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纯电动汽车复合电源能量管理控制策略研究

纯电动汽车复合电源能量管理控制策略研究

第2期2021年2月294机械设计与制造Machinery Design & Manufacture 纯电动汽车复合电源能量管理控制策略研究许兵,张维刚(湖南大学汽车车身先设计制造国家重点实验室,湖南长沙410082)摘要:蓄电池循环寿命短、充放电效率低等缺陷制约了纯电动汽车储能系统的发展,将蓄电池与超级电容器组合成复 合电源系统,并采用合理的能量管理控制策略,充分发挥两类能量源的优势,能有效降低纯电动汽车的能量消耗、提高储 能系统的使用寿命。

根据复合电源的工作方式设计了模糊逻辑能量管理控制策略,采用遗传算法对模糊控制器隶属度函数参数进行了优化。

通过MATLAB 与ADVISOR 联合仿真,结果表明,经遗传算法优化后的能量管理控制策略能够显著降低系统的总能耗,提高制动能量回收效率,改善蓄电池放电状态,并提高储能系统的使用寿命。

关键词:复合电源;能量管理策略;模糊控制;遗传算法中图分类号:TH16;U469.72 文献标识码:A 文章编号:1001-3997(2021 )02-0294-05Research on Energy Management Strategy of Hybrid EnergyStorage System in Pure Electric VehicleXU Bing, ZHANG Wei-gang(State Key Laboratory of Advanced Design and Manufacturing for Vehicle Body, Hu'nan University , Hu'nan Changsha 410082, China)Abstract :7%e defects of short cycle life and low charging/discharging efficiency of battery restricted the development of p ureelectric vehicle(^PEN)energy storage system, the hybrid energy storage system()IESS )combined with batteries and svpercacitors can effsctwel-y reduce the energy consumption of PEN and improve the service life of the energy storage system by adopting reasonable energy management control strategy and giving f ull platy to the advantages of both energy storages. The Juzzy logicenergy management control strategy was designed based on working way of HESS, the parameters of membership function cf fuzzy controller was optimized with genetic algorithm. The simulation was carried out with MATLAB and ADVISOR, the result shows that the total energy consumption of HESS is significantly reduced after optimization, the recycling efficiency ofregenerative braking is improved and the discharge state and service life of t he energy system is improved.Key Words :Hybrid Energy Storage System(HESS ); Energy Management Strategy; Fuzzy Control; Genetic Algorithm1引言日益严峻的能源短缺与环境污染问题使得电动汽车成为汽 车领域的研发热点,其高效的能量利用率及零污染排放的环境友好性使其受到各国研究机构的青睐叫目前,电动汽车主要采用单 _电池作为动力源,在汽车行驶过程中频繁变化的峰值功率会对电池造成较大的冲击从而降低电池的使用寿命,同时电池低比功 率的特性往往无法应对汽车急加速、爬坡等峰值功率需求0。

两级蓄冷跨临界压缩CO2混合工质储能系统特性分析

两级蓄冷跨临界压缩CO2混合工质储能系统特性分析

第 54 卷第 10 期2023 年 10 月中南大学学报(自然科学版)Journal of Central South University (Science and Technology)V ol.54 No.10Oct. 2023两级蓄冷跨临界压缩CO 2混合工质储能系统特性分析赵攀,吴汶泽,许文盼,刘艾杰,王江峰(西安交通大学 能源与动力工程学院,陕西 西安,710049)摘要:为了解决高压CO 2在高环境温度下难以冷凝的问题,提出两级蓄冷跨临界压缩CO 2混合工质储能系统。

采用CO 2与低沸点有机工质混合的方法提高工质的冷凝温度,同时,利用两级甲醇蓄冷实现系统内部冷能循环利用。

从环境性、临界温度、温度滑移、可混合性等方面确定合适的CO 2混合工质及其组分质量分数范围。

建立储能系统的热力学分析模型,探究节流压力、高压储液罐压力、有机工质质量分数等关键参数对系统性能的影响规律,并研究系统内部能量流动规律,得到主要部件的㶲损失。

研究结果表明:随着有机工质质量分数的增加,蓄冷介质温度增加,系统安全性提高;与纯CO 2工质相比,系统的充放电效率和能量密度略有降低;CO 2/R32混合工质的充放电效率最高为62.29%,CO 2/pentane 混合工质的能量密度最高为21.37 kW ∙h/m 3。

关键词:压缩CO 2储能;CO 2混合工质;热力学分析;敏感性分析;有机工质中图分类号:TK02 文献标志码:A 开放科学(资源服务)标识码(OSID)文章编号:1672-7207(2023)10-4150-13Performance analysis of a transcritical compressed CO 2-based mixture energy storage system with two-stage cold energy storageZHAO Pan, WU Wenze, XU Wenpan, LIU Aijie, WANG Jiangfeng(School of Energy and Power Engineering, Xi'an Jiaotong University, Xi'an 710049, China)Abstract: In order to solve the problem of difficult condensation of high-pressure CO 2 in higher ambient temperature, a transcritical compressed CO 2-based mixture energy storage system with two-stage cold energy storage was proposed. The CO 2-based mixture via blending CO 2 and organic working medium with low boiling point was selected to improve the condensation temperature. Meanwhile, a two-stage cold energy storage system via methanol was employed to store and recycle the cold energy. Firstly, the feasible CO 2-based mixtures and the related mass fraction ranges of organic working mediums were determined by considering the environment, critical temperature, temperature glide and miscibility. Then, the system thermodynamic models were established, and the effect of severalkey parameters on system performance was explored, such as throttling pressure, high-pressure storage tank pressure收稿日期: 2022 −10 −10; 修回日期: 2023 −02 −27基金项目(Foundation item):国家自然科学基金资助项目(51876152) (Project(51876152) supported by the National Natural ScienceFoundation of China)通信作者:赵攀,博士,教授,从事压缩气体储能技术基础与应用研究;E-mail :*****************DOI: 10.11817/j.issn.1672-7207.2023.10.032引用格式: 赵攀, 吴汶泽, 许文盼, 等. 两级蓄冷跨临界压缩CO 2混合工质储能系统特性分析[J]. 中南大学学报(自然科学版), 2023, 54(10): 4150−4162.Citation: ZHAO Pan, WU Wenze, XU Wenpan, et al. Performance analysis of a transcritical compressed CO 2-based mixture energy storage system with two-stage cold energy storage[J]. Journal of Central South University(Science and Technology), 2023, 54(10): 4150−4162.第 10 期赵攀,等:两级蓄冷跨临界压缩CO 2混合工质储能系统特性分析and mass fraction of organic working medium. At the same time, the system internal energy flow was analyzed, and the exergy destruction distribution of main components was obtained. The results show that the cold energy storage medium temperature increases and the system safety is enhanced with the increase of mass fraction of the organic working mediums. Compared with pure CO 2, the round-trip efficiency and energy density of CO 2-based mixture decrease slightly. The round-trip efficiency of CO 2/R32 mixture has the maximum value of 62.29%. The energy density with CO 2/pentane mixture reaches the maximum value of 21.37 kW ∙h/m 3.Key words: compressed CO 2 energy storage; CO 2-based mixture; thermodynamic analysis; sensitivity analysis; organic working medium能源是人类社会的物质基础,是经济发展的重要保障。

