Carbon Canister Modeling. Jon Brown Staff Engineer Exhaust Aftertreatment & Emissions CLEERS Workshop 2017
|
|
- Loren Horton
- 5 years ago
- Views:
Transcription
1 Cabon Caniste Modeling Jon Bown Staff Enginee Exhaust Afteteatment & Emissions CLEERS Wokshop 2017
2 Agenda Cabon caniste and EVAP system oveview Motivation, Backgound, and Objective Adsoption isothem Reaction Rate Model Results Conclusions
3 Cabon Caniste and EVAP System Oveview The cabon caniste is the cente piece of the evapoative emission contol system, efeed to as EVAP fo OBD2 Adsobs fuel vapo fom fuel tank, and desobs to the intake system when puged with ai The hydocabon (HC) mass escaping the EVAP system is egulated SHED test with diunal tempeatue cycle [1] Refeence fo figue: A Fuel Vapo Model (FVSMOD) fo Evapoative Emissions System Design and Analysis, Lavoie, G., Imai, Y., Johnson, P., 1998, SAE
4 Motivation Many ecent equests, despite being old technology OEMs, supplies, consultants, and univesities Reasons LEV III zeo fuel-hc emissions vehicle test equiement [2] Moe complex puge contol system equiements fo tubo-chaged GDI engines [3], and design tade-offs fo plug-in hybid applications Refeence fo figue: "EVAP System Fluid-Dynamics and Chemisty Modelling fo EMS Puge Contol Development and Optimization," Smith, L., Hussain, A., Pautasso, E., Sevetto, E., Gaziano, E., Bown, J., 2015, SIA Powetain Confeence.
5 Backgound and Objective "Cabon Caniste Modeling fo Evapoative Emissions: Adsoption and Themal Effects," Lavoie, G., Johnson, P., and Hood, J., 1996, SAE [4] Model and measuements, focused on equilibium state, but we need kinetic ates, site density, etc. Othes have used linea diving foce models typically in 3D CFD [5,6,7] The objective was to use steady-state adsoption isothem data to develop tansient kinetics fo a fast 1D, pedictive, and adaptable model fo diffeent fuels and caniste types Minimize the numbe of equied calibation vaiables Standad afteteatment modeling components in GT-SUITE
6 Adsoption Isothem
7 Adsoption Isothem Standad measuement steady-state adsoption isothem
8 Lavoie et al Adsoption Isothem Fitting Function Relative adsobed volume, v V v V Whee Vadsobed volume, V * satuation volume * Equivalent to coveage Fee enegy of adsoption pe unit liquid volume, f f ( ρ RT ) L W ln Whee ρ L liquid density, Rgas constant, Ttempeatue, Wmolecula weight, p sat satuation pessue, p vap vapo pessue Polanyi, Dubinin, et al type adsoption theoy [4,8], simila appoach to Pihl and Daw [9], but the fuel is assumed to adsob as liquid p p sat vap Function of tempeatue and concentation
9 Lavoie et al Adsoption Isothem Fitting Function Lavoie et al e-plotted the adsoption isothem data, and fit the data using two functions, one is elevant fo expected ange v V V n f * f 1 A e ; * f f * A * f 1 85 J/mL f * 4 J/mL n1.2 V * 0.83 ml/gc at T20 C
10 Reaction Rate
11 Deive the Net Reaction Rate The goal is to deive a net ate using tansient fowad and evese ates in tems of coveage θ and eactant concentation {C} The expected ate fom at equilibium: Substitute f into the fitting function, eplace v with θ, solve fo p vap, and convet p vap to {C eq }: ( ) } {, C d a θ ( ) 0 } { } { eq d a C C k { } n L A R T W f sat d a e T R P multi des C k 1 1 * ln _ θ ρ
