arrangements can be used with all EV 4-speed twin pump arrangements incorporating “a” and “b”motor overload protection with terminal box/wiring diagram 1B, 2C and 2F. The EV 2140-3 Change-over Panel is designed to give protection to both pumps at all speed settings, without adjustment, via the thermal overloads built-in to the winding. A 7-day clock is supplied as standard in this panel, which can be programmed to give a night setback facility. The panel is suitable for either automatic or manual operation of pump 1,pump 2 or both pumps in parallel. In case of pump failure, the standby pump will start up automatically.Dimensions in mm: H 220, W 260, D 140.Enclosure: Spec. IP 54.Material: High grade plastic.f e b . 2002 - 999.9999.121 - D e s l e r s B og t r y k k e r i - 2020075HQmax.Princip curve for IsoBarH 50%H min.IsoBar TM and Automatic ControlsSMEDEG RDOF DENMARKT. Smedegaard A/S • Sydvestvej 57-59DK 2600 Glostrup • DenmarkTel +45 43 96 10 28 • Fax +45 43 63 17 66E-mail:******************•Smedegaard AG • Pumpen- und MotorenbauIndustriestrasse 15 • CH-5712 Beinwil am See • Schweiz Tel +41 62 765 0500 • Fax +41 62 765 0501E-mail:******************•www.smedegaard.chSmedegaard Pumps • Unit 7 Barhams Close • Wylds Road Bridgwater • Somerset • TA6 4 DS • England Tel 01278 458686 • Fax 01278 452454E-mail:******************************•It is SMEDEGAARD's policy to continually improve and develop the product range. We reserve the right to change specifications without prior notice.Whilst every care has been taken to ensure that data is correct, no responsibility can be accepted for inaccuracies or misprints.。

