Adsorptive removal of Pb2+, Co2+ and Ni2+ by hydroxyapatite chitosan

合集下载

活性炭吸附汞共17页文档

活性炭吸附汞共17页文档
Sang-Sup Lee, et al 2009
Chemical Modification
Sang-Sup Lee, et al 2009
• Brominated activated carbon (Br; DARCO Hg-LH) • Cupric chloride-impregnated activated carbon (CuCl; C-AC)
Chemical Modification
Sang-Sup Lee, et al 2009
Thank you for your attention!
61、奢侈是舒适的,否则就不是奢侈 。—— CocoChanel 62、少而好学,如日出之阳;壮而好学 ,如日 中之光 ;志而 好学, 如炳烛 之光。 ——刘 向 63、三军可夺帅也,匹夫不可夺志也。 ——孔 丘 64、人生就是学校。在那里,与其说好 的教师 是幸福 ,不如 说好的 教师是 不幸。 ——海 贝尔 65、接受挑战,就可以享受胜利的喜悦 。—— 杰纳勒 尔·乔治 ·S·巴 顿
Physical Adsorption & Chemical Adsorption
• Chemical adsorption
Oxygen-containing: -COOH; COO-; Phenol; Carbonyl, et al.
Surface Oxygen: Hg on the surface of activated carbon is always together with Oxygen. (X-ray absorption fine structure spectroscopy )
Hg2+
Hale Waihona Puke N2 Hg0Physical Adsorption & Chemical Adsorption

水利部、工业和信息化部印发造纸等七项工业用水定额

水利部、工业和信息化部印发造纸等七项工业用水定额

《中国造纸》2021年第40卷第2期[31]Yousif Ahmed M ,Zaid Osama F ,El -Said Waleed A ,et al.SilicaNanospheres Coated Nanofibrillated Cellulose for Removal and Detection of Copper (II )Ions in Aqueous Solutions [J ].I &ECResearch ,2019,58(12):4828-4837.[32]Hokkanen Sanna ,Doshi Bhairavi ,Srivastava Varsha ,et al.Arsenic (III )removal from water by hydroxyapatite -bentonite clay -nanocrystalline cellulose [J ].Environmental Progress &Sustainable Energy ,2019,38(5):13147.[33]Zhou Yiming ,Fu Shiyu ,Zhang Liangliang ,et al ,Use ofcarboxylated cellulose nanofibrils -filled magnetic chitosan hydrogelbeads as adsorbents for Pb (II )[J ].Carbohydrare Polymers ,2014,101:75-82.[34]Wei Jie ,Yang Zhixing ,Sun Yun ,et al.Nanocellulose -basedmagnetic hybrid aerogel for adsorption of heavy metal ions fromwater [J ].Polymers ,2019,54(8):6709-6718.[35]Li Jian ,Xu Zhaoyang ,Wu Weibing ,et al.Nanocellulose/Poly (2-(dimethylamino )ethyl methacrylate )Interpenetrating polymer network hydrogels for removal of Pb (II )and Cu (II )ions [J ].Colloids and Surfaces A ,2018(538):474-480.[36]Li Jian ,Zuo Keman ,Wu Weibing ,et al.Shape memory aerogelsfrom nanocellulose and polyethyleneimine as a novel adsorbent for removal of Cu (II )and Pb (II )[J ].Carbohydrate Polymers ,2018,196:376-384.[37]TANG Juntao ,SONG Yang ,ZHAO Feiping ,et pressiblecellulose nanofibril (CNF )based aerogels produced via a bioinspired strategy for heavy metal ion and dye removal [J ].Carbohydrate Polymers ,2019(208):404.[38]Shahnaz Tasrin ,Fazil S Mohamed Madhar ,Padmanaban V C ,etal.Surface modification of nanocellulose using polypyrrole for theadsorptive removal of Congo red dye and chromium in binary mixture [J ].Biological Macromolecules ,2020(151):322-332.[39]Maatar Wafa ,Boufi Sami.Poly (methacylic acid -co -maleic acid )grafted nanofibrillated cellulose as a reusable novel heavy metalions adsorbent [J ].Carbohydrate Polymers ,2015(126):199-207.[40]Hokkanen Sanna ,Repo Eveliina ,SillanpääMika.Removal ofheavy metals from aqueous solutions by succinic anhydride modified mercerized nanocellulose [J ].Chemical Engineering Journal ,2013(223):40-47.[41]YU Xiaolin ,TONG Shengrui ,GE Maofa ,et al.Adsorption ofheavy metal ions from aqueous solution by carboxylated cellulose nanocrystals.[J ].Journal of Enviromental Science ,2013,25(5):933-943.[42]QIN Famei ,FANG Zhiqiang ,ZHOU Jie ,et al.Efficient Removalof Cu 2+in Water by Carboxymethylated Cellulose Nanofibrils :Performance and Mechanism [J ].Biomacromolecules ,2019,20(12):4466-4475.[43]Sharma Priyanka R ,Chattopadhyay Aurnov ,Sharma Sunil K ,etal.Nanocellulose from Spinifex as an Effective Adsorbent to Remove Cadmium (II )from Water [J ].ACS Sustailable Chenistry&Engineering ,2018,6(3):3279-3290.[44]Yao C ,Wang F ,Cai Z ,et al.Aldehyde -functionalized porousnanocellulose for effective removal of heavy metal ions from aqueoussolutions [J ].RSC Advances ,2016,6(95):92648-92654.[45]GENG Biyao ,WANG Haiying ,WU Shuai ,et al.Surface -TailoredNanocellulose Aerogels with Thiol -Functional Moieties for Highly Efficient and Selective Removal of Hg (II )Ions from Water [J ].ACS Sustainable Chemistry &Engineering ,2017,5(12):11715-11726.[46]Alipour A ,Zarinabadi S ,Azimi A ,et al.Adsorptive removal of Pb(II )ions from aqueous solutions by thiourea -functionalized magnetic ZnO/nanocellulose composite :Optimization by responsesurface methodology (RSM )[J ].Int.J.Biol.Macromol ,2020(151):124-135.[47]Anirudhan T S ,Shainy F ,Deepa J R.Effective removal of Cobalt(II )ions from aqueous solutions and nuclear industry wastewater usingsulfhydrylandcarboxylfunctionalisedmagnetitenanocellulose composite :batch adsorption studies [J ].Chemistryand Ecology ,2019,35(3):235-255.[48]Hong Hye -jin ,Lim Jin Seong ,Hwang Jun Yeon ,et al.Carboxymethlyated cellulose nanofibrils (CMCNFs )embedded in polyurethane foam as a modular adsorbent of heavy metal ions [J ].Carbohydrate Polymers ,2018,195:136-142.[49]Mo Liuting ,Pang Huiwen ,Tian Yi ,et al.3D multi -wall perforatednanocellulose -based polyethylenimine aerogels for ultrahigh effcient and reversible removal of Cu 2+ions from water [J ].ChemicalEngineering Journal ,doi :10.106/j ,eej.2019.122157.[50]Li Weixue ,Ju Benzhi ,Zhang Shufen.Preparation of cysteamine -modified cellulose nanocrystal adsorbent for removal of mercury ionsfrom aqueous solutions [J ].Cellulose ,2019,8(26):4971-4985.[51]Zhang Nan ,Long Guo ,Chen Zang ,et al.A novel TEMPO -mediated oxidized cellulose nanofibrils modified with PEI :Preparation ,characterization ,and application for Cu (II )removal [J ].Hazardous Materials ,2016(316):11-18.CPP(责任编辑:董凤霞)·消息·水利部、工业和信息化部印发造纸等七项工业用水定额2020年12月30日,为深入推进节约用水工作,水利部联合工业和信息化部印发造纸等七项工业用水定额的通知,定额标准自2021年3月1日起施行。

提高了吸收吸附二氧化碳效率 英文

提高了吸收吸附二氧化碳效率 英文

提高了吸收吸附二氧化碳效率英文The improvement of CO2 absorption and adsorption efficiency has been a hot topic in recent years due to the increasing levels of atmospheric carbon dioxide and the urgent need to reduce greenhouse gas emissions. This article will discuss the steps taken to enhance the absorption and adsorption efficiency of CO2 in various fields.Step 1: Developing New MaterialsOne way to improve CO2 absorption and adsorption efficiency is to develop new materials. Researchers have been exploring and synthesizing various materials, including zeolites, metal-organic frameworks (MOFs), carbon nanotubes, and graphene oxide. These materials have a high surface area and can effectively adsorb CO2, making them suitable candidates for CO2 capture and storage.Step 2: Optimizing Process ConditionsAnother strategy to improve CO2 absorption and adsorption efficiency is to optimize the process conditions. This involves adjusting various parameters, such as temperature, pressure, and flow rate, to maximize the amount of CO2 captured or adsorbed. For instance, researchers have used temperature swing adsorption (TSA) and pressure swing adsorption (PSA) to increase CO2 capture.Step 3: Developing Advanced TechniquesIn addition to developing new materials and optimizing process conditions, researchers have also developed advanced techniques to improve CO2 absorption and adsorption efficiency. For example, electrochemical CO2 reduction hasbeen proposed as a promising method for CO2 capture and utilization. This method involves converting CO2 into useful chemicals, such as methanol and formic acid, using renewable energy sources.Step 4: Integrating Multiple TechnologiesA more comprehensive approach to improving CO2 absorption and adsorption efficiency is to integrate multiple technologies. For example, researchers have combined absorption with membrane separation to enhance CO2 capture efficiency. This process involves using a membrane to separate the CO2 from other gases that are produced during the absorption process.In conclusion, the improvement of CO2 absorption and adsorption efficiency requires a multi-disciplinary effort, combining material science, engineering, and chemistry. By developing new materials, optimizing process conditions, developing advanced techniques, and integrating multiple technologies, we can make significant progress in reducing greenhouse gas emissions and mitigating climate change.。

微波改性的稻壳对Pb(Ⅱ)、Cd(Ⅱ)吸附性能的研究

微波改性的稻壳对Pb(Ⅱ)、Cd(Ⅱ)吸附性能的研究

微波改性的稻壳对Pb(Ⅱ)、Cd(Ⅱ)吸附性能的研究李渊【摘要】以稻壳为原料,采用微波处理制备出改性的吸附材料,用于吸附Pb2+、Cd2+的实验,探讨了溶液pH、搅拌时间及金属离子初始浓度等对吸附平衡的影响,利用扫描电镜和红外光谱(FTIR)分析,探讨微波处理后的稻壳吸附Pb2+、Cd2+等金属离子的吸附机理.结果表明:微波处理后的稻壳对Pb2+的最佳吸附pH=5,在60 min内建立吸附平衡,对Pb2+的最大吸附量为0.2324 mmol/g;在相同条件下对Cd2+的最大吸附量为0.1852 mmol/g.%A kind of modified adsorptive material has been prepared by microwave,using rice husks as raw materials. It is an experiment used for adsorbing Pb2+and Cd2+. The influences of solution pH,stirring time,initial concentration of metallic ions,etc. on adsorption equilibrium are discussed. The adsorption mechanisms of microwave-treated rice husks for metallic ions,such as Pb2+,Cd2+,etc. are analyzed by making use of SEM and FTIR and discussed. The re-sults show that the optimal conditions for the microwave-treated rice husks to adsorb Pb2+ are as follows:pH is 5 and the adsorption equilibrium should be set up within 60 min,the maximum adsorption capacity for Pb2+is 0.2324 mmol/g. Under the same conditions,the maximum adsorption capacity for Cd2+is 0.1852 mmol/g.【期刊名称】《工业水处理》【年(卷),期】2016(036)003【总页数】4页(P62-65)【关键词】稻壳;微波处理;吸附;金属离子【作者】李渊【作者单位】四川职业技术学院,四川遂宁629000【正文语种】中文【中图分类】X703近年来多地发生重金属污染事故,随着重金属环境污染的加剧以及人们对重金属危害认识的逐渐加深,对含重金属废水排放的控制开始越来越严格,因此寻找新型高效的低成本吸附剂就成为重金属废水处理的研究热点〔1-5〕。

Adsorption of CO2, CH4, and N2 on Gas Diameter Grade Ion-Exchange Small Pore Zeolites

Adsorption of CO2, CH4, and N2 on Gas Diameter Grade Ion-Exchange Small Pore Zeolites