12 Known and Unknown Vaiables Only 3 unknown vaiables to be calibated: k is an oveall ate multiplie, units of 1/s des_multi is a desoption multiplie, unit-less, nea 1 Enthalpy of fomation fo the stoed fuel coveage (h vap + bond) Popeties of the fuel ae known: W, ρ L, and p sat function of T fom Antoine Equation Remaining ae known fom fitting the adsoption isothem: f 1, A*, and n ae adsoption isothem fitting function paametes Site density (mol/m 3 ), ρ app Appaent cabon bed density (gc/ml) { } n L A R T W f sat d a e T R P multi des C k 1 1 * ln _ θ ρ 3 * 2933 _ m mol W V Density Site L app ρ ρ
13 Cabon Caniste Model Results
14 Cabon Caniste Model, Loading Tests 50/50, 20/80, and 10/90 mixtues by volume of n-butane C 4 H 10 with N 2 Expeiment 50% 20% 10% Avg. standad space velocity h Avg. RT Facto (<1 faste than RT) Maste dt0.1 s Fuel Vapo N 2 T 1/6 T 5/6 T 2/6 T 4/6
15 Caniste Loading vs. Time Vaied n-butane Inlet Concentation
16 Caniste Loading vs. Axial Location Compaison to Lavoie et al 1996, Loading 50/50
17 Caniste Bed Tempeatue vs. Time, Loading, 50/50 Paasitic heat tansfe not modeled, but negligible effect fo mass loading since no C 4 H 10 at these locations at this these times
18 Cabon Caniste Model, Puging Tests N 2 at 10, 20, and 30 L/min puge flow ates Expeiment 10 L/min 20 L/min 30 L/min Avg. standad space velocity h Avg. RT Facto (<1 faste than RT) Maste dt0.01 s Fuel Vapo N 2 T 5/6 T 1/6
19 Caniste Puging vs. Time Vaied Puge Flow Rate Measuement eo appeas to be pesent in the Indiect Measuements, scales with the volumetic flow ate, wheeas the model consistently conseves mass
20 Caniste Puging vs. Axial Location Compaison to Lavoie et al 1996, Puging 20 L/min
21 Caniste Bed Tempeatue vs. Time, Puging, 20 L/min
22 Going Full Cicle, Veification of Adsoption Isothem Steady-state loading, geat match at T20 C
23 Conclusions Developed a net eaction ate that chaacteizes the cabon caniste behavio Successfully pedicts the tansient loading and puging of fuel vapo Successfully epoduces the steady-state adsoption isothem Can be used to pedict cabon caniste woking capacity, beak-though mass, and fo EVAP contol system development Same appoach can be used fo othe adsoption/ desoption devices ai intake system HC taps, wate adsoption, fuel adsoption
24 Acknowledgements Thomas Payet-Buin Fome inten at Gamma Technologies Ed Bissett
25 Refeences [1] A Fuel Vapo Model (FVSMOD) fo Evapoative Emissions System Design and Analysis, Lavoie, G., Imai, Y., Johnson, P., 1998, SAE [2] ARB LEV III Attachment A-5: "CALIFORNIA EVAPORATIVE EMISSION STANDARDS AND TEST PROCEDURES FOR 2001 AND SUBSEQUENT MODEL MOTOR VEHICLES," 2012, [3] "EVAP System Fluid-Dynamics and Chemisty Modelling fo EMS Puge Contol Development and Optimization," Smith, L., Hussain, A., Pautasso, E., Sevetto, E., Gaziano, E., Bown, J., 2015, SIA Powetain Confeence. [4] "Cabon Caniste Modeling fo Evapoative Emissions: Adsoption and Themal Effects," Lavoie, G., Johnson, P., and Hood, J., 1996, SAE [5] "Modeling and Simulation of N-butane Adsoption/Desoption in a Cabon Caniste," Bai, X., Isaac, K. M., Banejee, R., Klein, D., Beig, W., and Olive, L., 2004, SAE [6] "Adsoption and Desoption Simulation of Cabon Caniste Using n-butane as Model Compound of Gasoline," Sato, K., Kobayashi, N., 2011, Jounal of Japan Petoleum Institute, 54, (3), [7] "Vehicula Emission Pefomance Simulation," Lin, J., Dong, M., Ali, S., Hipp, M., and Schneppe, C., 2012, SAE [8] Stoage of Chemical Species in Emission Contol Systems: The Role of Mathematical Modeling, Koltsakis, G., Stamatelos, A., 2001, Global Powetain Congess. [9] "NH3 Stoage Isothems: A Path Towad Bette Models of NH3 Stoage on Zeolite SCR Catalysts," Pihl, J., Daw, S., 2014, CLEERS Wokshop.