Fluke Calibration 8588A和8558A数字多功能电阻计说明书

Fluke Calibration 8588A和8558A数字多功能电阻计说明书

The 8588A Reference Multimeter is the world’s most stable digitizing multi-meter. Designed for calibration laboratories, this long-scale high-precision reference multi-meter features superior accuracy and long-term stability over a wide measurement range, with an intuitive user interface and a color display.The 8588A delivers reliable and reproducible measurements with exceptional performance suitable for primary levellaboratories. With more than 12 measurement functions, includ-ing the new digitize voltage, digitize current, capacitance, RF power, and external shunts for dc and ac current, the 8588A helps you consolidate your lab’s cost of test into a single mea-surement instrument. Its superb analog performance is aug-mented by Fluke Calibration’s new high-speed system design and the industry’s fastest direct digitizing capability, enabling significant throughput increase for many automated systems demanding a combination of the highest speed and best accuracy.The 8588A holds the indus-try’s best one-year dc voltage accuracy of 2.7 uV/V at 95 % confidence interval, or3.5 uV /V at 99 %, and best 24-hour stability of 0.5 uV/V (95 %) or 0.65 uV/V (99 %),enabling it to outperform other long-scale reference multimeters on the market. The 8588A fur-ther pushes the speed envelope by producing a stable 8.5 digits reading in a mere one second.The 8588A platform consists of two models. The 8588A and 8558A both feature a common intuitive user interface with an easy-to-navigate menu struc-ture for all configurations and a set of matching SCPI-compliantcommands for automated envi-ronments. In addition, both models support a minimum of 100,000 readings per second at 4.5 digits across GPIB, USB or Ethernet.TECHNICAL DATA8588A Reference Multimeter8558A 8.5-Digit Multimeter8588A: The world’s most stable digitizing multimeterThe 8588A is designed for calibration and metrology laboratories that require the highest stability for the most accurate measurements to maintain maximum confidence in traceability.8558A: The industry’s fastest direct 5 mega-samples-per-second digitizing for system automation in labs and manufacturing test environmentsThe 8558A offers a subset of 8588A functions and features at an extremely competitive accuracy and speed performance.8588A key features and performanceDC voltage• 100 mV to 1000 V, (1050 V max)• 2.02x full scale• Maximum resolution: 1 nV • 2.7 μV/V (95 %) 3.5 µV/V (99 %), 1 year• 0.5 μV/V (95 %) 0.65 µV/V (99 %), 24 hour stability • 0 to 10 s reading aperture (200 ns resolution)DC current• 10 uA to 30 A• 2.02x full scale• Maximum resolution: 1 pA • 6.5 µA/V (95 %), 8.4 µA/V (99 %), 1 year• 0 to 10 s reading aperture (200 ns resolution)AC voltage• 10 mV to 1000 V, 1 Hz to 10 MHz, (1050 Vrms max)• 2.02x full scale Vpp, 1.2x full scale Vrms• Maximum resolution: 1 nV • 60 µV/V (95 %), 77 µV/V (99 %), 1 yearAC current• 10 uA to 30 A• 2.02x full scale Vpp, 1 Hz to 100 kHz 1.2x FS Vrms• Maximum resolution: 1 pA • 250 µA/V (95 %), 323 µA/V (99 %), 1 year Resistance• 1Ω to 10 GΩ (20 GΩ max) • 2.02x full scale• Maximum resolution: 10 nΩ• 7 µΩ/Ω (95 %), 9 µΩ/Ω (99 %), 1 year• Low current mode,high voltage mode and current-reversal Tru Ohms™Digitize V• 100 mV to 1000 V, (1050 Vmax)• 2.02x full scale• Maximum resolution: 18 bits• 5 mega-samples per secondsample rate• Up to 20 MHz bandwidthDigitize I• 10 µA to 30 A• 2.02x full scale• Maximum resolution: 18 bits• 5 mega-samples per secondsample rate• Up to 4 MHz bandwidthFrequency or period• Voltage, up to 10 MHz• Current, up to 100 kHz• Frequency up to 100 MHzon BNC• 0.5 µHz/Hz, 1 yearCapacitance• 1 nF to 100 mF• 400 µF/F, 1 yearTemperature• PRT and thermocouple• 5 mK PRT, 25 mK TC, 1 yearRF power• Rhode & Schwarz NRP seriesDC I and AC I external shunt• A40B and any other externalshuntReading speed• 1reading/**************memory• 100,000readings/*****digit into memory• Up to 5,000,000 (5 MS/s)readings /s into volatilememory in digitize V and I• Up to 500,000 readings/stransfer through USB inbinary formatMeasurement memory• 15 million readings volitile• 7.5 million readings volitilewith time stamp* 16 GB non-volitileGPIB, USBTMC, Ethernet• Native SCPI compliant remotecommands• 8508A and 3458A emulationmode• Fully support MET/CAL™ cali-bration procedures library inFluke 8508A emulation• IVI driver• USB thumb drive for conve-nient data transfer in .csvformatTrigger mechanisms• Manual trigger• External BNC Trig In andTrig Out• Internal or level trigger• Timer trigger• Epoch trigger• Line trigger• BUS triggerCE and CSA compliantComparing the 8588A and the 8558AComparing the 8588A and the 8558AStability, simplicity and performance by design The 8588A incorporates excep-tional linearity, low noise and stability in the design. This best-in-class long-scale digital reference multimeter guarantees superior 3.5 ppm one-year dc voltage relative accuracy at99 % confidence level and long-term stability over awide measurement range and functions.The 8588A contains the world’s most stable voltage references and attenuators custom crafted at Fluke Cali-bration. These precision components eliminate the need for daily internal self-calibration to compensate for drift when less-precise components are used. Autozeroing also becomes unnecessary because the ampli-fier offsets are ultra-stable. The 8588A achieves an exceptional 8.5-digit resolution reading in one second, two times shorter than the next best in class, which amounts to considerable productivity improvements.The 8588A is easy and intui-tive to use. It is the ideal lab multimeter for metrologists and calibration laboratory manag-ers who expect and appreciate a straightforward setup that quickly achieves the maximum performance of the instrument.• 3.5 µV/V (99 %), 1 year relative accuracy, dc voltage, without internal self-calibra-tion or auto-adjustments • 0.65 µV/V (99 %), 24 hour stability, dc voltage• 9 µΩ/Ω (99 %), 1 year, resistance• 2.02x full scale stretches lower noise floor to higher signal levels to maximize higher accuracies from the instrument• 0 ns to 100 s aperture setting allows the industry’s widest flexibility to control data capture window Accuracy, offset andstability provide excellentac performanceThe 8588A provides the mostaccurate true ac rms mea-surement available in a FlukeCalibration multimeter.With a 5 mega-sam-ples-per-second samplinganalog-to-digital converterand an extraordinarily stabledc analog path, the 8588Aachieves remarkable ac rmsmeasurement performance thatis ten times faster, two timesless noisy, and more sensitivefor low level signals than otherinstruments in this class. Itutilizes digital rms calculationsto maintain full resolution of awide dynamic range of digitizedsignals.Rapid digital filters are moreeffective than their analogequivalents for faster settling.The digital filters eliminate thedielectric absorption on analogfilters, commonly associatedwith residual slow-tail char-acteristics. The digital filterseffectively shorten settling timeto within 6 cycles of the filterfrequency and less than 1 ppmof the fully settled value. This isup to 10 times faster than otherlong-scale precision digital mul-timeters at low frequencies.Low noise is achieved fromaveraging the collected high-resolution digitized data andthe inherently stable signalpath. De-coupling low levelsignal sensitivity from tempera-ture drift enables the 8588A tomake high accuracy low-levelac measurements. Therefore,temperature drift, offsets, andlong-term instability typicallyassociated with an analog rmsconverter are eliminated.• 77 µV/V (99 %), 1 yearrelative accuracy, for themost accurate ac voltagemeasurement• 323 µA/A (99 %), 1 yearrelative accuracy, ac current• 15 ms settling time at1 kHz ac filter accom-plishes 10x faster ac voltagemeasurement• 2.02x full scale Vpp, 1.2x fullscale Vrms• Up to 30 A for peak accurrent greatly extends accurrent measurement rangeAC voltage measurementAC voltage measurement settingsSoft menu keysLarge, bright full color display30 A terminal™ terminalsThe intuitive user interface and flatmenu structure makes it easy to access configurations and view trend plots,waveforms, FFT, histogram and statistics.easy to learn.Enables industry's widest current measurement range through a single terminal.Multi-language selectionChoice of English, Chinese, French,Japanese, Korean, Russian and Spanish.and easily to a flash drive.Run/Stop triggerToggles the continuous, or free run, measurement state.easily to a flash drive.Usability designed for metrologists by metrologistsThe 8588A is the ideal lab multimeter. It streamlines the measurement process while eliminating misunderstandings, with an easy-to-access user interface in English, Chinese, French, German, Japanese, Korean, Russian and Spanish. An intuitive graphical display lets you easily visualize trends, histograms, complex waveforms, and statistics and perform routine metrology tasks quickly. You can perform both real-time and post-capture analysis for short-term and long-term stabil-ity, identifying and quantifying drifts, run-around noise and uncertainty analysis without the need for an external com-puter or software. You can also quickly visualize post-processed frequency domain signals of fundamental and harmonic amplitude and phase content.Some popular system mul-timeters have complex menustructures and unintuitive com-mands, while others lack anyuser interface, presenting bar-riers to training and operation.By contrast, the 8588A/8558A feature an easy-to-access con-figuration menu that makes it easy to train new users.The front panel features many new usability improve-ments. Visual ConnectionManagement™ output terminals light up to show which termi-nals are active, guiding the user to make the correct connections. The handles are over-molded for comfort and easy transport. USB host ports are placed both on the front and rear of the instrument. Use the ports to export data to external memory devices or simplify firmware updates. For remote communi-cation with a PC, choose from Ethernet, GPIB or USBTMC con-nectors on the rear panel.The 8558A/8558A provide full emulation of the Fluke8508A Reference Multimeter and command compatibility of the Keysight 3458A Digital Multimeter via SCPI commands, making it an ideal replacement for these older instruments.• Graphical display thatenables instantaneousvisualization of trend plot, Trend plotAnalyze: Histogramstatistical analysis, histogramand FFT.• GPIB, USBTMC, Ethernetallows industry standard selection of remote interface.• USB thumb drive enablesquick and easy data transfer to PC in .csv format.• SCPI compliant commandswith 8508A and 3458A emulation mode sim-plifies and accelerates system upgrade process to 8588A/8558A• Programmable front/rearinput switching with scan measurement allows ratio, difference and deviationmeasurements between front and rear terminals in dc voltage and resistance, func-tions with state-of-the-art linearity, noise performance, superb transfer uncertainties. • Capacitance and RF powermeter readout from Rohde & Schwarz NRP Seriesexpands the utility of 8588A in calibrating multi-product calibrators for improved pro-ductivity in calibration labs.Accurate data, delivered amazingly fastShorter test time on the8588A/8558A high-speed digital platform enables you to increase throughput, improve yield and realize a greater return on your investment.The 8588A/8558A digitizesto memory at 200 nanosec-onds per reading and delivers 4.5 digit data to a PC via USB, Ethernet and GPIB at 100,000 readings per second. Fast, high resolution data capture gives you the quantity and quality of information you need to make timely, correct decisions affect-ing system throughput and efficiency.• 0 ns to 100 s aperture setting allows industry’s widest flex-ibility to control data capture window• Reading speed: 1 reading /s @ 8.5 digits to 100,000 reading/***********• Data transfer from memory to PC: up to 500,000 readings /s in binary format through USB, up to 200,000 through Ethernet and GPIBDebug and perfect your device under testThe 8588A/8558A features a5 mega-sample digitizing rate with up to 20 MHz analog band-width, making it the first and only instrument on the market that can characterize extremely low level transient signals at 18-bit resolution. This capabil-ity makes it easier to debug designs, uncover anomalies and perfect your devices under test for use in real life environments.• Voltage sensitivity to hun-dreds of nV and current sensitivity to hundreds of pA allows you uncover ultra-low level transient signals• Up to 20 MHz bandwidth for voltage and 4 MHz for current retains high bandwidth con-tent of the signal measured • 18-bit SAR analog-to-digital converter that achieves 5 mega-samples per second • 5 mega-samples per secondsample rate, into buffer,for capturing complex, fastchanging waveforms• 15 million readings memoryallows large amount of datastorage eliminating theimmediate need to transferdata to a PC• Graphical waveform displayenables real-time visualiza-tion of complex waveforms,increased productivity withfaster access to results andanswersFast, reliable and accuratesystem compatibilityInserting a new instrument intoa tightly synchronized systemcan create overhead and incom-patibility. The 8588A/8558A’sdigital platform includescommon connectivity interfacesplus precise triggering that letsit digitize and transfer data toanywhere in the system foranalysis, with minimal effortand the highest reliability.• GPIB, USBTMC, Ethernetallows industry standardselection of remote interface• USB thumb drive enablequick and easy data transferto PC in .csv format• SCPI compliant commandswith 8508A and 3458A emu-lation mode simplifies andaccelerates system upgradeprocess to 8588A/8558A• Fully supports MET/CALcalibration procedures librarythat commands the Fluke8508A• IVI Driver for industrystandard control of DMM on8588A/8558A• Trigger Mechanisms: ExternalBNC Trigger Trig In and TrigOut, Internal or level trigger,Timer trigger, Epoch trigger,Line trigger, Bus Trigger• Less than 100 ns triggerlatency with external BNCtrigger for digitize voltageand currentTrend PlotAnalyze: FFTTrigger SystemThe MET/CAL™ Calibration Management Software advantageBoth 8588A and 8558A work with Fluke CalibrationMET/CAL™ Calibration Software. With native MET/CAL support or using 8508A emulation mode, you can increase throughput up to four times that of traditional manual and multi-product meth-ods while ensuring calibrations are performed consistently every time. This powerful software documents calibra-tion procedures, processes and results for ease in complying with ISO 17025 and similar quality standards.Support and services when you need them Fluke Calibration offers testing,repair and calibration servicesto meet your needs quickly andat a fair cost while maintainingthe high level of quality that youexpect. Our electrical calibrationlaboratories are accredited forconformance to ISO Guide 17025and we maintain global calibra-tion and repair facilities.Get peace of mind anduptime with a Gold Care-Plan service packageThe 8588A/8558A multimeterscome with a standard one-year factory warranty. You canenhance warranty protectionwith a Priority Gold InstrumentCarePlan service package.A Priority Gold InstrumentCarePlan includes an expe-dited annual calibration toreduce downtime by a weekand extended warranty to helpensure the best long-term per-formance from your instruments.Choose from one-year, three-year or five-year CarePlans.(Note: Priority shipping timesvary by country. Contact yourlocal Fluke Calibration salesrepresentative for details.)Ordering informationModels Description8588A Reference Multimeter8558A8.5 Digit MultimeterStandard accessories Description8588A-LEAD KIT-OSP General purpose probe kit & pouch with 2x 4-way shorting PCBOptional accessories DescriptionY8588Rack mount kit (2U – 3.5 in)Y8588S Slide rack mount kit8588A/CASE Transit case8588A-LEAD Comprehensive measurement lead kitIncludes:• 1x 8588A-LEAD KIT-OSP, general purpose probe kit• 1x 1 m screened 322/0.1 copper (30 Amp Rating) with 6 mm gold plated copperspade terminals• 4x 8588A-LEAD/THERMAL, 1.5 m two core screened low thermal cable with 6 mmgold plated copper spade terminals• 2x Locking adaptor 4 mm binding post to safety8588A-SHORT4-way shorting PCB8588A-LEAD/THERMAL Low thermal lead cable, 1.5 m two core screened low thermal cable with6 mm gold plated copper spade terminals8588A-7000K Cal kit with 1 GOhm standard and connecting leads96000SNS R&S power sensor8588A Reference Multimeter / 8558A 8.5-Digit Multimeter Fluke Calibration 1112 Fluke Calibration 8588A Reference Multimeter / 8558A 8.5-Digit Multimeter Fluke Calibration PO Box 9090, Everett, WA 98206 U.S.A.Fluke Europe B.V. PO Box 1186, 5602 BD Eindhoven, The Netherlands Web access: http://www.flukecal.eu Fluke Calibration. Precision, performance, confidence.™For more information call: In the U.S.A. (877) 355-3225 or Fax (425) 446-5716 In Europe/M-East/Africa +31 (0) 40 2675 200 or Fax +31 (0) 40 2675 222 In Canada (800)-36-FLUKE or Fax (905) 890-6866 From other countries +1 (425) 446-6110 or Fax +1 (425) 446-5716 Web access: ©2019, 2020 Fluke Calibration. Specifications subject to change without notice. Printed in U.S.A. 2/2020 6011948b-en Modification of this document is not permitted without written permissionfrom Fluke Calibration.。

戴尔EqualLogic PS6100系列阵列说明书

戴尔EqualLogic PS6100系列阵列说明书

Dell and Partner Confidential. Do not share or distribute.* *Based on 2011 internal Dell testing.**Based on 2011 internal Dell testing comparing PS6100XV and PS6000XV with RW70/30, 4K and 8K I/O, 32 outstanding I/O, and RAID-50).Dell EqualLogic PS6100 SeriesWhat’s New?With innovative form factors that support either high-density 2.5” or high -capacity 3.5” drives , we extend the promise of EqualLogic —ease of management, integration with VMware, high performance for mid-range SANS, and an all-inclusive software model —supporting our customers’ growing needs. With the planned August 22, 2011announcement of EqualLogic PS 4100 and 6100 Series arrays, we bring to our customers a vast array of choices that scale linearly with capacity* to meet their needs using Dell Fluid Data™ technologies.PS6100 Series ArraysDell EqualLogic PS6100 Series arrays come in a variety of configurations to meet the needs of the most demanding applications and enterprise data centers, each of which offers increased density compared to the previous-generation corresponding model.Up to 60% IOPS improvements with EqualLogic PS4100 and PS6100 Serieson typical workloads over previous generation EqualLogic array.**Dell and Partner Confidential. Do not share or distribute. *Based on 2011 internal Dell testing.Copyright Dell 2011. All rights reserved. Dell, the DELL logo, the DELL badge, Fluid Data, and EqualLogic are trademarks of Dell Inc. Other trademarks and trade names may be used in this document to refer to either the entities claiming the marks and names or their products. Dell disclaims proprietary interest in the marks and names of others. This document is for informational purposes only. Dell reserves the right to make changes without further notice to any products herein. The content provided is as is and without express or implied warranties of any kind.PositioningThe new EqualLogic PS4100 and PS6100 series provide you with an opportunity to schedule time with your customers and discuss Dell’s vision for Fluid Data™ management and how the new EqualLogic hardware is delivering on that vision. Help your customer set the storage agenda and position EqualLogic as a strategic choice for primary or secondary storage.Elevator Pitch: Why buy EqualLogic?The latest EqualLogic PS Series arrays provide significant improvements for your customers including:∙Up to 50% more users or transactions supported on the EqualLogic PS4100 and PS6100 Series at the same performance criteria (transaction response time <=2 sec) over previous generation EqualLogic arrays.*∙ EqualLogic PS4100 and PS6100 Series are designed to provide link failure resiliency using the Vertical Port Sharing feature.*∙In a port-constrained environment, EqualLogic PS4100 and PS6100 Series with the Vertical Port Sharing feature are designed to maintain full bandwidth performance and connectivity with only half of the switch ports active.*With a variety of systems built for capacity and performance, there is a Dell EqualLogic solutiondesigned to suit your cust omers’ needs. And with comprehensive Dell Data Management Services that help plan, design, implement and support an efficient data management strategy and ecosystem, you can help your customers satisfy today’s data availability, retention and recovery requirements while preparing to meet the demands of tomorrow.Resources/PartnerLook for new product information for each array coming August 22, 2011.designed to help them move the right data to the right place at the righttime for the right cost.。