Adsorption of CO 2,CH 4,and N 2on Gas Diameter Grade Ion-Exchange Small Pore ZeolitesJiangfeng Yang,Qiang Zhao,Hong Xu,Libo Li,Jinxiang Dong,and Jinping Li *Research Institute of Special Chemicals,Taiyuan University of Technology,Taiyuan 030024,Shanxi,P.R.Chinastructure like CO 2.From the viewpoint of the equilibrium selectivity for CO 2and N 2or CO 2andof CO 2;K-zeolites with high S CO 2/N 2and S CH 4/N 2,adsorption potential order was K-zeolites >Na-zeolites >The removal of CO 2from gaseous mixtures is important for CO 2capture from flue gas,biogas,or land fill gases.These sources of natural gas mainly contain CH 4,CO 2,and N 2.Therefore,the separation of CO 2,CH 4and N 2mixtures canupgrade low quality natural energy gas and also mitigate the problem of excess CO 2emissions.1Of the available adsorption-based separation processes,energy (CH 4)and CO2capture isconsidered to be an energy-and cost-e fficient alternative.Thus,adsorption is an important solution for separation,CO 2capture,CH 4storage,and transportation.2−4This approach uses various types of sorbents or adsorption materials such as carbon materials (activated carbon and carbon molecular sieves),5,6molecular sieves (zeolites),7−10and the popular new metal −organic frameworks (MOFs).11−14Sorbents are considered to be the most important factors a ffecting adsorption techniques.A comparison of di fferent adsorption materials showed that carbon materials are di fficult to have a balance of small pores and large pores,for optimum balance between capacity and dynamics,and MOFs had lower thermal stability,but zeolites produced very homogeneous structures with high surface area and good thermal stability,and the size of the pore volume could be modulated.15,16Thus,zeolites are the most commonly used adsorbents in the field,such as LTA structures (4A,5A,and 13X).17The question is how do we choose appropriate zeolites for a speci fic application such as CO 2,CH 4,and N 2adsorption and First,an analysis of gases showed that nonpolar gases have very similar diameters and gas dynamics:CO 2=0.33nm,CH 4=0.38nm,and N 2=0.36nm,18while the adsorptionstrength of the sorbents was CO2>CH4>N2.19,20Therefore,the adsorption and separation of most gases by zeolites isreliant on their surface potential or the balance of ions in surface channels,particularly the low silicon Li-X zeolite usedfor O 2and N 2separation.21The pore diameters of zeolites areusually bigger than the gas molecules,so gases can di ffusethrough these pores.But what would happen if the pores had a similar size to or smaller than the molecular diameter of the three gases during zeolite adsorption?Titanium silicalite ETS-4had a pore size that is similar to the molecular diameter,and it can be modulated by temperature changes for the aperture separation of various gases,such as CO 2and CH 4,N 2,and CH 4,although its lower adsorptioncapacity limits theapplication of this approach.22−24The ori fice diameters of the zeolites,KFI,CHA,and LEV,are very close to the kinetic diameters of CO 2,CH 4,and N2(Figure 1).These three small-pore zeolites have cage-like structures,and the larger cavity in the hole is ideal for gas uptake.This type of small-pore size microporous zeolite is a hot research area in the field of catalysis and adsorption.25−27Received:August 28,2012Accepted:October 31,2012Published:November 7,2012Krishna and van Baten found frequent correlation e ffects with cage-type zeolites,such as LTA,CHA,and DDR,where narrow windows separated the cages.26Webley et al.studied the gas adsorption selectivity of M(Ca,K)-CHA and concluded that the high O 2/Ar selectivity was possibly due to partial pore blockage by a large K +located near the 8-member ring,producing a 20-hedron cage.28The small pore size and the metal cation balance probably plays an important role in the gas diameter grade structure of zeolites where it determines the adsorption capacity and shape-selective catalysis.It is less common to focus on these types of small pore size cage-like structures and the adsorption of gas molecules close to the aperture.In this study,we synthesized three types of zeolites,Na-LEV,K-CHA,and K-KFI,using the hydrothermal method,whereas Na-KFI,Li-KFI,Ca-KFI,Na-CHA,Li-CHA,and Ca-CHA were obtained by ion exchange.The aims of this study were to evaluate the pore size e ffect and the metal cation e ffect on the adsorption of CO 2,CH 4,and N 2.We also discuss the most suitable method for the separation of CO 2,CH 4,and N 2based on calculations of the adsorption equilibrium.■MATERIALS AND METHODSThe chemicals used in this study are described in more detail in Table 1.Partial Aluminum Potassium.[50.00g of water +29.76g of potassium hydroxide +15.80g of alumina]were heated to boiling until clear,cooled to room temperature,and corrected for any weight loss due to boiling.30,31K-KFI.The synthesis following the procedure reported by Johannes et al.30−32The batch composition was:7.2partial aluminum potassium/0.1strontium nitrate/7.5silicon dioxide/130water,and the typical procedure involved mixing the required amounts of partial aluminum potassium and water,followed by the addition of silica sol,and mixing until smooth (approximately 10min),before strontium nitrate was added to the mixture and stirred for 10min.The resulting mixture was transferred into a 23mL Te flon-lined autoclave and heated in an oven for 5days at 423K.After cooling to ambient temperature,the product was filtered,washed with water,and dried at 373K.The crystal structure of KFI and the degree of crystallinity were con firmed by powder X-ray di ffraction(XRD).Figure 1.Structures of zeolites KFI (a),CHA (b),and LEV (c).29Table 1.Purity of Chemicals Used in This Study and Their Detailschemical name source initial mass fraction purityalumina Aladdin,China >0.99silica sol QingdaoHaiyang Chemical Co.,Ltd.0.401,1-dimethylpiperidinium chloride Shanghai Bangcheng Chemical Co.,Ltd.0.98strontium nitrate Aladdin,China >0.99potassium hydroxide TianjinKemiou Chemical Reagent Co.,Ltd.0.82sodium hydroxide TianjinKemiou Chemical Reagent Co.,Ltd.0.96sodium chloride TianjinKemiou Chemical Reagent Co.,Ltd.0.99lithium hydroxide Tianjin Kemiou Chemical Reagent Co.,Ltd.0.98lithium chloride TianjinKemiou Chemical Reagent Co.,Ltd.0.97calcium hydroxide TianjinKemiou Chemical Reagent Co.,Ltd.0.95calcium chloride Tianjin Kemiou Chemical Reagent Co.,Ltd.0.96K-CHA.The synthesis method was similar to that for K-KFI,but the batch composition was:7.2partial aluminum potassium:0.1strontium nitrate:6silicon dioxide/130water,so there were lower levels of Si/Al.The crystal structure of CHA and the degree of crystallinity were con firmed by powder XRD.Na-LEV.This was prepared from:6partial aluminum sodium/10silicon dioxide/31,1-dimethylpiperidinium chlor-ide/200H 2O,which was made according to our previously reported method.33Ion Exchange.The Na-KFI described above was converted from its potassium form (K-KFI)via three consecutive ion exchanges.In general,300mL of 1M sodium chloride at pH =9(adjusted with 0.01M sodium hydroxide)was added to 5g of zeolite,and the solution was heated to 363K and stirred for 12h.The solution was decanted,and fresh solution was added.After successive washes with the requisite solution,the resulting zeolite was vacuum-filtered and washed with 500mL of deionized water.The zeolite was dried at 373K for 24h.Li-KFI was prepared from Na-KFI by five consecutive ion exchanges of Na-KFI with 2M lithium chloride (5g of zeolite:300mL of lithium chloride)at pH =9(adjusted with 0.01M lithium hydroxide).Ca-KFI was prepared from Na-KFI by five consecutive ion exchanges of Na-KFI with 1M calcium chloride (1g of zeolite:300mL of calcium chloride).The solution was heated at 353K for 12h and decanted,and fresh solution was added.This procedure was repeated five times.Finally,the Ca-KFI was filtered and washed with copious amounts of deionized water and dried at 373K overnight.Na-CHA,Li-CHA,and Ca-CHA,were prepared using the same procedure.34Characterization.The crystallinity and phase purity of the molecular sieves were measured by powder XRD using a Rigaku Mini Flex II X-ray di ffractometer with Cu K αradiation operated at 30kV and 15mA.The scanning range was from 5to 40°(2theta)at 1°/min.Morphological data were acquired by scanning electron microscopy (SEM)using a JEOL JSM-6700F scanning electron microscope operated at 15.0kV.The samples were coated with gold to increase their conductivity before scanning.The Si/Al ratio and the metal ion content of the zeolites were determined by elemental analysis using a spectrophotometer-723P.High-Pressure Gas Adsorption Measurements.The purity of the carbon dioxide was 99.999%,methane was 99.95%,and nitrogen was 99.99%.The adsorption isotherms were measured under high pressure using an Intelligent Gravimetric Analyzer (IGA 001,Hiden,UK).Before measuring the isotherm,a 50mg sample was predried under reduced pressure and then outgassed overnight at 673K under a high vacuum until no further weight loss was observed.Each adsorption/desorption step was allowed to approach equilibrium over a period of 20−30min,and all of the isotherms for each gas were measuredusing a single sample.■RESULTS AND DISCUSSION Synthesis,Ion Exchange,and Characterization.The zeolite K-KFI was synthesized according to a published method.32Figure 2a shows the XRD pattern of the synthesized molecular sieve K-KFI compared with the standard XRD data for the molecular sieve KFI.The peak positions and relative di ffraction intensity were similar to the reported values,which demonstrated that the molecular sieve K-KFI had been synthesized.Figure 2a also shows the XRD pattern of the molecular sieve K-KFI,which was calcined from (573to 1073)K.Its peak positions and relative di ffraction intensity were the same as a sample synthesized below 973K,while the skeleton collapse temperature was 1073K.The method used for the synthesis of K-CHA was similar to that used for K-KFI.Figure 2b shows the XRD pattern of the synthesized molecular sieve K-CHA compared with the standard XRD data for the molecular sieve CHA.The peak positions and relative di ffraction intensity were similar to the reported values,which demonstrated that the molecular sieve K-CHA had been synthesized.The samples had similar behavior at below 973K,while the skeleton collapse temperature was 1073K.The data showed that the structures of KFI and CHA had good thermal stability.The Si/Al values in K-KFI and K-CHA were 4.59and 2.63,respectively.The low Si/Al value indicated that K +occupied more channels in the zeolites,where the large space allowed access to small metal ions or divalent ion exchange.In addition,K-CHA with a lower Si/Al value indicated that more ions could be exchanged,while the size of the pore space could change greatly.However,the higher Si/Al value of K-KFI indicated lower ion exchange,so the size of the pore space could be regulated at a finer level.Table 2shows the experimental K-zeolites,which were changed to Na-zeolites via ion exchange,and the uncertainty is within ±0.005.This shows that the ion exchange degree was increased with temperature and frequency.K-CHA with a lower Si/Al value was produced more completely and easier than K-KFI with a higher Si/Al value from Na +exchanged with K +.The ion exchange degree of Na-CHA from K-CHA wasveryFigure 2.XRD patterns of KFI (a)and CHA (b).high in the first cycle,because the higher temperature is helpful to ion exchange in low Si/Al zeolites.35We selected the highest exchange degree for K +(Na-KFI with 0.91and Na-CHA with 0.99)and the Na-zeolites were used to obtain Li-zeolites and Ca-zeolites.Table 3shows that Li-KFI and Ca-KFI were 0.96and 0.83,respectively,based on Li +and Ca 2+exchange for Na +,while Li-CHA and Ca-CHA were 0.92and 0.96,respectively.The XRD patterns of the Na-,Li-,and Ca-zeolites showed that the zeolite structures were highly stable throughout ion exchange (Figure 3).The samples that changed in appearance are shown in Figure 4.The morphologies of the zeolites with KFI and CHA structures were observed by SEM.For K-KFI to Na-KFI,Li-KFI,and Ca-KFI,the morphologies of the crystals changed from regular cubic accumulations until they completely lost their regular structures.We also showed that there was a slight change in their appearance after a single exchange of materials,followed by a more obvious change after the secondary exchange of materials,particularly M 2+exchange with M +based on the morphologies of M-CHA (M-metal).The pore diameter of some of the samples was too small to be measured or analyzed using a liquid nitrogen adsorption isotherm,for LEV with the ori fice very close to the nitrogen-diameter,so the surfaces of all samples were measured andanalyzed using a CO 2adsorption isotherm at 273K (Figure 5).The microporous surface area and microporous volumes werecalculated using the Dubinin −Radushkevitch (D-R)equation(Table 4):β=−··⎡⎣⎢⎤⎦⎥V V B T PP log()log()log0202(1)where V was volume adsorbed at equilibrium pressure;V 0was the micropore capacity;P 0was saturation vapor pressure of gas attemperature T ;P was equilibrium pressure;B was a constant,βwasthe a ffinity coe fficient of analysis gas relative to P 0gas (for this application βis taken to be 1);T was the analysis bath temperature.36−38All of the samples with a high surface area could be used foradsorption;the surfaces and the pore volumes of the zeoliteswere changed very obvious by ion exchange.Table 4shows thesurface of the samples where the greatest changes were in theappearance of the M-CHAs with the lowest surface areas (K-CHA with 278.5m 2·g −1)and the highest (Li-CHA with 638m 2·g −1,the same situation also appear in the pore volumechange (K-CHA with 0.07cm 3·g −1and Li-KFI with 0.17cm 3·g −1).because they had lower Si/Al values and morebalanced metal ions could be exchanged,so with the smallersize of Li +instead of K +(Table 3),more space can be obtained.However,M-KFI had a higher Si/Al value than M-CHA,so the area of its surface and microporous volume that could be regulated by ion exchange was smaller;that is,the surface area ranges from 333.5m 2·g −1(Ca-KFI)to 566.2m 2·g −1(Na-KFI),and the pore volume ranges from 0.07cm 3·g −1(Ca-KFI)to 0.15cm 3·g −1(Na-KFI).We also found that the surfaces and pore volumes of Ca-zeolites were smaller than Li-or Na-zeolites,which showed that the introduction of Ca 2+reduced the number of balanced ions,while the plug was very strong because the size of Ca 2+larger than Li +and Na +.Li-KFI and Na-KFI had similar surfaces,so it was inferred from Li +that there was no hole in Na-KFI to produce major changes.The systematic errors of surface areas and pore volume have been estimated to be less than 5m 2·g −1and 0.01cm 3·g −1.Table 2.Ion Exchange Degree from K-Zeolite to Na-Zeolite at Di fferent Exchange Times and Temperatures of (323and 363)K a 0.5870.7570.8800.910363Na-CHA 