关于新能源充电管理系统的外文文献

关于新能源充电管理系统的外文文献

关于新能源充电管理系统的外文文献
对于新能源充电管理系统的外文文献,我们可以从多个角度来
寻找相关信息。

首先,我们可以从学术数据库如Google 学术、
IEEE Xplore、ScienceDirect等搜索相关的期刊论文和学术文章。

在搜索时,可以使用关键词如"new energy charging management system"、"renewable energy charging system"、"electric vehicle charging system"等来获取相关的外文文献。

另外,我们还可以查阅相关的国际会议论文集,例如国际清洁
能源大会(International Conference on Clean Energy)或国际
电力系统与清洁能源大会(International Conference on Power Systems and Clean Energy)等会议的论文集,这些会议通常会涵
盖新能源充电管理系统的最新研究成果。

此外,还可以寻找相关的专业书籍和技术报告,这些书籍和报
告通常会详细介绍新能源充电管理系统的原理、设计和应用。

通过
搜索国际出版的书籍和技术报告,可以获取到丰富的外文文献资料。

除了以上途径,还可以关注国际知名能源管理和电力系统领域
的学者和专家的研究成果,他们在国际期刊上发表的论文和专著都
是宝贵的外文文献资源。

总的来说,要全面了解新能源充电管理系统的外文文献,我们需要充分利用学术数据库、国际会议论文集、专业书籍和技术报告等多种渠道,从不同的角度获取相关信息,以便全面深入地了解该领域的最新研究成果和发展动态。

氧化石墨烯基吸附剂吸附金属离子及有机污染物研究进展

氧化石墨烯基吸附剂吸附金属离子及有机污染物研究进展

第49卷第9期2020年9月应用化工Appeoed ChemocaeIndusteyVoe.49No.9Sep.2020氧化石墨烯基吸附剂吸附金属离子及有机污染物研究进展张倩倩“,王三反“(1-兰州交通大学环境与市政工程学院,甘肃兰州730070&2-寒旱区水资源综合利用教育部工程研究中心,甘肃兰州730070)摘要:综述了石墨烯和氧化石墨烯的理化性质和发展前景,从吸附重金属离子和有机染料的角度出发,概述了氧化石墨烯及其复合材料对Cu2+*Pb2+和MB的吸附效果及对金属离子和有机染料的吸附机理。

最后针对全文研究 进展做了总结同时对未来高效吸附剂的开发做了展望。

关键词:氧化石墨烯;重金属离子;有机染料;吸附机理中图分类号:TQ20&TQ23文献标识码:A文章编号:1671-3206(2020)09-2355-03Reeearchprogreeonadeorptionofmetafioneandorganicpo fetanteby graphenecbaeedadeorbenteZHANG Qian-jian1,2,WANG San-fan1,2(1-School of Environmental and Municipal Enginee/ng,Lanzhou Jiaotong University,Lanzhou730070,China;2-Enginee/ng Research Center fez Cold and A/b Regions Water Resource Comprehensive UPlOadon,MonosteyoeEducatoon,Lanzhou730070,Chona)Abstract:The physical and chemical pmpeaivs and development prospects of graphene and graphene ox­ode we ee ee eoewed.F eom the pe espec toee oeadso ep toon oeheaeymetaeoonsand oeganocdyes,theadsoeptoon dfecl of graphene oxide and its composite materials on Cu2°,Pb2O and MB and the adsom/w mechanism oemetaeoonsand oeganocdyeaeesummaeozed.Fona e y,otsummaeozestheeeseaech peogee s oetheeu e teit and peospec ts thede eeeopmen toehogh-e e ocoencyadsoeben ts on theeutuee.Key worde:geapheneoiode;heaeymetaeoons;oeganocdyes;adsoeptoon mechanosm现阶段从水中将污染物去除采用的方法大致有三种:生物法*物理法和化学法$吸附法具有如下优点:使用设备仪器简单、操作方便快捷、不会产生副反应并造成二次污染等,因此可用于脱除水中污染物。

基于分子动力学的熔盐热物性研究进展

基于分子动力学的熔盐热物性研究进展

第 12 卷第 12 期2023 年 12 月Vol.12 No.12Dec. 2023储能科学与技术Energy Storage Science and Technology基于分子动力学的熔盐热物性研究进展付殿威,张灿灿,娜荷芽,王国强,吴玉庭,鹿院卫(北京工业大学传热强化与过程节能教育部重点实验室,传热与能源利用北京市重点实验室,北京100124)摘要:熔盐作为高温传热蓄热介质,在太阳能光热发电、火电厂灵活性改造等场景中广泛应用。

本文首先对熔盐分子动力学的势函数进行归纳分析,发现针对硝酸盐更适合使用带有库仑力的Buckingham势函数,碳酸盐和氯化盐采用BMH势函数计算可以减小模拟误差。

其次对熔盐热物性进行分析,发现加入Ca2+可以降低太阳盐的熔点但会增加其黏度,硝酸盐中随NO-2浓度的增加比热容降低;Li+离子浓度的增加会提高氯化盐的比热容和热导率,但会导致模拟误差增大,K+离子浓度增加会导致比热容误差减小,但其余热物性计算误差增大;碳酸盐模拟误差相对较小,与实验数据吻合较好。

K+、Li+等对模拟结果产生的误差较大,离子增多后离子间势能的增加导致部分粒子丢失,引入边界条件后边界效应的影响会使误差增大。

通过增加整体分子数量、校正位能截断距离、增加模拟时间步长等方法来减小误差。

目前对同种阳离子、不同阴离子的熔盐分子动力学研究比较欠缺,探究纳米流体对熔盐分子动力学的影响、降低分子动力学模拟误差、开展基于分子动力学的熔盐腐蚀特性研究可以作为下一步熔盐分子动力学的研究方向。