26 Questions?
27 Additional Infomation
28 Cabon Caniste Model Infomation 1D Packed Bed Reacto Model Fontal Aea3330 mm^2 Total Bed Length300 mm Total Bed Volume1 L Void Faction0.366 Paticle Diamete0.677 mm C f and Nu/Sh functions of Re paticle fom classical efeences dx5 mm (60 sub-volumes) dt 0.1 s loading /0.01 s puging Paasitic heat loss between chambes not modeled Flow ate too low fo QS Implicit solution with d/dt tems
29 Deive the Net Reaction Rate The goal is to have a net eaction ate in tems of coveage θ and eactant concentation {C} ( θ, { C} ) Only infomation available is isothem data fo a geneal equilibium state g At equilibium the following must be tue a d g( v, pvap ) ( θ,{ C}) f ( T ) g( v, p ) vap 0
30 Deive the Net Reaction Rate Reaanging v(f) f(v) and setting equal to the oiginal adsoption enegy tem f f 1 ln ( ρ RT ) Single adsobing species, fuel vapo A v * 1 n L W p vap { C} RT ln p p sat vap Solving fo the equilibium concentation { C eq } psat RT e f1w ln LRT ρ * A v 1 n
31 Deive the Net Reaction Rate The expected ate fom is: Plug in {C eq } Replace v with θ (intoduce desoption multiplie tem) Mathematically flip ln() tem fo potection if θ 0 Final fom: ( ) 0 } { } { eq d a C C k { } n L A R T W f sat d a e T R P multi des C k 1 1 * ln _ θ ρ
32 Reaction Rate Paametes and Constants Calibated inputs, and calculated site density Fo tunove ate in 1/s, multiply site density by ate_multiplie Fuel popeties and adsoption fitting function paametes Refeence fo the constants ae fom [4]: Cabon Caniste Modeling fo Evapoative Emissions: Adsoption and Themal Effects, Lavoie, G., Johnson, P., Hood, J., 1996, SAE
Lecture 2 - Thermodynamics Overview
2.625 - Electochemical Systems Fall 2013 Lectue 2 - Themodynamics Oveview D.Yang Shao-Hon Reading: Chapte 1 & 2 of Newman, Chapte 1 & 2 of Bad & Faulkne, Chaptes 9 & 10 of Physical Chemisty I. Lectue Topics:
More informationEntropy and Free Energy: Predicting the direction of spontaneous change The approach to Chemical equilibrium
Lectue 8-9 Entopy and Fee Enegy: Pedicting the diection of spontaneous change The appoach to Chemical equilibium Absolute entopy and the thid law of themodynamics To define the entopy of a compound in
More informationSupporting information
Electonic Supplementay Mateial (ESI) fo Physical Chemisty Chemical Physics. This jounal is the Owne Societies 18 Suppoting infomation Nonstoichiometic oxides as a continuous homologous seies: linea fee-enegy
More informationNumerical solution of diffusion mass transfer model in adsorption systems. Prof. Nina Paula Gonçalves Salau, D.Sc.
Numeical solution of diffusion mass tansfe model in adsoption systems Pof., D.Sc. Agenda Mass Tansfe Mechanisms Diffusion Mass Tansfe Models Solving Diffusion Mass Tansfe Models Paamete Estimation 2 Mass
More informationDownloaded from
Chapte Notes Subject: Chemisty Class: XI Chapte: Themodynamics Top concepts 1. The banch of science which deals with study of diffeent foms of enegy and thei inteconvesion is called themodynamics. 2. A
More informationis the instantaneous position vector of any grid point or fluid
Absolute inetial, elative inetial and non-inetial coodinates fo a moving but non-defoming contol volume Tao Xing, Pablo Caica, and Fed Sten bjective Deive and coelate the govening equations of motion in
More informationCSTR - PFR - PBR
1. Mole Balances o The Rate of Reaction, - o The Geneal Mole Balance Equation o Continuous low Reactos - CSTR (Continuous-Stied Tank Reacto) - PR (Tubula Reacto) - PBR (Packed-Bed Reacto) o Industial Reactos
More informationSubstances that are liquids or solids under ordinary conditions may also exist as gases. These are often referred to as vapors.