0.7500.7640.9240.9343230.9240.9710.9740.991363a Uncertainties are:U (exchange degree)=0.005;U (T )=0.1K.Table 3.Ion Exchange Degree of Li and Ca-Zeolite from Na-Zeolite a zeolites cation ionic radius (nm)Na +per unit cell (wt %)exchange degree for Na +K-KFI 0.133Na-KFI 0.095 5.29Li-KFI 0.0680.200.96Ca-KFI 0.0990.900.83K-CHA 0.133Na-CHA 0.0957.94Li-CHA 0.0680.640.92Ca-CHA 0.0990.290.96a Uncertainties are:U (Na +contents)=0.02wt %;U (exchange degree)=0.005.Figure 3.XRD patterns of Na,Li,and Ca-KFI (a)and Na,Li,and Ca-CHA (b).Gas Sorption Isotherm Measurements.The CO 2,CH 4,and N 2adsorption and desorption isotherms of the samples are shown in Figure 6,where all of the isotherms have a Langmuir I form and the relative uncertainties of adsorption volumes are estimated to be 0.05V .Most of the samples exhibited rapid desorption,and this correlated with their adsorption curve.Only sample K-CHA exhibited desorption hysteresis during CH 4adsorption.We inferred that the pore size of K-CHA was too close to the kinetics of the di ffusion diameter of CH 4,so it had a very strong CH 4adsorption potential,whereas desorption was hindered by the steric e ffect of the micropores.Table 5also shows the orders of the volumes for CO 2,CH 4,and N 2adsorption of the samples at 0.1MPa.The order of CO 2adsorption at 298K corresponded to the surfaces of the samples.Based on the CO2adsorption,we can also determine the zeolites with Li +and Na +exchange with bigger surfaces and greater adsorption volumes.Based on the high levels (>100cm 3·g −1)of CO 2adsorption with Li,Na-KFI,and Li,Na-CHA at high pressurea,we conclude that micropore Li-zeolites and Na-zeolites could be used for CO 2capture and storage (CCS).The smallest CH 4adsorption volume was found with Na-LEV,so we inferred that CH4adsorption would not occur in itsmicropores because the levels were far less than with othersamples.We conclude that CH4could not di ffuse through theholes in Na-LEV because the ori fice diameter (0.36×0.48nm)was too small.The CH 4adsorption results showed thatM-Figure 4.SEM of the samples:(a)K-KFI,(b)Na-KFI,(c)Li-KFI,(d)Ca-KFI,(e)K-CHA,(f)Na-CHA,(g)Li-CHA,(h)Ca-CHA.CHA was better than M-KFI,so CH 4adsorption or storage was based on the surface features and the ori fice diameter (CHA with 0.38×0.38nm,KFI with 0.39×0.39nm),which indicated a higher adsorption potential.39The low N 2adsorption with Na-LEV shows that molecules could not di ffuse through its pores.N 2adsorption was not a ffected by the metal ion or the structure,so the pore size or surfaces of porous materials were always su fficient for liquid nitrogen adsorption.In the other samples,the N 2adsorption results showed that the pores were expanded by small metal ions or divalent ion exchange,that is,twice then once,because the order was Li,Ca-zeolite >Na-zeolite >K-zeolite (Table 5).Adsorption Equilibrium Selectivity.To evaluate the adsorption equilibrium selectivity and predict the adsorption of the gas mixture from the pure component isotherms,the adsorbent selection parameter S i /j is de fined in the following equation:=ΔΔS qq a i j i j /12/(2)where Δq 1and Δq 2are the adsorption equilibrium capacity di fferences at the adsorption pressure and desorption pressure for components 1and 2.The adsorption equilibrium selectivity a i /j between components i and j is de fined as follows:==a K K q b q b i j i j mi imj j /(3)Henry ’s law:=q Kp (4)Langmuir isotherm model:=+q q bpbp 1m (5)where q m and b are Langmuir isotherm equation parameters,which can be determined from the slope and intercept of a linear Langmuir plot of (1/q )versus (1/p )where q m i and q m jand b i and b j are the Langmuir equation constants for components i and j ,respectively.The equilibrium selectivity de fined in the above equation is basically the ratio of Henry ’s constants for the two components.40Based on the results for S CO 2/CH 4and S CO 2/N 2(in Table 6andthe relative uncertainties of S i /j are estimated to be 0.05S ),all ofthe micropore zeolites produced excellent results in the evaluations,because of the high adsorption of CO 2in the gas diameter grade micropore structures.Na-LEV was the bestmicroporous sieve for gas materials with the highest S CO 2/CH 4=137and S CO 2/N 2=934due to the almost total nonadsorption ofCH 4and N 2but high adsorption of CO 2,which is rare among sorbents.41The second best was Na-KFI (S CO 2/CH 4=92andS CO 2/N 2=374),which had produced better results than otherM-KFIs.In addition,Na-CHA had a higher SCO 2/CH 4than K andLi-CHA,and at the same time Na-CHA also had a higher S CO 2/N 2than Li,Ca-CHA,so we can conclude that Na-zeoliteshad higher CO 2adsorption.A reanalysis of the data showed that Li-zeolites were followed by Na-zeolite,so the e ffects of the smaller Li +were lower than the e ffects of the bigger Na +,and we inferred that the size of the metal ions was an important impact in zeolites.The aerodynamic diameter and physicochemical propertiesof CH 4and N 2were very similar,so separating CH4and N 2wasmuch more di fficult than CO 2and CH4or CO 2and N 2separation which used an adsorption technique.The exper-imental data for S CH 4/N 2in Table 6also con firmed this point.K-CHA had the highest S CH 4/N 2=14.5,while the second was K-KFI (S CH 4/N 2=8.5),which indicated that the introduction of alarge K +increased the potential adsorption of CH4.The Na-zeolites and Li-zeolites have very low data for S CH 4/N 2.Based on the relatively good K-zeolite data for S CO 2/N 2and the smallersurface pores,we can conclude that K +had a signi ficant role in the adsorption of CH4and CO 2,although a smaller hole did not allow greater nitrogen di ffusion.From the perspective of the adsorption potential,we conclude that the large K +was better than Na +and the small Li +;the order was K-zeolites >Na-zeolites >Li-zeolites,indicating that bigger ions had a stronger a ffinity.While the introduction of divalent ions could halve the total number of ions,thus,Ca 2+formed fewer of these small pore type zeolites,and it did not produce very good resultsfor adsorption separation.■CONCLUSION We prepared nine di fferent surfaces of gas diameter grade small pore zeolites,which were characterized by XRD,SEM,and elemental analysis.We synthesized K-CHA with a lower Si/Al value,and more balanced metal ions could be exchanged,so the surfaces and microporous volumes were changedgreatly.Figure 5.CO 2adsorption of the samples on 273K.Table 4.Microporous Surface (MS)and Microporous Volume (MV)of the Samples Obtained from CO 2Adsorption Isotherms at 273K a K-KFI 430.40.10Na-KFI 566.20.15Li-KFI 550.60.14Ca-KFI 333.50.07K-CHA 278.50.07Na-CHA 594.80.16Li-CHA 638.00.17Ca-CHA 487.20.12a Uncertainties are:U (MS)=5m 2·g −1;U (MV)=0.01cm 3·g −1.However,K-KFI had a higher Si/Al value,and the area of its surface and microporous volumes could be modulated to make it smaller.We focused on the CO 2,CH 4,and N 2adsorption isotherms of the samples under high pressure (1MPa)at room temperature (298K),and we found that the smaller Li +and Na +exchanged more with the surface and they had higher adsorption volumes,whereas the larger K +led to severe channel congestion.We calculated and evaluated the adsorption equilibrium selectivity of CO 2/CH 4/N 2,which showed that the ori fice diameter had a very important role in the sieving of CO 2and N 2or CO 2and CH 4,where Na-LEV produced the best sieving e ffect.From the viewpoint of the adsorption equilibria,the Na-zeolites produced the best results for adsorption equilibrium selectivity with CO 2and N 2or CO 2and CH 4,followed by Li-zeolites,whereasK-zeolites withhigh Figure 6.CO 2(▲),CH 4(■),and N 2(●)adsorption (solid)and desorption (hollow)isotherm of the samples at 298K and 1MPa:(a)K-KFI,(b)K-CHA,(C)Na-LEV,(d)Na-KFI,(e)Li-KFI,(f)Ca-KFI,(g)Na-CHA,(h)Li-CHA,(i)Ca-CHA.Table 5.Volumes of CO 2,CH 4,and N 2Adsorption on the Samples at 0.1MPa a K-KFI 67.317.57.1Na-KFI 93.617.79.5Li-KFI 88.315.99.3Ca-KFI 54.816.29.5K-CHA 47.119.1 5.5Na-CHA 104.330.316.7Li-CHA 106.633.016.9Ca-CHA 83.221.418.7a The relative uncertainties of adsorption volumes are estimated to be 0.05V .Table 6.Separation Factor of CH 4/N 2,CO 2/CH 4,and CO 2/N 2Calculated from Pure Component Adsorption Isothermsof the Samplesa zeolite S CO 2/CH 4S CO 2/N 2S CH 4/N 2Na-LEV 137934 6.8K-KFI 353038.5Na-KFI 92374 4.1Li-KFI 80237 3.0Ca-KFI 1959 3.0K-CHA 2435214.5Na-CHA 42187 4.3Li-CHA 32154 4.7Ca-CHA 51127 1.6a The relative uncertainties of Si /j are estimated to be 0.05S .S CH 4/N 2and S CO 2/N 2.Based on the adsorption equilibrium selectivity results,we can conclude that the adsorption potential order was K-zeolites >Na-zeolites >Li-zeolites,so the bigger ions had a stronger a ffinity.Divalent ions were less likely to be captured in the structures than univalent ions,so their separation was somewhat poorer.■AUTHOR INFORMATION Corresponding Author *E-mail:Jpli211@.Tel.:86-3516010908.Fax:86-3516010908.Funding We gratefully acknowledge financial support from the National Natural Science Foundation of China (Nos.21136007,51002103)and Research Fund for the Doctoral Program of Higher Education of China (No.20091402110006).This work was financially supported by the program for the Top Science and Technology Innovation Teams of Higher Learning Institutions of Shanxi.Notes The authors declare no competing financial interest.■REFERENCES (1)Kikkinides,E.S.;Yang,R.T.;Cho,S.H.Concentration and recovery of CO 2from flue gas by pressure swing adsorption.Ind.Eng.Chem.Res.1993,32,2714−2720.(2)Hao,G.P.;Li,W.C.;Qian,D.;Wang,G.H.;Zhang,W.P.;Zhang,T.;Wang,A.Q.;Schu t h,F.;Bongard,H.J.;Lu,A.H.Structurally Designed Synthesis of Mechanically Stable Poly-(benzoxazine-co-resol)-Based Porous Carbon Monoliths and TheirApplication as High-Performance CO 2Capture Sorbents.J.Am.Chem.Soc.2011,133,11378−11388.(3)Matranga,K.R.;Myers,A.I.;Glandt,E.D.Storage of natural gas by adsorption on activated carbon.Chem.Eng.Sci.1992,47,1569−1579.(4)Matranga,K.R.;Stella,A.;Myers,A.L.;Glandt,E.D.Molecular simulation of adsorbed natural gas.Sep.Sci.Technol.1992,27,1825−1836.(5)Liu,Y.;Wilcox,J.Effects of Surface Heterogeneity on the Adsorption ofCO 2in Microporous Carbons.Environ.Sci.Technol.2012,46,1940−1947.(6)Chen,J.;Loo,L.S.;Wang,K.An Ideal Absorbed Solution Theory (IAST)Study of Adsorption Equilibria of Binary Mixtures ofMethane and Ethane on a Templated Carbon.J.Chem.Eng.Data 2011,56,1209−1212.(7)Ducrot-Boisgontier,C.;Parmentier,J.;Faour,A.;Patarin,J.;Pirngruber,G.D.FAU-Type Zeolite Nanocasted Carbon Replicas for CO 2Adsorption and Hydrogen Purification.Energy Fuels 2010,24,3595−3602.(8)Jayaraman,A.;Hernandez-Maldonado,A.J.;Yang,R.T.;Chinn,D.;Munson,C.L.;Mohr,D.H.;Donald,H.Clinoptilolites for nitrogen/methane separation.Chem.Eng.Sci.2004,59,2407−2417.(9)Wang,Y.;LeVan,M.D.Adsorption Equilibrium of BinaryMixtures of Carbon Dioxide and Water Vapor on Zeolites 5A and 13X.J.Chem.Eng.Data 2010,55,3189−3195.(10)Bao,Z.;Yu,L.;Dou,T.;Gong,Y.;Zhang,Q.;Ren,Q.;Lu,X.;Deng,S.Adsorption Equilibria of CO 2,CH 4,N 2,O 2,and Ar on High Silica Zeolites.J.Chem.Eng.Data 2011,56,4017−4023.(11)Coudert,F.O.-X.;Mellot-Draznieks,C.;Fuchs,A.H.;Boutin,A.Prediction of Breathing and Gate Opening Transitions Upon Binary Mixture Adsorptionin Metal −Organic Frameworks.J.Am.Chem.Soc.2009,131,11329−11331.(12)Zheng,S.T.;Bu,J.T.;Li,Y.;Wu,T.;Zuo,F.;Feng,P.;Bu,X.Pore Space Partition and Charge Separation in Cage-within-Cage Indium −Organic Frameworks with High CO 2Uptake.J.Am.Chem.Soc.2010,132,17062−17064.(13)He,Y.;Xiang,S.;Chen,B.A Microporous Hydrogen-BondedOrganic Framework for Highly Selective C 2H 2/C 2H 4Separation at Ambient Temperature.J.Am.Chem.Soc.2011,133,14570−14573.(14)Sumida,K.;Rogow,D.L.;Mason,J.A.;McDonald,T.M.;Bloch,E.D.;Herm,Z.R.;Bae,T.H.;Long,J.R.Carbon Dioxide Capture in Metal −Organic Frameworks.Chem.Rev.2012,112,724−781.(15)Gemma,L.H.;Edward,B.;Martin,C.S.;Neil,C.H.;Ewan,M.M.;Paul,F.M.;Joseph,A.H.High-Pressure and Temperature IonExchange of Aluminosilicate and Gallosilicate Natrolite.J.Am.Chem.Soc.2011,133,13883−13885.(16)Aguilar-Armenta,G.;Hernandez-Ramirez,G.;Flores-Loyola,E.;Ugarte-Castaneda, A.;Silva-Gonzalez,R.;Tabares-Munoz, C.;Jimenez-Lopez,A.;Rodriguez-Castellon,E.Adsorption Kinetics of CO 2,O 2,N 2,and CH 4in Cation-Exchanged Clinoptilolite.J.Phys.Chem.B 2001,105,1313−1319.(17)Walton,K.S.;Abney,M.B.;LeVan,D.M.CO 2adsorption in Yand X zeolites modified by alkali metal cation exchange.Microporous Mesoporous Mater.2006,91,78−84.(18)Yang,R.T.Adsorbents:Fundamentals and Applications ;Wiley-Interscience:New York,2003.(19)Van den Bergh,J.;Mittelmeijer-Hazeleger,M.;Kapteijn,F.Modeling Permeation of CO 2/CH 4,N 2/CH 4,and CO 2/Air Mixturesacross a DD3R Zeolite Membrane.J.Phys.Chem.C 2010,114,9379−9389.(20)Dunne,J.A.;Mariwala,R.;Rao,M.;Sircar,S.;Gorte,R.J.;Myers, A.L.Calorimetric Heats of Adsorption and Adsorption Isotherms.1.O 2,N 2,Ar,CO 2,CH 4,C 2H 6,and SF6on Silicalite.Langmuir 1996,12,5888−5895.(21)Baksh,M.S.A.;Kikkinde,E.S.;Yang,R.T.Lithium Type XZeolite as a Superior for Air Separation.Sep.Sci.Technol.1992,27,277−294.(22)Kuznicki,S.M.;Bell,V.A.;Nair,S.;Hillhouse,H.W.;Jacubinas,R.M.;Braunbarth,C.M.;Toby,B.H.;Tsapatsis,M.A titanosilicatemolecular sieve with adjustable pores for size-selective adsorption ofmolecules.Nature 2001,412,720−724.(23)Marathe,R.P.;Farooq,S.;Srinivasan,M.P.Modeling GasAdsorption and Transport in Small-Pore Titanium ngmuir2005,21,4532−4546.(24)Pillai,R.S.;Peter,S.A.;Jasra,R.V.Adsorption of carbondioxide,methane,nitrogen,oxygen and argon in NaETS-4.Micro-porous Mesoporous Mater.2008,113,268−276.(25)Altwasser,S.;Welker,C.;Traa,Y.;Weitkamp,J.Catalyticcracking of n-octane on small-pore zeolites.Microporous MesoporousMater.2005,83,345−356.(26)Krishna,R.;van Baten,J.M.Onsager coefficients for binary mixture diffusion in nanopores.Chem.Eng.Sci.2008,63,3120−3140.(27)Saxton,C.G.;Kruth,A.;Castro,M.;Wright,P.A.;Howe,R.F.Xenon adsorption in synthetic chabazite zeolites.Microporous Mesoporous Mater.2010,129,68−73.(28)Singh,R.K.Adsorption of N 2,O 2,and Ar in PotassiumChabazite.Adsorption 2005,11,173−177.(29)Baerlocher,Ch.;McCusker,L.B.;Olson,D.H.Atlas of Zeolite Framework Types ,6th revised ed.;Elsevier:New York,2007.(30)Johannes,V.Zeolite ZK-5.U.S.Patent US4994249,1991(31)Robson,H.How to read a patent.Microporous Mesoporous Mater.1998,22,551−662.(32)Schwarz,S.;Corbin,D.R.;Sonnichsen,G.C.The effect ofcrystal size on the methylamines synthesis performance of ZK-5zeolites.Microporous Mesoporous Mater.1998,22,409−418.(33)Dong,J.;Wang,X.;Xu,H.;Zhao,Q.;Li,J.Hydrogen storage inseveral microporous zeolites.Int.J.Hydrogen Energy 2007,32,4998−5004.(34)Zhang,J.;Singh,R.;Webley,P.A.Alkali and alkaline-earthcation exchanged chabazite zeolites for adsorption based CO2capture.Microporous Mesoporous Mater.2008,111,478−487.(35)Xu,R.;Pang,W.Chemistry-Zeolites and Porous Materials(Chinese);Science Press:Beijing,2004.。