关键词:熔盐;分子动力学;势函数;热物性doi: 10.19799/ki.2095-4239.2023.0708中图分类号:TK 512 文献标志码:A 文章编号:2095-4239(2023)12-3873-10 Review of the molecular dynamics of molten salt thermalphysical propertiesFU Dianwei, ZHANG Cancan, NA Heya, WANG Guoqiang, WU Yuting, LU Yuanwei(MOE Key Laboratory of Enhanced Heat Transfer and Energy Conservation, BeijingKey Laboratory of Heat Transfer and Energy Conversion, College of Environmental and Energy Engineering, Beijing University of Technology,Beijing 100124, China)Abstract:As a high-temperature heat transfer and storage medium, molten salt is widely used for solar thermal power generation and the flexible transformation of thermal power plants.First, the potential functions of the molecular dynamics of molten salt were summarized and analyzed. This indicated that to reduce simulation errors, the Buckingham potential with coulomb force is more suitable for nitrate and the BMH potential is more suitable for carbonate and chloride salt. Second, an analysis of the thermal properties of molten salt indicated that the addition of Ca2+to solar salt decreased its melting point and increased its viscosity, and the specific heat capacity of nitrate decreased with increasing NO2- concentration. Increased收稿日期:2023-10-11;修改稿日期:2023-11-03。

供热管网智能管控平台在高校供热系统中的节能应用

供热管网智能管控平台在高校供热系统中的节能应用

应 用·APPLICATION102供热管网智能管控平台在高校供热系统中的节能应用文_张雯 青岛大学摘要:通过分析某高校供热管网运行中存在的常见问题,针对性地应用供热管网智能管控平台进行节能管理。

结合校园各类建筑的供热需求,提出在供热管网水力平衡基础上的分时分区控制方式,并通过eQUSET能耗模拟软件进行模拟分析,结果表明具有较为明显的节能效果,可降低供热运行能耗达20%以上。

关键词:供热管网;分时分区控制;水力平衡;能耗模拟Energy Saving Application of Heating Network Intelligent Management and ControlPlatform in University Heating SystemZHANG Wen[ Abstract ] By analyzing the common problems existing in the operation of heating pipe network in a university, the intelligent management and control platform of heating pipe network is applied for energy-saving management. Combined with the heating demand of all kinds of buildings in the campus, the time-sharing and district control mode based on the hydraulic balance of the heating network is proposed, and the simulation analysis is carried out by the equsset energy consumption simulation software. The results show that it has obvious energy-saving effect, and can reduce the heating operation energy consumption by more than 20%.[ Key words ] heating network;time sharing and partition control; hydraulic balance;energy consumption simulation随着我国“碳达峰、碳中和”目标的提出,绿色低碳发展成为国家战略的重要一环。

On the Difference of Energy between the Einstein and M{o}ller Prescription

On the Difference of Energy between the Einstein and M{o}ller Prescription

a r X i v :g r -q c /0212099v 1 24 D e c 2002On the Difference of Energy between the Einsteinand Møller PrescriptionI-Ching Yang †1and Irina Radinschi ‡2†Department of Natural Science Education andAdvanced Science and Technology Research Center,National Taitung Teachers College,Taitung,Taiwan 950,Republic of Chinaand‡Department of Physics,“Gh.Asachi”Technical University,Iasi,6600,RomaniaABSTRACTIn some black hole solutions,these do not exist the same energy-momentum complexes associated with using definition of Einstein and Møller in given coordinates.Here,we consider the difference of energy between the Einstein and Møller prescription,and compare it with the energy density of those black hole solutions.We found out a special relation between the difference of energy between the Einstein and Møller prescription and the energy density for considered black hole solutions.PACS No.:04.20.-q,04.50.+hIn the theory of general relativity,many physicists,like Einstein[1],Lan-dau and Lifshitz[2],Tolman[3],Papapetrou[4],Møller[5],and Weinberg[6], had given different definitions for the energy-momentum complex.Specifi-cally,the Møller energy-momentum complex allows to compute the energy in any spatial coordinate system.Some results recently obtained[7,8,9,10] sustain that the Møller energy-momentum complex is a good tool for obtain-ing the energy distribution in a given space-time.Also,in his recent paper, Lessner[11]gave his opinion that the Møller definition is a powerful concept of energy and momentum in general relativity.In his paper Virbhadra[12] point out that several energy-momentum complexes(ELLPW)give the same result for a general non-static spherically symmetric space-time of the Kerr-Schild class.In particular,whatever coordinates do not exist the same energy com-plexes associated with using definitions of Einstein and Møller in some space-time solutions[7,13].According to the definition,the Einstein energy com-plex is[1]E Ein=1∂x ld3x,(1)whereH0l0=g00−g∂8π ∂χ0l0−gg0βg lα ∂g0α∂xα .(4) Where the Latin indices take values from1to3,and the Greek indices run from0to3.Let us look into the difference of energy between the Einstein and Møller prescription,which be defined as∆E=E Ein−E Møl(5) In this article,we would discuss the problem within the difference between Einstein and Møller energy-momentum complexes.In thefirst case,we think of two solutions of Einstein vacuumfield equa-tion:(i)Schwarzschild space-timeThe metric form of Schwarzschild space-time isds2=fdt2−f−1dr2−r2dθ2−r2sin2θdϕ2,(6) where f=1−2M/r.It is a well-known results that the energy complexes of Einstein and Møller of Schwarzschild space-time areE Ein=M,(7)E Møl=M,(8)and the difference is∆E=0.(9) (ii)Kerr solutionThe metric form of Kerr solution is considered asds2=αdt2−βdr2−γdθ2−δdφ2−2σdtdϕ,(10) whereα=1−2Mr/Σ,β=Σ/∆,γ=Σ,δ=r2+a2+2Ma2r sin2θ/Σandσ=2Mar sin2θ/Σ.HereΣ≡r2+a2cos2θand∆≡r2−2Mr+a2.To use the results in the Virbhadra articles[14]and to set these Q=0,we could obtain the enrgy-momentum complexes of Einstein and Møller of Kerr space-time areE Ein=M,(11)E Møl=M,(12) and the difference is∆E=0.(13) For Einstein’s vacuumfield equation,the energy density isT00=0.(14) We wouldfind that∆E equal to the value of T00.Next,we consider two case of the coupled system of the Einsteinfield and electromagneticfield:(iii)Reissner-Nordstr¨o m space-timeThe metric form of Reissner-Nordstr¨o m space-time isds2=fdt2−f−1dr2−r2dθ2−r2sin2θdϕ2,(15) where f=1−2M/r+Q2/r2.Previously,the energy-momentum complexes of Einstein and Møller of Reissner-Nordstr¨o m space-time had been calculated withE Ein=M−Q2r,(17)and the difference is∆E=Q2r4.(19)(iv)charged regular black holeThe metric form of charged regular black hole is[15]ds2=fdt2−f−1dr2−r2dθ2−r2sin2θdϕ2,(20)where f=1−2M2Mr)).Using the results of Radinschi’s arti-cles[10],the energy-momentum complexes of Einstein and Møller of charged regular black hole areE Ein=M 1−tanh(Q22Mr) −Q22Mr) ,(22) and the difference is∆E=Q22Mr) .(23)However,the energy density of the coupled system of the Einsteinfield and nonlinear electrodynamicsfield isT00=Q22Mr) .(24)Here the relation between∆E and the energy density is written as∆E=T00×(r38πε0.According to the results of our articles[17],the energy-momentum complexes of Einstein and Møller of the static spherically symmetric nonsin-gular black hole areE Ein=M−M exp(−r3r3∗)−3r3r3∗),(28)and the difference is∆E=3r3r3∗).(29)Notice that the energy density of the static spherically symmetric nonsingular black hole be assumed asT00=3r3∗).(30)The relation between∆E and the energy density is written as∆E=T00×r3.(31) Although,we could summarize that the general relation between∆E and the energy density T00be written as∆E=T00×(kr3),(32) with k=1/2and k=1.But,it is still an open question why the special rela-tion has between∆E and the energy density T00.Further study is needed to understand the difference between the Einstein and Møller energy complexes of more varied black hole solutions.AcknowledgementsI.-C.Yang thanks the National Science Council of the Republic of China for financial support under the contract number NSC90-2112-M-143-003.References[1]A.Trautman,in Gravitation:an Introduction to Current Research,edited by L.Witten(Wiley,New York,1962),pp169-198.[2]ndau and E.M.Lifshitz,The Classical Theory of Fields(Addison-Wesley,Reading,MA,1962),2nd ed.[3]R.C.Tolman,Phys.Rev.35,875(1930).[4]A.Papapetrou,Proc.R.Ir.Acad.A52,11(1948);S.N.Gupta,Phys.Rev.96,1683(1954);D.Bak,D.Cangemi,and R.Jackiw,Phys.Rev.D49,5173(1994).[5]C.Møller,Ann.Phys.(NY)4,347(1958).[6]S.Weinberg,Gravitation and Cosmology(Wiley,New York,1972).[7]I-Ching Yang,Wei-Fui Lin and Rue-Ron Hsu,Chin.J.Phys.37,113(1999).[8]S.S.Xulu,gr-qc/0010062.[9]I.Radinschi,gr-qc/0110058.[10]I.Radinschi,Mod.Phys.Lett.A16,673(2001).[11]G.Lessner,Gen.Relativ.Gravit.28,527(1996).[12]K.S.Virbhadra,Phys.Rev.D60,104041(1999).[13]I.-C.Yang,R.-R.Hsu,C.-T.Yeh and C.-R.Lee,Int.J.Mod.Phys.D5,251(1997).[14]K.S.Virbhadra,Phys.Rev.D42,2919(1990).[15]E.Ay´o n-Beato and A.Garica,Phys.Lett.B464,25(1999).[16]I.G.Dymnikova,Gen.Rel.Grav.24,235(1992).[17]I.-C.Yang,Chin.J.Phys.38,1040(2000);I.Radinschi,Mod.Phys.Lett.A15,803(2000).。