Metrology Wells 产品说明书

Metrology Wells 产品说明书

Recently, we introduced Metrology Wells, which provide the very best performance in portable temperature calibration. The new 914X Series Field Metrology Wells extend high performance to the indus-trial process environment by maximizing portability, speed, and func-tionality with little compromise to metrology performance.Field Metrology Wells are packed with functionality and are remarkably easy to use. They are lightweight, small, and quick to reach temperature set points, yet they are stable, uniform, and accu-rate. These industrial temperature loop calibrators are perfect for performing transmitter loop calibrations, comparison calibrations, or simple checks of thermocouple sensors. With the “process” option, there is no need to carry additional tools into the field. This optional built-in two-channel readout reads resistance, voltage, and 4–20 mA current with 24 volt loop power. It also has on-board documentation. Combined, the three models (9142, 9143, and 9144—each with a “process” option) cover the wide range of –25 °C to 660 °C.High performance for the industrial environmentField Metrology Wells are designed for the industrial process environ-ment. They weigh less than 8.2 kg (18 lb) and have a small footprint, which makes them easy to transport. Optimized for speed, Field Metrology Wells cool to –25 °C in 15 minutes and heat to 660 °C in 15 minutes.Field environment conditions are typically unstable, having wide temperature variations. Each Field Metrology Well has a built-in gradient-temperature compensation (patent pending) that adjusts control characteristics to ensure stable performance in unstable environments. In fact, all specifications are guaranteed over the environmental range of 13 °C to 33 °C.Field Metrology WellsTechnical Data•Lightweight, portable, and fast•Cool to –25 °C in 15 minutes and heat to 660 °C in 15 minutes•Built-in two-channel readout for PRT, RTD, thermocouple,4-20 mA current•True reference thermometry with accuracy to ± 0.01 °C •On-board automation and d ocumentation•Metrology performance in accuracy,stability, uniformity, and loadingProvided by: (800)404-ATECAdvanced Test Equipment Corp .®Rentals • Sales • Calibration • ServiceBuilt-in features to address large workloads and common applicationsWhether you need to calibrate 4-20 mA transmitters or a simple thermostatic switch, a Field Metrology Well is the right tool for the job. With three models covering the range of –25 °C to 660 °C, this family of Metrology Wells calibrates a wide range of sensor types. The optional process version (models 914X-X-P) provides a built-in two-channel ther-mometer readout that measures PRTs, RTDs, thermocouples, and 4-20 mA transmitters which includes the 24 V loop supply to power the transmitter.Each process version accepts an ITS-90 reference PRT. The built-in readout accuracy ranges from ± 0.01 °C to ± 0.07 °C depending on the measured temperature. Ref-erence PRTs for Field Metrology Wells contain individual calibration constants that reside in a memory chip located inside the sensor housing, so sensors may be used inter-changeably. The second channel is user-selectable for 2-, 3-, or 4-wire RTDs, thermocouples, or 4-20 mA transmitters. For comparison calibration, don’t hassle with carrying mul-tiple instruments to the field. Field Metrology Wells do it all as a single instrument.Traditionally, calibrations of temperature transmittershave been performed on the measurement electronics, while the sensor remained uncalibrated. Studies have shown, however, that typically 75 % of the error in the transmitter system (transmitter electronics and temperature sensor) is in the sensing element. Thus, it becomes important to calibrate the whole loop—both electronics and sensor.The process option of Field Metrology Wells makes transmitter loop calibrations easy. The transmitter sensor is placed in the well with the reference PRT and the trans-mitter electronics are connected to the front panel of the instrument. With 24 V loop power, you are able to power and measure the transmitter current while sourcing andmeasuring temperature in the Field Metrology Well. This allows for the measurement of as-found and as-left data in one self-contained calibration tool.All Field Metrology Wells allow for two types of auto-mated thermostatic switch test procedures—auto or manual setup. Auto setup requires the entry of only the nominal switch temperature. With this entry, it will run a 3-cycle calibration procedure and provide final results for the dead band temperature via the display. If you need to customizethe ramp rate or run additional cycles, the manual setup allows you to program and run the procedure exactly how you would like. Both methods are fast and easy and make testing temperature switches a virtual joy!Metrology performance for high-accuracy measurementsUnlike traditional dry-wells, Field Metrology Wells maximize speed and portability without compromising the six key metrology performance criteria laid out by the EA: accuracy, stability, axial (vertical) uniformity, radial (well-to-well) uni-formity, loading, and hysteresis. All criteria are important in ensuring accurate measurements in all calibration applications.Field Metrology Well displays are calibrated with high-quality traceable and accredited PRTs. Each device (pro-cess and non-process versions) comes with an IEC-17025 NVLAP-accredited calibration certificate, which is backed by a robust uncertainty analysis that considers temperature gradients, loading effects, and hysteresis. The 9142 and 9143 have a display accuracy of ± 0.2 °C over their fullrange, and the 9144 display accuracy ranges from ± 0.35 °C at 420 °C to ± 0.5 °C at ± 660 °C. Each calibration is backed with a 4:1 test uncertainty ratio.New control technology guarantees excellent performance in extreme environmental conditions. The 9142 is stable to ± 0.01 °C over its full range and the mid-range 9143 is stable from ± 0.02 °C at 33 °C and ± 0.03 °C at 350 °C. Even at 660 °C, the 9144 is stable to ± 0.05 °C. But this is not all! Thermal block characteristics provide radial (well-to-well) uniformity performance to ± 0.01 °C. Dual-zone control helps these tools achieve axial uniformity to ± 0.05 °C at 40 mm (1.6 in).Automation and documentation make each unit a turnkey solutionSo you now have a precision calibration instrument that has field-ready characteristics, accredited metrology per-formance, built-in two-channel thermometry, and automa-tion—what else could you ask for? How about all this and aWith the ability to measure a reference PRT, mA current, and source 24 V looppower, Field Metrology Wells can automate and save up to 20 different tests.turnkey solution that will automate and document the results?The process versions of Field Metrology Wells have on-board non-volatile memory for documentation of up to 20 tests. Each test can be given a unique alphanumeric ID and will record block temperature, reference temperature, UUT values, error, date, and time. Each test can be easily viewed via the front panel or exported using Model 9930 Interface -it software, which is included with each shipment. Interface -it allows you to pull the raw data into a calibration report or an ASCII file.Operation is as easy as 1-2-3You’ll find Field Metrology Wells intuitive and easy to use. Each unit is equipped with a large, easy-to-read LCD display, function keys, and menu navigation but-tons. Its “SET PT.” button makes it straightforward and simple to set the block temperature. Each product has a stability indicator that visually and audibly tells you the Field Metrology Wells is stable to the selectable criteria. Each unit offers pre-programmed calibration routines stored in memory for easy recall, and all inputs are easily acces-sible via the front panel of the instrument.Never buy a temperature calibration tool from a com-pany that only dabbles in metrology (or doesn’t even know the word). Metrology Wells from Fluke are designed and manufactured by the same people who equip the calibration laboratories of the world’s leading temperature scientists. These are the people around the world who decide what a Kelvin is! We know a thing or two more about temperature calibration than the vast majority of the world’s dry-wellsuppliers. Yes, they can connect a piece of metal to a heater and a control sensor. But we invite you to compare all our specs against the few that they publish. (And by the way,we meet our specs!)The process version of Field Metrology Wells can save up to 20 different tests.Simplified schematic illustrating the airflow design (patents applied for) to minimize potential heat damage to sensor handles and transition junctions.Base Unit Specifications914291439144Temperature Range at 23 °C –25 °C to 150 °C(–13 °F to 302 °F)33 °C to 350 °C(91 °F to 662 °F)50 °C to 660 °C(122 °F to 1220 °F)Display Accuracy± 0.2 °C Full Range± 0.2 °C Full Range± 0.35 °C at 50 °C± 0.35 °C at 420 °C± 0.5 °C at 660 °CStability± 0.01 °C Full Range± 0.02 °C at 33 °C± 0.02 °C at 200 °C± 0.03 °C at 350 °C ± 0.03 °C at 50 °C ± 0.04 °C at 420 °C ± 0.05 °C at 660 °CAxial Uniformity at 40 mm (1.6 in)± 0.05 °C Full Range± 0.04 °C at 33 °C± 0.1 °C at 200 °C± 0.2 °C at 350 °C± 0.05 °C at 50 °C± 0.2 °C at 420 °C± 0.3 °C at 660 °CRadial Uniformity± 0.01 °C Full Range± 0.01 °C at 33 °C± 0.015 °C at 200 °C± 0.02 °C at 350 °C ± 0.02 °C at 50 °C ± 0.05 °C at 420 °C ± 0.14 °C at 660 °CLoading Effect (with a 6.35 mm reference probe and three 6.35 mm probes)± 0.006 °C Full Range± 0.015 °C Full Range± 0.015 °C at 50 °C± 0.025 °C at 420 °C± 0.035 °C at 660 °CHysteresis0.0250.030.1 OperatingConditions0 °C to 50 °C, 0 % to 90 % RH (non-condensing)EnvironmentalConditions (for allspecifications excepttemperature range)13 °C to 33 °CImmersion (Well)Depth150 mm (5.9 in)Insert OD30 mm (1.18 in)25.3 mm (1.00 in)24.4 mm (0.96 in)Heating Time16 min: 23 °C to140 °C23 min: 23 °C to150 °C25 min: –25 °C to150 °C 5 min: 33 °C to 350 °C15 min: 50 °C to660 °CCooling Time15 min: 23 °C to–25 °C25 min: 150 °C to–23 °C 32 min: 350 °C to 33 °C14 min: 350 °C to100 °C35 min: 660 °C to50 °C25 min: 660 °C to100 °CResolution0.01 °Display LCD, °C or °F user-selectableSize (H x W x D)290 mm x 185 mm x 295 mm (11.4 x 7.3 x 11.6 in) Weight8.16 kg (18 lb)7.3 kg (16 lb) 7.7 kg (17 lb)Power Requirements100 V to 115 V(± 10 %) 50/60 Hz,632 W230 V (± 10 %) 50/60Hz, 575 W100 V to 115 V (± 10 %), 50/60 Hz, 1380 W230 V (± 10 %), 50/60 Hz, 1380 WComputerInterfaceRS-232 and 9930 Interface-it control software included 4 Fluke Calibration Field Metrology WellsOrdering Information for 91429142-X Field Metrology Well, –25 °C to 150 °C, w/9142-INSX 9142-X-P Field Metrology Well, –25 °C to 150 °C, w/9142-INSX, w/Process ElectronicsX in the above model numbers to be replaced with A, B, C, D, E, or F as appropriate for the desired insert. See the inserts illustration and listing below.9142-INSA Insert “A” 9142, Imperial Misc Holes9142-INSB Insert “B” 9142, Imperial Comparison Holes9142-INSC Insert “C” 9142, 0.25-inch Holes9142-INSD Insert “D” 9142, Metric Comparison Holes9142-INSE Insert “E” 9142, Metric Misc Holes w/0.25-inch Hole 9142-INSF Insert “F” 9142, Metric Comparison Misc Holesw/0.25-inch Hole9142-INSZ Insert “Z” 9142, BlankOrdering Information for 91439143-X Field Metrology Well, 33 °C to 350 °C, w/9143-INSX 9143-X-P Field Metrology Well, 33 °C to 350 °C, w/9143-INSX, w/Process ElectronicsX in the above model numbers to be replaced with A, B, C, D, E, or F as appropriate for the desired insert. See the inserts illustration and listing below.9143-INSA Insert “A” 9143, Imperial Misc Holes9143-INSB Insert “B” 9143, Imperial Comparison Holes9143-INSC Insert “C” 9143, 0.25-inch Holes9143-INSD Insert “D” 9143, Metric Comparison Holes9143-INSE Insert “E” 9143, Metric Misc Holes w/0.25-inch Hole 9143-INSF Insert “F” 9143, Metric Comparison Misc Holesw/0.25-inch Hole9143-INSZ Insert “Z” 9143, BlankOrdering Information for 91449144-X Field Metrology Well, 50 °C to 660 °C, w/9144-INSX 9144-X-P Field Metrology Well, 50 °C to 660 °C, w/9144-INSX, w/Process ElectronicsX in the above model numbers to be replaced with A, B, C, D, E, or F as appropriate for the desired insert. See the inserts illustration and listing below.9144-INSA Insert “A” 9144, Imperial Misc Holes9144-INSB Insert “B” 9144, Imperial Comparison Holes9144-INSC Insert “C” 9144, 0.25-inch Holes9144-INSD Insert “D” 9144, Metric Comparison Holes9144-INSE Insert “E” 9144, Metric Misc Holes w/0.25-inch Hole 9144-INSF Insert “F” 9144, Metric Comparison Misc Holesw/0.25-inch Hole9144-INSZ Insert “Z” 9144, BlankOrdering Information for All Field Metrology Wells9142-CASE Carrying Case, 9142-4 Field Metrology WellsFluke Calibration Field Metrology Wells 56 Fluke Calibration Field Metrology WellsFluke CalibrationPO Box 9090, Everett, WA 98206 U.S.A.Fluke Europe B.V.PO Box 1186, 5602 BD Eindhoven, The NetherlandsFluke Calibration. Precision, performance, confidence.™For more information call:In the U.S.A. (877) 355-3225 or Fax (425) 446-5116In Europe/M-East/Africa +31 (0) 40 2675 200 or Fax +31 (0) 40 2675 222In Canada (800)-36-FLUKE or Fax (905) 890-6866From other countries +1 (425) 446-5500 or Fax +1 (425) 446-5116Web access: ©2007-2012 Fluke Calibration.Specifications subject to change without notice. Printed in U.S.A. 8/2012 3082057B D-EN-N Pub_ID: 11272-eng Rev 02Modification of this document is not permitted without written permissionfrom Fluke Calibration.。