牡蛎壳改性花生壳生物炭吸附去除水体中的磷

牡蛎壳改性花生壳生物炭吸附去除水体中的磷

猱艺科枚Journal of Green Science and Technology第23卷第2期2021年1月牡蛎壳改性花生壳生物炭吸附去除水体中的磷李浩,夏港,关昊为,易群伟,李嘉融,刘妥淇,张静(武汉轻工大学土木工程与建筑学院,湖北武汉430023)摘要:基于牡蛎壳富含碳酸钙成分,采用800°C高温改性方法制备牡蛎壳改性花生壳生物炭,考察了其对溶液中稀的吸附性能。

实验结果表明:牡蛎壳改性后的花生壳生物炭对磷的吸附量显著高于未改性的花生壳生物炭。

溶液初始磷浓度为200mg/L,添加0.02g的生物炭.,在25°C下反应48h后,牡蛎壳及性花生壳生物炭磷吸附容量为197.3mg/g,约为未改性花生壳生物炭的17倍。

关键词:牡蛎壳改性;吸附性能;花生壳;生物炭;磷中图分类号:X172文献标识码:A文章编号:1674-9944(2021)02-0072-021引言磷是水生生物新陈代谢中不可或缺的一种元素口O 但当水体中磷浓度超标时,会刺激水体中藻类的生长,减少水体中的溶解氧浓度,使水生生物窒息而死,造成水体富营养化,对水体生态系统产生负面影响凤旳。

在我国,根据《城镇污水处理厂污染物排放标准》GB18918 -2002规定,排入自然水体的污废水的磷限值为0.5 mg/L,美国对排入湖泊的污废水的磷限量规定为0.05 mg/L"】。

工业、农业和生活污废水是磷进入自然水体环境的主要来源,含磷浓度为4〜15mg/L,远远超过规定限制旳。

因此,开发有效去除废水中磷的方法是亟待解决的一个重要的全球性问题。

目前,控制水体磷污染的有效方法主要有物理处理法(微滤、反渗透、电渗析、磁选)、化学处理法(沉淀、结晶、阴离子交换和吸附)和生物处理(同化、强化生物除磷、人工湿地、废水稳定池)[6~9\在众多的处理方法中,吸附处理法具有成本低、效率高、选择性好、操作简单,以及对废水pH值无明显影响等优点,而备受欢迎与传统炭质吸附剂相比,生物炭不仅具有传统炭质类材料的吸附特点,而且原材料易获得、制备方法简单、成本低廉,因而,成为一种备受关注的新型吸附剂[10>11\然而,由于生物炭的金属阳离子含量低以及其热解过程中金属离子的过度损耗,生物炭作为吸附剂一般对阳离子和有机污染物有很强的吸附能力,但它对阴离子污染物的吸附能力有限卫扛因此,需要对生物炭进行改性以提高其对阴离子污染物的吸附性。

蒙脱石材料的吸附作用研究—矿物材料学资料文档

蒙脱石材料的吸附作用研究—矿物材料学资料文档

蒙脱石材料的吸附作用研究姓名:张晓晨学号: 1100012623院系:地球与空间科学学院专业:地球化学指导教师:传秀云教授摘要:蒙脱石是一种应用广泛的矿物材料.。

它独特的矿物结构造成了独特的层间域特性,使其具有良好的吸附性。

这种吸附性具有广泛的应用价值。

本文总结了蒙脱石的基本特征,以及蒙脱石的应用。

在治理环境污染领域,蒙脱石能够有效地吸附重金属离子,经有机化改性后的蒙脱石还能够有效地吸附废水中的有机污染物。

在医学领域,蒙脱石能够吸附表面带电荷的细菌,并能吸附具有杀菌作用的金属离子,因此蒙脱石可以被用于杀菌。

蒙脱石分布广泛,成本低廉,能够应用于多个领域,是一种应用价值极高的矿物材料。

关键字:矿物材料科学;蒙脱石;环境治理;抗菌Researches on the Adsorptive Action of Montmorillonite MaterialsXiaochen ZHANG ( Geochemistry )Directed by Prof. Xiuyun CHUANAbstract:Montmorillonite is widely used as a kind of mineral material. Its mineral structure leads to unique interlayer characteristics, giving it extraordinary adsorption abilities. This paper focused on the basic characteristics and applications of montmorillonite. In the environmental field, montmorillonite can effectively adsorb heavy metal ions, as well as organic pollutants in wastewater. In medicine, montmorillonite is used to adsorb the bacteria with charged surface, or metal ions with a bactericidal effect. Moreover, montmorillonite is widely distributed, of low cost. It has a widely application prospect.Keywords:mineral-material science; montmorillonite; environmental governance; antibacterial1 引言矿物学出现后的几个世纪以来,矿物学的资源属性一直受到人们的重视和利用,矿物材料学的发展日新月异。

