Extended Data: Safety issues caused by internal short circuits. in lithium-ion batteries
|
|
- Cassandra Walton
- 5 years ago
- Views:
Transcription
1 Electronic Sulementary Material (ESI) for Journal of Material Chemitry A. Thi journal i The Royal Society of Chemitry 18 Extended Data: Safety iue caued by internal hort circuit in lithium-ion batterie 1 Introduction Abuive condition, uch a mechanical loadin, over-heat and over-chare oe a threatenin ituation for the otential hazardou cenario for LIB. Thoe neative effect may directly trier the ISC for the cell, followed by a equence of hyical, chemical and electrical chane for the material (Fi. S1). With the onet of ISC, roduced heat by ohm law raie the temerature. SEI (Solid-Electrolyte-Interhae) may reolve above 9, followed by the inerted lithium in anode reaction with electrolyte. Searator uually tart to melt from 1. Decomoition of electrolyte initiate at around and binder for the active article on electrode involve into reaction above 6. Above 66, Al collector tart meltin. Whether there i a afety boundary/vicinity if the ISC i triered and how many tyical tye of electrochemical behavior of cell after ISC till remain unknown. 1
2 Fi. S1. Phyical an chemical roce of internal hort-circuit of lithium battery. Exerimental.1. Penetration tet. Four reeated tet were conducted to make ure the reeatability and confidence of the indentation tet to trier the ISC (Fi. S). The hihly conitent reult aain directly rove the credibility of uch methodoloy.
3 Fi. S. Reeated exeriment reult for Hih SOC (95%) batterie. Table S1. Secification of equiment for exeriment of Cae 1 and. Equiment Tye Rane Frequency Preciion Reolution ratio Univeral material tetin machine INSTRON 45 ±5 kn 1 Hz ±(5% RD +.5% 1 kn) 5 N Diital voltmeter Multi-channel temerature enor Battery erformance Ailent 441A ~1 V Hz ±(.15 RD ANBAI AT458 ~ 1 BK688AR ~5 V ~5 A +.4ΔT).1 mv 1 Hz ±..1 1 Hz ±(.5%RD +.5%FS) 1 mv 1 ma
4 tetin machine.. Contact reitance meaurement exeriment. The relationhi between contact reitance and contact tre wa hown in Fi.S. Fi. S. contact tre -reitance curve.. Modelin and calibratin FE of LIB Fi. S4. The comarion of exeriment and imulation for (a) cathode comreion, (b) cathode tenion, (c) anode comreion, (d) anode tenion, (e) earator tenion, (f) cover hell tenion. 4
5 Table S Parameter and etu for mechanical model of LIB Cover Material Al latic film Thickne Mechanical Youn Modulu Yield tre (um) model (MPa) (MPa) 76 Elatic-latic Hardenin curve (MPa) Element tye cov cov cov S4R Searator PP 8 Elatic-latic e e e CD8R Current collector (Anode) Current collector (cathode) Cu 6 Elatic-latic 744. Al 1 Elatic-latic 5 6. ncc ncc ncc S4R cc cc cc S4R Anode LiC x 14 Cruhable foam ne ne cc. CD8R Cathode LiCoO 17 Cruhable foam 5.1 o o o CD8R 5
6 4. Multi-hyic method of LIB Fi. S. Comarion reult for exeriment and imulation for LIB durin dichare. 6
7 Table S Governin equation of all ub-model Model Function name Function Cell otential E E E cell, o, ne o ne l v v v Cell current i cell R l ol r A cell e cell, I A i, e e V L e cell e cell A Chare balance i ò A cell v, miloc, m A, i V m v dl dl r c c D t r r c, D R, r rr Diffuion equation c r r Battery model 1- R v, m n F N v Am / r m m hae E Q A i E E T eq eq, m ò v, m loc, m(, m ) m T, Battery heat Q ol i V l cell cell A e Q Q Q Q ba ne o ol Thermal runaway model 4, 5 Electrode kinetic exreion SEI decomoition l o ( ) ne ne a ( ) o ( max ) ne c i F k k c c ( c ) o ( ) l c i loc ne o F F i ex ex RT RT ei ei ei ei Ea Q H Wc A ex[ ] c dc dt ei A ei ei Ea ex[ ] c ei ei, ref 7
8 ae dca ae z Ea A ex[ ]ex[ ] c dt z a anode electrolyte reaction ae a-e ae ae z Ea c z RT Q H W A ex[ ]ex[ ] c a ae dz a-e z Ea A ex[ ]ex[ ] c dt z a cathode electrolyte reaction electrolyte decomoition reaction thermal runaway heat Q H W A ce E (1 )ex[ ] ce ce ce ce ce a d dt ce A ce E (1 )ex[ ] ce ce ce a e e e e Ea Q H We A ex[ ] c dc dt tr e e e Ea A ex[ ] ce Q Q Q Q Q ei a e ce e e Mechanical model 6 Governin u ( F ) F X L S equation t Governin equation j= St r Q, r r j j r t St V Short circuit model 6, 7 Thermal model 4, 8 Meltin of earator and current collector Electric conductivity Governin equation dc dt dc dt A e E ex[ ] c e e a cc A cc cc Ea ex[ ] c cc cc cc, e *(1 ce ) c cc e cc e e e e ( T C ),, u T q Q q kt t 8