《bp世界能源统计年鉴》2016版英文

《bp世界能源统计年鉴》2016版英文

《bp世界能源统计年鉴》2016版英文As an AI language model trained by OpenAI, I am capable of providing a comprehensive response to the topic of the "BP Statistical Review of World Energy 2016" in English. I will aim to present the information in a coherent and natural manner, without the use of transitional phrases or explicit paragraph structure.The BP Statistical Review of World Energy is an annual publication that provides a comprehensive overview of global energy trends and developments. The 2016 edition, which covers data up to the end of 2015, offers a detailed analysis of the state of the world's energy landscape, including the production, consumption, and trade of various energy sources.One of the key findings of the 2016 report is the continued growth in global energy consumption. In 2015, the world's total primary energy consumption increased by 1%, reaching a level of 13,147 million tonnes of oil equivalent (Mtoe). This growth was primarily driven by increasing energydemands in emerging economies, particularly in Asia, where countries like China and India have experienced rapid industrialization and economic development.The report also highlights the shifting dynamics in the global energy mix. While fossil fuels, including oil,natural gas, and coal, still account for the majority ofthe world's primary energy consumption, the share of renewable energy sources, such as hydropower, wind, and solar, has been steadily increasing. In 2015, renewable energy sources contributed 3.1% to the global energy mix, a significant increase from the 2.6% recorded in 2014.Another notable trend observed in the 2016 report is the continued decline in global coal consumption. In 2015,global coal consumption fell by 1.8%, marking the second consecutive year of decline. This trend can be attributedto a combination of factors, including the increasing competitiveness of natural gas and renewable energy sources, as well as policy initiatives aimed at reducing greenhouse gas emissions and promoting cleaner energy alternatives.The report also provides insights into the production and trade patterns of various energy sources. For instance, in 2015, global oil production increased by 2.5%, with the majority of the growth coming from OPEC countries, particularly Saudi Arabia and Iraq. Conversely, global natural gas production grew by only 1.7%, with the United States and Russia remaining the largest producers.In terms of energy trade, the report highlights the increasing importance of liquefied natural gas (LNG) in the global energy market. In 2015, global LNG trade reached a record high of 245.2 billion cubic meters (bcm), driven by the growing demand for clean energy sources in Asia, particularly in China and Japan.Overall, the 2016 edition of the BP Statistical Review of World Energy provides a comprehensive and insightful analysis of the global energy landscape, reflecting the ongoing trends and changes in the production, consumption, and trade of various energy sources. The report serves as a valuable resource for policymakers, industry stakeholders,and researchers alike, informing decision-making and shaping the future of the global energy sector.。