波斯奇运动汽车:模型与配置指南说明书

波斯奇运动汽车:模型与配置指南说明书

The models featured in this publication are approved for road use in Germany. Some items of equipment are available as extra-cost options only. The availability of models and options may vary from market to market due to local restrictions and regulations. For information on standard and optional equipment, please consult your Porsche Centre. All information regarding construction, features, design, performance, dimensions, weight, fuel consumption and running costs is correct to the best of our knowledge at the time of going to print (04/2018). Porsche reserves the right to alter speci cations, equipment and delivery scopes without prior notice. Colours may di er from those illustrated. Errors and omissions excepted.Sportscar Together.CayenneCayenne Turbo Cayenne E-HybridDesign.Cayenne TurboCayenne E-HybridCayenne Turbo837465121New light strip with three-dimensional ‘PORSCHE’ logo 2‘e-hybrid’ model designation with corona in Acid Green on the tailgate 3New taillights with LED technology with three-dimensional lighting graphics and integrated four-point brake lights 4 21-inch Exclusive Design wheel with wheel arch extension in exterior colour Porsche Exclusive Manufaktur5 Roof spoiler painted in exterior colour 6New rear apron with horizontal contouring and accentuated wide look 7Rear apron in exterior colour 8 21-inch AeroDesign wheels with wheel arch extensions in exterior colour6471231L ED main headlights with matrix beamincluding PDLS Plus2Slats with black (high-gloss) inlaysin the air intakes – only in conjunctionwith exterior package in black(high-gloss)3N ew front apron with largecentral air intake4‘Power dome’ on bonnet5Independent Turbo front apronwith signi cantly larger air intakes6M ixed tyres7D ouble-row Turbo front lightsin LED bre optics541231Porsche Communication Management(PCM) with full-HD 12-inch touchscreendisplay including online navigation module2A scending centre console with grab handles3Sports seats in front (18-way, electric)with integrated headrests4Multifunction Sports steering wheelwith gearshi paddlesCayenne S1Porsche Communication Management (PCM) with full-HD 12-inch touchscreen display including online navigation module 2 Centre console with Direct Touch Control 3 High-resolution displays4Multifunction sports steering wheel with gearshi paddles 5 Mode switch (Sport Chrono Package)6Trim in aluminium, wood or carbon. Image features trim in black (high-gloss)7Sport Chrono clock Cayenne E-Hybrid 433352176Cayenne E-Hybrid.Cayenne Turbo.Cayenne S.Cayenne.Cayenne Turbo, Cayenne S and CayenneCayenne E-HybridDriveand chassis.Cayenne Turbo5641273Cayenne E-Hybrid 1 3.0-litre V6 combustion engine 2Power electronics 3Electric motor 4High-voltage cable 5 On-board charger 6 Vehicle charge port 7 High-voltage batteryCayenne E-HybridCayenne TurboCayenneE FD C B ACayenneCayenne S12Cayenne Turbo1Cayenne Turbo4215310951271211863413Comfort and infotainment.Cayenne Turbo1265Seats | Comfort and infotainment2312 131236558917441Burmester® two-way centre speaker 2 3D surround speaker 3Tweeter (air motion transformer, AMT)4 Midrange speaker 5 Bass speaker 6Tweeter 7 Two-way 3D surround speaker 8Burmester® active subwoofer with 400-watt class D digital ampli er 9B urmester® 21-channel, 1,055-watt digital ampli er1223461 BOSE® centre speaker2 Tweeter3 Midrange speaker 4Bass speaker 5 Bass-midrange speaker 6 Surround speaker 7 BOSE® 14-channel, 710-watt digital ampli er 8 BOSE® passive subwoofer 7815Porsche Connect.Lighting and assistance systems.1 2122 11。