9 Q = Q Q Q ba t tr Boundary condition cell -nq h ( T T ) fl amb nq 4 4 df Df B D ( Tamb T ), Nomenclature A : Arrheniu contant (1) A v: active ecific urface area c: concentration ( mol/m ) c ei : dimenionle amount of lithium-containin metatable ecie in the olid electrolyte interhae (SEI) (1) : initial value of the dimenionle amount of lithium-containin metatable ecie in c ei the SEI (1) c a c a : dimenionle amount of lithium intercalated within carbon (1) : initial value of the dimenionle amount of lithium intercalated within carbon (1) c cc : dimenionle amount of olid hae of current collector (1) : dimenionle concentration of electrolyte (1) c e : initial value of the dimenionle concentration of electrolyte (1) c e c e : dimenionle amount of olid hae of earator (1) C : heat caacity ( J/(k K) ) D: diffuion coefficient ( m / ) E : Youn modulu (MPa) 9
10 E E a : Potential (V) : exerimental activation enery (J/mol) 4 F : Faraday contant ( C/mol ) H : heat tranfer coefficient(j/) h : heat tranfer coefficient ( W/(m K) ) I : current (A) i : current denity ( A/m ) i : exchane current denity ( A/m ) i loc : local intercalation current denity ( A/m ) i dl : double layer current denity ( A/m ) k: thermal conductivity ( W/(m K) ) SOC : tate of chare value t : time () t + : tranfer data W c W : volume-ecific carbon content ( /m ) : volume-ecific oitive active content ( /m ) W e volume-ecific electrolyte content in the jellyroll ( /m ) z : dimenionle meaure of the SEI layer thickne (1) z : reference dimenionle meaure of the SEI layer thickne (1) Q : heat ource ( W/m ) 1
11 Qba : heat for battery model ( W/m ) Qt : heat from the hort-circuit model ( W/m ) Qtr : heat from the thermal runaway model ( W/m ) q: heat flux ( W/m ) q fl : heat flux by conduction ( W/m ) q df R : heat flux by radiation ( W/m ) : radiu (mm) R Rr : a contant : reitance ( ) : molar flux of lithium at the article urface R : tranfer data t T: temerature (K) T abm : Ambient temerature : converion deree (1) : initial value of the converion deree (1) m : ratio of tenion and comreion (1) : denity ( k/m ) 8 4 B D : Stefan Boltzmann contant ( W/(m K ) ) : yield tre (MPa) : latic train (1) 11
12 : thickne (mm) ò: volume fraction : train (1) Df : urface emiivity (1) : electrical conductivity (S/m) : initial electrical conductivity (S/m) e : electrical conductivity after meltin (S/m) : Poion ratio :Stoichiometric coefficient of the intercalatin ecie v : otential (V) dlnf 1 d ln l c : molar activity coefficient Subcrit eff: modified Suercrit a-e: anode electrolyte reaction c-e: cathode electrolyte reaction cell: the cell (LIB) cov: cover hell 1
13 e: electrolyte decomoition eq: equilibrium D: diffuion LB: lithium-ion battery l: liquid (electrolyte) ncc: neative collector ne: neative electrode cc: oitive collector o: oitive electrode ei: SEI decomoition reaction : olid (electrode) e: earator ol: olution St: hort-circuit model 1
14 Sulementary Video Video 1. Exeriment roce of triered internal hort-circuit and thermal runway of lithium-ion ouch cell at 95% SOC. Video. Multihyic ub-model imulation roce of lithium-ion ouch cell with 95% SOC by mechanical indentation. Video. Multihyic ub-model imulation roce of lithium-ion ouch cell with 6% SOC by mechanical indentation. Reference 1. C. M. Doyle, T. F. Fuller and J. S. Newman, Journal of The Electrochemical Society, 199, 14, T. F. Fuller, M. Doyle and J. Newman, Journal of the Electrochemical Society, 1994, 141, C. M. Doyle, Doctor, Univerity of California, T. D. Hatchard, D. D. Macneil, A. Bau and J. R. Dahn, Journal of the Electrochemical Society, 1, 148, A755-A G. H. Kim, A. Pearan and R. Sotnitz, J. Power Source, 7, 17, B. Liu, H. Zhao, H. Yu, J. Li and J. Xu, Electrochimica Acta, 17, DOI: htt://doi.or/1.116/j.electacta B. Liu, S. Yin and J. Xu, Alied Enery, 16, 18, K.-C. Chiu, C.-H. Lin, S.-F. Yeh, Y.-H. Lin and K.-C. Chen, J. Power Source, 14, 51,
A Single Particle Thermal Model for Lithium Ion Batteries
A Single Particle Thermal Model for Lithium Ion Batterie R. Painter* 1, B. Berryhill 1, L. Sharpe 2 and S. Keith Hargrove 2 1 Civil Engineering, Tenneee State Univerity, Nahville, TN, USA 2 Mechanical
More informationTemperature Sensitive Paint Heat Flux Measurements in Hypersonic Tunnels
Temerature Senitive Paint Heat Flux Meaurement in Hyeronic Tunnel Tianhu Liu, Z. Cai, B. Wang Wetern Michigan Univerity, Kalamazoo, MI 49008 J. Rubal, J. P. Sullivan, S. Schneider Purdue Univerity, Wet
More informationUSE OF INTERNET TO DO EXPERIMENTS IN DYNAMICS AND CONTROL FROM ZACATECAS MEXICO IN THE LABORATORY OF THE UNIVERSITY OF TENNESSEE AT CHATANOOGAA.