Chapte 0. Gases Chaacteistics of Gases All substances have thee phases: solid, liquid, and gas. Substances that ae liquids o solids unde odinay conditions may also exist as gases. These ae often efeed
More informationStudy of C5/C6 isomerization on Pt/H-zeolite catalyst in industrial conditions
Ovidius Univesity Annals of Chemisty Volume, Numbe, pp. -6, Study of / isomeization on Pt/H-zeolite catalyst in industial conditions Claudia Iina KONCSAG*, Ioan Alexandu TUTUN and Cistian SAFTA Ovidius
More informationNewton s Laws, Kepler s Laws, and Planetary Orbits
Newton s Laws, Keple s Laws, and Planetay Obits PROBLEM SET 4 DUE TUESDAY AT START OF LECTURE 28 Septembe 2017 ASTRONOMY 111 FALL 2017 1 Newton s & Keple s laws and planetay obits Unifom cicula motion
More informationPulse Neutron Neutron (PNN) tool logging for porosity Some theoretical aspects
Pulse Neuton Neuton (PNN) tool logging fo poosity Some theoetical aspects Intoduction Pehaps the most citicism of Pulse Neuton Neuon (PNN) logging methods has been chage that PNN is to sensitive to the
More informationChapter 2: Conversion and Reactor Sizing
CHEMICL RECTIO EGIEERIG (SK3223) Chapte 2: Convesion and Reacto Sizing W ORHRYTI W SLLEH hayati@petoleum.utm.my RIZI MD. KSMI afiziana@petoleum.utm.my Convesion, To quantify how fa a eaction has pogessed
More informationChem 453/544 Fall /08/03. Exam #1 Solutions
Chem 453/544 Fall 3 /8/3 Exam # Solutions. ( points) Use the genealized compessibility diagam povided on the last page to estimate ove what ange of pessues A at oom tempeatue confoms to the ideal gas law
More informationPhysics: Work & Energy Beyond Earth Guided Inquiry
Physics: Wok & Enegy Beyond Eath Guided Inquiy Elliptical Obits Keple s Fist Law states that all planets move in an elliptical path aound the Sun. This concept can be extended to celestial bodies beyond
More informationYoun-Woo Lee School of Chemical and Biological Engineering Seoul National University , 599 Gwanangro, Gwanak-gu, Seoul, Korea
hemical Reacto esign Y W L Youn-Woo Lee School of hemical and iological Engineeing 55-74, 599 Gwanango, Gwana-gu, Seoul, Koea ywlee@snu.ac. http://sfpl.snu.ac. hapte 6 Multiple Reactions hemical Reaction
More informationAdsorption and Desorption Kinetics for Diffusion Controlled Systems with a Strongly Concentration Dependent Diffusivity
The Open-Access Jounal fo the Basic Pinciples of Diffusion Theoy, Expeient and Application Adsoption and Desoption Kinetics fo Diffusion Contolled Systes with a Stongly Concentation Dependent Diffusivity
More informationSupplementary Figure 1. Circular parallel lamellae grain size as a function of annealing time at 250 C. Error bars represent the 2σ uncertainty in
Supplementay Figue 1. Cicula paallel lamellae gain size as a function of annealing time at 50 C. Eo bas epesent the σ uncetainty in the measued adii based on image pixilation and analysis uncetainty contibutions
More informationDerivation of Thermal Relaxation Time between Two-Phase Flow under the Effect of Heating Sink
Appl. Math. Inf. Sci. 9, No., 299-5 25 299 Applied Mathematics & Infomation Sciences An Intenational Jounal http://dx.doi.og/.2785/amis/924 Deivation of Themal Relaxation Time between Two-Phase Flow unde
More information9.2 Reaction rate and rate equation
9.2.1 Expession of eaction ate The ate () of a chemical eaction is defined as the concentation change of a eactant o a poduct pe unit time. mean ate [A] c c = t t t 2 1 2 1 c c 1 instantaneous ate: Physical
More informationModeling of trickle bed reactor for hydrotreating of vacuum gas oils: effect of kinetic type on reactor modeling
17 th Euopean ymposium on Compute Aided Pocess Engineeing ECAPE17 V. Plesu and P.. Agachi (Editos) 007 Elsevie B.V. All ights eseved. 1 Modeling of tickle bed eacto fo hydoteating of vacuum gas oils: effect
More informationDesigning a Sine-Coil for Measurement of Plasma Displacements in IR-T1 Tokamak
Designing a Sine-Coil fo Measuement of Plasma Displacements in IR-T Tokamak Pejman Khoshid, M. Razavi, M. Ghoanneviss, M. Molaii, A. TalebiTahe, R. Avin, S. Mohammadi and A. NikMohammadi Dept. of Physics,
More informationThree dimensional flow analysis in Axial Flow Compressors
1 Thee dimensional flow analysis in Axial Flow Compessos 2 The ealie assumption on blade flow theoies that the flow inside the axial flow compesso annulus is two dimensional means that adial movement of
More informationCoupled Electromagnetic and Heat Transfer Simulations for RF Applicator Design for Efficient Heating of Materials
Coupled Electomagnetic and Heat Tansfe Simulations fo RF Applicato Design fo Efficient Heating of Mateials Jeni Anto 1 and Raj C Thiagaajan 2 * 1 Reseache, Anna Univesity, Chennai, 2 ATOA Scientific Technologies
More informationCorrelation between System (Lagrangian) concept Control-volume (Eulerian) concept for comprehensive understanding of fluid motion?