基于二氧化钒的可调双宽带太赫兹超材料吸收器

基于二氧化钒的可调双宽带太赫兹超材料吸收器

第50卷第4期2023年北京化工大学学报(自然科学版)Journal of Beijing University of Chemical Technology (Natural Science)Vol.50,No.42023引用格式:许中璞,赵永鹏.基于二氧化钒的可调双宽带太赫兹超材料吸收器[J].北京化工大学学报(自然科学版),2023,50(4):107-112.XU ZhongPu,ZHAO YongPeng.A tunable dual broadband terahertz metamaterial absorber based on vanadium dioxide[J].Journal of Beijing University of Chemical Technology (Natural Science),2023,50(4):107-112.基于二氧化钒的可调双宽带太赫兹超材料吸收器许中璞1 赵永鹏2*(1.武威职业学院信息技术学院,武威 733000;2.四川农业大学机电学院,雅安 625000)摘 要:基于VO 2的相变特性提出一种具有双宽带特性的太赫兹超材料吸收器,包括对角放置的VO 2图案层㊁电介质层以及金反射层共3层结构㊂对吸收器的结构建模㊁吸收效果及吸收特性等进行了仿真分析,仿真结果表明,所设计吸收器吸收率大于90%的两个带宽分别为0.73THz 和0.6THz㊂在通过热控制诱导VO 2从绝缘态到金属态的相变过程中,吸收率分别在31%~93.1%和30%~95.2%之间实现连续可调㊂另外,通过研究不同偏振角及入射角下所设计超材料吸收器的吸收性能发现,该吸收器具有偏振无关㊁偏振不敏感以及大入射角吸收特性㊂所设计吸收器有望在如太赫兹通信㊁成像和探测器等利用太赫兹波段领域得到广泛应用㊂关键词:VO 2相变特性;超材料;太赫兹吸收器;连续可调中图分类号:O436 DOI :10.13543/j.bhxbzr.2023.04.014收稿日期:2023-02-13基金项目:四川省自然科学基金(2023NSFSC0435)第一作者:男,1988年生,硕士*通信联系人E⁃mail:zhaoyp@引 言太赫兹波的工作频率在0.1~10THz,相应的波长在0.03~3mm [1]㊂大多数天然材料在太赫兹频率下表现出微弱的电磁响应,这种现象被称为 太赫兹间隙”㊂而超材料是一种人工设计的周期性结构材料,具有天然材料所不具备的超常物理属性,其奇异的光学特性由所设计的人工周期性结构决定[2]㊂基于超材料的电磁特性,有学者研究了其在操纵太赫兹辐射方面的实用性[3]㊂太赫兹吸收器是太赫兹领域最具吸引力的研究课题之一,由于其在探测㊁成像和调制方面的重要应用前景,受到了人们的广泛关注㊂随着超材料这一概念的引入,太赫兹超材料吸收器得到快速发展㊂在太赫兹波段,关于吸收器已有了大量研究,如超宽带吸收器[4-5]㊁宽带吸收器[6-8]以及窄带吸收器[9-11]等㊂然而,上述绝大多数的吸收器存在一个功能上的限制,即大多数吸收器的电磁波吸收率是不可以调节的,一旦设计完成,其功能就己经固定了㊂因此为了面对日益复杂的电磁应用环境,需要设计一种吸收率可调节的超材料吸收器㊂要实现吸收器的吸收率可调,主要手段是在超材料结构中引入活性材料(如相变材料㊁石墨烯等),使其主动控制超材料吸收器的光学特性㊂二氧化钒(VO 2)是控制器件的理想选择,当施加热㊁外部电场或光学刺激时,可诱导VO 2发生从绝缘态到金属态的可逆相变[12],相变过程中伴随着电导率发生改变,从而实现超材料吸收器的吸收率可调㊂近年来,针对宽带可调太赫兹超材料吸收器已有不少研究,如张婷等[13]基于VO 2设计了一种90%以上吸收带宽为1.06THz 以及吸收率在4%~99.5%之间可调的超材料吸收器;Wang 等[14]基于VO 2设计了一种90%以上的吸收带宽为0.65THz 且吸收率在30%~98%的可调吸收器;Song 等[15]基于VO 2设计了一种90%以上吸收带宽为0.33THz 且吸收率在30%~100%的可调吸收器;Huang 等[16]基于VO 2设计了一种80%以上吸收带宽分别为0.88THz 和0.77THz 且吸收率在20%~90%的可调双宽带吸收器;刘苏雅拉图[17]提出一种二氧化钒开口环阵列组成的宽带可调谐吸收器;晋豪[18]提出一种表面由石墨烯圆盘构成的 葫芦形”图案的超材料吸收器;樊怡等[19]提出基于VO 2相变特性的温度可调控双频太赫兹超材料吸收器;马燕燕[20]提出了一种双频可调谐㊁双频可切换㊁宽带可切换的超材料吸收器;王佳云[21]设计了一种极化可控的单频/五频段超材料吸收器;杨森等[22]设计出一种基于光激发动态可切换的超材料吸收器㊂基于以上分析,目前对于超材料吸收器的研究主要集中在拓宽工作带宽㊁实现宽带可调谐以及提高吸收率和吸收性能等方面㊂为了进一步拓宽工作带宽和提高可调谐范围,本文提出一种基于VO 2的双宽带太赫兹超材料吸收器,其由两个相同的VO 2图案在经典的金属-电介质-金属结构的顶部对角排列而成㊂通过在热控制下诱导VO 2发生从绝缘态到金属态的相变,可以连续调节两个频段的吸收率㊂该吸收器具有偏振无关㊁偏振不敏感以及大入射角吸收特性,在太赫兹波段具有广泛的应用前景,如太赫兹通信㊁成像和探测器等㊂图1 双宽带太赫兹超材料吸收器单元结构示意图Fig.1 Schematic view of the dual broadband terahertzmetamaterial absorber structure1 太赫兹超材料吸收器的结构设计本文提出的双宽带太赫兹超材料单元结构示意图如图1所示㊂该结构包括3层,从上到下依次为对角放置的VO 2图案层㊁电介质层和底部金反射层,其中金的电导率为4.56×107S /m[23],SiO 2的相对介电常数为3.9+0.03i [16]㊂最优结构参数取值如下:单元结构周期P =180μm,金反射层厚度h 1=0.2μm,SiO 2电介质层厚度h 2=36μm,VO 2图案层厚度t =0.1μm,VO 2图案到周期边界的间隙g =11μm,对角图案开口宽度w =23μm,对角图案开口长度l =110μm㊂本文使用CST MICROWAVE STU⁃DIO 软件,通过有限元方法进行全波电磁仿真,在仿真过程中采用频域求解器,使用四面体自适应网格剖分㊂在x 和y 方向采用unit cell 边界条件,在z 方向采用open(add space)边界条件㊂图2 VO 2介电常数随电导率的变化Fig.2 Variation of the permittivity of VO 2withconductivity该结构的光学介电常数可由Drude 模型[24]描述ε(ω)=ε∞-ω2p (σ)ω2+i γω(1)式中,ε∞=12为高频介电常数,γ=5.75×1013rad /s 为碰撞频率,σ处的等离子体频率ω2p (σ)=σσ0ω2p (σ0),ωp (σ0)=1.4×1015rad /s,σ0=3×105S /m㊂在热控制下,VO 2可以发生由绝缘态到金属态的可逆相变,其电导率σ可由2×102S /m 变化到2×105S /m㊂根据式(1),利用Matlab 软件计算了VO 2介电常数随电导率的变化情况,结果如图2所示㊂可以看出,不同电导率下介电常数实部的变化远小于虚部,当电导率取值为2×102S /m 时,表现为绝缘体特性,当电导率取值为2×105S /m 时,表现为金属特性㊂在仿真过程中,采用Drude 模型对VO 2的电导率进行取值,与Matlab 计算过程一致㊂当通过热刺激使VO 2温度略高于室温时,可以实现从绝缘体到金属的转变,在相变温度点其电导率提高了㊃801㊃北京化工大学学报(自然科学版) 2023年10000倍,晶体结构由单斜相转变为四方相㊂2 太赫兹超材料吸收器的性能分析在本文中,吸收率定义如下[25]:A(ω)=1-R(ω)-T(ω)=1-|S11(ω)|2-|S21(ω)|2,其中A(ω)㊁R(ω)和T(ω)分别表示吸收率㊁反射率和透射率,S11(ω)和S21(ω)分别为反射系数和透射系数㊂由于底部金反射层的厚度远远大于入射电磁波的趋肤深度,使得入射电磁波无法透过该金属薄膜继续传播,因此T(ω)=0㊂吸收器的吸收率可进一步简化为A(ω)=1-R(ω)=1-|S11(ω)|2㊂横电模(TE)和横磁模(TM)两种偏振方式下吸收器的吸收率㊁反射率以及透射率变化情况的仿真结果如图3(a)所示㊂在0.67THz~1.4THz和2.9THz~3.5THz频率范围内,吸收率大于90%的带宽分别为0.73THz和0.6THz,在0.86THz㊁2.93THz以及3.39THz这3个频率点处吸收率接近于1,表示这些点的吸收接近完美吸收㊂另外,从图中可以看出,两种偏振方式下的吸收率㊁反射率以及透射率变化保持高度一致,表明所设计的超材料吸收器具有偏振无关特性㊂两种偏振方式下的透射率为零,表明理论分析与仿真结果一致㊂在TE偏振下吸收谱随偏振角的变化情况如图3(b)所示,可以看出,改变偏振角对吸收器的吸收性能没有任何影响,表明所设计的吸收器具有偏振不敏感特性㊂另外,由于所设计的VO2图案的对称性,TM偏振下的吸收光谱与TE偏振下的吸收光谱是重合的,这里不再赘述㊂通过热控制诱导VO2从绝缘态到金属态的相变过程中,可以连续调节两个频带的吸收率和带宽,如图4所示㊂从图中可以看出,在VO2电导率由2×102S/m变化到2×105S/m过程中,第一个频带(0.67THz~1.4THz)的吸收率可由31%增大到93.1%,第二个频带(2.9THz~3.5THz)的吸收率可由30%增大到95.2%㊂因此,通过控制VO2电导率可以实现吸收器两个带宽的连续可调㊂为了更好地理解吸收器的吸收性能,引入阻抗匹配理论,在正入射下太赫兹波的相对阻抗可描述为[25]Z r=(1+S11(ω))2-S221(ω)(1-S11(ω))2-S221(ω)(2)式中,Z r=Z/Z0,Z和Z0分别为吸收器的有效阻抗图3 双宽带吸收器的反射谱㊁透射谱和吸收谱以及不同偏振角下的吸收光谱图Fig.3 Reflection,transmission and absorption spectra of the dual broadband absorber and the absorption spectrawith different polarization angles图4 吸收器吸收率随电导率变化情况Fig.4 Variation of the absorption with conductivity 和自由空间阻抗㊂当Z r=Z/Z0=1时,吸收器有效阻抗与自由空间阻抗匹配,吸收率最大㊂当相对阻抗的实部为1,虚部为0时,可以实现阻抗匹配㊂图5为不同电导率下相对阻抗实部和虚部的变化㊂可以看出,当VO2电导率为2×105S/m(金属态)㊃901㊃第4期 许中璞等:基于二氧化钒的可调双宽带太赫兹超材料吸收器时,在0.67THz ~1.4THz 和2.9THz ~3.5THz 两个频率范围内,相对阻抗的实部接近于1,虚部接近于0,实现了完美吸收,与理论分析结果一致㊂图5 不同电导率下相对阻抗实部和虚部的变化Fig.5 Variation of real and imaginary parts of the relativeimpedance for different VO 2conductivities进一步研究了TE 和TM 两种偏振方式下不同入射角对吸收器吸收性能的影响,结果如图6所示㊂TE 偏振入射下(图6(a)),对于第一个频带(0.67THz ~1.4THz),当入射角小于60°时,吸收器能够保持良好的吸收性能,对于第二个频带(2.9THz ~3.5THz),当入射角小于20°时,吸收器能够保持良好的吸收性能;入射角继续增大,第一个宽带的吸收率急剧下降,第二个宽带的中心频率出现蓝移现象,且带宽逐渐变窄㊂在TM 偏振下(图6(b)),对于第一个频带(0.67THz ~1.4THz),当入射角小于60°时,吸收器能够保持良好的吸收性能;对于第二个频带(2.9THz ~3.5THz),当入射角小于20°时,吸收器也能够保持良好的吸收性能,入射角进一步增大,两个频带内的吸收率都显著降低㊂本文所设计吸收器与文献中的吸收器性能对比如表1所示㊂可以看出,与双频吸收器相比,本文所设计的双宽带吸收器在工作带宽和吸收率可调范围两个方面的性能都有所提高;与单频吸收器相比,本文部分工作带宽有所拓宽㊂图6 吸收率随入射角的变化Fig.6 Variation of absorption with incident angle 表1 本文设计吸收器与文献中吸收器的性能对比Table 1 Comparison of the performance of the absorberdesigned in this paper with absorbers reported in the literature吸收器来源材料工作带宽/THz吸收率可调范围文献[13]VO 21.06(吸收率>90%)4%~99.5%文献[14]VO 20.65(吸收率>90%)30%~98%文献[15]VO 20.33(吸收率>90%)30%~100%文献[16]VO 20.88和0.77(吸收率>80%)20%~90%本文设计VO 20.73和0.6(吸收率>90%)30%~95.2%3 结论本文提出了一种由对角放置的VO 2图案层㊁介质层以及金反射层组成的双宽带太赫兹超材料吸收器结构,并根据超材料吸收器的吸收机理对吸收器的吸收性能作出分析㊂仿真结果表明,该吸收器吸收率达90%以上的吸收带宽分别为0.73THz 和㊃011㊃北京化工大学学报(自然科学版) 2023年0.6THz㊂当VO2的电导率由2×102S/m变化到2×105S/m时,两个频带的吸收率分别可在31%~ 93.1%和30%~95.2%之间连续调节㊂根据阻抗匹配理论分析可知,该吸收器具有偏振无关㊁偏振不敏感以及大入射角吸收特性,因此其在太赫兹通信㊁成像和探测器等方面具有广泛的应用前景㊂参考文献:[1] QIAN J J,ZHOU J,ZHU Z,et al.Polarization⁃insensi⁃tive broadband THz absorber based on circular graphenepatches[J].Nanomaterials,2021,11(10):2709. [2] REN Z,CHENG L,HU L,et al.Photoinduced broad⁃band tunable terahertz absorber based on a VO2thin film[J].ACS Applied Materials&Interfaces,2020,12(43):48811-48819.[3] WANG T L,ZHANG Y P,ZHANG H Y,et al.Dual⁃controlled switchable broadband terahertz absorber basedon a graphene⁃vanadium dioxide metamaterial[J].Opti⁃cal Materials Express,2020,10(2):369-386. [4] ZHU J F,MA Z F,SUN W J,et al.Ultra⁃broadbandterahertz metamaterial absorber[J].Applied Physics Let⁃ters,2014,105(2):021102.[5] RI K J,RI C H,RI S Y.Ultra⁃broadband terahertzmetamaterial absorber using a simple design method[J].Optics Communications,2022,515:128191. [6] GRANT J,MA Y,SAHA S,et al.Polarization insensi⁃tive,broadband terahertz metamaterial absorber[J].Op⁃tics Letters,2011,36(17):3476-3478. [7] WEN Y Z,MA W,BAILEY J,et al.Broadband tera⁃hertz metamaterial absorber based on asymmetric resona⁃tors with perfect absorption[J].IEEE Transactions onTerahertz Science and Technology,2015,5(3):406-411.[8] CHENG Y Z,ZOU H J,YANG J J,et al.Dual andbroadband terahertz metamaterial absorber based on acompact resonator structure[J].Optical Materials Ex⁃press,2018,8(10):3104-3114.[9] HU D,MENG T H,WANG H Y,et al.Ultra⁃narrow⁃band terahertz perfect metamaterial absorber for refractiveindex sensing application[J].Results in Physics,2020,19:103567.[10]WANG Y,YUE L S,CUI Z J,et al.Optically tunablesingle narrow band all⁃dielectric terahertz metamaterialsabsorber[J].AIP Advances,2020,10(4):045039.[11]CHEN F,CHENG Y Z,LUO H.Temperature tunablenarrow⁃band terahertz metasurface absorber based on InSbmicro⁃cylinder arrays for enhanced sensing application[J].IEEE Access,2020,8:82981-82988. [12]REN Y,ZHOU T L,JIANG C,et al.Thermally switc⁃hing between perfect absorber and asymmetric transmis⁃sion in vanadium dioxide⁃assisted metamaterials[J].Op⁃tics Express,2021,29(5):7666-7679. [13]张婷,杨森,于新颖.基于二氧化钒的可调宽带太赫兹完美吸收器设计[J].激光与光电子学进展,2021,58(21):250-256.ZHANG T,YANG S,YU X Y.Tunable broadband tera⁃hertz perfect absorber design based on vanadium dioxide[J].Laser and Optoelectronics Progress,2021,58(21):250-256.(in Chinese)[14]WANG S X,CAI C F,YOU M H,et al.Vanadium di⁃oxide based broadband THz metamaterial absorbers withhigh tunability:simulation study[J].Optics Express,2019,27(14):19436-19447.[15]SONG Z Y,WANG K,LI J W,et al.Broadband tunableterahertz absorber based on vanadium dioxide metamateri⁃als[J].Optics Express,2018,26(6):7148-7154.[16]HUANG J,LI J N,YANG Y,et al.Active controllabledual broadband terahertz absorber based on hybrid meta⁃materials with vanadium dioxide[J].Optics Express,2020,28(5):7018-7027.[17]刘苏雅拉图.基于石墨烯和二氧化钒的太赫兹可调谐超材料吸收器[D].呼和浩特:内蒙古大学,2022.LIU S Y.Terahertz tunable metamaterial absorber basedon graphene and vanadium dioxide[D].Hohhot:InnerMongolia University,2022.(in Chinese) [18]晋豪.基于石墨烯圆盘的超材料吸收器的研究[D].成都:四川师范大学,2022.JIN H.Study on metamaterial absorbers based on gra⁃phene disks[D].Chengdu:Sichuan Normal University,2022.(in Chinese)[19]樊怡,杨荣草.基于VO2温度可调控双频超薄太赫兹超材料吸收器[J].量子光学学报,2022,28(1):46-54.FAN Y,YANG R C.Temperature⁃tunable dual⁃band ul⁃tra⁃thin terahertz metamaterial absorber based on vanadi⁃um dioxide[J].Journal of Quantum Optics,2022,28(1):46-54.(in Chinese)[20]马燕燕.双频及宽带可调控超材料吸收器的研究[D].太原:山西大学,2021.MA Y Y.Research on dual⁃band and broadband control⁃lable metamaterial absorbers[D].Taiyuan:Shanxi Uni⁃versity,2021.(in Chinese)[21]王佳云.多频/宽频电磁超材料吸收器和极化转换器的研究[D].太原:山西大学,2021.㊃111㊃第4期 许中璞等:基于二氧化钒的可调双宽带太赫兹超材料吸收器WANG J Y.Study on multi⁃band/broadband absorbersand polarization converters based on electromagneticmetamaterials[D].Taiyuan:Shanxi University,2021.(in Chinese)[22]杨森,袁苏,王佳云.一种光激发可切换的双频太赫兹超材料吸收器[J].光学学报,2021,41(2):0216001.YANG S,YUAN S,WANG J Y.Light⁃excited andswitchable dual⁃band terahertz metamaterial absorber[J].Acta Optica Sinica,2021,41(2):0216001.(inChinese)[23]YAN D X,MENG M,LI J S,et al.Vanadium dioxide⁃assisted broadband absorption and linear⁃to⁃circular polar⁃ization conversion based on a single metasurface designfor the terahertz wave[J].Optics Express,2020,28(20):29843-29854.[24]WANG S X,KANG L,WERNER D H.Hybrid resona⁃tors and highly tunable terahertz metamaterials enabled byvanadium dioxide(VO2)[J].Scientific Reports,2017,7:4326.[25]CHE Z G,LI Z X,ZHANG G M,et al.Active controlla⁃ble broadband absorber based on vanadium dioxide[C]∥2021Photonics&Electromagnetics Research Symposium(PIERS).Hangzhou:IEEE,2021:604-608.A tunable dual broadband terahertz metamaterial absorberbased on vanadium dioxideXU ZhongPu1 ZHAO YongPeng2*(rmation Technology College,Wuwei Vocational College,Wuwei733000;2.College of Mechanical and Electrical Engineering,Sichuan Agricultural University,Ya’an625000,China) Abstract:A terahertz metamaterial absorber with dual broadband characteristics based on the phase transition char⁃acteristics of VO2has been fabricated.The absorber is composed of three layers,a diagonally placed VO2pattern layer,a dielectric layer and a gold reflector.The simulation results show that there are two bandwidths with absorp⁃tivity greater than90%at0.73THz and0.6THz.During the phase transition from the insulating state to the me⁃tallic state of VO2induced by thermal control,the absorption rate is continuously tunable in the range31%-93.1%and30%-95.2%,respectively.In addition,by studying the absorption performance of the metamaterial absorber at different polarization angles and incidence angles,it is found that the absorber has polarization⁃inde⁃pendent,polarization⁃insensitive and large incidence angle absorption characteristics.The absorber has broad pros⁃pects for applications in the terahertz band region,such as in terahertz communication,imaging and detectors. Key words:VO2phase transition property;metamaterial;terahertz absorber;continuously tunable(责任编辑:吴万玲)㊃211㊃北京化工大学学报(自然科学版) 2023年。

氧化石墨烯-羧基碳纳米管-多乙烯多胺三维蜂窝状材料吸附CO2

氧化石墨烯-羧基碳纳米管-多乙烯多胺三维蜂窝状材料吸附CO2

CHEMICAL INDUSTRY AND ENGINEERING PROGRESS 2016年第35卷第11期·3576·化工进展氧化石墨烯-羧基碳纳米管-多乙烯多胺三维蜂窝状材料吸附CO2胡航标,张涛,崔征,唐盛伟(四川大学化学工程学院,四川成都 610065)摘要:以氧化石墨烯-羧基碳纳米管水溶液为原料,葡萄糖酸β内酯为交联促进剂,通过冷冻干燥法制得负载有多乙烯多胺的氧化石墨烯-羧基碳纳米管三维多孔气凝胶。

通过在制备过程中改变多乙烯多胺的加入量可以调节其负载量。

FTIR、XRD、TG、SEM、XPS、Raman、N2吸脱附等测试表征发现:多乙烯多胺通过酰胺键与基体连接,所得材料呈蜂窝状,且比表面积、孔容和平均孔径随胺类负载量的增加而逐渐降低,引入多乙烯多胺后的气凝胶材料通过化学作用实现CO2吸附。

在200kPa、328K下,多乙烯多胺含量为55.8%的改性吸附剂的CO2吸附量可达3.9mmol/g,为相同条件下未改性吸附剂的9.8倍。

结果表明,将多乙烯多胺、氧化石墨烯和羧基碳纳米管制备成三维蜂窝状多孔材料能有效提高CO2吸附性能。

关键词:纳米材料;二氧化碳;凝胶;吸附中图分类号:TQ 424.29 文献标志码:A 文章编号:1000–6613(2016)11–3576–09DOI:10.16085/j.issn.1000-6613.2016.11.029Preparation of three-dimensional honeycomb-like material of graphene oxide -carboxylated carbon nanotube-polyethylenepolyamine toadsorb CO2HU Hangbiao,ZHANG Tao,CUI Zheng,TANG Shengwei(College of Chemical Engineering,Sichuan University,Chengdu 610065,Sichuan,China)Abstract:Using graphene oxide and carboxylated carbon nanotube as base material and gluconic acid β lactone as crosslinking promoter,we prepared a three-dimensional(3D)porous aerogel material functionalized by polyethylenepolyamine(PEPA)with a freeze-drying method. The PEPA loading was adjusted by changing the PEPA dosage. The as-synthesized 3D porous aerogel material were characterized by FTIR,XRD,TG,SEM,XPS,Raman and N2 adsorption-desorption. The results indicated that PEPA was grafted by an amide bond between PEPA and graphene oxide. The 3D porous material had a honeycomb like-appearance. The specific surface area,pore volume and average pore size were decreased with increasing PEPA loading. The adsorption of CO2 on the 3D honeycomb-like material was based on a mechanism of chemisorption. At 200kPa and 328K,the CO2 adsorption capacity on the 3D porous material with a PEPA content of 55.8% reached up to 3.9mmol/g,which was9.8 times to that on the aerogel without PEPA loading. The results showed that crosslinkingpolyethylenepolyamine with graphene oxide sheet and carboxylated carbon nanotube to prepare 3D porous aerogel material effectively improved the CO2 adsorption capacity.Key words:nanomaterials;carbon dioxide;gels;adsorption温室效应造成的全球气候问题已成为人类进入21世纪以来面临的最大生存挑战。