USE OF INTERNET TO DO EXPERIMENTS IN DYNAMICS AND CONTROL FROM ZACATECAS MEXICO IN TE LABORATORY OF TE UNIVERSITY OF TENNESSEE AT CATANOOGAA. Jim enry *, Joé Alberto González Guerrero, Benito Serrano Roale..
More informationOnline supplementary information
Electronic Supplementary Material (ESI) for Soft Matter. Thi journal i The Royal Society of Chemitry 15 Online upplementary information Governing Equation For the vicou flow, we aume that the liquid thickne
More informationPerformance Modeling of the Metal Hydride Electrode
Performance Modeling of the Metal Hydride Electrode by Bala S. S. Haran, Anand Durairajan, Branko N. Popov and Ralph E. E. White Center for Electrochemical Engineering Department of of Chemical Engineering
More informationChapter 3- Answers to selected exercises
Chater 3- Anwer to elected exercie. he chemical otential of a imle uid of a ingle comonent i gien by the exreion o ( ) + k B ln o ( ) ; where i the temerature, i the reure, k B i the Boltzmann contant,
More informationQ.1. x A =0.8, ε A =δ A *y A = 0.8*5=4 (because feed contains 80 mol% A, y A = 0.8, δ A =((6-1)/1)=5) k= 0.3 hr -1. So, θ = hr Q.
Q.1 k [ 1 ln(1 x)] x x =.8, ε =δ *y =.8*5=4 (becaue feed contain 8 mol%, y =.8, δ =((6-1)/1)=5) k=. hr -1 So, θ = 16.157 hr Q.2 Q.2 Continue (c) V PFR
More informationUncertainty Analysis in Potential Transformer Calibration Using a High Voltage Capacitance Bridge
Journal of Electrical Engineering & Technology, ol., No. 3,. 4~47, 4 Uncertainty Analyi in Potential Tranformer Caliration Uing a High oltage Caacitance Bridge Jae Ka Jung, Sang Hwa Lee*, Jeon Hong Kang*,
More informationParameter Sensitivity Analysis to Improve Material Design for Novel Zn-MnO 2 Batteries with Ionic Liquid Electrolytes
Parameter Senitivity Analyi to Improve Material Deign for Novel Zn-MnO Batterie with Ionic Liquid Electrolyte Zachary T. Gima & Bernard J. Kim CE 95: Spring 06 Abtract Battery deign at the material level
More informationUNITS FOR THERMOMECHANICS
UNITS FOR THERMOMECHANICS 1. Conitent Unit. Every calculation require a conitent et of unit. Hitorically, one et of unit wa ued for mechanic and an apparently unrelated et of unit wa ued for heat. For
More informationÜbung zu Globale Geophysik I 05 Answers
Übung zu Globale Geohyik I 05 Anwer Übung zu Globale Geohyik I: Wedneday, 6:00 8:00, Thereientr. 4, Room C49 Lecturer: Heather McCreadie Comanion cla to Globale Geohyik I: Monday, :00 4:00, Thereientr.
More informationSoftware Verification
EXAMPLE 17 Crack Width Analyi The crack width, wk, i calculated uing the methodology decribed in the Eurocode EN 1992-1-1:2004, Section 7.3.4, which make ue of the following expreion: (1) w = ( ),max ε
More informationME 315 Exam 3 8:00-9:00 PM Thursday, April 16, 2009 CIRCLE YOUR DIVISION
ME 315 Exam 3 8:00-9:00 PM Thurday, Aril 16, 009 Thi i a cloed-book, cloed-note examination. There i a formula heet at the back. You mut turn off all communication device before tarting thi exam, and leave
More informationPelagia Research Library. Acetaldehyde combustion using platinum catalyst
Available online at www.pelaiareearchlibrary.com Pelaia Reearch Library Der Chemica Sinica, 11, (1): 164-17 Acetaldehyde combution uin platinum catalyt Sanchita Chauhan ISSN: 976-855 CODEN (USA) CSHIA5
More informationNumerical Investigation of Heat Transfer and Fluid Flow around the Rectangular Flat Plane Confined by a Cylinder under Pulsating Flow
Journal of Alied Fluid Mechanic, Vol. 9, No.,. 1569-1577, 216. Available online at www.jafmonline.net, ISSN 1735-3572, EISSN 1735-365. DOI: 1.18869/acadub.jafm.68.235.21 Numerical Invetigation of Heat
More informationMass Transfer (Stoffaustausch) Fall Semester 2014
Ma Tranfer (Stoffautauch) Fall Semeter 4 Tet 5 Noember 4 Name: Legi-Nr.: Tet Duration: 45 minute Permitted material: NOT permitted: calculator copy of Culer book Diffuion ( nd or rd edition) printout of
More informationThe International Association for the Properties of Water and Steam
IAPWS SR7-9 he International Aociation for the Proertie of Water and Steam Doorwerth, he Netherland Setember 9 Sulementary Releae on a Comutationally Efficient hermodynamic Formulation for Liquid Water
More informationModeling of Transport and Reaction in a Catalytic Bed Using a Catalyst Particle Model.