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A metal–organic framework-derived bifunctional oxygen electrocatalystBao Yu Xia,Ya Yan,Nan Li,Hao Bin Wu,Xiong Wen(David)Lou*and Xin Wang*Oxygen electrocatalysis is of great importance for many energy storage and conversion technologies,including fuel cells, metal–air batteries and water electrolysis.Replacing noble metal-based electrocatalysts with highly e cient and inexpensive non-noble metal-based oxygen electrocatalysts is critical for the practical applications of these technologies.Here we report a general approach for the synthesis of hollow frameworks of nitrogen-doped carbon nanotubes derived from metal–organic frameworks,which exhibit higher electrocatalytic activity and stability for oxygen reduction and evolution than commercial Pt/C electrocatalysts.The remarkable electrochemical properties are mainly attributed to the synergistic e ect from chemical compositions and the robust hollow structure composed of interconnected crystalline nitrogen-doped carbon nanotubes.The presented strategy for controlled design and synthesis of metal–organic framework-derived functional nanomaterials o ers prospects in developing highly active electrocatalysts in electrochemical energy devices.O xygen electrochemistry involves oxygen reduction(ORR) and evolution(OER)reactions,which are the two mostimportant reactions for electrochemical energy storage and conversion technologies,including fuel cells,metal–air batteries and water electrolysis1,2.A highly active and stable electrocatalyst for the ORR and the OER is the key for these electrochemical applications3.Noble metals are normally good electrocatalysts for these applications.For example,platinum (Pt)-based nanocomposites are the most efficient commercial electrocatalysts for the ORR,whereas precious ruthenium(Ru)-and iridium(Ir)-based nanocomposites are commonly used in the OER process4.However,the poor stability,scarcity and high cost of these noble metal-based oxygen electrocatalysts are major barriers for the large-scale implementation of these technologies5,6.Thus, it is urgent to develop highly efficient and durable alternatives with low cost,ideally with the bifunctional capability for the ORR and OER(ref.7).In the past decade,a wide range of alternative materials,including nanocarbons8,metal oxides9,carbides/nitrides and their composites10–13,have been found electroactive towards the oxygen electrochemical processes14–16.Among them,nanocarbons have been demonstrated with promising catalytic activity and stability4,8,17,and the catalytic properties could be further enhanced by the introduction of heteroatoms,including N,S,B and so on18,through the modification of the electronic and geometric structures19.In particular,various N-doped graphitic nanocarbons, including carbon nanotubes(CNTs),graphene,mesoporous carbons and their nanocomposites,have been reported as possible replacements for Pt catalysts20–22.The enhanced performance is believed to be related to the modified electronic structure and carbon defects induced by the foreign heteroatoms23.However,few reports of nanocarbons have so far shown excellent activity and durability comparable to that of Pt/C catalysts24.Recently,metal–organic frameworks(MOFs)have emerged as a new platform for the synthesis of new nanocarbon composites25–27. As a subclass of MOFs,zeolitic imidazolate frameworks(ZIFs) are excellent precursors for nanocarbon electrocatalysts in view of the existence of abundant carbon and nitrogen species28–30.The nitrogen species would form chemical bonds with metal nanoparticles and serve as the heteroatoms in the N-doped carbon materials formed31.Such N-doped nanocarbons may be promising electrocatalysts for the ORR and the OER(ref.32).Unfortunately, the MOF-derived nanocomposites are mostly microporous and of poor graphitic degree33—factors which are considered unfavourable for ion and electron transport.Although a number of MOF-derived nanocarbons/metal oxides have been investigated as electrocatalysts34–36,most of them exhibit unsatisfactory electrochemical activity.Moreover,the use of MOFs as the single precursor for the preparation of N-doped CNTs(NCNTs)structures has rarely been reported so far37,38.Yang et al.demonstrated the synthesis of NCNTs through the pyrolysis of Zn–Fe–ZIFs.In their synthesis,dicyandiamide(DCDA)is introduced as both the inducer of the graphitic structure and an extra N source,and the NCNTs formed do not retain any secondary microstructure39.Herein,we report the direct synthesis of N-doped carbon nanotube frameworks(NCNTFs)derived from MOFs as an active and stable bifunctional electrocatalyst for the ORR and the OER.The as-prepared hollow structures retain the well-defined morphology of the initial ZIF-67particles,with hierarchical shells of interconnected crystalline NCNTs.With many advantageous features in composition,structure and optimum graphitic degree and N-doping level,the resultant NCNTFs show enhanced activity and durability as well as methanol tolerance when benchmarked with a commercial Pt/C electrocatalyst under the same testing conditions.Their electrocatalytic activities in terms of onset and half-wave potentials for the ORR compare favourably with various nanocarbons reported so far.It is also important to point out that the MOFs material is the single precursor for the formation of NCNTs structures in this work.Electrocatalyst preparation and characterizationThe NCNTFs material is synthesized by a simple thermal treatment of purple ZIF-67particles(Supplementary Fig.1)containing abundant C,Co and N atoms at700◦C in an Ar/H2atmosphere, followed by acid treatment of the resulting material with0.5MSchool of Chemical and Biomedical Engineering,Nanyang Technological University,62Nanyang Drive,Singapore637459,Singapore. *e-mail:xwlou@.sg;WangXin@.sgDOI:10.1038/NENERGY.2015.60.36 nmabcd e fFigure 1|Morphology and structural characterization of NCNTFs obtained at 700◦C in the presence of H 2.a –c ,FESEM images.d ,TEM image.e ,f ,HRTEM images.In f ,0.36nm refers to the lattice spacing indicated by the white dashed lines,on the carbon (002)plane.Arrows in e and f indicate the direction of the graphitic layers.The inset of a is a digital photo,scale bar is 1cm.Scale bars:a ,10µm;b ,c ,1µm;d ,500nm;e ,f ,5nm.H 2SO 4for 6h to remove the accessible Co nanoparticles.Figure 1a shows a typical field-emission scanning electron microscopy (FESEM)image of the as-obtained NCNTFs.The size and polyhedral shape of the ZIF-67nanoparticles are retained well after thermal treatment,while the surface of the particles becomes much rougher (Fig.1b).Many tiny CNTs can be observed on the rough surface.Moreover,some particles show open voids,indicating the formation of hollow structures.The hierarchical shell,with a thickness of about 200nm,is composed of interconnected CNTs (Fig.1c).The microstructure is further investigated by transmission electron microscopy (TEM;Supplementary Fig.2).Figure 1d confirms the hollow structure with a shell composed of CNTs,several hundred nanometres in length.The TEM image also reveals the presence of Co nanoparticles encapsulated by a few-layered carbon shell,especially at the tip of the CNTs (Fig.1e).These carbon-encased Co nanoparticles are inaccessible to reactants as they remain completely encapsulated within the graphitic carbon shell even after acid leaching.Furthermore,a high-resolution (HR)TEM image reveals that these thick multiwalled CNTs are crystalline and the lattice fringes with an inter-planar distance of ∼0.36nm correspond to the C(002)plane (Fig.1f).It is interesting to observe that the graphitic layers in the CNT walls are not perfectly parallel to the axis direction of the CNTs,thus abundant edges rather than the basal plane are exposed on the surface of the CNTs (Fig.1e,f),which would be beneficial to the enhanced electrocatalytic properties.The crystalline nature of the carbon material in the frameworks is further confirmed by powder X-ray diffraction (XRD)in Fig.2a.The peak at about 26.2◦corresponds to the C(002)plane,and the other peak at about 44.3◦is attributed to metallic Co.Raman spectra of the products also reveal the characteristic G and D bands of carbon,which are related to the graphitic sp 2-carbon and disordered or defect carbon,respectively (Supplementary Fig.3a,b).The chemical composition and the effect of N doping are investigated by X-ray photoelectron spectroscopy (XPS;Supplementary Fig.3c).The high-resolution C 1s spectrum can be deconvolved into twobands,corresponding to C–C at ∼284.5eV and C=N at ∼285.6eV (Fig.2b).The high-resolution N1s spectrum reveals the presence of two types of nitrogen species,pyridinic N at ∼398.5eV and pyrrolic N at ∼400.8eV (Fig.2c and Supplementary Fig.4).The atomic percentage of N dopant is about 2.4%for the NCNTFs obtained at 700◦C (Supplementary Fig.3d).The Co 2p spectrum exhibits two prominent bands at 779.2eV and 794.7eV ,readily assigned to Co 2p 3/2and Co 2p 1/2,respectively (Supplementary Fig.5a).On the basis of thermogravimetric analysis (TGA),the Co atomic fraction is found to be about 3.1%(Supplementary Fig.5b),which is larger than the value of 1.14%given by XPS analysis,probably owing to the limited sampling depth of XPS.A slight increase in the content of the surface Co species with higher pyrolysis temperature is observed from the XPS results (Supplementary Fig.3d),which may be explained by the enhanced graphitic degree with the increase in pyrolysis temperature.N 2sorption isotherms of NCNTFs can be identified as type-IV isotherms,with a pronounced hysteresis loop,suggesting the existence of a mesoporous structure (Fig.2d and Supplementary Fig.6).Moreover,the NCNTFs sample shows a relatively broad mesopore distribution,with an average pore size of ∼7.8nm (inset of Fig.2d).The specific surface area estimated by the Brunauer–Emmett–Teller (BET)method and the total pore volume are 513m 2g −1and 1.16cm 3g −1,respectively (Supplementary Fig.6d).During the heat treatment,the H 2atmosphere plays a critical role in the formation of hollow-structured hierarchical CNTs frameworks.Metallic Co nanoparticles are quickly formed in the presence of the H 2atmosphere,followed by the catalytic growth of NCNTs and eventual formation of NCNTFs.In this process,ZIF-67particles serve not only as the C and N source for growth of NCNTs with the assistance of metallic Co catalysts,but also as the self-template for the framework morphology 40.The fast pyrolysis of imidazolate and gradual consumption of C by growing CNTs take place simultaneously,leading to the formation of the inner hollow structure 41.It is worth noting that the hollow structure is formed during the heat treatment process,as evident from the observationDOI:10.1038/NENERGY.2015.6C(002)Co(111)Pyridinic N 398.5 eVPyrrolic N 400.8 eVC−C 284.5 eV285.6 eVC=N 20I n t e n s i t y (a .u .)I n t e n s i t y (a .u .)I n t e n s i t y (a .u .)4060280285290Diffraction angle, 2 (°)θBinding energy (eV)395400405Binding energy (eV)Relative pressure (P /P 0)600400200V o l u m e a d s o r b e d (c m 3 g −1, S T P )abc dFigure 2|Compositional and structural information of NCNTFs obtained at 700◦C.a ,XRD pattern.b ,c ,High-resolution XPS spectra of C 1s (b )andN 1s (c ).In b ,the fitted peaks correspond to C–C (284.5eV)and C=N (285.6eV).In c ,the fitted peaks correspond to pyridinic N (398.5eV)and pyrrolic N (400.8eV).In b and c ,black traces are data,green and purple traces are fits to individual peaks,red traces are double-peak fits and blue traces are the background.d ,N 2adsorption–desorption isotherms.The inset of d shows the average pore size (7.8nm)and pore size distribution derived from the adsorption branch by the Barrett–Joyer–Halenda (BJH)method.of samples without the acid leaching treatment (Supplementary Figs 7and 8).Only polyhedron-shaped particles are obtained in the absence of H 2,even for pyrolysis temperatures up to 900◦C (Fig.3a,b),which is similar to previous reports about ZIF-derived nanocarbon composites (Supplementary Figs 9and 10)29,34,42.To better understand the evolution of NCNTFs,ZIF-67particles pyrolysed in the presence of H 2at different temperatures are further investigated.At a lower temperature of 600◦C,the surface of the framework nanoparticles shows some openings and numerous short CNTs clusters (Supplementary Fig.11),which are mainly attributed to the incomplete pyrolysis of ZIFs and insufficient growth of CNTs (Fig.3c).With the increase of temperature to 900◦C (Fig.3d),more complete pyrolysis allows the formation of longer CNTs with a higher density,while the surface of particles becomes much rougher (Supplementary Figs 12–15).It is therefore remarkably different from all previous reports of the formation of microporous nanocarbon and/or metal oxide nanocomposites by direct carbonization of MOFs under an inert atmosphere.Similar carbon nanotube frameworks can also be obtained when the present pyrolysis method is applied on other ZIF particles (Fig.4).Therefore,the current approach offers a versatile new strategy for the controlled design and synthesis of MOF-derived nanomaterials considering the large variety of MOFs particles available.Electrocatalyst activity and stabilityThe electrocatalytic activity of the as-prepared NCNTFs is first investigated by cyclic voltammetry (CV).As shown in Fig.5a,no obvious redox peak is observed for NCNTFs in N 2-saturated KOHsolution.In contrast,when the solution is saturated with O 2,a well-defined cathodic peak is clearly observed at ∼0.87V ,indicating the excellent electrocatalytic activity for the ORR.Linear sweep voltammetry (LSV)measurements at different rotation rates for all NCNTFs samples prepared at different temperatures are further conducted with a rotating disk electrode (RDE)set-up (Fig.5b and Supplementary Fig.16).Although all NCNTFs samples ex-hibit prominent catalytic activity for the ORR,the more positive onset potential of the NCNTFs sample obtained at 700◦C sug-gests its superior activity (Supplementary Fig.17a).The kinetic parameters are analysed by the Koutecky–Levich (K–L)equation (Supplementary Note 1),and the linearity of the K–L plots indicates the first-order reaction kinetics with regard to the concentration of dissolved oxygen and similar electron transfer numbers (n )at various potentials (Fig.5c).The value of n is calculated to be in the range 3.97–3.99for the potential range 0.3–0.7V ,which is close to