钙铝和铁铝水滑石的制备及其吸附水中六价铬的性能

钙铝和铁铝水滑石的制备及其吸附水中六价铬的性能

中国粉体技术CHINA POWDER SCIENCE AND TECHNOLOGY 第27卷第3期2021年5月Vol. 27 No. 3May 2021文章编号:1008-5548 (2021) 03-0059-09 doi : 10.13732/j.issn.l008-5548.2021.03.008钙铝和铁铝水滑石的制备及其吸附水中六价铅的性能王鹏瑞V,杨 丹1,张 雪1,李 静1,闫良国1(1.济南大学水利与环境学院,山东济南250022 ; 2.济南市市中区环境监测站,山东济南250001)摘要:为寻找高效吸附水中六价<(Gr(VI))的水滑石功能材料,以水热法制备钙铝(CaAl-LDH)和铁铝水滑石(FeAl- LDH)2种吸附剂,通过X 射线衍射仪、红外光谱仪、扫描电镜和比表面积测定仪研究其结构和性质,采用批次平衡实验 比较研究其对水中Gr(VI)的吸附性能。

结果表明:CaAl-LDH 和FeAl-LDH 具有水滑石的特征衍射峰和介孔结构,呈六 边形片状,比表面积分别为&746、159.5 m 2/g ;2种材料对Cr(VI)的吸附速率较快,在30 miri 达到平衡,且吸附过程不 受溶液pH 值的影响,溶液中存在的常见阴离子对Cr(VI)影响较小;吸附动力学和等温线数据分别符合拟二级动力学方 程和Langmuir 等温线模型,CaAl-LDH 和FeAl-LDH 对Cr(VI)的最大吸附量分别为34.92、51.31 g/kg o 关键词:钙铝水滑石;铁铝水滑石;六价鎔;吸附;水热法中图分类号:X52 文献标志码:APreparation of CaAl- and FeAl-layered double hydroxides andadsorptive removal Cr( VI) in aqueous solutionsWANG Pengrui^2, YANG Dan , ZHANG Xue 1, LI Jing 1, YAN Liangguo 1(1. School of Water Conservancy and Environment , University of Jinan , Jinan 250022, China ;2. Jinan Shizhong Environmental Monitoring Station , Jinan 250001, China)Abstract : To obtain layered double hydroxide ( LDH ) based functional materials for efficient removal hexavalent chromium (Cr( VI)) from water , CaAl-LDH and FeAl-LDH were prepared by the hydrothermal method. The structure and property were investigated by X-ray diffraction pattern ( XRD) , Fourier transform infrared spectroscopy , scanning electron microscopy and specific surface area measurement. Batch equilibrium experiments were used to evaluate the adsorption performance of the as-prepared CaAl-LDH and FeAl-LDH for aqueous Cr( VI). The experimental results show that CaAl-LDH and FeAl-LDH have typical XRD peaks of LDH, mesoporous structure and hexagonal laminar shape. The specific surface areas are 8. 746 and 159.5 m 2/g. The adsorption processes of Cr( VI) by CaAl-LDH and FeAl-LDH are fast and reache equilibrium within 30 min, andare not affected by the initial solution pH value and the common coexisting anions. The kinetic and isothermal data follow the pseudo-second-order kinetic equation and the Langmuir model , respectively. The maximum adsorption capacities of CaAl-LDH and FeAl-LDH for aqueous Cr( VI) are 34. 92 and 51.31 g/kg.Keywords : CaAl-LDH ; FeAl-LDH ; hexavalent chromium ; adsorption ; hydrothermal method水滑石,又称层状双金属氢氧化物(layered double hydroxides , LDHs),归类为胶体纳米材料。

Adsorption of Pb(II) onto Modified Rice Bran

Adsorption of Pb(II) onto Modified Rice Bran

Adsorption of Pb(II) onto Modified Rice Bran Hengpeng Ye;Zhijuan Yu【期刊名称】《自然资源(英文)》【年(卷),期】2010(1)2【摘要】In this study, the modified rice bran was tested to remove Pb(II) from water. Batch experiments were carried out to evaluate the adsorption characteristics of the modified rice bran for Pb(II) removal from aqueous solutions. The adsorption isotherms, thermodynamic parameters, kinetics, pH effect, and desorbability were examined. The results show that the maximum adsorption capacity of the modified rice bran was approximately 70.8 mg Pb(II)/g absorbent at temperature of 25℃ and at the initial Pb(II) concentration of 400 mg/L and pH 7.0. And the adsorption isotherm data could be well fitted by both Langmuir equation and Freundlich equation. Thermodynamic studies confirmed that the process was spontaneous and endothermic. The adsorbed amounts of Pb(II) tend to increase with the increase of pH. The adsorption kinetic data can be satisfactorily described by either of the power functions and simple Elovich equations. The desorbability of Pb(II) is about 15-20%, and it is relatively difficult for the adsorbed Pb(II) to be desorbed. The relatively low cost and high capabilities of the rice bran make it potentially attractive adsorbent for the removal of Pb(II) from wastewater.【总页数】6页(P104-109)【关键词】Rice;Bran;Pb(II);Removal;Adsorption;Capacity;Adsorption;Isotherm【作者】Hengpeng Ye;Zhijuan Yu【作者单位】不详【正文语种】中文【中图分类】O6【相关文献】1.<i>In-Vitro</i>Fermentation by Human Fecal Bacteria and Bile Salts Binding Capacity of Physical Modified Defatted Rice Bran Dietary Fiber [J], Cheickna Daou;Hui Zhang;Camel Lagnika;Oumarou Hama Moutaleb2.Chemically Modified <i>Cornulaca monacantha</i>Biomass for Bioadsorption of Hg (II) from Contaminated Water: Adsorption Mechanism [J], A. Hashem;Khalid A. Al-Kheraije3.Biosorption of Cu(II), Pb(II) and Zn(II) Ions from Aqueous Solutions Using Selected Waste Materials: Adsorption and Characterisation Studies [J], Wiwid Pranata Putra;Azlan Kamari;Siti Najiah Mohd Yusoff;Che Fauziah Ishak;Azmi Mohamed;Norhayati Hashim;Illyas Md Isa4.Adsorption of Cu(II), Ni(II), Zn(II), Cd(II) and Pb(II) onto Kaolin/Zeolite Based- Geopolymers [J], Bassam El-Eswed;Mazen Alshaaer;Rushdi Ibrahim Yousef;Imad Hamadneh;Fawwaz Khalili5.Removal of Cu(II), Pb(II) and Zn(II) Ions from Aqueous Solutions Using Selected Agricultural Wastes: Adsorption and Characterisation Studies [J], Siti Najiah Mohd Yusoff;Azlan Kamari;Wiwid Pranata Putra;Che Fauziah Ishak;Azmi Mohamed;Norhayati Hashim;Illyas Md Isa因版权原因,仅展示原文概要,查看原文内容请购买。

碳掺杂六方氮化硼氧化脱硫性能的理论研究

碳掺杂六方氮化硼氧化脱硫性能的理论研究

第50卷第3期辽 宁化工V〇1.50, No. 3 2021 # 3 ^1_______________________________Liaoning Chemical Industry_______________________________March,2021碳掺杂六方氮化硼氧化脱硫性能的理论研究吕乃霞(兴义民族师范学院,贵州兴义562400)摘要:采用密度泛函方法计算了包括苯并噻吩(B T),二苯并噻吩(D B T),二甲基二苯并噻吩(D M D B T)在内的芳香性硫化合物在掺杂碳的六方氮化硼表面的吸附及氧化机理。

结果表明,02在掺杂碳的氮化硼首先被活化为〇2_,〇2_作为活性氧物种进一步将硫化物氧化为亚砜或砜。

三种芳香性硫化物在碳掺杂氮化硼表面的脱硫性能按照D M D B T,D B T,B T的顺序降低。

关键词:密度泛函;氧化脱硫;碳掺杂;六方氮化硼中图分类号:T Q013文献标识码:A文章编号:1004-0935 (2021 ) 03-0285-04随着燃料中硫含量标准日趋严格,传统的加氢 脱硫工艺(HDS)对苯并噻吩(BT)、二苯并噻吩(DBT)及其衍生物4,6-二甲基二苯并噻吩(DMDBT)的脱 除效率较低,因此必须寻找新的方法及工艺以更有 效的脱除芳香性硫化物[M]。

吸附脱硫(ADS)[5%和氧化脱硫技术(ODS)[>9]应运而生。

其中,0D S因其温和的操作条件和高效的脱硫性能引起了人们的 关注。

通过O D S工艺,苯并噻吩类硫化物最终转 化为高极性的亚砜或砜,这些亚砜或砜很容易通过 萃取或吸附去除。

因此寻找合适的催化剂,实现温 和条件下硫化物的氧化是O D S反应的关键。

近年来,作为一种新型二维材料,六方氮化硼 (h-BN)具有高的化学稳定性,优良的热稳定性和大 的比表面积,已在吸附、催化及功能材料等领域应 用[1〇_12]。

有趣的是在h-B N的制备过程中B-或者 N-点缺陷位极易获得,而这些缺陷位点又赋予了 h-B N极大的化学活性,并为在缺陷位点引入非金 属或者金属原子形成掺杂类型的氮化硼提供了可 能[13]。

一锅法制备三嗪基多孔聚合物及对Pb^2的吸附研究

一锅法制备三嗪基多孔聚合物及对Pb^2的吸附研究

2019年第7期广东化工第46卷总第393期 ·7 ·一锅法制备三嗪基多孔聚合物及对Pb2+的吸附研究彭荣鑫,满瑞林*(中南大学化学化工学院,湖南长沙410083)[摘要]以三聚氰胺和对苯二甲酸,间苯二甲酸,邻苯二甲酸为合成单体,采用一锅缩聚法制备了一系列三嗪基多孔有机物聚合物(NPM,NMM,NOM)。

探究了该聚合物对重金属Pb2+在不同条件下的吸附性能,吸附过程相比Freundlich模型更加符合Langmuir模型。

动力学研究表明此类聚合物对Pb2+的吸附符合拟二级动力学。

在实验中,吸附剂NPM、NMM和NOM对Pb2+最大吸附容量分别为159.4、141.6、147.1 mg/g。

聚合物具有优异的重复使用性能,在重复吸附测试五次的情况下,吸附量依然能达到最初的79.21%。

[关键词]多孔有机聚合物;Pb2+;吸附[中图分类号]TQ [文献标识码]A [文章编号]1007-1865(2019)07-0007-03One-pot Synthesis of Triazine-based Porous Organic Polymers for Pb2+ AdsorptionRemovalPeng Rongxin, Man Ruilin*(School of Chemistry and Chemical Engineering, Central South University, Changsha 410083, China) Abstract: A series of triazine-based porous organic polymers (NPM, NMM, NOM) were prepared by one-pot polycondensation method using melamine and terephthalic acid, isophthalic acid, phthalic acid as synthetic monomers. The adsorption properties of the polymer for Pb2+under different conditions were investigated. The adsorption process is more consistent with the Langmuir model than the Freundlich model. Kinetic studies indicate that the adsorption of Pb2+ is consistent with psedo-second-order. The maximum adsorption capacities of the adsorbents NPM, NMM and NOM for Pb2+were 159.4, 141.6 and 147.1 mg/g, respectively. The polymer has excellent reusability, and the adsorption amout can still reach the initial 79.21% in the case of repeated adsorption tests 5 times.Keywords: porous organic polymer;Pb2+;adsorption1 引言随着工业化的发展,氯碱、电镀、采矿、冶金、电池和石化等行业对自然水域中排放的含重金属废水对环境造成严重污染[1]。

活性炭与碳纳米管材料改性及其对重金属的吸附

活性炭与碳纳米管材料改性及其对重金属的吸附

活性炭与碳纳米管材料改性及其对重金属的吸附Absorption of heavy mental ions on modified materials:active carbon and Carbon nanotubes摘要:总结多种不同原材料制备和改性活性炭及碳纳米管的方法、吸附机理。

通过吸附等温线、表面结构性质(比表面积、总表面酸性官能团、等电点等特征)分析这两类材料改性后对单一重金属的吸附性能。

论述多种重金属共存时改性材料对金属离子的吸附影响。

最后展望改性材料的存在问题及应用前景。

关键词:材料改性活性炭碳纳米管吸附重金属Abstract:Sum the methods of making and modifying active carbon and carbon nanotubes from differents of raw materials and adsorption mechanism of modified materials.The single heavy mental ions adsorption performance on these two materials isinvestigated by measuring different properties such asspecific surface area,PZC,total surface acidic groups as well as adsorption isotherm.The adsorption capacities of many heavy mental ions on modified material were studied.Modify of materials has some defects as well as widely used.Key words:modification of material active carbonCarbon nanotubes absorption heavy mental ions 引言:目前冶炼、电解、医药、油漆、合金、电镀、纺织印染、造纸、陶瓷与无机颜料制造等行业每年排放大量含有多种重金属离子的工业废水[1].污水中大部分重金属属于有效态,具有生物富集、生物浓缩、生物放大效应,对生物体危害很大,受到国内外的重视。

二氧化碳热催化英文

二氧化碳热催化英文

二氧化碳热催化英文English:Carbon dioxide (CO2) thermal catalysis refers to the process of using a catalyst to promote the conversion of CO2 into useful products, such as fuels or chemicals, through a series of chemical reactions. This process is important in the field of renewable energy and environmental sustainability, as it offers a potential solution for reducing CO2 emissions and utilizing CO2 as a feedstock for valuable products. In CO2 thermal catalysis, the catalyst plays a crucial role in lowering the activation energy of the chemical reactions, thereby accelerating the conversion of CO2 and facilitating the formation of desired products. Various catalysts, including transition metals, metal oxides, and zeolites, have been studied for their effectiveness in CO2 thermal catalysis. Research in this area also focuses on understanding the reaction mechanisms, optimizing catalyst performance, and exploring new catalytic materials to enhance the efficiency and selectivity of CO2 conversion.中文翻译:二氧化碳(CO2)热催化指的是利用催化剂促进CO2转化为燃料或化学品等有用产品的过程,通过一系列化学反应。

膜 吸附 磷酸根

膜 吸附 磷酸根

膜吸附磷酸根膜吸附磷酸根是一种常见的水处理技术,用于去除水体中的磷酸根离子。

膜吸附是一种通过物质与膜表面之间的吸附作用,将目标污染物从水中分离的过程。

在膜吸附磷酸根的过程中,往往会使用一些特定的吸附剂或吸附材料,下面是关于膜吸附磷酸根的相关参考内容。

1. Zhang L, Li J, Liu L, et al. Adsorptive removal of phosphate from water using graphene oxide-incorporated nanofiltration membranes[J]. Journal of Membrane Science, 2016, 501: 110-118. 这篇文章介绍了一种利用石墨烯氧化物(GO)改性的纳滤膜来吸附去除水中磷酸根的方法。

实验结果表明,GO纳滤膜具有良好的吸附去除磷酸根的性能。

2. Bastami T R, Bueken B, Denayer J F M, et al. Microporous coordination polymers as adsorbents for phosphate removal from water[J]. Chemical Engineering Journal, 2019, 360: 1124-1133.这篇文章研究了一种基于微孔配位聚合物(MCPs)的磷酸根吸附剂,通过调节MCPs的孔径和表面化学性质,实现了高效去除水中磷酸根的目的。

3. Khan M I, Lee J, Ilyas H, et al. Ultrathin graphene oxide membranes for effectively removing phosphate from water[J]. Nanotechnology, 2018, 29(41): 415701.该研究报道了一种利用超薄氧化石墨烯膜高效去除水中磷酸根的方法。