Excerpt from the Proceeding of the COMSOL Conference 2010 Boton Modeling of Tranport and Reaction in a Catalytic Bed Uing a Catalyt Particle Model. F. Allain *,1, A.G. Dixon 1 1 Worceter Polytechnic Intitute
More informationDepartment of Chemical and Biomolecular Engineering, University of California, Berkeley, CA, 94720
Supporting Information for The Most Promising Routes to a High Li + Transference Number Electrolyte for Lithium Ion Batteries Kyle M. Diederichsen, Eric J. McShane, Bryan D. McCloskey* Department of Chemical
More informationFluid-structure coupling analysis and simulation of viscosity effect. on Coriolis mass flowmeter
APCOM & ISCM 11-14 th December, 2013, Singapore luid-tructure coupling analyi and imulation of vicoity effect on Corioli ma flowmeter *Luo Rongmo, and Wu Jian National Metrology Centre, A*STAR, 1 Science
More informationLecture 15 - Current. A Puzzle... Advanced Section: Image Charge for Spheres. Image Charge for a Grounded Spherical Shell
Lecture 15 - Current Puzzle... Suppoe an infinite grounded conducting plane lie at z = 0. charge q i located at a height h above the conducting plane. Show in three different way that the potential below
More informationDevelopment of First Principles Capacity Fade Model for Li-Ion Cells
A196 Journal of The Electrochemical Society, 151 2 A196-A203 2004 0013-4651/2004/151 2 /A196/8/$7.00 The Electrochemical Society, Inc. Development of First Principles Capacity Fade Model for Li-Ion Cells
More informationConstitutive models. Part 2 Elastoplastic
Contitutive model art latoplatic latoplatic material model latoplatic material are aumed to behave elatically up to a certain tre limit after which combined elatic and platic behaviour occur. laticity
More informationVolume IV, Issue IX, September 2015 IJLTEMAS ISSN
Volume IV, Iue IX, Setember 15 IJLEMAS ISSN 78-54 A Comutational Study of A Multi Solid Wall Heat Conduction Made U of Four Different Building Contruction Material Subected to Variou hermal Boundary Condition.
More informationA Boundary Condition for Porous Electrodes
Electrochemical Solid-State Letters, 7 9 A59-A63 004 0013-4651/004/79/A59/5/$7.00 The Electrochemical Society, Inc. A Boundary Condition for Porous Electrodes Venkat R. Subramanian, a, *,z Deepak Tapriyal,
More informationHeat Transfer Modeling Within Graphite/PCM Composite Materials For High Temperature Energy Storage
OJE DISOR Heat raner Modelin Within Graphite/PCM Compoite Material For Hih emperature Enery Storae V. Morion, E. Palomo Del Bario, M. Rady Ecotock - Pomona - 31 May 2 June 26 Context o the Project DISOR
More informationA novel protocol for linearization of the Poisson-Boltzmann equation
Ann. Univ. Sofia, Fac. Chem. Pharm. 16 (14) 59-64 [arxiv 141.118] A novel protocol for linearization of the Poion-Boltzmann equation Roumen Tekov Department of Phyical Chemitry, Univerity of Sofia, 1164
More informationThe Correlation of the Performance of Duct Lining Materials with Their Normal Incidence Properties
Purdue Univerity Purdue e-pub Publication of the Ray W. Herrick Laboratorie School of Mechanical Engineering 8-005 The Correlation of the Performance of Duct Lining Material with Their Normal Incidence
More informationLecture 23 Date:
Lecture 3 Date: 4.4.16 Plane Wave in Free Space and Good Conductor Power and Poynting Vector Wave Propagation in Loy Dielectric Wave propagating in z-direction and having only x-component i given by: E
More informationChapter 7. Principles of Unsteady - State and Convective Mass Transfer
Suppleental Material for Tranport Proce and Separation Proce Principle hapter 7 Principle of Unteady - State and onvective Ma Tranfer Thi chapter cover different ituation where a tranfer i taking place,
More information2.7 Aerosols and coagulation
1 Note on 1.63 Advanced Environmental Fluid Mechanic Intructor: C. C. Mei, 1 ccmei@mit.edu, 1 617 53 994 December 1,.7 Aerool and coagulation [Ref]: Preent, Kinetic Theory of Gae Fuch, Mechanic of Aerool
More informationProposal of the Thin Film Pirani Vacuum Sensor Still Sensitive Above 1 Atmosphere ABSTRACT INTRODUCTION
P1.11 Propoal of the Thin Film Pirani Vacuum Senor Still Senitive Above 1 Atmophere Takahima Noriaki and Kimura Mituteru Faculty of Engineering, Tohoku Gakuin Univerity 13-1, Chuo-1, Tagajo, Miyagi, 985-8537,
More informationBattery Design Studio Update
Advanced Thermal Modeling of Batteries Battery Design Studio Update March 20, 2012 13:30 13:55 New Features Covered Today 3D models Voltage dependent diffusion Let s start with brief introduction to Battery
More information18 Problem 1. 7 d Sketch a cross section of a switched reluctance machine and explain the principle of operation.