MATRIX 120

MATRIX 120

MATRIX 120™APPLICATION• Electronics: Track and trace PCB board manufacturing• Factory Automation: Print & Apply – label verification• Factory Automation: Food & Beverage – traceability• OEM: Kiosks: ticketing machine• Healthcare: Clinical Lab – vials identification • Chemical and biomedical analysis machineHIGHLIGHTS• Ultra compact dimensions for easy integration • WVGA – 1.2 MP and wide angle models• Smart user selectable focus for high application flexibility• Digimarc Barcode reading technology for added value decoding applications • Embedded Ethernet connectivity• Serial and USB options on the same model • ESD versions for electronic applications• Polarized Version for 90° mounting and reflecting surfaces• Models equipped with shorter output cables (100mm of length) for easier integration in OEM machines • Top industrial grade: IP65; operating temperatures: 0-45 ºC / 32 – 133 ºF • DL.CODE software configurator for outstanding ease of setup• Xpress, Datalogic’s ‘Green Spot’ technology and intuitive HMI for top ease of useThe Matrix 120 is the smallest ultra-compact industrial 2D imager range in the market to fit any integration space and the smallest compact 2D imager with embedded Ethernet connectivity.The Matrix 120 is available in different models, including a WVGA sensor for standard applications or a 1.2 MP sensor for high resolution bar codes. Moreover, a wide angle version makes the Matrix 120 the perfect solution for proximity reading.The Matrix 120 with the red light model is the first stationaryindustrial scanner in the market able to read Digimarc Barcode for added value decoding applications.The Matrix 120 features the top industrial grade parts in its class (IP65 and 0-45 ºC / 32 – 133 ºF), with ESD safe models for applications in the electronic industry and a glass-free reading window, suitable for the Food and Beverage environment.Sulfur gas protection allows the use of Matrix 120 in tires applications through rough manufacturing, final finishing and inspection stations.As part of the full Matrix series, the Matrix 120 leads the market for customer ease of use because of DL.CODE™ configuration software, X-Press™ button and intuitive HMI.The Matrix 120 is the entry level model of the best-in-class Matrix family of high performance industrial 2D imagers.The Matrix 120 is the perfect solution when small dimension, simple integration and performance are the key drivers. The Matrix 120 models with shorter output cables (only 100 mm of length) allow an easier integration in OEM machines, making this product ideal for customers belonging to Chemical/Biomedical Industry and Print & Apply applications. Additionally, this imager is perfect for entry level applications in the Factory Automation arena: Electronics, Packaging and Food/Beverage.MATRIX 120™TECHNICAL DATAOPTICAL FEATURESSensor CMOS sensor with Global Shutter/WVGA - 752x480 pxCMOS sensor with Global Shutter/1.2 MP - 1280x960 pxFrame Rate up to 57 full-frame/s (WVGA model) , up to 36 full-frame/s(1.2 MP model)Illumination White Internal IlluminatorFocusing System Manual adjustment in three precalibrated positions(45, 70, 125mm - WVGA ; 45, 80, 125mm - 1.2 MP)DATALOGIC PRODUCT OFFERINGSafety Light Safety Laser Laser Marking Mobile ComputersVision SensorsHand Held MODELSCODE 937800000937800001937800002937800003937800004937800005。

农学专业英语3复习题

农学专业英语3复习题

Accrue:自然增加,产生Deplete:耗尽,使衰竭Deterioration:恶化,退化Duration:持续时间,为期Elimination:消除Fragile:易碎的,脆的Hammering:捶打,击打Humid:潮湿的,湿润的,多湿气的Impetus:推动力,促进Irrefutable:不能反驳的,不能驳倒的No-tillage:免耕salination:盐化(作用)Muloh:覆盖)Stubble-muloh: 秸秆覆盖Amenity :使人愉快的事物或环境Deceleration:减速Elasticity: 弹性,伸缩性Incremental:增长性Infrastructure:基础,基本建设Ingredient:成分,调料Pronounced:明显的Scenario:方案Strident:尖锐的Subsector:亚区,分布,部分Substantially:实质的Welfare:幸福,健康,福利Acquisition:获得,获得物Cytoplasmic: 细胞质的Cytoplasmic male sterility :细胞质雄性不育Genotype:基因型Hybrid:杂交的Hybridization:杂交Pollinate:授粉Since the 1940s,andparticularly during the last thirty years, maize and wheat have become increasingly important in developing countries. In the early 1960s,the developing world accounted for just over a third of global maize production and less than 30% of global wheat output . By the early 1990s , developing countries accounted for more than 45% of total world production of both cereals. Maize production in developing countries grew at an annual rate of 3.6% from 1961 to 1995; wheat production at an even faster rat自1940年代以来,特别是在过去的三十年,玉米和小麦在发展中国家中发挥了变的越来越重要。

IBM Cognos Transformer V11.0 用户指南说明书

IBM Cognos Transformer V11.0 用户指南说明书
Dimensional Modeling Workflow................................................................................................................. 1 Analyzing Your Requirements and Source Data.................................................................................... 1 Preprocessing Your ...................................................................................................................... 2 Building a Prototype............................................................................................................................... 4 Refining Your Model............................................................................................................................... 5 Diagnose and Resolve Any Design Problems........................................................................................ 6

Series 7250 Ruska Pressure Controller Calibrator说明

Series 7250 Ruska Pressure Controller Calibrator说明

Technical DataFeatures• Pressure ranges from 0 to 5 and 0 to 3 000 psi (0 to 35 kPa and 0 to 21 MPa)• Model 7250xi and 7250i provide advanced precision of 0.005 % of reading• Model 7250 provides 0.003 % of full scale precision• Stability: 0.0075 % of reading per year • Time to setpoint: 20 seconds with no overshoot• Control stability: 10 ppm• Active matrix color screen with enhanced navigation menus• Languages: English, French, Chinese, German, Japanese, Spanish and ItalianSeries 7250Ruska Pressure Controller/CalibratorThe Series 7250 high speed digital pressure controllers represent the fifth generation of automatic pressure controllers from Fluke Cali-bration and offers unmatched performance, an active matrix color screen and enhanced control stability. Utilizing multiple sensors and ranges in a single instrument, the Series 7250 combines precision, stability, speed and affordability. Models 7250xi, 7250i and 7250, up to 2 500 psi (17.2 MPa), use a unique quartz sensor, the most accurate pressure sensingtechnology in a pressure calibrator. Each quartz sensor is manufactured and tested to provide the ultimate performance required by a Fluke Calibration pressure calibrator, ensuring that every customer receives quality, precision and stability in their instrument.Advanced precision Models 7250xi and 7250i offer advanced per-cent of reading precision for increased capability with a single instrument, reducing the invest-ment required to calibrate a wide variety ofpressure devices and ranges. The Model 7250xi provides 0.005 % of reading precision from5 % to 100 % of the instrument’s range. Thisunmatched precision is achieved through unique quartz pressure sensing technology and mul-tiple quartz sensors in a single instrument. The 7250xi is available with any full scale range from 20 to 2 500 psi (140 kPa to 17.2 MPa). The Model 7250i provides 0.005 % of reading from 25 % to 100 % of range and is available with any full scale range from 5 to 2 500 psi (35 kPa to 17.2 MPa).For pressure below the lower threshold of 5% for the 7250xi and 25 % for the 7250i, the precision becomes 0.005 % of the lower value. For example, a 1 000 psi (7 MPa) Model 7250xi provides 0.005 % of reading from 50 to 1 000 psi (35 kPa to 7 MPa); the precision for pressures from 0 to 50 psi (0 to 35 kPa) is 0.005 % of 50 psi (35 kPa).Selecting the full scale range of the 7250xiand 7250i to purchase is simplified with thepercent of reading capability. Simply determine the highest pressure required and then decide if 0.005 % of reading is required down to 25 % or 5 % to maintain the appropriate calibration ratio. The complex analysis associated with selectingthe appropriate single or multirange instruments with percent of full scale performance is no 19812 Fluke Calibration Series 7250 Ruska Pressure Controller/Calibratorlonger required. And, since the performance of the 7250xi and 7250i is continuous throughout the range, the time consuming task of control-ling to atmosphere and switching ranges is eliminated.The 7250xi and 7250i not only provide unequalled precision, but also excellent long term stability due to the inherent properties of quartz in combination with several enhance-ments implemented over the last few years. The total uncertainty of the 7250xi and 7250i over a one year calibration interval is 0.009 % ofreading down to 5 % and 25 %, respectively (see the table, above right). Simplified specifications eliminate guesswork and “specmanship” to allow you to determine the actual performance delivered with every instrument.Standard precision For applications that do not require the level of performance provided in the 7250xi or 7250i, the Model 7250 offers an economical approach to automatic pressure testing and calibration with a precision of 0.003 % of full scale for ranges to 2 500 psi (17.2 MPa). High pressure precision For applications that require pressures up to3 000 psi (21 MPa), the Model 7250HP provides total uncertainty (one year calibration interval) of 0.013% of reading down to 30% of the fullscale. The 7250HP provides the high speedcontrol and performance of the standard 7250with a full scale pressure range of 3 000 psi(21 MPa) absolute.High-speed pressurecontrolAll Series 7250 instruments up to 2 500 psi (172 bar) reach setpoint in 20 seconds or less into a 15 cubic inch (245 cc) volume, with no overshoot, to allow high-speed pressure test and calibration.Dual control modesThe Series 7250 also provides two user-selectable control modes: active and passiveThe Series 7250 features a unique fused-quartz sensor. This rugged transducer offersunequalled precision and a stability of 0.0075% of reading per year.mode. In active mode, the 7250 is continually maintaining the setpoint and can compensate for small leaks and pressure changes due to temperature. In passive mode, the user defines a control band and the 7250 will turn off the controller once it achieves the setpoint within the control band. In a leak-free and tempera-ture-stable system, passive mode contributes no additional uncertainty, providing optimum performance.Automating pressure test and calibrationThe 7250xi, 7250i and 7250 are easy to use and can automate your calibrations in several ways:Step up/down: for calibrations where the increments are fixed intervals, enter a user-defined step value. The Series 7250 increasesor decreases the pressure by the step amount with the jog dial—no more lengthy keystroke sequences to program.Sweep test: for simple exercising routines, as with dial gauges, enter a start value, a stop value, and number of times to repeat the cycle. The Series 7250 will automatically exercise thedevice under test prior to the calibration run.Onboard programs: For frequently used orlengthy calibrations, the Series 7250 can store up to 20 user-defined programs/profiles with up to 1000 steps total in internal memory.Computer interface: Every Series 7250 is provided with both an RS-232 and IEEE-488 interface, and Series 7250 syntax follows SCPI protocol for easy programming. CoMPASS ®, an off-the-shelf software package is avail-able in addition to the LabVIEW ® driver, a free download and optional MET/CAL ® driver. As a standard feature, software written for the previous generation Series 7215, 7010 and 6000instruments is fully supported by the Series 7250. The Series 7250 can also be set to 510 emulation mode to use software originally writ-ten for the DPI 510. Firmware updates can also be performed over the RS-232 interface.Versatility to handle any pneumaticpressure calibrationThe Series 7250 is versatile enough to handle almost any type of pneumatic pressure calibration.Wide pressure range: available with any full scale pressure between 5 and 2 500 psi (35 kPa and 17.2 MPa) or for higher pressures select the 3 000 psi absolute (21 MPa) range.Pressure units/scales: Select from over twelve standard units of measure, including inHg at 0 °C and 60 °F, kPa, bar, psi, inH2o at 4 °C, 20 °C and 60 °F, kg/cm2, mmHg at 0 °C, cmHg at 0 °C, and cmH2o at 4 °C, and two user-defined units.Head pressure: Automatic correction for head pressure differencesAbsolute mode: The 7250i and 7250 offer three different methods to make absolute pres-sure measurements. The barometric reference option provides the most convenient method and is available on ranges 15 psi (1.0 bar) and higher. Alternatively, the vacuum reference option allows the connection of an externalvacuum pump to the reference port of the instrument. An onboard vacuum sensor monitors the reference vacuum and allows for automatic zeroing in absolute mode. This option provides the lowest overall uncertainty since it does not include the additional uncertainty of a second-ary barometric reference sensor. For pressure to 50 psia (350 kPa) permanent absolute models are also available. The 7250xi is only available with the barometric reference option for abso-lute measurement.Autovent and autozero: With few keystrokes, the Series 7250 will vent the test port to atmo-sphere or automatically zero itself (autovent is not applicable to permanent absolute models). Protection of the device under test: Set upper and lower pressure limits to ensure protection of the device under test.OptionsThe Series 7250 can be provided for gauge mode operation, or with:•optional vacuum (negative gauge) mode for bidirectional devices•optional barometric reference for absolute mode calibrations•Permanent absolute ranges to 50 psia (350 kPa) full scale which include a tare feature for simulated gauge mode operationThe Series 7250 Pressure Controller/Calibrator can easily automate your test and calibration workload. All are easy to use, easy to main-tain, and have the reliability, performance and features that you want. The Series 7250 features an easy-to-navigate menu structure with full text descriptions for menus and commands.The large color display allows the pressure value to be displayed even when viewing a submenu selection such as the units selection screen shown above.All Series 7250s are fully programmable and can store up to 20separate programs with up to 1000 steps.3 Fluke Calibration Series 7250 Ruska Pressure Controller/Calibrator4 Fluke Calibration Series 7250 Ruska Pressure Controller/CalibratorSpecificationsFluke CalibrationPo Box 9090, Everett, WA 98206 U.S.A.Fluke Europe B.V.Po Box 1186, 5602 BD Eindhoven, The NetherlandsFluke Calibration. Precision, performance, confidence.™For more information call:In the U.S.A. (877) 355-3225 or Fax (425) 446-5116In Europe/M-East/Africa +31 (0) 40 2675 200 or Fax +31 (0) 40 2675 222 In Canada (800)-36-FLUKE or Fax (905) 890-6866From other countries +1 (425) 446-5500 or Fax +1 (425) 446-5116Web access: ©2010 Fluke Corporation.Specifications subject to change without notice. Printed in U.S.A. 9/2011 3833773B D-EN-NModification of this document is not permittedwithout written permission from Fluke Corporation.1and hysteresis throughout the operating temperature range.2Total uncertainty is the maximum deviation from the true value of pressure including precision, stability, temperature effects and the calibration standard. This assumes routine zeroing of the instrument. Expression of uncertainty conforms with the recommendations of the ISO Guide to the Expression of Uncertainty in Measurement.。