CO2 adsorption on carbon molecular sieves 2012 164 280-7

CO2 adsorption on carbon molecular sieves 2012 164 280-7

CO 2adsorption on carbon molecular sievesA.Wahby,J.Silvestre-Albero,A.Sepúlveda-Escribano ⇑,F.Rodríguez-ReinosoLaboratorio de Materiales Avanzados,Departamento de Química Inorgánica –Instituto Universitario de Materiales de Alicante (IUMA),Universidad de Alicante,Apartado 99,E-03080Alicante,Spaina r t i c l e i n f o Article history:Available online 19July 2012Keywords:Carbon molecular sieves CO 2adsorptionImmersion calorimetrya b s t r a c tThe effect of the textural properties of a series of commercial carbon molecular sieves (CMS),prepared from different polymeric precursors,on their ability for CO 2adsorption at different temperatures has been studied.The adsorbents have been characterized by N 2and CO 2adsorption at 77and 273K,respectively,together with measurements of immersion calorimetry into liquids of different molecular dimensions.The studied CMSs cover a wide range of porosity,from purely microporous carbons to samples containing wide micropores as well as a certain proportion of mesoporosity.Studies of CO 2adsorption,at atmospheric pressure (1bar)and three different temperatures (273,298and 323K),have shown that a high CO 2adsorption capacity requires the presence of a well-developed microporosity,as well as a high volume of narrow micropores.On the other hand,narrow micropores seem to be the key factor leading to a max-imum capacity of CO 2adsorption,even at temperatures close to that of anthropogenic emissions of CO 2.Ó2012Elsevier Inc.All rights reserved.1.IntroductionEnergy consumption,together with the progressive growth of world’s population,has soared during the 20th century,led by a great revolution entitled ‘‘transport’’.Moreover,the invention of vehicles,energy-powered trains and aircrafts has created a new world that has become progressively dependent on the use of fossil fuels such as gasoline,diesel and jet-fuel.However,the environ-ment is already paying ‘‘the tax’’of this spectacular socio-economic progress.In fact,serious environmental problems due to emissions of many pollutants from the combustion of solid,liquid and gas fuels in various mobile/stationary energy systems,together with the harmful emissions generated by industrial plants,have been reported as major global problems involving not only pollutants such as NOx,SOx and soot,but also greenhouse gases like carbon dioxide and methane.There are more concerns about global cli-mate change [1–3]and,therefore,an increased interest in reducing emissions of greenhouse gases,particularly CO 2[4–7].The reuse of the latter is nowadays a challenging task due to the continuous and significant rise in atmospheric CO 2concentrations,the increased consumption of carbon-based energy worldwide,the exhaustion of available sources of carbon and the low efficiency of the current energy systems.Nevertheless,the reuse of CO 2undergoes several limitations,such as:(i)cost of storage,separation,purification and transport;and (ii)energy requirement for chemical conversion (source and cost of reagents).There are several methods to sepa-rate CO 2from flow gases for large-scale applications [8].Among them,the most widely used are cryogenic distillation,membrane purification,liquid absorption and adsorption by means of porous solids.Cryogenic distillation is not considered to be practical for CO 2separation because of the involved energy consumption.Membrane-based separation of CO 2has been widely investigated [9].Traditionally,absorption using basic solvents (mainly amine solutions)has been widely used [10,11],although this technology suffers important drawbacks.In this sense,adsorption processes using porous sorbents can be an excellent alternative to the other mentioned processes for CO 2removal/recovery by physical adsorp-tion.Zeolites,activated carbons,carbon molecular sieves,meso-porous silicas and,more recently,metal–organic framework materials (MOF)have been proposed as promising candidates for CO 2adsorption [9,12–16].Carbon molecular sieves (CMS)are carbonaceous materials with a narrow pore size distribution,endowed with a selective adsorp-tion capacity of certain components of a mixture.They can dis-criminate molecules on the basis of size,shape or on a difference in adsorption equilibrium or,even,in adsorption rate.Thus,micro-porous CMS require the presence of a specific porous network con-taining pore mouths of molecular dimensions,together with a relatively high micropore volume.These features will confer them with a high adsorption capacity and selectivity into a given appli-cation.Hence,a proper molecular sieve must exhibit high adsorp-tion capacity and fast adsorption kinetics of certain components of a gas mixture which leads to high selectivity.CMS are commonly prepared from a variety of carbonaceous materials such as cellulosic precursors [17,18],coals [19],carbon fibers [20,21],res-ins [22,23],etc.In general,there are two main methods to manu-facture microporous CMS;the first one is based on controlled1387-1811/$-see front matter Ó2012Elsevier Inc.All rights reserved./10.1016/j.micromeso.2012.06.034Corresponding author.Tel.:+34965903974;fax:+34965903454.E-mail address:asepul@ua.es (A.Sepúlveda-Escribano).pyrolysis of a carbon precursor and the other one is based on the modification of the existing porous structure by means of carbon vapor deposition technique(CVD)[24,25].The last one is particu-larly considered to be an appropriate technique,and it has received considerable attention in the last few years.The CVD process leads to activated carbons with a tailored porosity if the reduction of the pore mouth is controlled.In practice,commercial microporous CMS are mainly produced by controlled deposition of pyrolytic car-bon at the pore mouth.Thefinal porous structure is defined by the nature of the precursor and the pyrolysis conditions applied.It is worth mentioning that CMS,compared to conventional zeolites, have some advantages such as higher hydrophobicity,higher resis-tance to both alkaline and acid media,thermal stability under inert atmosphere at higher temperatures,and higher selectivity towards planer molecules.Within the wide range of industrial applications of CMS,typical examples are:separation/purification of binary gas mixtures,for instance,separation of linear and branched hydrocar-bons,removal of CO2from gas/air steams,separation of N2and O2 from air,and so on.[17,18,20,26–31].In this sense,the aim of the present work is to analyze the por-ous structure of commercial carbon molecular sieves recently developed by Supelco ing a combination of N2and CO2 adsorption at77and273K,respectively,together with immersion calorimetry measurements into liquids of different molecular dimensions.Additionally,the adsorption capacity of CO2at atmo-spheric pressure and different temperatures(273,298and323K) will be analyzed.The effect of temperature on CO2adsorption capacity will be studied and correlated with the porous structure of the different CMS.The presence of a well-defined porous struc-ture(pore mouth opening)will allow determining the optimum size required for CO2adsorption.This correlation will allow per-forming a relative simulation of the real conditions of pressure and temperature of the typical CO2released from industrial chimneys.2.ExperimentalCarbon molecular sieves were prepared from polymeric precur-sors.The selected CMS cover different pore size distributions,and all of them are commercially available from Supelco.Preparation conditions and particle size distribution,for some CMS,were de-tailed elsewhere[32].Several techniques have been used in order to analyze the porous structure of these CMS.Adsorption isotherms of N2at77K and CO2 at273K were carried out using a fully automated manometric equipment,designed and constructed by the Advanced Materials group(LMA),now commercialized as N2Gsorb-6[33].Before the adsorption experiments,samples were degassed at423K during 4h under vacuum(10À7bar).The‘‘apparent’’surface area was obtained applying the BET method in the relative pressure range p/p0=0.001–0.1.The total micropore volume(V0)was deduced from the N2adsorption data using the Dubinin–Radushkevich(DR)equa-tion,whereas the mesoporous volume(V meso)was obtained as the difference between the total pore volume(V t),corresponding to the amount adsorbed at p/p0%0.95,and V0.The pore volume corre-sponding to the narrow microporosity(V n)was obtained by apply-ing the D-R equation to the CO2adsorption data at273K[34].Immersion calorimetry measurements into liquids of different molecular dimensions(dichloromethane,0.33nm;benzene, 0.37nm;cyclohexane,0.48nm;2,2-dimethylbutane,0.56nm and a-pinene,0.7nm)were carried out in a Setaram Tian-Calvet C80D calorimeter at303K.A complete description of the experi-mental setup can be found elsewhere[35].Briefly,prior to the experiment the samples were outgassed at423K for4h in a glass tube connected to vacuum equipment.After completing the heat treatment,the bulb containing the sample was sealed in vacuum and then introduced into the calorimetric cell containing the immersion liquid.Once thermal equilibrium was reached,the tip of the glass bulb was broken and the wetting liquid was allowed to contact the sample.The heat evolution resulting from the inter-action between the liquid and the clean surface was registered as a function of time.The integration of the signal,after making the appropriate corrections(those arising from the breaking of the tip(exothermic)and from the evaporation of the immersion liquid tofill the void volume of the bulb with the vapor at the corre-sponding vapor pressure(endothermic)),provides the total immer-sion enthalpy(ÀD H imm).Both mentioned corrections were previously calibrated using empty glass bulbs with different vol-umes.Experimental errors related to the measurement of immer-sion enthalpies are below3–4%.The total area accessible to the wetting liquid was estimated from the immersion enthalpy(J/g) of the CMS by using a nonporous graphitized carbon black(V3G; S BET:62m2/g)as a reference.The CO2adsorption isotherms on the different CMS were per-formed on the manometric equipment previously described,at atmospheric pressure and temperatures of273,298and323K. Before the adsorption experiment,samples were degassed at 423K for4h under vacuum(10À7bar).3.Results and discussion3.1.N2and CO2adsorption isothermsFig.1shows the N2adsorption–desorption isotherms for the dif-ferent CMS.Additionally,Table1collects the‘‘apparent’’BET surface area(S BET),the total micropore volume(V0),the total pore volume (V t),and the mesopore volume(V meso),obtained from the N2adsorp-tion data at77K,together with the volume corresponding to the narrow micropores(V n),obtained from the CO2adsorption iso-therms at273K[34].As it can be observed in Fig.1,the N2adsorp-tion isotherms are quite different among the different samples, showing that these CMS samples exhibit completely different tex-tural properties depending on both the polymer precursor and the synthesis conditions applied.There are:(i)pure microporous CMS (carbons C-1012,C-1018,C-1021,C-G60and C-SIII)exhibiting a type I isotherm,characteristic of typical microporous carbons;(ii) a pure mesoporous sample(carbon C-1016),with the amount ad-sorbed sharply increasing above a relative pressure of0.8,due to the presence of large sized mesopores and(iii)three carbons (C-569,C-1000and C-1003)with molecular sieving properties at micropore and mesopore scale,the later producing a sharp increase in the amount adsorbed at high relative pressures(above p/p0%0.8).A rigorous inspection of the different adsorption isotherms al-lows a more detailed description of the porous structure of these carbons.In this sense,although sample C-1012presents a wide plateau at high relative pressure range,characteristic of strictly microporous adsorbents,the wide knee of the N2isotherm at low relative pressures(below p/p0%0.2)indicates the presence of a wide micropore size distribution.Thisfinding is also confirmed by comparing the large difference between the volume of narrow micropores(V n),deduced from the CO2adsorption data,and the volume of total micropores(V0),deduced from the N2adsorption data.It is noteworthy to mention that in the absence of kinetic restrictions the comparison of these two values(V0and V n)pro-vides a good evaluation toward the micropore size distribution. In fact,these two values are very similar for carbons exhibiting a narrow and homogeneous microporosity,while they become dif-ferent(V0>V n)with the widening of microporosity[34].Samples C-1018,C-1021,C-G60and C-SIII also exhibit type I isotherms.However,the porous structure of samples C-1018andA.Wahby et al./Microporous and Mesoporous Materials164(2012)280–287281C-1021is more complex.Both samples show a small type H2hys-teresis loop in the relative pressure (p/p 0)range from 0.4to 0.8,that reflects an additional contribution of a certain proportion of mesopores.The comparison of the adsorption data from these two samples highlights the difference between the volume of nar-row micropores and the total microporosity,despite the clear sim-ilarity observed in the development of porosity.In fact,(V 0ÀV n )is greater in the case of C-1018compared to C-1012,implying a larger portion of wide micropores in the former carbon.Sample C-G60exhibits a flat isotherm profile at high relative pressures,as in the case of carbon C-1012.Although the knee in the adsorp-tion isotherm is narrower at relative pressures below 0.2,carbon C-G60exhibits a wide pore size distribution with wider micropores (V 0>V n ).Sample C-SIII also shows a flat profile at high relative pressures.However,the narrower knee at low relative pressures (p/p 0<0.1)denotes the presence of a narrow microporosity,with a pore size distribution even narrower and more homogenous,since the values of V 0and V n are rather similar.As described above,samples C-1000and C-1003show,in addi-tion to the high N 2adsorption capacity at low relative pressures,a high adsorption at relative pressures above 0.8.A similar situation is observed for carbons C-569and C-1016,despite the absence of a high N 2adsorption at p/p 0<0.1.This behavior can be attributed,in the case of sample C-1016,to the nature of the material,since it is a non-microporous graphitized polymeric carbon material.In the case of sample C-569,the presence of a highly narrow and homog-enous microporosity can clearly be observed.In all four cases,the high N 2adsorption capacity is accompanied by a type H3–H1hysteresis loop on carbons C-1000,C-1003and C-1016,and by a type H2hysteresis loop on sample C-569.In principle,the high adsorption capacity together with the hysteresis loop reflects the presence of mesopore volume ranging from V meso =0.2to 0.6cm 3/g (Table 1).The ‘‘apparent’’surface area of the synthesized CMS ranges from 77m 2/g,in the case of nonporous sample C-1016,up to 2000m 2/g on sample C-1012.In summary,textural characterization results obtained from gas adsorption measurements show that the carbon molecular sieves prepared from polymeric precursors cover a wide range of pore sizes,depending on both the nature of the polymer precursor and the synthesis conditions used.CMS studied range from purely microporous materials to CMS that combine a well-developed microporosity together with a secondary porosity in the large micropores -small mesopores range.It is clear that some of them should not be structurally considered as proper molecular sieves.3.2.Immersion calorimetry measurementsThe heat of immersion of certain porous solids into liquids can be used to evaluate the porous structure,as well as the surface chemistry of the material [35–37].In the absence of specific inter-actions at the solid–liquid interface,the heat of immersion can be considered as an indirect measurement of the surface area accessi-ble to a certain molecule.Consequently,the selection of the appro-priate liquid in terms of molecular dimensions can be used to evaluate the surface area accessible to each molecule,that is,the experimental micropore size distribution.Fig.2shows the enthalpyTable 1Textural characteristics of the different carbon molecular sieves deduced from the N 2and CO 2adsorption isotherms at 77and 273K,respectively.aSample S BET (m 2/g)V 0(cm 3/g)V meso (cm 3/g)V t (cm 3/g)V n (cm 3/g)V 0ÀV n C-1016770.060.500.560.010.05C-5695480.220.200.420.200.02C-10216950.280.070.350.240.04C-10187570.300.060.360.230.07C-SIII 9920.400.000.400.330.07C-100010100.400.440.840.300.10C-G6011470.450.000.450.360.09C-100312600.480.59 1.080.340.14C-101220000.730.110.840.460.27aS BET :‘‘Apparent’’surface area calculated using the BET method;V 0:Micropore volume calculated by applying the DR equation to the N 2adsorption data at 77K;V t :Total pore volume obtained from the amount of N 2adsorbed at p/p0%0.95;V meso :Mesopore volume obtained by subtracting V t from V 0;V n :Volume of narrow micropores calculated by applying the DR equation to the CO 2adsorption data.282 A.Wahby et al./Microporous and Mesoporous Materials 164(2012)280–287of immersion(J/g)for the different CMSs into various liquids,cov-ering a wide range of kinetic diameters,from0.33nm(dichloro-methane)up to0.7nm(a-pinene).Carbon C-1012exhibits the highest enthalpy of immersion for all liquids studied,in agreement with the large surface area available on this sample.Nevertheless, the presence of similar values of immersion enthalpy indepen-dently of the size of the probe molecule clearly reflects the absence of important molecular sieving effects for the liquids used,up to 0.70nm,i.e.a wide micropore size distribution.For carbons C-1003,C-1000and C-G60there is a continuous but relatively small decrease in the enthalpy of immersion when increasing the molec-ular size of the probe molecule.The relatively high enthalpy of immersion observed for a large molecule such as a-pinene on these samples reflects the absence of significant restrictions for mole-cules below0.7nm.By contrast,samples C-SIII,C-1018,C-1021 and C-569present a large heat of immersion into DCM(0.33nm) and benzene(0.37nm)that sharply decreases,thus indicating the inaccessibility of the inner porosity to molecules of a similar dimen-sion to cyclohexane(0.48nm)and2,2-DMB(0.56nm).N2and CO2 adsorption measurements described above showed that carbon molecular sieves C-569and C-SIII exhibit a narrow pore size distri-bution,since the volume of narrow micropores,deduced from the CO2adsorption data,was quite similar to the total volume of micropores,deduced from the N2adsorption[34].This observation is clearly confirmed by calorimetric measurements.Carbons C-1018and C-1021have a slightly wider micropore size distribu-tion as deduced from the slightly larger difference between V n and V0,and the higher enthalpy of immersion for cyclohexane. These results suggest that carbons C-569,C-SIII,C-1021and C-1018are microporous carbon molecular sieves with a narrow pore mouth(pore diameter60.48nm for thefirst two and 60.56nm for the other two).Finally,sample C-1016exhibits a low enthalpy of immersion($7J/g)independently of the immer-sion liquid.This behavior is explained based on the textural charac-terization results which showed a low‘‘apparent’’surface area,in close agreement with the available surface areas obtained from immersion calorimetry(Table2).3.3.CO2adsorption at atmospheric pressureThe CO2adsorption,separation and/or storage on carbon materials by means of physical/chemical adsorption or combina-tion of both processes have created great expectations because of the promising results reported in the literature[38–41].As mentioned above,the nature of the precursor and the preparation conditions,more specifically,post-synthesis treatments as well as the pore structure(micropore volume,total surface area,pore size/shape,etc.)are key parameters defining the total adsorption capacity.In order to evaluate the potential performance of CMS on this issue,CO2adsorption isotherms at different temperatures (273,298and323K)were carried out at atmospheric pressure (<1bar).The profile of the CO2adsorption isotherms at273K is rather similar for all CMSs(Fig.3a),except in the case of sample C-1016 for which the adsorption capacity is practically nil over the whole pressure range.This observation anticipates that CO2adsorption requires the presence of micropores,since carbon C-1016does not adsorb CO2even at low temperatures.Taking a closer look at the other CMS,there is a clear increase in the amount of CO2ad-sorbed with the development of porosity,up to a maximum on sample C-1012,with a total amount adsorbed of232mg/g,i.e.23.3wt.%(Table3).The amount of CO2adsorbed at273K for these CMSs(except for sample C-1016)ranges from153mg/g(C-569)to 232mg/g(C-1012).Table2Total surface area available for dichloromethane(0.33nm),benzene(0.37nm),cyclohexane(0.48nm),2,2-dimethyl-butane(0.56nm)and a-pinene(0.7nm)obtained from immersion calorimetry measurements at303K for the different CMS.BET surface area is included for the sake of comparison.Sample S BET(m2/g)S DCM(m2/g)S BZ(m2/g)S cyclohexane(m2/g)S2,2DMB(m2/g)S a-pinene(m2/g)C-1016776471705649C-5695487266661058576C-10216958367282279554C-101875791987448212965C-SIII99211501143762824C-10001010118010921108907844 C-G60114715271264114581159C-100312601265129912871030884 C-1012200016761678163414571584A.Wahby et al./Microporous and Mesoporous Materials164(2012)280–287283The profile of the CO2adsorption at298K is rather similar among the different CMS,at least at low relative pressures,the dif-ferentiation among samples being clearer close to atmospheric pressure(Fig.3b).In addition,the results presented in Table3 show that the total CO2adsorption capacity ranges from100mg/ g on sample C-569up to a maximum of164mg/g,in the case of the C-G60carbon.Finally,the CO2adsorption isotherms at323K maintain the observed similarity concerning the adsorption pro-files for all CMS at273and298K(Fig.3c).To better understand the role of the porous structure in the CO2 adsorption behavior of CMS at the three studied temperatures,the total amount adsorbed at atmospheric pressure was correlated with the different textural parameters obtained from the N2 adsorption measurements at77K(BET surface area,the total284 A.Wahby et al./Microporous and Mesoporous Materials164(2012)280–287volume of pores,V t )and CO 2at 273K (i.e.the total volume of nar-row micropores,V n ).Fig.4a shows that the amount of CO 2ad-sorbed is practically independent of the total volume of pores.However,Fig.4b shows that there is a somewhat better relation-ship between the CO 2adsorption and the BET surface area.Since no correlation was found with the total pore volume one has to as-sume that there should be a specific pore size which is the key fac-tor defining the total adsorption capacity on the studied materials.In this sense,Fig.4c shows the correlation between the adsorbed amount of CO 2and the total volume of narrow micropores,ob-tained by applying the DR equation to the CO 2adsorption data at 273K.In this case,a better correlation can be clearly observed,thus confirming the importance of a specific porosity for CO 2adsorption/capture [42,43].On the basis of the textural character-ization results described above,it is clear that CO 2adsorption at atmospheric pressure and different temperatures requires the presence of a high volume of narrow micropores together with a well-developed ‘‘apparent’’surface area.In this sense,carbon C-1012exhibits the highest adsorption capacity (232mg/g)at 273K among all CMS studied.This sample,with a wider pore size distribution (V 0ÀV n =0.27),exhibits the highest BET surface area (2000m 2/g)and the maximum micropore volume (0.73cm 3/g)as well as the maximum volume of narrow micropores (0.46cm 3/g)already suggested as primarily responsible for the observed up-take.Despite these excellent properties,sample C-1012exhibits a slightly lower CO 2uptake than expected from the extrapolation of the other samples (Fig.4c).This finding must be related to the wide micropore size distribution of carbon C-1012(Fig.2);this means that although the volume of narrow micropores is high in this carbon,not all narrow micropores (the widest ones)are effec-tive for an optimum adsorption capacity;a comparison of samples C-1012and C-SIII reflects a similar adsorption capacity in spite of the larger textural parameters for the former sample.The presence of a narrow micropore size distribution,i.e.narrow micropores below 0.48nm (see Fig.2)clearly confirms the necessity of a well-developed specific porosity below 0.5nm.In these narrow micropores,the overlapping potential allows a better packing of the CO 2molecules giving rise to a larger adsorption capacity.Carbons C-G60,C-SIII and C-1003exhibit quite similar CO 2adsorp-tion capacities (around 220mg/g)at 273K,since these samples possess a very similar volume of narrow micropores (around 0.35cm 3/g).In summary,the total amount of CO 2adsorbed at 273K increases with increasing volume of narrow micropores,thus confirming the observed correlations.Excluding sample C-1016,the calculated CO 2densities for these CMSs (Table 4),considering only the narrow micropore volume,range from 0.77g/cm 3for samples with a narrow pore size distri-bution (e.g.C-569),to an average value of 0.50g/cm 3in the case of samples with a wider pore size distribution (e.g.C-1012).The high-est density of CO 2adsorbed is presented by sample C-569,with theTable 3Total amount of CO 2adsorbed at 1bar and different temperatures (273,298and 323K)for the different carbon molecular sieves.Amount of CO 2adsorbed (mg/g)Sample/Temperature 273K 298K 323K C-101223213279.3C-102116410772.6C-100321812583.8C-56915310068.3C-SIII 22214595.2C-10167.5 4.08 3.37C-G60224164109C-100017712378.1C-101815711780.2Table 4Average CO 2density on narrow micropores for the different carbon molecular sieves at 273K and 1bar.Sample CO 2density (g/cm 3)C-10120.5043C-10210.6833C-10030.6412C-5690.7650C-SIII 0.6727C-1016-C-G600.6222C-10000.5900C-10180.6826A.Wahby et al./Microporous and Mesoporous Materials 164(2012)280–287285narrowest micropore size distribution(V0ÀV n=0.02).However, this sample exhibits the lowest CO2adsorption capacity for all studied CMS because of low V n and S BET values.This observation must be attributed to the presence of a certain mesoporosity,not contributing to the adsorption of CO2,together with the presence of a poor-developed narrow microporosity.Consequently,in order to reach a high amount of adsorbed CO2(mg/g),the presence of a high volume of narrow micropores,together with a high adsorp-tion density(g/cm3),and a narrow pore size distribution seem mandatory requirements.To confirm thisfinding,the isosteric heat of CO2adsorption(Q)was calculated for the different CMSs as a function of the surface specific coverage n x and at the different temperatures,by applying the Clausius–Clapeyron equation[44].Fig.5shows that the isosteric heat of adsorption remains con-stant or slightly increases with coverage on most carbons,the in-crease being larger for samples C-1018,C-569and C-1021. Carbons C-569and C-SIII exhibit the maximum values of Q,which practically remain constant on the latter($25.4kJ/mol).Excluding sample C-1016(for which the isosteric heat of adsorption de-creases from9to7.7kJ/mol when the surface coverage increases), the increase in isosteric heat with increasing surface coverage can be explained by the presence of intermolecular interactions be-tween the adsorbed CO2species.By contrast,sample C-1016, which is non-microporous,exhibits a very limited CO2adsorption capacity that implies a lower value of Q.The decrease in isosteric heat when increasing surface coverage suggests the energetic het-erogeneity of the adosorption sites(the mesoporous size distribu-tion).Table5shows the values of isosteric heat of adsorption at zero coverage for all studied carbonsðq0stÞ;excluding the heat gen-erated by interactions between CO2adsorbed molecules.The value of q0stranges from10kJ/mol on the non-microporous carbon (C-1016)to25kJ/mol in the case of microporous CMSs with a nar-row pore size distribution(e.g.C-569and C-SIII).The high value of the isosteric heat of adsorption at zero coverage,indicates the pres-ence of strong interactions between CO2adsorbed molecules and the walls of the narrow micropore.In general,CMSs with a high volume of narrow micropores,together with a narrow pore size distribution,exhibit a high adsorption capacity at the three studied temperatures,as well as a high density of CO2adsorbed in the nar-row micropores(e.g.C-SIII).In summary,the analysis of a series of commercial carbon molecular sieves indicates that a narrow micropore size distribu-tion,a pore entrance below0.48nm and,indirectly,a maximum density of CO2adsorbed,are the necessary conditions for an opti-mal adsorption capacity[40].At the three studied temperatures, samples with a high volume of narrow micropores exhibit higher amounts of CO2adsorbed.These narrow pores are postulated to be the key factor of the CO2adsorption process.On the other hand, the densities calculated for the different CMS of the adsorbed CO2, at atmospheric pressure,strengthen the need for a narrow pore size distribution.This is confirmed by the isosteric heat of adsorp-tion calculated,for all samples at zero coverage.4.ConclusionsA series of commercial carbon molecular sieves(CMS)prepared from different polymeric precursors have been characterized by means of adsorption of N2at77K and CO2at273K,together with measurements of immersion calorimetry into liquids of different molecular dimensions.Experimental results show that these CMSs cover a wide range of porosity,from purely microporous carbons to samples containing wide micropores together with a certain proportion of mesoporosity.CO2adsorption studies on these well-characterized CMS,at atmospheric pressure(1bar)and three different temperatures(273,298and323K)confirm that a high CO2adsorption capacity requires the presence of a well-developed microporosity,as well as a high volume of narrow micropores. Additionally,the narrow micropores seem to be the key factor, leading to a maximum capacity of CO2adsorption,even when per-forming the adsorption at a temperature similar to that of anthro-pogenic emissions of CO2.AcknowledgementsAuthors acknowledgefinancial support from Generalitat Valen-ciana(PROMETEO/2009/002-FEDER).References[1]S.A.Levin,Ecology73(1992)1943.[2]J.M.Melillo,A.D.Mcguire,D.W.Kicklighter,B.Moore,C.J.Vorosmarty,A.L.Schloss,Nature363(1993)234.[3]D.S.Schimel,Glob.Change Biol.1(1995)77.[4]J.Paul,C.-M.Pradier(Eds.),Carbon Dioxide Chemistry:Environmental Issues,Royal Society of Chemistry,Cambridge,UK,1994.p.405.[5]M.M.Halmann,M.Steinberg,Greenhouse Gas Carbon Dioxide Mitigation:Science and Technology,Lewis Publishers,Boca Raton,FL,1999.p.568. [6]M.M.Maroto-Valer, C.S.Song,Y.Soong,Environmental Challenges andGreenhouse Gas Control for Fossil Fuel Utilization in the21st Century, Kluwer Academic/Plenum Publishers,New York,2002.p.447.[7]DOE/NETL,Carbon Sequestration.Technology Roadmap and Program Plan Department of Energy,National Energy Technology Laboratory,May 2005.[8]D.Aaron,C.Tsouris,Sep.Purif.Rev.40(2005)321.[9]S.Choi,J.H.Drese,C.W.Jones,Chem.Sus.Chem.2(2009)796.[10]P.V.Danckwerts,Chem.Eng.Sci.34(1979)443.[11]P.V.Danckwerts,M.M.Sharma,Trans.Inst.Chem.Eng.44(1966)244.[12]K.T.Chue,J.N.Kim,Y.J.Yoo,S.H.Cho,R.T.Yang,Ind.Eng.Chem.Res.34(1995)591.Table5Isosteric heat of adsorption at zero loading(kJ/mol)for thedifferent CMS.Sample q0st(kJ/mol)C-101218.792C-102115.215C-100317.552C-56924.285C-SIII25.176C-10169.9421C-G6023.036C-100022.324C-101821.415286 A.Wahby et al./Microporous and Mesoporous Materials164(2012)280–287。