Exam Electrical Machine and Drive (ET4117) 9 November 01 from 14.00 to 17.00. Thi exam conit of 3 roblem on 3 age. Page 5 can be ued to anwer roblem 4 quetion a. The number before a quetion indicate how
More informationRADIATION THERMOMETRY OF METAL IN HIGH TEMPERATURE FURNACE
XVII IMEKO World Congre Metrology in the 3rd Millennium June 22 27, 2003, Dubrovnik, Croatia RADIATION THERMOMETRY OF METAL IN HIGH TEMPERATURE FURNACE Tohru Iuchi, Tohru Furukawa and Nobuharu Sato Deartment
More informationBASIC INDUCTION MOTOR CONCEPTS
INDUCTION MOTOS An induction motor ha the ame phyical tator a a ynchronou machine, with a different rotor contruction. There are two different type of induction motor rotor which can be placed inide the
More informationParticle to Gas Heat Transfer in a Circulating Fluidized Bed Riser
Enineerin Conference International ECI Diital Archive 10th International Conference on Circulatin Fluidized Bed and Fluidization echnoloy - CFB-10 Refereed Proceedin Srin 5-3-2011 Particle to Ga Heat ranfer
More informationChapter 2 Homework Solution P2.2-1, 2, 5 P2.4-1, 3, 5, 6, 7 P2.5-1, 3, 5 P2.6-2, 5 P2.7-1, 4 P2.8-1 P2.9-1
Chapter Homework Solution P.-1,, 5 P.4-1, 3, 5, 6, 7 P.5-1, 3, 5 P.6-, 5 P.7-1, 4 P.8-1 P.9-1 P.-1 An element ha oltage and current i a hown in Figure P.-1a. Value of the current i and correponding oltage
More informationCapacity fade studies of Lithium Ion cells
Capacity fade studies of Lithium Ion cells by Branko N. Popov, P.Ramadass, Bala S. Haran, Ralph E. White Center for Electrochemical Engineering, Department of Chemical Engineering, University of South
More informationME 3560 Fluid Mechanics
Sring 018 ME 3560 Fluid Mechanic Chater III. Elementary Fluid Dynamic The Bernoulli Equation 1 Sring 018 3.1 Newton Second Law A fluid article can exerience acceleration or deceleration a it move from
More informationSimulation of Wound Rotor Synchronous Machine under Voltage Sags
Simulation of Wound Rotor Synchronou Machine under oltage Sag D. Aguilar, G. azquez, Student Member, IEEE, A. Rolan, Student Member, IEEE, J. Rocabert, Student Member, IEEE, F. Córcole, Member, IEEE, and
More informationPhysics 2212 G Quiz #2 Solutions Spring 2018
Phyic 2212 G Quiz #2 Solution Spring 2018 I. (16 point) A hollow inulating phere ha uniform volume charge denity ρ, inner radiu R, and outer radiu 3R. Find the magnitude of the electric field at a ditance
More informationImproved Adaptive Time Delay Estimation Algorithm Based on Fourth-order Cumulants
Available online www.jocr.com Journal of hemical and Pharmaceutical Reearch, 016, 8(5):889-894 Reearch Article ISSN : 0975-784 ODEN(USA) : JPR5 Imroved Adative Time Delay Etimation Algorithm Baed on Fourth-order
More informationLiquid cooling
SKiiPPACK no. 3 4 [ 1- exp (-t/ τ )] + [( P + P )/P ] R [ 1- exp (-t/ τ )] Z tha tot3 = R ν ν tot1 tot tot3 thaa-3 aa 3 ν= 1 3.3.6. Liquid cooling The following table contain the characteritic R ν and
More informationBasics of a Quartz Crystal Microbalance
Baic of a Quartz Crytal Microbalance Introduction Thi document provide an introduction to the quartz crytal microbalance (QCM) which i an intrument that allow a uer to monitor mall ma change on an electrode.
More informationMODELLING OF FRICTIONAL SOIL DAMPING IN FINITE ELEMENT ANALYSIS
MODELLING OF FRICTIONAL SOIL DAMPING IN FINITE ELEMENT ANALYSIS S. VAN BAARS Department of Science, Technology and Communication, Univerity of Luxembourg, Luxembourg ABSTRACT: In oil dynamic, the oil i
More informationStress analysis of lithium-based rechargeable batteries using micro and macro scale analysis
Stress analysis of lithium-based rechargeable batteries using micro and macro scale analysis Utsav Kumar Atanu K. Metya Jayant K. Singh Department of Chemical Engineering IIT Kanpur INTRODUCTION Christensen
More informationElectrical Conduction. Electrical conduction is the flow of electric charge produced by the movement of electrons in a conductor. I = Q/t.