大模型lora微调原理

大模型lora微调原理

大模型lora微调原理LoRa (Long Range) is a low-power wide-area network (LPWAN) technology that enables long-range communication between devices with low data rates. It is designed to provide efficient and reliable connectivity for Internet of Things (IoT) applications. Large-scale LoRa models are often used in scenarios where a high number of devices need to be connected over a wide area, such as smart cities, industrial automation, and agriculture.The process of fine-tuning a large-scale LoRa model involves optimizing its performance by adjusting various parameters and configurations. This is done to ensure that the model can effectively handle the specific requirements of the application it is being used for. One of the key aspects of fine-tuning is optimizing the communication range and data rate.To achieve this, the LoRa model can be tuned by adjusting the spreading factor, which determines the datarate and range of the communication. A higher spreading factor results in a longer communication range but lower data rate, while a lower spreading factor provides higher data rates but shorter range. By finding the optimal spreading factor for a given application, the model can strike a balance between range and data rate.Another important parameter that can be fine-tuned is the bandwidth, which determines the amount of frequency spectrum used for communication. A wider bandwidth allowsfor higher data rates but requires more power, while a narrower bandwidth conserves power but limits the data rate. By selecting the appropriate bandwidth, the model can optimize its energy consumption and data transmission capabilities.In addition to these parameters, the LoRa model canalso be fine-tuned by adjusting the coding rate, which affects the robustness of the communication. A highercoding rate provides better resistance to noise and interference but reduces the data rate, while a lowercoding rate offers higher data rates but is moresusceptible to errors. Finding the right coding rate is crucial to ensure reliable and efficient communication in challenging environments.Moreover, the transmission power of the LoRa model can be fine-tuned to optimize its coverage and energy consumption. Higher transmission power allows for longer range but consumes more energy, while lower transmission power conserves energy but limits the coverage area. By adjusting the transmission power based on the specific requirements of the application, the model can achieve the desired balance between coverage and energy efficiency.Furthermore, the network architecture and deployment strategy play a vital role in fine-tuning a large-scale LoRa model. The placement and density of gateways, which act as the communication infrastructure, need to be carefully planned to ensure optimal coverage and connectivity for all devices. The network topology, including the number of gateways and their distribution, should be optimized to minimize interference and maximize network performance.In conclusion, fine-tuning a large-scale LoRa model involves optimizing various parameters such as spreading factor, bandwidth, coding rate, and transmission power. By adjusting these parameters based on the specific requirements of the application, the model can achieve the desired balance between range, data rate, energy consumption, and reliability. Additionally, careful planning of the network architecture and deployment strategy is essential to ensure optimal coverage and connectivity. Fine-tuning a large-scale LoRa model requires a thorough understanding of the application requirements and a systematic approach to optimize its performance.。

GBDT与感知机融合的充电桩故障诊断方案

GBDT与感知机融合的充电桩故障诊断方案
断路器跳闸;断路器器件损坏;短路或者 过流
为描述充电桩故障检测问题,本文使用向量 x∈ L×1表示从充电桩上采集的 1 组物理量,例如电
压的总谐波失真、电流的总谐波失真、电子锁驱动 信号等。 本文任务是根据向量 x 将充电桩分成正常 和有故障两类,其类别标签可由变量 y∈{0,1}表示。
因此,充电桩故障诊断模型可以表示为
2.2 模型实现细节
根 据 集 成 学 习 的 Stacking 框 架 与 理 论[14],建 立
多个独立的 GBDT 模型。 考虑到充电桩故障的数据
量,本方案使用了 2 个 GBDT 层,如图 4 所示。 充电桩
数据向量 x 输入第一个 GBDT 层,该层由 5 个 GBDT
模 型 构 成 。 第 二 个 GBDT 层 由 3 个 GBDT 模 型 构
故障描述 绝缘检测故障 充电模块输出过电压
充电模块输出过电流
直流母线输出过电压 交流输入故障
交流断路器故障
故障原因
设备接地;绝缘检测模块故障
单模块输出电压过大引起系统过电压保 护 99%
充电模块输出电流超过系统预先设定的 阈值
直流母线输出侧冲击电压过大,模块输出 失控
交流断电;交流输入缺相;交流输入过电压
反馈 信号
IGBT 驱动
控制电路
控制电路
变压器及 输出滤波
输出 负载
输出 信号
图 1 充电桩的系统结构 Fig.1 System architecture framework of charging pile
直流充电设施控制回路原理如图 2 所示。 直流 充电桩(非车载充电机)与电动汽车通过车辆插头
Automation & Instrumentation 2024,39穴4雪

大模型微调应用场景

大模型微调应用场景

大模型微调应用场景The application scenarios of large model fine-tuning are vast and diverse, encompassing various industries and tasks. In the realm of natural language processing, fine-tuning is often employed to adapt pre-trained language models to specific tasks such as sentiment analysis, text classification, and question answering. These tasks require the model to understand the context and meaning of text, making fine-tuning a crucial step in achieving accurate and reliable results.大模型微调的应用场景广泛而多样,涵盖了多个行业和任务。

在自然语言处理领域,微调常常用于将预训练的语言模型适应于特定的任务,如情感分析、文本分类和问答等。

这些任务要求模型理解文本的上下文和含义,因此微调是实现准确可靠结果的关键步骤。

In the field of computer vision, fine-tuning large models is commonly used for image recognition, object detection, and image segmentation. By leveraging the powerful feature extraction capabilities of pre-trained models, fine-tuning can help improve the accuracy and efficiency of these tasks. Additionally, with the rise of multimodal learning, fine-tuning is also being explored for tasks that involve both text and image data, such as image captioning and visual question answering.在计算机视觉领域,大模型的微调常用于图像识别、目标检测和图像分割等任务。