the theoretical value of 4.00for Pt/C,indicating a complete 4e ORR pathway.The NCNTFs sample is benchmarked with a commercial Pt/C electrocatalyst for the ORR (Supplementary Fig.17b),which also exhibits a nearly 4e ORR pathway (n =3.96,Supplementary Fig.17c).Remarkably,the NCNTFs sample obtained at 700◦C ex-hibits higher ORR activity than the commercial Pt/C electrocatalyst in terms of half-wave potential (E 1/2;0.87V versus 0.84V in Fig.5d).The better ORR activity of the NCNTFs is further confirmed by a smaller Tafel slope (∼64mV decade −1versus ∼77mV decade −1for Pt/C,Supplementary Fig.17d).Importantly,the present NCNTFs material also exhibits attractive electrocatalytic activity in terms of the onset and half-wave potentials for the ORR among numerousDOI:10.1038/NENERGY.2015.6abc d Figure 3|Morphology and structural characterization of ZIF-derived composites.a –d ,FESEM images of ZIF-67heat-treated at 600◦C (a )and 900◦C (b )in the absence of H 2,and heat-treated at 600◦C (c )and 900◦C (d )in the presence of H 2.All scale bars are 500nm.nanocarbons reported so far and MOF-derived electrocatalysts (Supplementary Table 1and Supplementary Figs 18and 19).To monitor the hydrogen peroxide yield (%H 2O 2),rotating ring-disk electrode (RRDE)measurements are carried out and the results are presented in Fig.5e,f.In the potential range investigated,the yield of H 2O 2is below 1.6%and the calculated electron transfer number ranges from 3.96to 4.00(Supplementary Fig.20),which is consistent with the results obtained from the K–L plots based on RDE results (Fig.5c).Furthermore,unlike most non-Pt electrocatalysts,the NCNTFs catalyst also exhibits high ORR activity in 0.5M H 2SO 4solution,with an onset potential of ∼0.85V .The linearity of the K–L plots and the calculated electron transfer number of ∼3.88in acidic solution also confirm the excellent activity of the NCNTFs catalyst (Supplementary Fig.21).The possible fuel crossover effect and durability are important issues for cathodic catalysts in fuel cells.The fuel crossover effect is examined by cycling the NCNTFs and Pt/C catalysts from 0.2to 1.2V in both O 2-saturated 0.1M KOH and O 2-saturated 0.1M KOH +0.5M methanol solutions.No obvious change in the current density on the NCNTFs catalyst is observed with or without the presence of 0.5M methanol in the solution (Fig.6a),whereas for Pt/C,the cathodic ORR peak vanishes and one pair of anodic peaks at 1.09and 1.03V appears for the oxidation of methanol (Supplementary Fig.22).In addition,the chronoamperometric response at 0.6V is measured on both Pt/C and NCNTFs catalysts in O 2-saturated 0.1M KOH solution with a rotation rate of 1,600r.p.m.A significant decrease in the current density is observed upon the addition of 50ml of methanol in the case of the Pt/C catalyst,whereas the current density is not sensitive to the addition of methanol for the NCNTFs catalyst (Fig.6b).The above results indicate that the NCNTFs catalyst has excellent tolerance to methanol crossover.Furthermore,the short-term stability of NCNTFs and Pt/C catalysts are investigated at 0.6V for 100,000s in O 2-saturated 0.1M KOH solution with a rotation rate of 1,600r.p.m.(Fig.6c).During the period,about 96%of the original current density is retained for the NCNTFs electrode,whereas the Pt/C electrode shows a much higher current loss of ∼29%,suggesting the superior stability of the former.The NCNTFs catalyst is further subjected to a CV test from 0.2to 1.2V for 5,000cycles.LSV curves of NCNTFs show negligible performance loss after the test (Supplementary Fig.23a).There is only a negative shift of ∼7mV in the E 1/2value at 1,600r.p.m.(Fig.6d)and theTafelabc dFigure 4|Morphology and structural characterization of di erentZIF-derived NCNTFs.a ,b ,FESEM images of NCNTFs obtained from ZIF-67with sizes of ∼500nm (a )and ∼1.5µm (b )in the presence of H 2.c ,d ,FESEM images of NCNTFs derived from ZIFs prepared with di erent molar ratios of Co and 2-methylimidazole:1:2(c )and 1:4(d )in the presence of H 2.All scale bars are 500nm.slope remains virtually unchanged (Supplementary Fig.23b).The excellent stability of NCNTFs is ascribed to the robust framework structure composed of interconnected crystalline NCNTs,which retains its original morphology and structure after the cycling test,as confirmed by TEM analysis (Supplementary Fig.23c,d).The oxygen evolution activities of the NCNTFs and Pt/C catalysts are also investigated and compared.As shown in Fig.7a,the NCNTFs catalyst gives a current density of 10mA cm −2(based on geometric electrode area)at a potential of 1.60V versus reversible hydrogen electrode (RHE),which compares favourably to other reported nanocarbon-based catalysts (Supplementary Table 2)and IrO 2/C catalyst (10mA cm −2,1.60V;ref.22).For the Pt/C catalyst,the potential required to generate a current density of 10mA cm −2is about 1.78V ,roughly ∼180mV higher than that of NCNTFs.The current density is also normalized by the specific surface area and electrochemical active surface area,and the results show a similar trend (Supplementary Figs 24and 25).The much smaller Tafel slope of NCNTFs further confirms the superior electrochemical OER performance compared to that of the Pt/C catalyst (93versus 118mV decade −1in Fig.7b).The OER activity of different NCNTFs catalysts prepared at various temperatures is given in Fig.7c and further compared with other MOF-derived materials (Supplementary Fig.26).Again the sample obtained at 700◦C exhibits the best OER activity,as it requires the smallest overpotential to achieve the same current density (for example,10mA cm −2).The stability test results demonstrate that the NCNTFs catalyst is very stable for the OER (Fig.7d and Supplementary Fig.27),whereas Pt/C exhibits a continuous current loss during the stability test.These results suggest that the NCNTFs material is an efficient bifunctional electrocatalyst for reversible oxygen reduction and evolution (Supplementary Tables 1and 2).Mechanistic study on electrocatalyst activityThe superior electrocatalytic activities of NCNTFs may mainly be attributed to the chemical composition and structure of the NCNTs formed as well as the overall framework structure.In the synthesis,the pyrolysis temperature is clearly a critical factor here.In general,as the pyrolysis temperature is increased from 700to 1,000◦C,the electrocatalytic activity of resultant NCNTFs decreases,as seen from the negative shift of E 1/2and the decreased current densityDOI:10.1038/NENERGY.2015.610−2−10−2−4−60.20.40.60.8 1.0 1.2Potential (V versus RHE)Potential (V versus RHE)20150105O 2N 20.60.40.2−1/2 (s 1/2 rad −1/2)ωaj (m A c m −2)j (μA c m −2)j (m A c m −2)j −1 (m A −1 c m 2)cebFigure 5|and O 2-saturated of Pt/C and Potential (V versus RHE)Potential (V versus RHE)−2−4−6100050Time (s)30,00060,00090,000Time (s)NCNTFs Pt/C96%71%R e l a t i v e j (%)j (m A c m −2)cdFigure 6|Electrochemical methanol tolerance and durability of NCNTFs obtained at 700◦C.a ,CV profiles (black and red curves indicate CV curves recorded in O 2-saturated 0.1M KOH and O 2-saturated 0.1M KOH +0.5M CH 3OH solution,respectively).b ,Chronoamperometric response at 0.6V after the introduction of 50ml of methanol into 150ml of 0.1M KOH