Electrical Conduction e- in wire e- out Electrical conduction is the flow of electric charge produced by the movement of electrons in a conductor. The rate of electron flow (called the current, I, in amperes)
More informationEELE 3332 Electromagnetic II Chapter 10
EELE 333 Electromagnetic II Chapter 10 Electromagnetic Wave Propagation Ilamic Univerity of Gaza Electrical Engineering Department Dr. Talal Skaik 01 1 Electromagnetic wave propagation A changing magnetic
More informationLecture 7 Grain boundary grooving
Lecture 7 Grain oundary grooving The phenomenon. A polihed polycrytal ha a flat urface. At room temperature, the urface remain flat for a long time. At an elevated temperature atom move. The urface grow
More informationRecent progress in fire-structure analysis
EJSE Special Iue: Selected Key Note paper from MDCMS 1 1t International Conference on Modern Deign, Contruction and Maintenance of Structure - Hanoi, Vietnam, December 2007 Recent progre in fire-tructure
More informationNUMERICAL SIMULATION OF DESICCATION CRACKING PROCESS BY WEAK COUPLING OF DESICCATION AND FRACTURE
Geotec., Cont. Mat. & Env., ISSN:86-990, Japan, DOI: http://dx.doi.org/0.660/07.33.535 NUMERICAL SIMULATION OF DESICCATION CRACKING PROCESS BY WEAK COUPLING OF DESICCATION AND FRACTURE *Sayako Hirobe and
More informationSTUDY OF THE INFLUENCE OF CONVECTIVE EFFECTS IN INCIDENT RADIATIVE HEAT FLUX DENSITY MEASUREMENT UNCERTAINTY
XIX IMEKO World Congre Fundamental and Applied Metrology September 6, 009, Libon, Portugal SUDY OF HE INFLUENCE OF CONVECIVE EFFECS IN INCIDEN RADIAIVE HEA FLUX DENSIY MEASUREMEN UNCERAINY L. Lage Martin,
More informationSCIENCES & TECHNOLOGY
Pertanika J. Sci. & Technol. 22 (2): 645-655 (2014) SCIENCES & TECHNOLOGY Journal homepage: http://www.pertanika.upm.edu.my/ Numerical Modelling of Molten Carbonate Fuel Cell: Effects of Gas Flow Direction
More informationSimulations of electromechanical shape transformations of Au nanoparticles
Phy. Statu Solidi B 252, No. 1, 144 148 (2015) / DOI 10.1002/b.201400140 Simulation of electromechanical hae tranformation of Au nanoarticle hyica tatu olidi baic olid tate hyic Vahur Zadin *,1,2, Arkady
More informationNONISOTHERMAL OPERATION OF IDEAL REACTORS Plug Flow Reactor
NONISOTHERMAL OPERATION OF IDEAL REACTORS Plug Flow Reactor T o T T o T F o, Q o F T m,q m T m T m T mo Aumption: 1. Homogeneou Sytem 2. Single Reaction 3. Steady State Two type of problem: 1. Given deired
More informationPulsed Magnet Crimping
Puled Magnet Crimping Fred Niell 4/5/00 1 Magnetic Crimping Magnetoforming i a metal fabrication technique that ha been in ue for everal decade. A large capacitor bank i ued to tore energy that i ued to
More informationOperational transconductance amplifier based voltage-mode universal filter
Indian Journal of Pure & Alied Phyic ol. 4, etember 005,. 74-79 Oerational tranconductance amlifier baed voltage-mode univeral filter Naeem Ahmad & M R Khan Deartment of Electronic and Communication Engineering,
More informationThe Measurement of DC Voltage Signal Using the UTI
he Meaurement of DC Voltage Signal Uing the. INRODUCION can er an interface for many paive ening element, uch a, capacitor, reitor, reitive bridge and reitive potentiometer. By uing ome eternal component,
More informationELECTROMAGNETIC WAVES AND PHOTONS
CHAPTER ELECTROMAGNETIC WAVES AND PHOTONS Problem.1 Find the magnitude and direction of the induced electric field of Example.1 at r = 5.00 cm if the magnetic field change at a contant rate from 0.500
More informationUgur Pasaogullari, Chao-Yang Wang Electrochemical Engine Center The Pennsylvania State University University Park, PA, 16802
Computational Fluid Dynamics Modeling of Proton Exchange Membrane Fuel Cells using Fluent Ugur Pasaogullari, Chao-Yang Wang Electrochemical Engine Center The Pennsylvania State University University Park,
More informationInfinite-Dimensional Boundary Observer for Lithium-Ion Battery State Estimation
Syddank Univeritet Infinite-Dimenional Boundary Oberver for Lithium-Ion Battery State Etimation Haan, Agu Imail; Jouffroy, Jerome Publihed in: Energy Procedia DOI: 0.06/j.egypro.07..065 Publication date:
More informationMassachusetts Institute of Technology Dynamics and Control II
I E Maachuett Intitute of Technology Department of Mechanical Engineering 2.004 Dynamic and Control II Laboratory Seion 5: Elimination of Steady-State Error Uing Integral Control Action 1 Laboratory Objective:
More informationConduction Heat transfer: Unsteady state
Conduction Heat tranfer: Unteady tate Chapter Objective For olving the ituation that Where temperature do not change with poition. In a imple lab geometry where temperature vary alo with poition. Near
More informationComparison of approximate solution methods for the solid phase diffusion equation in a porous electrode model
Journal of Power Sources 165 (2007 880 886 Short communication Comparison of approximate solution methods for the solid phase diffusion equation in a porous electrode model Qi Zhang, Ralph E. White Center
More informationFinite Element Analysis of a Fiber Bragg Grating Accelerometer for Performance Optimization
Finite Element Analyi of a Fiber Bragg Grating Accelerometer for Performance Optimization N. Baumallick*, P. Biwa, K. Dagupta and S. Bandyopadhyay Fiber Optic Laboratory, Central Gla and Ceramic Reearch
More informationNumerical Simulation of Triaxial Compression Stress Paths Tests for Unsaturated Soil
Numerical Simulation of Triaxial Comreion Stre Path Tet for Unaturated Soil Dong Jian-jun Key Laboratory Of Mechanical Reliability For Heavy Equiment And Large Structure of Hebei Province, Yanhan Univerity,
More informationCh. 13 Fundamentals of Electrochemistry
Ch. 13 Fundamentals of Electrochemistry 13.1 13-1. Basic Concepts of electrochemistry redox reaction : reactions with electron transfer oxidized : loses electrons reduced : gains electrons Fe 3+ + V 2+
More informationA FUNCTIONAL BAYESIAN METHOD FOR THE SOLUTION OF INVERSE PROBLEMS WITH SPATIO-TEMPORAL PARAMETERS AUTHORS: CORRESPONDENCE: ABSTRACT
A FUNCTIONAL BAYESIAN METHOD FOR THE SOLUTION OF INVERSE PROBLEMS WITH SPATIO-TEMPORAL PARAMETERS AUTHORS: Zenon Medina-Cetina International Centre for Geohazard / Norwegian Geotechnical Intitute Roger
More informationFigure 2: Simulation results of concentration by line scan along the x-axis at different partitioning coefficients after 0.48 ms.