The Reynolds Tanspot Theoem Coelation between System (Lagangian) concept Contol-volume (Euleian) concept fo compehensive undestanding of fluid motion? Reynolds Tanspot Theoem Let s set a fundamental equation
More informationPROBLEM SET #3A. A = Ω 2r 2 2 Ω 1r 2 1 r2 2 r2 1
PROBLEM SET #3A AST242 Figue 1. Two concentic co-axial cylindes each otating at a diffeent angula otation ate. A viscous fluid lies between the two cylindes. 1. Couette Flow A viscous fluid lies in the
More informationEntropy and reaction spontaneity
A quote of the week (o camel of the week): Minds ae like paachutes they only function when open Thomas Dewa 1 Entopy and eaction spontaneity Back to the II law ot themodynamics A spontaneous change is
More informationChapter 1: Mole Balances
CHEMICL RECTION ENGINEERING (SK3223) Chapte : Mole Balances WN NORHRYTI WN SLLEH hayati@petoleum.utm.my RIZIN MD. KSMNI afiziana@petoleum.utm.my Rate of Reaction The eaction ate is the ate at which a species
More informationA NEW VARIABLE STIFFNESS SPRING USING A PRESTRESSED MECHANISM
Poceedings of the ASME 2010 Intenational Design Engineeing Technical Confeences & Computes and Infomation in Engineeing Confeence IDETC/CIE 2010 August 15-18, 2010, Monteal, Quebec, Canada DETC2010-28496
More information17.1 Electric Potential Energy. Equipotential Lines. PE = energy associated with an arrangement of objects that exert forces on each other
Electic Potential Enegy, PE Units: Joules Electic Potential, Units: olts 17.1 Electic Potential Enegy Electic foce is a consevative foce and so we can assign an electic potential enegy (PE) to the system
More informationF g. = G mm. m 1. = 7.0 kg m 2. = 5.5 kg r = 0.60 m G = N m 2 kg 2 = = N
Chapte answes Heinemann Physics 4e Section. Woked example: Ty youself.. GRAVITATIONAL ATTRACTION BETWEEN SMALL OBJECTS Two bowling balls ae sitting next to each othe on a shelf so that the centes of the
More informationMagnetometer Calibration Algorithm Based on Analytic Geometry Transform Yongjian Yang, Xiaolong Xiao1,Wu Liao
nd Intenational Foum on Electical Engineeing and Automation (IFEEA 5 Magnetomete Calibation Algoithm Based on Analytic Geomety ansfom Yongjian Yang, Xiaolong Xiao,u Liao College of Compute Science and
More information= 4 3 π( m) 3 (5480 kg m 3 ) = kg.
CHAPTER 11 THE GRAVITATIONAL FIELD Newton s Law of Gavitation m 1 m A foce of attaction occus between two masses given by Newton s Law of Gavitation Inetial mass and gavitational mass Gavitational potential
More informationME 425: Aerodynamics
ME 5: Aeodynamics D ABM Toufique Hasan Pofesso Depatment of Mechanical Engineeing, BUET Lectue- 8 Apil 7 teachebuetacbd/toufiquehasan/ toufiquehasan@mebuetacbd ME5: Aeodynamics (Jan 7) Flow ove a stationay
More informationCASCADE OPTIMIZATION AND CONTROL OF BATCH REACTORS
CASCADE OPIMIZAION AND CONROL OF BACH REACORS Xiangming Hua, Sohab Rohani and Athu Jutan* Depatment of Chemical and Biochemical Engineeing Univesity of Westen Ontaio, London, Canada N6A B9 * ajutan@uwo.ca
More informationDuality between Statical and Kinematical Engineering Systems
Pape 00, Civil-Comp Ltd., Stiling, Scotland Poceedings of the Sixth Intenational Confeence on Computational Stuctues Technology, B.H.V. Topping and Z. Bittna (Editos), Civil-Comp Pess, Stiling, Scotland.