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Performance Models for Large Scale Multiagent Systems: Using Distributed POMDP Building BlocksHyuckchul Jung,Milind T ambeComputer Science Department,University of Southern California941W.37th Place,Los Angeles,CA90089-0781,USAjungh,tambe@ABSTRACTGiven a large group of cooperative agents,selecting the right coor-dination or conflict resolution strategy can have a significant impact on their performance(e.g.,speed of convergence).While perfor-mance models of such coordination or conflict resolution strategies could aid in selecting the right strategy for a given domain,such models remain largely uninvestigated in the multiagent literature. This paper takes a step towards applying the recently emerging dis-tributed POMDP(partially observable Markov decision process) frameworks,such as MTDP(Markov team decision process),in service of creating such performance models.To address issues of scale-up,we use small-scale models,called building blocks that represent the local interaction among a small group of agents.We discuss several ways to combine building blocks for performance prediction of a larger-scale multiagent system.We present our approach in the context of DCSPs(distributed constraint satisfaction problems),where wefirst show that there is a large bank of conflict resolution strategies and no strategy dom-inates all others across different domains.By modeling and com-bining building blocks,we are able to predict the performance of five different DCSP strategies for four different domain settings, for a large-scale multiagent system.Our approach thus points the way to new tools for strategy analysis and performance modeling in multiagent systems in general.1.INTRODUCTIONIn many large-scale applications such as distributed sensor nets, distributed spacecraft and disaster response simulations,collabora-tive agents must coordinate their actions or resolve conflicts over shared resources or task assignments[6,9,13].Selecting the right coordination or conflict resolution strategy can have a significant impact on performance of such agent communities.For instance,in distributed sensor nets,tracking targets quickly requires that agents controlling different sensors adopt the right strategy to resolve con-flicts regarding shared sensors.Unfortunately,selecting the right coordination strategy is diffi-cult.First,there are often a wide diversity of strategies available, and they can lead to significant variations in the rate of conflictPermission to make digital or hard copies of all or part of this work for personal or classroom use is granted without fee provided that copies are not made or distributed for profit or commercial advantage and that copies bear this notice and the full citation on thefirst page.To copy otherwise,to republish,to post on servers or to redistribute to lists,requires prior specific permission and/or a fee.Copyright2002ACM X-XXXXX-XX-X/XX/XX...$5.00.resolution convergence in multiagent systems.For instance,when distributed agents must resolve conflicts over shared resources such as shared sensors,they could select a strategy that offers maximum possible resources to most constrained agents,or that distributes re-sources equally among all agents requiring such resources,and so on.Each strategy may create a significant variation in the conflict resolution convergence rate[6,13].Furthermore,faced with cer-tain types of problem domains,a single agent cannot immediately determine the appropriate coordination or conflict resolution strat-egy,because it is typically not just this agent’s actions,but rather the actions of the entire community that determine the outcome. Performance modeling of multiagent coordination and conflict resolution could help predict the right strategy to adopt in a given domain.Unfortunately,performance modeling has not received significant attention in mainstream multiagent research commu-nity;although within subcommunities such as mobile agents,per-formance modeling has been considerably investigated[15].For-tunately,recent research in distributed POMDPs(partially observ-able Markov decision processes)and MDPs(Markov decision pro-cesses)has begun to provide key tools to aid multiagent researchersin modeling the performance of multiagent systems[14,1,17].In the context of this paper,we will use the MTDP model[14]for performance modeling,although other models could be used. There are at least two major problems in applying such distributed POMDP models.First,while previous work has focused on model-ing communication strategies within very small numbers of agents[14], we are interested in strategy performance analysis for large-scale multiagent systems.Second,techniques to apply such models to in-vestigate other types of coordination and conflict resolution strate-gies have not been investigated.We address these limitations in the context of DCSPs(distributed constraint satisfaction problems),which is a major paradigm of the research on conflict resolution[18,16,5,19].Before address-ing the limitations,we introduce DCSPs and our previous work in which we have illustrated the presence of multiple conflict resolu-tion strategies and showed that cooperative strategies can improve performance in conflict resolution convergence.Ourfirst contri-bution in this paper is to illustrate that more strategies exist and that indeed no single strategy dominates all others.Since the best strategy varies over different domains,given a specific domain,se-lecting the best strategy is essential to gain maximum efficiency and it is a great challenge for us.Our second key contribution is to illustrate the use of MTDPto model the performance of different strategies to select the right strategy.To address the limitations in the MTDP modeling intro-duced above,wefirst illustrate how DCSP strategies can be mod-eled in MTDP.Next,to address scale-up issues,we introduce small-scale models called”building blocks”that represent the local inter-Agent A3LC2LC3LC4Agent A4C13C24C34C12Agent A1LC1X1X2X3X4V1V2V3V4(a)Agent A2(b)Figure 1:Model of agents in DCSPaction among a small group of agents.We discuss several ways to combine building blocks for performance prediction of a larger-scale multiagent system.2.BACKGROUNDDCSP techniques have been used for coordination and conflict resolution in many multiagent applications such as distributed sen-sor network [9].In this section,we introduce the DCSP and effi-cient DCSP strategies.2.1Distributed Constraint Satisfaction Prob-lems (DCSPs)A Constraint Satisfaction Problem (CSP)is commonly defined by a set of variables,=,...,,each element associ-ated with value domains ,...,respectively,and a set of constraints,=,...,.A solution in CSP is the value as-signment for the variables which satisfies all the constraints in .A DCSP is a CSP in which variables and constraints are distributed among multiple agents [18].Formally,there is a set of m agents,=,...,.Each variable ()belongs to an agent .There are two types of constraints based on whether variables in a constraint belong to a single agent or not:For a constraint ,if all the variables in belong to a single agent,it is called a local constraint .For a constraint ,if variables in belong to different agents in ,it is called an external constraint .Figure 1-a illustrates an example of a DCSP:each agent (de-noted by a big circle)has a local constraint and there is an external constraint between and .As illustrated in Fig-ure 1-b,each agent can have multiple variables.There is no lim-itation on the number of local/external constraints for each agent.Solving a DCSP requires that agents not only satisfy their local constraints,but also communicate with other agents to satisfy ex-ternal constraints.Note that DCSPs are not concerned with speed-ing up centralized CSPs via parallelization;rather,it assumes that the problem is originally distributed among agents.2.2Asynchronous Weak Commitment (A WC)Search AlgorithmAsynchronous Weak Commitment (AWC)search algorithm is the best published DCSP algorithm[18].In the AWC approach,agents asynchronously assign values to their variables from do-mains of possible values,and communicating the values to neigh-boring agents with shared constraints.Each variable has a non-negative integer priority that changes dynamically during search.A variable is consistent if its value does not violate any constraints with higher priority variables.A solution is a value assignment in which every variable is consistent.To simplify the description of the algorithm,suppose that each agent has exactly one variable and the constraints between variables are binary.When the value of an agent’s variable is not consistent with the values of its neighboring agents’variables,there can be two cases:(i)a good case where there exists a consistent value in the variable’s domain;(ii)a nogood case that lacks a consistent value.In the good case with one or more value choices available,an agent selects a value that minimizes the number of conflicts with lower priority agents.On the other hand,in the nogood case,an agent increases its priority to max+1,where max is the highest pri-ority of its neighboring agents,and selects a new value that min-imizes the number of conflicts with all of its neighboring agents.This priority increase makes previously higher agents select new values.Agents avoid the infinite cycle of selecting non-solution values by saving the nogood situations.2.3Cooperativeness-based StrategiesWhile AWC is one of the most efficient DCSP algorithms,real-time and dynamism in multi-agent domains demands very fast con-flict resolution convergence.Thus,novel DCSP strategies were in-troduced for fast conflict resolution convergence [6].While AWC relies on the min-conflict heuristic [8]that minimizes conflicts with other agents,the new strategies enhanced by local constraint com-munication consider how much flexibility (choice of values)is given towards other agents by a selected value.By considering neighbor-ing agents’local constraints,an agent can generate a more locally cooperative response,potentially leading to faster conflict resolu-tion convergence.The concept of local cooperativeness goes beyond merely satis-fying constraints of neighboring agents to accelerate convergence.That is,an agent cooperates with a neighbor agent by select-ing a value for its variable that not only satisfies the constraint with ,but also maximizes ’s flexibility (choice of values).Then has more choices for a value that satisfies ’s local constraints and other external constraints with its neighboring agents,which can lead to faster convergence.To elaborate this notion of local cooperativeness,the followings were defined in [6].Definition 1:For a value and a set of agents(a set of neighboring agents),a flexibility function is defined as =such that and is the number of values of that are consistent with .Definition 2:For a value of ,local cooperativeness of is defined as .That is,the local cooperativeness of measures how much flexibility (choice of values)is given to all of ’s neighbors by .As an example of the flexibility function ,suppose agent has two neighboring agents and ,where a value leaves 70consistent values to and 40to while another value leaves 50consistent values for and 49to .Now,assuming that values are ranked based on flexibility,an agent will prefer to :=110and =99.These definitions of flexibility function and local cooperativeness are applied for the cooperative strategies defined as follows::Each agent selects a value based on min-conflict heuristics (the original strategy in the AWC algorithm);:Each agent attempts to give maximum flexibility towards its higher priority neighbors by selecting a value that maximizes ;501001502002503003504000%20%40%60%80%100%percentage of locally constrained agentsc y c l e sFigure 2:Strategy comparison with cycles:Each agent attempts to give maximum flexibilitytowards its lower priority neighbors by selecting a value that maximizes ;:Each agent selects a value that maximizes ,i.e.max flexibility to all neighbors.These four strategies can be applied to both the good and nogood cases.(Refer to [6]for detailed information.)Therefore,there are sixteen strategy combinations for each flexibility base.Since,we will only consider strategy combinations,henceforth,we will refer to them as strategies for short.Note that all the strategies are en-hanced with constraint communication and propagation.Here,two exemplar strategies are listed::This is the original AWC strategy.Min-conflict heuristic is used for the good and nogood cases.:For the good case,an agent is most locallycooperative towards its lower priority neighbor agents by us-ing .