Executive Summary One of the critical hurdles of the success of many clean energy technologies is energy storage. For this, new and advanced computational tools to predict battery properties are very important.
More informationBolt stress inspection by Electromagnetic Acoustic Transducer(EMAT) and PZT
Bolt tre inpection by Electromagnetic Acoutic Tranducer(EMAT) and PZT Y.P. Shen 1, G.B. Ma 2,3, C. Ma 2, X.X. Zhu 1 and J.H. Zhao 1 More info about thi article: http://www.ndt.net/?id=22223 Abtract 1 Phaerie
More informationAbstract: 1 Introduction. Walid NASRI a,b, Adinel GAVRUS a, Afia KOUADRI-DAVID a, Kacem SAI b
ème Conrè Françai de Mécanique Lyon, 4 au 8 Août 15 Exerimental and numerical tudy concernin the aniotroic behavior of an AA4-T351 thick heet uin the unified formalim, a multi-mechanim model and a olycrytalline
More informationMolecular Dynamics Simulations of Nonequilibrium Effects Associated with Thermally Activated Exothermic Reactions
Original Paper orma, 5, 9 7, Molecular Dynamic Simulation of Nonequilibrium Effect ociated with Thermally ctivated Exothermic Reaction Jerzy GORECKI and Joanna Natalia GORECK Intitute of Phyical Chemitry,
More informationCHAPTER 3 LITERATURE REVIEW ON LIQUEFACTION ANALYSIS OF GROUND REINFORCEMENT SYSTEM
CHAPTER 3 LITERATURE REVIEW ON LIQUEFACTION ANALYSIS OF GROUND REINFORCEMENT SYSTEM 3.1 The Simplified Procedure for Liquefaction Evaluation The Simplified Procedure wa firt propoed by Seed and Idri (1971).
More informationROOT LOCUS. Poles and Zeros
Automatic Control Sytem, 343 Deartment of Mechatronic Engineering, German Jordanian Univerity ROOT LOCUS The Root Locu i the ath of the root of the characteritic equation traced out in the - lane a a ytem
More informationEffect of Varying Electrolyte Conductivity on the Electrochemical Behavior of Porous Electrodes
A984 Journal of The Electrochemical Society, 52 5 A984-A988 2005 003-465/2005/525/A984/5/$7.00 The Electrochemical Society, Inc. Effect of Varying Electrolyte Conductivity on the Electrochemical Behavior
More informationBlackbody radiation. Main radiation laws. Sun as an energy source. Solar spectrum and solar constant.
Lecture 3. lackbody radiation. Main radiation law. Sun a an energy ource. Solar pectrum and olar contant. Objective:. Concept of a blackbody, thermodynamical equilibrium, and local thermodynamical equilibrium..
More informationLithium Batteries. Rechargeable batteries
Lithium Batteries One of the main attractions of lithium as an anode material is its position as the most electronegative metal in the electrochemical series combined with its low density, thus offering
More informationTypes of Heat Transfer
Type of Heat Tranfer Dv Dt x = k dt dx v T S 2 * * ( v GrT * z = + z H vap lat uject in the coure conduction (Fourier Law forced convection (due to flow ource term free convection (fluid motion due to
More informationEP225 Note No. 5 Mechanical Waves
EP5 Note No. 5 Mechanical Wave 5. Introduction Cacade connection of many ma-pring unit conitute a medium for mechanical wave which require that medium tore both kinetic energy aociated with inertia (ma)
More information3.185 Problem Set 6. Radiation, Intro to Fluid Flow. Solutions
3.85 Proble Set 6 Radiation, Intro to Fluid Flow Solution. Radiation in Zirconia Phyical Vapor Depoition (5 (a To calculate thi viewfactor, we ll let S be the liquid zicronia dic and S the inner urface
More information17.1 Redox Chemistry Revisited
Chapter Outline 17.1 Redox Chemistry Revisited 17.2 Electrochemical Cells 17.3 Standard Potentials 17.4 Chemical Energy and Electrical Work 17.5 A Reference Point: The Standard Hydrogen Electrode 17.6
More informationLecture 10. Erbium-doped fiber amplifier (EDFA) Raman amplifiers Have replaced semiconductor optical amplifiers in the course
ecture 1 Two tye of otical amlifier: Erbium-doed fiber amlifier (EDFA) Raman amlifier Have relaced emiconductor otical amlifier in the coure Fiber Otical Communication ecture 1, Slide 1 Benefit and requirement
More informationDesign of Two-Channel Low-Delay FIR Filter Banks Using Constrained Optimization
contrained otimization, CIT Journal of Comuting and Information Technology, vol. 8, no 4,. 34 348, 2. Deign of Two-Channel Low-Delay FIR Filter Bank Uing Contrained Otimization Abtract Robert Bregović
More informationInput Impedance and Transfer Function of N-Stage Cockcroft-Walton Voltage Multiplier
Input Impedance and Tranfer Function of N-Stae ockcroft-walton Voltae ltiplier Xavier Le Polozec Abtract Thi paper provide theoretical prediction of the differential input impedance, tranfer function,