solution.c ,Chronoamperometric response at 0.6V.d ,ORR polarization curves (1,600r.p.m.)of NCNTFs before and after 5,000cycles.of the ORR (Supplementary Fig.17a).This may be related to the lower defect density generated as a result of the higher pyrolysis tem-perature (Supplementary Fig.3b).These defect sites are normally believed to be more active than basal planes (Fig.1e,f).Moreover,the N-doping level also decreases with the increase of pyrolysis temperature due to the instability of N atoms at high temperature,as determined by XPS (Supplementary Figs 3c,d and 4).The N doping not only induces the electronic interaction with nearby carbon/metal atoms to provide catalytically active sites,but alsoproduces structural defects in CNTs to form the O 2adsorption sites 43,44.However,NCNTFs obtained at 600◦C have the highest N-doping content and defect density,but exhibit the lowest ac-tivity,which might be explained by the incomplete pyrolysis of ZIFs (ref.45).Moreover,the residual metallic Co nanoparticles encapsulated by carbon shells are also believed to play an important role in the excellent electrocatalytic activity 46.It has been previously reported that nanocarbon electrocatalysts have enhanced activity in the presence of metallic nanoparticles owing to the electronicDOI:10.1038/NENERGY.2015.61.01.21.41.61.8Potential (V versus RHE)1.01.21.41.61.8Potential (V versus RHE)P o t e n t i a l (V v e r s u s R H E )20406002040601004080Time (s)60−0.50.00.51.01.5log |j | (mA cm −2)1.41.61.8Pt/C Pt/C NCNTFsNCNTFs1,000 °C 900 °C 800 °C 700 °C 600 °C10 mA cm −2118 mV d ec ad e−193 mV d ec ade −1aj (m A c m −2)j (m A c m −2)R e l a t i v e j (%)bcdFigure 7|Electrochemical oxygen evolution on NCNTFs.a ,LSV curves of NCNTFs (red)and Pt/C (black)catalysts.b ,Tafel slopes of NCNTFs (red)and Pt/C (black)catalysts.c ,LSV curves of NCNTFs catalysts synthesized at di erent temperatures.d ,Chronoamperometric response at 1.7V.interaction between metal nanoparticles and CNTs (refs 23,47,48).Furthermore,the high surface area and three-dimensional hier-archical porous hollow structure are also beneficial for enhanced mass transport during the electrochemical reaction 49,50.The robust framework structure consisting of interconnected NCNTs is also very critical for the enhanced electrocatalytic activity and stability,because they give excellent conductivity and remarkable corrosion resistance in a harsh operating environment.ConclusionsIn summary,starting with ZIF-67particles as the single precursor,we synthesize a hollow framework constructed from interconnected crystalline NCNTs as an efficient and stable bifunctional electrocatalyst for the ORR and the OER.During the pyrolysis synthesis,ZIF-67particles not only provide the C and N source for growth of NCNTs catalysed by the in-situ -formed metallic Co nanoparticles but also serve as the template for the formation of the hollow framework.The as-prepared NCNTFs exhibit remarkable electrocatalytic activity and stability,and even outperform a commercial Pt/C electrocatalyst as a bifunctional electrocatalyst.The exceptional electrocatalytic activity might be mainly attributed to the chemical composition and structure of the crystalline NCNTs formed,as well as their robust overall framework structure.The facile strategy demonstrated here can be applied for the preparation of many other MOF-derived functional nanomaterials and opens up a new avenue for developing highly active MOF-derived electrocatalysts for different electrochemical energy technologies.MethodsSynthesis of ZIF-67particles.In a typical synthesis,2-methylimidazole (1.97g)is dissolved in a mixed solution of 20ml of methanol and 20ml of ethanol.Co(NO 3)2·6H 2O (1.746g)is dissolved in another mixed solution of 20ml of methanol and 20ml of ethanol.The above two solutions are then mixed under continuous stirring for 10s,and the final solution is kept for 20h at room temperature.The purple precipitate is collected by centrifugation,washed in ethanol several times and dried at 80◦C.Other ZIF particles are also obtained using the same method,except for the use of different molar concentrations of Co(NO 3)2·6H 2O and 2-methylimidazole.All chemicals are used as received.Synthesis of hollow NCNTFs.The ZIF-67particles are dispersed in a ceramic boat,heated to 350◦C and maintained for 1.5h in a tube furnace.Thetemperature in the furnace is further raised to a set temperature (600,700,800,900,and 1,000◦C)at a ramp rate of 2◦C min −1and kept at that temperature for 3.5h.After that,the furnace is cooled down to room temperature naturally.During the pyrolysis process,the furnace is under Ar/H 2flow (90%/10%in volume ratio).The as-prepared black powder products are treated in 0.5M H 2SO 4solution for 6h.The resulting samples are collected by centrifugation,repeatedly washed with DI water,then dried at 80◦C.Materials characterizations.The morphologies and structures are characterized by field-emission scanning electron microscopy (FESEM;JEOL,JSM-6701F,5kV)and transmission electron microscopy (TEM;JEOL,JEM-2010,200kV).Powder X-ray diffraction (XRD)patterns are recorded using a Bruker diffractometer with Cu K αradiation (D8Advance X-ray diffractometer,Cu K α,λ=1.5406Å,40kV and 40mA)to study the crystallographic structure.The N 2sorption isotherms are collected using a Quantachrome Instruments Autosorb AS-6B atliquid-nitrogen temperature.Raman spectra are collected using a Renishaw System 1000micro-Raman spectroscope (Renishaw).The surface properties of the samples are analysed by X-ray photoelectron spectroscopy (XPS;VGESCALAB MKII instrument)with a Mg K αX-ray source.Before the analysis,all the samples are dried under vacuum at 80◦C.Thermogravimetric analysis (TGA,Perkin Pyris Diamond)is performed under air flow (200ml min −1)with a temperature ramp of 10◦C min −1.Electrochemical measurements.All electrocatalytic measurements are carried out in a three-electrode cell using a rotating disk electrode (RDE,PINE Research Instrumentation)with an Autolab bipotentiostat (Model PGSTAT-72637)workstation at ambient temperature.A platinum foil and Ag/AgCl (3.0M KCl)are used as the counter and reference electrodes,respectively.All potentials in this study refer to RHE,E (RHE)=E (Ag/AgCl)+0.059×pH +0.210.A RDE with glassy carbon (GC)disk electrode (5mm in diameter)and a rotating ring-disk electrode (PINE AFE6R2GCPT)with a Pt ring (6.5mm inner diameter and 8.5mm outer diameter)and a GC disk (5.5mm diameter)are used as the substrate for the working electrodes.Before use,the GC electrodes in RDE/RRDE are polished using aqueous alumina suspension on felt polishing pads.The catalyst suspension is prepared by dispersing 5mg of catalyst in 1ml of solution containing 0.98ml of ethanol and 20µl of 0.5wt%Nafion solution,followed by ultrasonication for 30min.Then a certain volume of catalyst suspension is pipetted onto the GC surface to give a 0.2mg cm −2loading for all samples including commercial Pt/C (40wt%,Johnson Matthey).Before tests,N 2/O 2flow is used through the electrolyte in the cell to achieve the N 2/O 2-saturated solution.The cyclic voltammetry (CV)profiles are obtained in N 2-or O 2-saturated 0.1M KOH。

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