相关主题
  1. 1、下载文档前请自行甄别文档内容的完整性,平台不提供额外的编辑、内容补充、找答案等附加服务。
  2. 2、"仅部分预览"的文档,不可在线预览部分如存在完整性等问题,可反馈申请退款(可完整预览的文档不适用该条件!)。
  3. 3、如文档侵犯您的权益,请联系客服反馈,我们会尽快为您处理(人工客服工作时间:9:00-18:30)。

Adsorptive removal of Pb2+,Co2+and Ni2+by hydroxyapatite/chitosan composite from aqueous solutionNeha Gupta,Atul K.Kushwaha,M.C.Chattopadhyaya*Environmental Chemistry Research Laboratory,Department of Chemistry,University of Allahabad,Allahabad,(U.P.)211002,India1.IntroductionWater pollution by heavy metals through the discharge ofindustrial effluents,is a worldwide environmental problem.Studies have proved that the metals such as copper,lead,zinc,cobalt,nickel,chromium and mercury are considered to be toxic.Cobalt containing compound are widely used in many industrialapplications such as mining,metallurgical,paints,pigments andelectronics[1].Small amount of cobalt is essential for humanhealth because it is a part of vitamin B12.However,higherconcentration of cobalt may cause paralysis,diarrhoea,low bloodpressure,lung irritation and bone defects.Nickel is being widelyused in electroplating industries.It is also used in fertilizers.Exposure to nickel can cause dermatitis and allergic sensitization.Inhalation of Ni can cause respiratory cancer[2].Lead compound iswidely used in painting,plastics and batteries.At low concentra-tion lead can adversely affect the brain,the central nervous system,blood cells,and kidneys[3].Therefore,removal methods of heavy metals from wastewaterhave been investigated considerably for past several years.Anumber of physical and chemical processes exists which includeprecipitation,solvent extraction,membrane processes,filtration,ion-exchange and adsorption.Among them,adsorption is anefficient and economical process.The efficiency of techniquedepends on the nature of adsorbent.The adsorbent such asactivated carbon[4],clay[5],activated alumina[6],chitosan[7],silica[8],zeolite[9]and hydroxyapatite[10]were used for heavymetal removal.Hydroxyapatite Ca10(PO4)6(OH)2(HAp)is a main mineralconstituent of teeth,bones and phosphate mineral rocks.Itbelongs to apatite mineral family.HAp was shown to be efficientfor the removal of many toxic metal ions such as lead,cobalt,nickel,copper,zinc,cadmium and uranium in aqueous solutions[11–16].However,characteristic of HAp existing in the formof white powder therefore isolating the suspendedfine solidsfrom aqueous solutions after adsorption of metal ions is noteasy[17].Therefore,it is needed to bind HAp with polymer to solve thisproblem.There are several polymers available in nature which canbe use as binding material for HAp.In the present study we havesynthesized hydroxyapatite–chitosan(HApC)composite by precip-itation method and its application was explored as an adsorbent forthe removal of heavy metals such as lead,cobalt and nickel fromaqueous solution.The reason behind choosing chitosan as a bindingmaterial for HAp is its high abundance in nature and specialcharacteristics such as hydrophilicity,biocompatibility,biodegrad-ability,non-toxicity,adsorption properties,etc.The presence ofamino and hydroxyl groups in chitosan can serve as the active sitesfor adsorption.Journal of the Taiwan Institute of Chemical Engineers43(2012)125–131A R T I C L E I N F OArticle history:Received6March2011Received in revised form12July2011Accepted31July2011Available online17October2011Keywords:AdsorptionCobaltNickelLeadIsothermKineticsHydroxyapatite/chitosan compositeA B S T R A C TIn the present work hydroxyapatite/chitosan(HApC)composite was synthesized by precipitationmethod and was characterized by Fourier transform infrared(FT-IR)spectroscopy,X-ray diffraction(XRD)crystallography and scanning electron microscopy(SEM).The HApC composite was tested for theadsorption of lead,cobalt and nickel from aqueous solution and compared its removal capacity withhydroxyapatite(HAp).Effect of various physico-chemical parameters such as pH,adsorbent dose,contacttime,initial metal ion concentration and temperature on adsorption of metal ions onto HApC compositewas investigated.The adsorption process followed pseudo-second order kinetics and intra-particlediffusion model.Equilibrium data werefitted well in the Langmuir and Freundlich isotherm models.Thenegative values of Gibb’s free energy change(D G8)showed that the adsorption process was feasible andspontaneous in nature.The positive values of enthalpy change(D H8)indicated that the process wasendothermic.The positive values of entropy change(D S8)showed increased randomness at the solid/solution interface.ß2011Taiwan Institute of Chemical Engineers.Published by Elsevier B.V.All rights reserved.*Corresponding author.Tel.:+915322462393;fax:+915322541786.E-mail addresses:neha.evs07@(N.Gupta),atulkk2008@(A.K.Kushwaha),mcc46@(M.C.Chattopadhyaya).Contents lists available at ScienceDirectJournal of the Taiwan Institute of Chemical Engineersj ou r n a l h o m e p a g e:w w w.e l s e v i e r.co m/l o c a t e/j t i c e1876-1070/$–see front matterß2011Taiwan Institute of Chemical Engineers.Published by Elsevier B.V.All rights reserved.doi:10.1016/j.jtice.2011.07.0092.Materials and methods2.1.Synthesis of hydroxyapatite–chitosan compositeChitosan(75–85%deacetylated)was supplied by Sigma Aldrich,India.(NH4)2HPO4and Ca(NO3)2Á4H2O were obtained from Merck and was used without further purification.The HAp was synthesized by mixing the solution of Ca(NO3)2Á4H2O and (NH4)2HPO4with stoichiometric ratio of Ca/P(1.67).The pH value during mixing was maintained10–11with ammonia solution.The precipitate formed was rinsed with double distilled water to bring the pH level to7and was dried at808C for24h [18].HApC composite was also synthesized by precipitation method.Chitosan(5wt%)was dissolved in1%acetic acid and added to the mixture of diammonium hydrogen phosphate and calcium nitrate.The precipitate formed was rinsed with double distilled water to bring the pH level to7and was dried at808C for24h.2.2.Characterization of materialsFTIR study was carried out on FTLA2000spectrophotometer to analyze functional groups,using potassium bromide(KBr) disk method and the morphology of adsorbents was investigated by FEI Quanta200scanning electron microscope operated at 20kV accelerated voltage.XRD was performed on X’Pert-Pro, PANalytical diffractometer operated at30kV/30mA,to deter-mine crystallinity of the material using CuK a1radiation with wavelength of1.54A˚in the wide angle region from108to508on 2u scale.2.3.Adsorption experimentsStock solution(1000mg/L)of each metal ion was prepared by dissolving required amount of nitrate salt of metal ion(Pb(NO3)2, Co(NO3)2Á6H2O and Ni(NO3)2Á6H2O obtained from Merck)into double distilled water.The experimental solution of desired concentration was prepared by successive dilution of stock solution.In order to determine the effect of physicochemical parameters such as pH,adsorbent dose,contact time,initial metal ion concentration of solution and temperature.The adsorption experiments were performed by batch equilibrium method.The experiments were carried out in150ml of conical flasks by mixing a pre-weighed amount of adsorbent with50ml of metal ion solution.Initial pH of solutions was adjusted by 0.1M NaOH or0.1M HNO3.All experiments were performed at room temperature and kept for stirring for given period of time. Thereafter the mixture was centrifuged(Remi Research centri-fuge)and the initial andfinal metal ion concentrations were determined by Atomic Absorption Spectrophotometer(ECIL-4141).The%removal of metal ion and amount of metal ion adsorbed on HApC composite(q e)was calculated by Eqs.(1)and (2),respectively:removalð%Þ¼100C0ÀC eC0(1)q e¼ðC0ÀC eÞVM(2)where q e is the amount of metal ion adsorbed on adsorbent at equilibrium(mg/g),C0and C e are the initial and equilibrium concentration(mg/L)of metal ion in solution respectively,V is the volume of solution(L)and M is the mass of adsorbent(g).All adsorption experiments were performed in triplicate and the mean values were used in data analysis.3.Results and discussion3.1.Characterization of materialsThe IR spectra of HAp(a),Chitosan(b)and HApC(c)were recorded in the region of4000–500cmÀ1and are shown in Fig.1. The spectra of HAp showed a broad band at1113cmÀ1due to asymmetric stretching of PO43Àand corresponding symmetric stretching was observed at825cmÀ1.The absorption band at 1398cmÀ1suggested the presence of CO32À[19],which was supposed to have come from atmosphere during the precipitation process.The broad band at3500to3200cmÀ1and1636cmÀ1was due to stretching and bending of O–H groups,respectively,present in HAp[20].The FT-IR spectra of HApC showed a band at 1032cmÀ1which was due to stretching vibration of C–O–C group of chitosan confirms formation of composite.The peak of PO43Àgroup shifted from1113to1092cmÀ1due to interaction with chitosan.The stretching and bending vibration mode of–NH group of chitosan occurred at3452and1627cmÀ1,respectively which was overlapped with the bands of O–H groups in HApC composite.XRD spectra of HApC composite(a),HAp(b)and Chitosan(c)are presented in Fig.2.The crystalline peaks of HAp at2u=268,31.98, 33.18,34.28and39.98are also found in HApC composite with very small shifting in2u.This may be due to binding of HAp with chitosan.This indicated that there was no marked change in the peak structure after the composite formation and confirmed that the crystal structure of HAp is retained in HApC composite[21]. Fig.3shows the morphology of HAp(a)and HApC composite(b). The HAp powder exhibited as particles but in case of HApC composite aggregates appeared andfilm of chitosan over HAp, confirmed the formation of HApC composite.3.2.Effect of pHTo study the effect of pH on adsorption,experiments were carried out in the pH range2–5.5for Pb2+and2–6for Co2+and Ni2+.Fig.4 shows that the removal of metal ions was increased with increasing initial pH of metal ion solution and maximum value was reached at pH5.5for Pb2+and6.0for Co2+and Ni2+.The pH above5.5for Pb2+and 6for Co2+and Ni2+was not used in order to avoid the precipitation of metal ions in the form of their hydroxides[22].At lower pH, adsorption of metal ions decreased due to increased competition with H+ions for active adsorption sites.However,at higher pH values,TransmittanceWavenu mber (cm-1)Fig.1.Infrared spectra of HAp(a),chitosan(b)and HApC composite(c).N.Gupta et al./Journal of the Taiwan Institute of Chemical Engineers43(2012)125–131 126presence of H+ion in solution decreased and adsorbent surface also deprotonated,make increased adsorption of metal ions.3.3.Effect of adsorbent doseFig.5shows that the adsorption of metal ions increased from78 to93.5%,71to86%and64to77%for Pb2+,Co2+and Ni2+,respectively, as HApC dose increased from1to3g/L.This is because at higher dose of adsorbent,due to increased surface area,more adsorption sites are available causing higher removal of Pb2+,Co2+and Ni2+.Further increase in adsorbent dose,did not cause any significant increase in% removal of metal ion.This was due to the concentration of metal ions reached at equilibrium status between solid and solution phase.3.4.Effect of contact timeInfluence of contact time on adsorption of Pb2+,Co2+and Ni2+on HApC was investigated in the range of5–60min for the initial concentration of10mg/L for each metal ion(Fig.6).Maximum rate of removal occurred within5min of contact time thereafter removal rate became slow and after30min of contact time no change was observed for Pb2+(93.5%)which established that the system has reached the equilibrium point.For Co2+(88.72%)and Ni2+(80%),the equilibrium point was found to be40min.3.5.Effect of equilibrium metal ion concentrationThe effect of different concentration of Pb2+,Co2+and Ni2+on the adsorption has been investigated at303K,Pb2+,Co2+and Ni2+ adsorption capacities of HApC were given as a function of equilibrium concentration in Fig.7.It was clear that Pb2+,Co2+ and Ni2+adsorption capacities of HApC increased with increase of equilibrium concentration.The Increase in adsorption capacity with increase in equilibrium metal ion concentration for different metal ions was in the order Pb2+>Co2+>Ni2+.3.6.Kinetics of adsorptionSeveral kinetic models have been proposed to clarify the mechanism of a solute adsorption from aqueous solution onto an adsorbent.The rate constant of adsorption was determined from the pseudo-first order rate expression Eq.(3)[23]:dq t¼k1ðq eÀq tÞ(3)where q t and q e are the amount of metal ions adsorbed at time t (mg/g)and at equilibrium(mg/g),respectively and k1is the pseudo-first order rate constant(minÀ1).Integrating theaboveFig.3.SEM micrograph of HAp(a)and HApC composite(b).Fig.4.Effect of pH on adsorption of Pb2+,Co2+and Ni2+on HApC composite.1020304050cbaIntensity(a.u.)2 Th eta (degr ee)Fig.2.XRD spectra of HApC composite(a),HAp(b)and chitosan(c).N.Gupta et al./Journal of the Taiwan Institute of Chemical Engineers43(2012)125–131127equation using the boundary condition,q t =0at t =0leads to:ln ðq e Àq t Þ¼ln q e Àk 1t(4)The values of k 1and q e were calculated from the slopes and intercepts of the linear plots of ln (q e Àq t )vs.t (Fig.8)and are presented in Table 1.As shown in Table 1the values of regression correlation coefficients (R 2)were not close to unity and a large difference in the values of q e,cal and q e,exp for the adsorption of Pb 2+,Co 2+and Ni 2+onto HApC composite revealed that the pseudo-first order kinetic model was not suitable to describe the kinetic profile of the adsorption.The pseudo-second order kinetic model is presented as [24]:dq tdt¼k 2ðq e Àq t Þ2(5)where q t and q e are the amount of metal ions adsorbed at time t (mg/g)and at equilibrium (mg/g)respectively and k 2is the pseudo-second order rate constant (g/mg/min).Integrating the above equation using the boundary condition,q t =0at t =0leads to:t t ¼12eþt e (6)The values of k 2and q e were calculated from the intercepts and slopes of the linear plots of t /q t vs.t (Fig.9),respectively and are presented in Table 1.Results showed that the calculated q e values were very close to that of experimentally obtained q e and the values of correlation coefficients (R 2)were closer to unity confirmed that the adsorption of Pb 2+,Co 2+and Ni 2+on HApC composite followed pseudo-second order kinetics.Adsorption is multistep process involving the transfer of solute from bulk of solution to surface of adsorbent.Intra-particle diffusion plays an important role in the extent of adsorption and can be expressed as [25]:q t ¼k i t 0:5þI(7)where q t is the amount of metal ion adsorbed at time t (mg/g)and k iis intra-particle diffusion rate constant (mg/g/min 0.5).The values of I give an idea about the thickness of boundary layer.The values of k i and I were obtained from the slopes (k i )and intercepts (I )of the plots of q t vs.t 0.5(Fig.10),respectively and are presented in Table 1.Results showed that the diffusion rate of12345678q e (m g /g )C e (mg/L)Fig.7.Effect of equilibrium metal ion concentration on adsorption of Pb 2+,Co 2+and Ni 2+on HApC composite.-5-4-3-2-11l n (q e -q t )t (min )Fig.8.Pseudo-first order kinetic model for adsorption of Pb 2+,Co 2+and Ni 2+onHApC composite.404550556065707580859095100% R e m o v a lAdsorbent dose (g/L )Fig.5.Effect of adsorbent dose on adsorption of Pb 2+,Co 2+and Ni 2+on HApCcomposite.% R e m o v a lConta ct ti me (min )Fig. 6.Effect of contact time on adsorption of Pb 2+,Co 2+and Ni 2+on HApCcomposite.N.Gupta et al./Journal of the Taiwan Institute of Chemical Engineers 43(2012)125–131128different metal ions decreased in the order Pb 2+>Co 2+>Ni 2+which can be explained on the basis of their hydrated ionic radii,ionic mobility and diffusion rate constant [26].The hydrated ionic radius of different metal ions increases in the order Pb 2+<Co 2+<Ni 2+.Smaller the hydrated ionic radius of metal ion,higher is the ionic mobility and the rate of diffusion.Fig.10showed that all the lines did not pass through the rger the value of I ,greater was the contribution of the surface adsorption in the rate-limiting step [27].Results confirmed the presence of both surface adsorption and intraparticle diffusion mechanism.3.7.Adsorption isothermThe analysis of equilibrium data to construct adsorption isotherms is usually important for design of adsorption systems.Adsorption isotherms express the mathematical relationship between the quantity of adsorbate and equilibrium concentration of adsorbate remaining in the solution at a constant temperature.The most common types of isotherms are Langmuir and Freundlich models.The Langmuir isotherm model is applicable to monolayer adsorptions and can be expressed as:C e q e¼1bq max þ1q max C e(8)where C e is concentration of metal ions in solution at equilibrium (mg/L),q e is the amount of metal ions at equilibrium in unit mass of adsorbent (mg/g),q max and b are the Langmuir coefficient related to adsorption capacity (mg/g)and adsorption energy (L/mg),respectively.The Langmuir isotherm parameters q max and b were determined from slope (1/q max )and intercept (1/bq max )of the plot of C e /q e vs.C e (Fig.11),respectively.The empirical Freundlich isotherm is based on adsorption on a heterogeneous surface and express by the following equation:ln q e ¼ln K F þ1nln C e(9)K F and n are the Freundlich coefficient related to adsorption capacity [mg/g (mg/L)À1/n ]and adsorption intensity of adsorbent,respectively.The values of Freundlich constants n and K F were obtained from the slope (1/n )and intercept (ln K F )of the plot of ln q e vs.ln C e (Fig.12),respectively.The plots give straight lines,indicating that the adsorption of Pb 2+,Co 2+and Ni 2+onto HApC composite followed both theTable 1Kinetic parameters for adsorption of Pb 2+,Co 2+and Ni 2+on HApC composite.Metal ionsq e,exp(mg/g)Pseudo-first orderPseudo-second orderIntraparticle diffusionq e,cal (mg/g)k 1(min À1)R 2q e,cal (mg/g)k 2(g/mg/min)R 2k i (mg/g/min 0.5)IR 2Pb 2+ 3.11 2.080.1360.932 3.170.2730.9950.198 2.030.992Co 2+ 2.95 1.410.0980.895 2.980.3090.9970.117 2.210.995Ni 2+2.661.630.1190.9092.700.3000.9970.1171.930.991t /q t (m i n /m g /g )t (min )Fig.9.Pseudo-second order kinetic model for adsorptionof Pb 2+,Co 2+and Ni 2+onHApC composite.2.02.22.42.62.83.03.23.4q t (m g /g )t 0.5(mi n 0.5)Fig.10.Intraparticle diffusion model for adsorption of Pb 2+,Co 2+and Ni 2+on HApCcomposite.0.20.40.60.81.01.21.41.6C e /q e (g /L )C e (mg/L )ngmuir isotherm model for adsorption of Pb 2+,Co 2+and Ni 2+on HApCcomposite.N.Gupta et al./Journal of the Taiwan Institute of Chemical Engineers 43(2012)125–131129Langmuir and Freundlich isotherm models.The Langmuir and Freundlich isotherms constants and regression coefficients are listed in Table 2.The experimental results indicated that the order of adsorption capacity of HApC for metal ions was as follows:Pb 2+>Co 2+>Ni 2+.The values of n >1also indicated favourable adsorption conditions [28].3.8.Effect of temperature and thermodynamic parametersThe effect of temperature on the adsorption of Pb 2+,Co 2+and Ni 2+on HApC composite was investigated by conducting experi-ments for 10mg/L of initial metal ion concentrations at 303,313,and 323K.It was observed that on increasing the temperature percentage removal of metal ions increased.This showed that the adsorption process was endothermic in nature.The thermodynamic parameters Gibb’s free energy (D G 8),enthalpy (D H 8)and entropy (D S 8)were calculated using the following equations:lnq e m e ¼D S o þÀD H o(10)D G o ¼D H o ÀT D S o(11)where m is the adsorbent dose (g/L),C e is concentration of metal ions in solution at equilibrium (mg/L),q e is the amount of metal ions at equilibrium in unit mass of adsorbent (mg/g),q e /C e is called the adsorption affinity.D H 8,D S 8and D G 8are change in enthalpy (kJ/mol),entropy (J/(mol K))and free energy (kJ/mol),respectively.R is the gas constant (8.314J/mol/K)and T is the temperature (K).The values of D H 8and D S 8were obtained from the slopes and intercepts of the Van’t Hoff plots of ln (q e m /C e )vs.1/T (Fig.13),respectively,thereafter D G 8values were determined from Eq.(11).The values of thermodynamic parameters are presented in Table 3.The results showed that the D G 8values are negative and increased in their absolute values with temperature.This result suggested that a high temperature is favoured for the adsorption of Pb 2+,Co 2+and Ni 2+on HApC,indicated a spontaneous adsorption process.The values of D G 8for Pb 2+is the highest,indicated that the adsorption of Pb 2+ion was more spontaneous than Co 2+and Ni 2+ions.The values of heat of adsorption,D H 8is positive for all metal ions,indicated that the adsorption process of Pb 2+,Co 2+and Ni 2+on HApC was endothermic.A positive D S 8suggested that heavy metal ions were not stable on the adsorption sites of HApC probably due to the increase in translational energy of heavy metal ions.parative studyIn addition to the HApC composite,HAp was also used as anadsorbent for the removal of Pb 2+,Co 2+and Ni 2+and a comparative data are presented in Table 4.Study shows that the %removal of metal ion by HApC composite was almost similar to HAp which confirmed that the removal capacity of HAp was retained in HApC composite.Chitosan did not affect the adsorption capacity of HApI n q elnC eFig.12.Freundlich isotherm model for adsorption of Pb 2+,Co 2+and Ni 2+on HApC composite.Table 2Isotherm parameters for adsorption of Pb 2+,Co 2+and Ni 2+on HApC composite.Metal ions Langmuir constantsFreundlich constantsq max (mg/g)b (L/mg)R2K F [mg/g (mg/L)À1/n ]nR2Pb 2+12.040.5720.997 4.039 1.530.994Co 2+10.630.3490.994 2.619 1.590.997Ni 2+8.540.2110.993 1.5771.640.997l n (q e m /C e )1/T (K -1)Fig.13.The plots of ln (q e m /C e )vs.1/T for the adsorption of Pb 2+,Co 2+and Ni 2+on HApC composite.Table 4Comparative study of %removal of metal ions on HAp and HApC composite.Metal ions Removal of metal ions (%)Experimental condition HApHApC pHDose (g/L)Temperature (K)Contact time (min)C 0(mg/L)Pb 2+92.093.5 5.633033010Co 2+81.588.72633034010Ni 2+7680633034010Table 3Thermodynamic parameters for adsorption of Pb 2+,Co 2+and Ni 2+on HApC composite.Metal ionsD H 8(kJ/mol)D S 8(Jmol/K)ÀD G 8(kJ/mol)303K313K323KPb 2+104.861366.626 6.2269.89213.558Co 2+35.404134.041 5.209 6.5507.890Ni 2+32.537118.8873.4854.6745.863N.Gupta et al./Journal of the Taiwan Institute of Chemical Engineers 43(2012)125–131130for metal ions,it bind the HAp powder,form aggregates which prevent its dispersion in aqueous solution makes it convenient to use because dispersed HApfine particle in solution is difficult to recover.4.ConclusionsThis study showed that the binding of HAp powder with chitosan makes it convenient to use practically and its removal capability was also retained in HApC which makes HApC composite as an effective adsorbent for the removal of Pb2+,Co2+and Ni2+from aqueous solution.The order of removal efficiency(Pb>Co>Ni)for HApC composite was same as in case of pure HAp.The adsorption kinetics followed pseudo-second order kinetics and intraparticle diffusion model.The adsorption of Pb2+,Co2+and Ni2+onto the HApC composite followed both,Langmuir and Freundlich isotherm models.The negative values of D G8suggested that the adsorption was spontaneous in nature.The positive value of D H8and D S8 indicated endothermic adsorption process and increased random-ness at surface–solution interface,respectively. AcknowledgementAuthors are thankful to the NCEMP,Allahabad University for recording XRD and Prof. A.C.Pandey and Mr.P.K.Sharma of Nanotechnology Application Centre,University of Allahabad,India, for recording SEM.References[1]Ghassabzadeh H,Mostaedi MT,Mohaddespour A,Maragheh Md G,Ahmadi SJ,Zaheri P.Characterizations of Co(II)and Pb(II)removal process from aqueous solutions using expanded perlite.Desalination2010;261:73–9.[2]Turtureanu A,Georgescu C,Oprean L.Nickel Removal from Aqueous Solutionsby Flotation with Cationic Collector Determination of the Optimum Separation Conditions.Chem Bull‘‘POLITEHNICA’’Univ(Timisoara)2008;53:1–2.[3]Inglezakis VJ,Stylianou MA,Gkantzou D,Loizidou MD.Removal of Pb(II)fromaqueous solutions by using clinoptilolite and bentonite as adsorbents.Desali-nation2007;210:248–56.[4]Zaini MAA,Amano Y,Machida M.Adsorption of heavy metals onto activatedcarbons derived from polyacrylonitrilefiber.J Hazard Mater2010;180: 552–60.[5]Abu-Eishah SI.Removal of Zn,Cd,and Pb Ions from water by Sarooj clay.ApplClay Sci2008;42:201–5.[6]Bishnoi NR,Bajaj M,Sharma N,Gupta A.Adsorption of Cr(VI)on activated ricehusk carbon and activated alumina.Bioresour Technol2004;91:305–7. [7]Paulino AT,Guilherme MR,Reis AV,Tambourgi EB,Nozaki J,Muniz EC.Capacity of adsorption of Pb2+and Ni2+from aqueous solutions by chitosanproduced from silkworm chrysalides in different degrees of deacetylation.J Hazard Mater2007;147:139–47.[8]Aguado J,Arsuaga JM,Arencibia A,Lindo M,Gascon V.Aqueous heavy metalsremoval by adsorption on amine-functionalized mesoporous silica.J Hazard Mater2009;163:213–21.[9]Motsi T,Rowson NA,Simmons MJH.Adsorption of heavy metals from acidmine drainage by natural zeolite.Int J Miner Process2009;92:42–8.[10]Xu HY,Yang L,Wang P,Liu Y,Peng MS.Kinetic research on the sorption ofaqueous lead by synthetic carbonate hydroxyapatite.J Environ Manage 2008;86:319–28.[11]Bailliez S,Nzihou A,Beche E,Flamant G.Removal of Lead(Pb)by hydroxyapa-tite sorbent.Process Saf Environ Protect2004;82:175–80.[12]Smiciklas I,Dimovic S,Plecas I,Mitric M.Removal of Co2+from aqueoussolutions by hydroxyapatite.Water Res2006;40:2267–74.[13]Mobasherpour I,Salahi E,Pazouki M.Removal of nickel(II)from aqueoussolutions by nano-crystalline calcium hydroxyapatite.J Saudi Chem Soc 2011;15:105–12.[14]Corami A,Mignardi S,Ferrini V.Copper and zinc decontamination from single-and binary-metal solutions using hydroxyapatite.J Hazard Mater2007;146: 164–70.[15]Zhu R,Yu R,Yao J,Mao D,Xing C,Wang D.Removal of Cd2+from aqueoussolutions by hydroxyapatite.Catal Today2008;139:94–9.References and further reading may be available for this article.To view references and further reading you must purchase this article.[16]Simon FG,Birmann V,Peplinski B.Uranium removal from groundwater usinghydroxyapatite.Appl Geochem2008;23:2137–45.[17]Choi S,Jeong Y.The removal of heavy metals in aqueous solution by hydroxy-apatite/cellulose composite.Fiber Polym2008;9:267–70.[18]Mobasherpour I,Heshajin MS,Kazemzadeh A,Zakeri M.Synthesis of nano-crystalline hydroxyapatite by using precipitation method.J Alloy Compd 2007;430:330–3.[19]Leyva AQG,Marrero J,Smichowski P,Cicerone D.Sorption of antimony ontohydroxyapatite.Environ Sci Technol1994;28:1472–80.[20]Rayanaud S,Champion E,Assollant DB,Thomas P.Calcium phosphate apatiteswith variable Ca/P atomic ratio I Synthesis,characterisation and thermal stability of powders.Biomaterials2002;23:1065–72.[21]Sundaram CS,Viswanathan N,Meenakshi S.Uptake offluoride by nano-hydroxyapatite/chitosan composite,a bioinorganic composite.Bioresour Technol2008;99:8226–30.[22]Afkhamia A,Tehranib Md S,Bagherib H.Simultaneous removal of heavy-metalions in wastewater samples using nano-alumina modified with2,4-dinitro-phenylhydrazine.J Hazard Mater2010;181:836–44.[23]Lagergren S.About the theory of so called adsorption of soluble substances.Ksver Veterskapsakad Handl1898;24:1–6.[24]Ho YS,McKay G.Pseudo-second order model for sorption processes.ProcessBiochem1999;34:451–65.[25]Weber Jr WJ,Morris JC.Kinetics of adsorption on carbon from solution.J SanitEng Div ASCE1963;89(SA2)::31–59.[26]Ricordel S,Taha S,Cisse I,Dorange G.Heavy metals removal by adsorptiononto peanut husks carbon:characterization,kinetic study and modelling.Sep Purif Technol2001;24:389–401.[27]Kannan K,Sundaram MM.Kinetics and mechanism of removal of methyleneblue on adsorption of various carbons-a comparative study.Dyes Pigment 2001;51:25–40.References and further reading may be available for this article.To view references and further reading you must purchase this article..[28]Hameed BH,Mahmoud DK,Ahmad AL.Equilibrium modeling and kineticstudies on the adsorption of basic dye by a low-cost adsorbent:Coconut(Cocos nucifera)bunch waste.J Hazard Mater2008;158:65–72.N.Gupta et al./Journal of the Taiwan Institute of Chemical Engineers43(2012)125–131131。

相关文档
最新文档