(Note that the selected value doesn’t violate the constraints with higher neighbors).On the contrary,for the nogood situations,an agent attempts to be most locally coop-erative towards its higher priority neighbors by using.2.4Experimental EvaluationAn initial principled investigation of these strategies can improveour understanding not only of DCSP strategies,but potentially shed some light on how cooperative an agent ought to be towards its neighbors,and with which neighbors.To that end,a number of DCSP experiments were done with an abstract problem setting.Here,agents (variables)are in a 2D grid configuration (each agent is externally constrained with four neighbors except for the ones on the grid boundary).All agents share an identical binary constraint by which a value in an agent is not compatible with a set of val-ues in its neighboring agent.This grid configuration is motivated by the research on distributed sensor network [9]where multiple agents must collaborate to track targets.For additional justification and domains,refer to [6].In the experiments,the total number of agents was 512and each agent has 36(=66)values in its domain.In addition to the exter-nal binary constraint,agents can have a unary local constraint that restricts legal values into a set of randomly selected values among its original 36values.The evaluation followed the method used in [18].In particular,performance evaluation is measured in terms of cycles consumed until a solution is found,and the experimentsranged over all possible strategies.In Figure 2,for expository pur-pose,only five strategies are presented,which does not change the conclusions in [6].The vertical axis plots the number of cycles and the horizontal axis plots the percentage of locally constrained agents.The performance difference between different strategies are proved to be statistically significant by performing -test.A key point to note is that choosing the right strategy has signif-icant impact on convergence.Certainly,choosing(the top line in Figure 2)may lead to significantly slower conver-gence rate while appropriately choosingor can lead to significant improvements in convergence.How-ever,we may not need to consider all the strategies for selecting the best since significant performance improvement can be achieved byalone.3.MORE COOPERATIVE STRATEGIESWhile novel cooperative strategies in Section 2improved con-flict resolution convergence,two questions remain unanswered:(i)can we apply for conflict resolution across different domains?;(ii)in addition to the strategies defined in Section 2,are there more local cooperativeness based strategies?In this section,to address these two questions,first,we provide more possible DCSP strategies based on the local cooperativeness.Second,experimental results in different types of domains are pre-sented.The results show that there is no single dominant strategy (like )across all domains.3.1New Basis for CooperativenessWhile the novel value ordering strategies (proposed in [6])im-proved the performance in conflict resolution,the definition of the flexibility function using summation ()may not be the most ap-propriate way to compute the local cooperativeness.Example :suppose we are given two neighboring agentsand ,where a value leaves 99consistent values to and 1to while another value leaves 50consistent val-ues for and 49to .Now,according to the cooperative-ness definition in Section 2.3,an agent will prefer to :=100and =99.However,leaving one value choice to by the value can have high chances of conflicts for in the future.Here,we extend the flexibility function to accommodate differ-ent types of possible local cooperativeness:Definition 3:For a value and a set of agents ,flexibility function is defined as =()where (i);(ii)is the number of values of that are consistent with ;and (iii),referred to as a flexibility base ,can be ,,,,,etc.;With this new definition,for the above example,if is set to instead of ,an agent will rank higher than :=1and =49.We can apply theseextended definitions of the flexibility function to the cooperative strategies defined in [6].That is,the cooperative strategies defini-tions hold with the only change in the flexibility function.3.2New Experimental EvaluationTo provide the evaluation of these extended strategies,a number of DCSP experiments were done with the problem setting used in [6].Here,to test the performance of strategies in various problem501001502002503003504000%20%40%60%80%100%percentage of locally constrained agents c y c l e sFigure 3:Strategy comparison in high flexibility setting withas a flexibility basesettings,we make a variation in the problem setting by modify-ing the external constraint:in a new setting,each agent gives less flexibility (choice of values)towards its neighboring agents given a value in its domain.Henceforth,the previous setting is referred as a high flexibility setting ,and the new setting with less choice of values to neighbors is referred as a low flexibility setting .Experiments were performed in the two problem settings (the high flexibility setting and the low flexibility setting ),and both and were used as a flexibility base ().Other than this exter-nal constraint variation,the parameters for the experiments remain same.Each data point in the figures was averaged over 500test runs.While all the possible strategies for each flexibility base were tried,for expository purpose,only five strategies are presented in Figure 3and 4,which does not change our conclusion.Figure 3shows the case where is used as a flexibility base in the high flexibility setting .Here,note that shows much worse performance than in some cases.Over-all,in this domain,strategies with as a flexibility base do not improve performance over the strategies with as a flexibilitybase.Figure 4shows the case whereis used as a flexibility base,but the problem instances are generated in the low flexibil-ity setting .Note that the experimental results shown in Figure 2were also based on as a flexibility base but they were from the high flexibility setting .The significant difference between the high flexibility setting (Figure 2)and the low flexibility setting (Fig-ure 4)is thatis not the overall dominant strategy in the low flexibility setting .Furthermore,(that performed well in the high flexibility setting )showed worse performance than the original AWC strategy ,in particular when the percentage of locally constrained agents is low.These experimental results show that different flexibility bases also have an impact on performance.For instance,choosing as a flexibility base ()instead of may degrade performance for some cooperative strategies.Furthermore,these results clearly show that choosing the right strategy given a domain has a signif-icant impact on convergence.Certainly,when 80%of agents are locally constrained,and showed the same performance in the high flexibility setting (Figure 2).How-ever,in the low flexibility setting (Figure 4),showed 10fold speedup over .To conclude,no single strategy dominates in different domains.As shown above,the best strategy in a domain could produce 10times worse performance than others in another domain.Thus,to gain maximum efficiency in conflict resolution,it is essential to predict the right strategy in a given domain.as a flexibilitybase3.3Long tail distribution in ConvergenceThe key factor in determining the performance of strategies is in the long tail where only a small number of agents are in conflicts.As illustrated in Figure 5that shows the number of conflicts at each cycle for two different strategies,in the beginning of conflict reso-lution,both strategies show similar performance in resolving con-flicts.However,the performance difference appears in the long tail part.While strategy 1quickly solves a given problem,strategy 2has a long tail with a small number of conflicts remaining unre-solved.This type of long tail distribution has been also reported in many constraint satisfaction problems [4].4.PERFORMANCE ANALYSISSection 3shows that,given the dynamic nature of multiagent systems,predicting the right strategy to use in a given domain is essential to maximize the speedup of conflict resolution conver-gence,and the critical factor for strategy performance is in the long tail part where a small number of conflicts exist.Here,we provide formal models for performance analysis and the mapping of DCSP onto the models,and present the results of performance prediction.4.1Distributed POMDP-based ModelAs a formal framework for strategy performance analysis,we use a distributed POMDP model called MTDP (Multiagent Team De-cision Process)model[14].The MTDP model has been proposed as a framework for teamwork analysis.Distributed POMDP-basedmodel is an appropriate formal framework to model strategy perfor-mance in DCSPs since it has distributed agents and the agentView in DCSPs(other agents’values,priorities,etc.)can be modeled as observations.In DCSPs,the exact state of the system is only partially observable to an agent since the received information for the agent is limited to its neighboring agents.Therefore,there is strong correspondence between DCSPs and distributed POMDPs. While we focus on the MTDP model in this paper,other distributed POMDP models such as DEC-POMDP[1]could be used. Here,we illustrate the actual use of the MTDP model in analyz-ing DCSP strategy performance.The MTDP model provides a tool for varying key domain parameters to compare the performance of different DCSP strategies,and thus select the most appropriate strategy in a given situation.Wefirst briefly introduce the MTDP model.Refer to[14]for more details.4.1.1MTDP modelThe MTDP model involves a team of agents operating over a set of world states during a sequence of discrete instances.At each instant,each agent chooses an action to perform and the actions are combined to affect a transition to the next instance’s world state. Borrowing from distributed POMDPs,the current state is not fully observed/known and transitions to new world states are probabilis-tic.Each agent makes its own observations to compute its own beliefs,and the performance of the team is evaluated based on a joint reward function over world states and combined actions. More formally,an MTDP for a team of agents,,is a tuple,.S is a set of world states.is a set of combined actions where is the set of agent ’s actions.controls the effect of agents’actions in a dynamic en-vironment:.is a set of combined observations.Observation function,specifies a probability distribution over the observations of an agents team. Belief state is derived from the observations.is a reward function over states and joint actions.A policy in the MTDP model maps individual agents’belief states to actions.A DCSP strategy is mapped onto a policy in the model.Thus,we compare strategies by evaluating policies in this model.Our ini-tial results from policy evaluation in this model match the actual experimental strategy performance results shown before.Thus,the model could potentially form a basis for predicting strategy perfor-mance in a given domain.4.1.2Mapping from DCSP to MTDPIn a general mapping,thefirst question is selecting the right state representation for the MTDP.One typical state representation could be a vector of the values for all the variables in a DCSP.However, this representation leads to a huge state space.For instance,if there are10variables(agents)and10possible values per variable,the number of states is.To avoid this combinatorial explosion in state space,we use an abstract state representation in the MTDP model.In particular,as described in the previous section,each agent can be abstractly characterized as being in a good or nogood state in the AWC algorithm.We use this abstract characterization in our MTDP model.Henceforth,the good state and the nogood state are denoted by and respectively.Here,an initial state of the MTDP is a state where all the agents are in state since,in the AWC,an agentfinds no inconsistency for its initial values until it receives the values of its neighboring agents.Note that,for sim-plicity,the case where agents have no violation is not considered. In this mapping,the reward function is considered as a costC CCCC C CCCU CCCUC(a)(b)(c)CCCC U CCUUUCCCUU(d)(e)(f)Figure6:Building blockfunction.The joint reward(cost)is proportional to the number of agents in the state.This reward is used for strategy evalu-ation based on the fact that the better performing strategy has less chance of forcing neighboring agents into the state than other strategies:as a DCSP strategy performs worse in a given problem setting,more agents will be in the states.In the AWC algorithm(a base DCSP algorithm in this paper), each agent receives observations only about the states of its neigh-boring agents and its current state as well.However,the world is not individually observable but rather it is collectively observable (in the terminology of Pynadath and Tambe[14]),and hence the mapping does not directly reduce to an MDP.Initially,we assume that these observations are perfect(without message loss in com-munication).This assumption can be relaxed in our future work with unreliable communication.Here,,,,and in DCSPs are mapped onto the actions for agents in the MTDP model.A DCSP strategy pro-vides a local policy for each agent in the MTDP model,e.g.,the strategy implies that each agent selects action when its local state is good,and action when its local state is nogood.The state transition in the MTDP model is controlled by an agent’s own action as well as its neighboring agents’actions. The transition probabilities can be derived from the simulation on DCSPs.4.1.3Building BlockWhile the abstract representation in the mapping above can re-duce the problem space,for a large-scale multiagent system,if we were to model belief states of each agent regarding the state of the entire system,the problem space would be enormous even with the abstract representation.For instance,the number of states in the MTDP model for the system with512agents would be:each agent can be either or.To further reduce the combinatorial explosion,we use small-scale models,called building blocks.Each building block represents the local situation amongfive agents in the2D grid configuration.In the problem domains for the experiments shown in Section 2.4and3.2,each agent’s local situation depends on whether it has a unary local constraint or not:each agents can be either constrained (a portion of its original domain values are not allowed)under a local constraint()or unconstrained().Figure6illustrates some exemplar building blocks for the domain used in the experiments. For instance,Figure6-a represents a local situation where all the five agents are constrained()while Figure6-b represents a local situation where an agent in the left side is unconstrained()but。

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