More informationSupplementary Figures
Supplementary Figure Supplementary Figure S1: Extraction of the SOF. The tandard deviation of meaured V xy at aturated tate (between 2.4 ka/m and 12 ka/m), V 2 d Vxy( H, j, hm ) Vxy( H, j, hm ) 2. The
More informationComputational fluid dynamics simulation of a very dense liquid-solid flow using a Eulerian model
Comutational Method in Multihae Flow III 305 Comutational fluid dynamic imulation of a very dene liuid-olid flow uing a Eulerian model J. Yang & R. J. Chalaturnyk Deartment of Civil and Environmental Engineering,
More informationTime [seconds]
.003 Fall 1999 Solution of Homework Aignment 4 1. Due to the application of a 1.0 Newton tep-force, the ytem ocillate at it damped natural frequency! d about the new equilibrium poition y k =. From the
More informationConvective Heat Transfer
Convective Heat Tranfer Example 1. Melt Spinning of Polymer fiber 2. Heat tranfer in a Condener 3. Temperature control of a Re-entry vehicle Fiber pinning The fiber pinning proce preent a unique engineering
More informationA Comparison of Correlations for Heat Transfer from Inclined Pipes
A Comparion of Correlation for Heat Tranfer from Inclined Pipe Krihperad Manohar Department of Mechanical and Manufacturing Engineering The Univerity of the Wet Indie St. Augutine, Trinidad and Tobago
More informationNOTE: The items d) and e) of Question 4 gave you bonus marks.
MAE 40 Linear ircuit Summer 2007 Final Solution NOTE: The item d) and e) of Quetion 4 gave you bonu mark. Quetion [Equivalent irciut] [4 mark] Find the equivalent impedance between terminal A and B in
More informationMULTISCALE MODELING OF EQUAL CHANNEL ANGULAR EXTRUDED ALUMINIUM WITH STRAIN GRADIENT CRYSTAL PLASTICITY AND PHENOMENOLOGICAL MODELS
MULTISCALE MODELING OF EQUAL CHANNEL ANGULAR EXTRUDED ALUMINIUM WITH STRAIN GRADIENT CRYSTAL PLASTICITY AND PHENOMENOLOGICAL MODELS L. Duchêne, M.G.D. Geer, W.A.M. Brekelman, E. Chen, B. Verlinden and
More informationThermal & Electrochemical Simulation of Battery Pack Systems Steve Hartridge Director, Electric & Hybrid Vehicles
Thermal & Electrochemical Simulation of Battery Pack Systems Steve Hartridge Director, Electric & Hybrid Vehicles CD-adapco Battery Modeling Technology Micro-structure Electrochemistry Virtually test SEM
More informationTheory and Practice Making use of the Barkhausen Effect
Theory and Practice aking ue of the Barkhauen Effect David C. Jile Anon arton Ditinguihed Profeor Palmer Endowed Chair Department of Electrical & Computer Engineering Iowa State Univerity Workhop on Large
More informationResearch on DC resistivity for an arbitrarily anisotropic earth using circular scanning measurement
Reearch on DC reitivity for an arbitrarily aniotroic earth uing circular canning meaurement Zhilong Yang* Changchun Yin Xiuyan Ren Changkai Qiu Xiaoyue Cao Jilin Univerity Jilin Univerity Jilin/RMIT Univerity
More informationECSE 4440 Control System Engineering. Project 1. Controller Design of a Second Order System TA
ECSE 4440 Control Sytem Enineerin Project 1 Controller Dein of a Secon Orer Sytem TA Content 1. Abtract. Introuction 3. Controller Dein for a Sinle Penulum 4. Concluion 1. Abtract The uroe of thi roject
More informationPolarization Invariants and Retrieval of Surface. Parameters Using Polarization Measurements in. Remote Sensing Applications
Thi i a rerint coy of an article ublihed in Alied Otic (Shetoaloff Yu. K. Polarization Invariant and Retrieval of Surface Parameter Uing Polarization Meaurement in Remote Sening Alication, Alied Otic,
More informationElectrochemical Cell - Basics
Electrochemical Cell - Basics The electrochemical cell e - (a) Load (b) Load e - M + M + Negative electrode Positive electrode Negative electrode Positive electrode Cathode Anode Anode Cathode Anode Anode
More informationModeling Volume Changes in Porous Electrodes
Journal of The Electrochemical Society, 53 A79-A86 2006 003-465/2005/53/A79/8/$20.00 The Electrochemical Society, Inc. Modeling olume Changes in Porous Electrodes Parthasarathy M. Gomadam*,a,z John W.
More informationDistributed Thermal-Electrochemical Modeling of a Lithium-Ion Battery to Study the Effect of High Charging Rates
Preprints of the 19th World Congress The International Federation of Automatic Control Distributed Thermal-Electrochemical Modeling of a Lithium-Ion Battery to Study the Effect of High Charging Rates Sohel
More information