More informationSIMULATION OF AUTOGENOUS AND DRYING SHRINKAGE BASED ON MICRO-PORE STRUCTURE AND INTERNAL MOISTURE STATE
SIMULATION OF AUTOGENOUS AND DRYING SHRINKAGE BASED ON MICRO-PORE STRUCTURE AND INTERNAL MOISTURE STATE Y. Luan (1), T. Ishida (1) (1) Depatment of Civil Engineeing, the Univesity of Tokyo, Japan Abstact
More informationSchool of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007
School of Electical and Compute Engineeing, Conell Univesity ECE 303: Electomagnetic Fields and Waves Fall 007 Homewok 8 Due on Oct. 19, 007 by 5:00 PM Reading Assignments: i) Review the lectue notes.
More informationANALYSIS OF GLOBAL WARMING MITIGATION BY WHITE REFLECTING SURFACES
Intenational Confeence CO Summit: Technology and Oppotunity Vail, Coloado June 6-10 010 ANALYSIS OF GLOBAL WARMING MITIGATION BY WHITE REFLECTING SURFACES Fedeico Rossi, Andea Nicolini Univesity of Peugia,
More informationField emission of Electrons from Negatively Charged Cylindrical Particles with Nonlinear Screening in a Dusty Plasma
Reseach & Reviews: Jounal of Pue and Applied Physics Field emission of Electons fom Negatively Chaged Cylindical Paticles with Nonlinea Sceening in a Dusty Plasma Gyan Pakash* Amity School of Engineeing
More information4. Some Applications of first order linear differential
August 30, 2011 4-1 4. Some Applications of fist ode linea diffeential Equations The modeling poblem Thee ae seveal steps equied fo modeling scientific phenomena 1. Data collection (expeimentation) Given
More informationInteraction of Feedforward and Feedback Streams in Visual Cortex in a Firing-Rate Model of Columnar Computations. ( r)
Supplementay mateial fo Inteaction of Feedfowad and Feedback Steams in Visual Cotex in a Fiing-Rate Model of Columna Computations Tobias Bosch and Heiko Neumann Institute fo Neual Infomation Pocessing
More informationDesign of a Fuel Processor System for
ChE class and home poblems The object of this column is to enhance ou eades collections of stimulating poblems in chemical engineeing education. Ideal poblems, which may be open-ended, ae those that motivate
More informationMultiphase Flow and Heat Transfer
Multiphase Flow and Heat Tansfe ME546 -Sudhee Siddapueddy sudhee@iitp.ac.in Pendant and Sessile Dops Pendant doplet detachment sequence Sessile wate doplet immesed in oil and esting on a bass suface Inteface
More informationBasic Bridge Circuits
AN7 Datafoth Copoation Page of 6 DID YOU KNOW? Samuel Hunte Chistie (784-865) was bon in London the son of James Chistie, who founded Chistie's Fine At Auctionees. Samuel studied mathematics at Tinity
More informationA Radiative Flamelet Combustion Model For Turbulent, Premixed Methane-Air Flames
Jounal of Multidisciplinay Engineeing Science and Technology (JMEST) A Radiative Flamelet Combustion Model Fo Tubulent, Pemixed Methane-Ai Flames Cai Y. Ma School of Chemical and Pocess Engineeing Univesity
More informationEELE 3331 Electromagnetic I Chapter 4. Electrostatic fields. Islamic University of Gaza Electrical Engineering Department Dr.
EELE 3331 Electomagnetic I Chapte 4 Electostatic fields Islamic Univesity of Gaza Electical Engineeing Depatment D. Talal Skaik 212 1 Electic Potential The Gavitational Analogy Moving an object upwad against
More informationMitscherlich s Law: Sum of two exponential Processes; Conclusions 2009, 1 st July
Mitschelich s Law: Sum of two exponential Pocesses; Conclusions 29, st July Hans Schneebege Institute of Statistics, Univesity of Elangen-Nünbeg, Gemany Summay It will be shown, that Mitschelich s fomula,
More informationRecent Advances in Chemical Engineering, Biochemistry and Computational Chemistry
Themal Conductivity of Oganic Liquids: a New Equation DI NICOLA GIOVANNI*, CIARROCCHI ELEONORA, PIERANTOZZI ARIANO, STRYJEK ROAN 1 DIIS, Univesità Politecnica delle ache, 60131 Ancona, ITALY *coesponding
More informationCBE Transport Phenomena I Final Exam. December 19, 2013
CBE 30355 Tanspot Phenomena I Final Exam Decembe 9, 203 Closed Books and Notes Poblem. (20 points) Scaling analysis of bounday laye flows. A popula method fo measuing instantaneous wall shea stesses in
More information10. Groundwater in geotechnical problems
. Goundwate in geotechnical poblems Goundwate plays a key ole in many geotechnical poblems. We will look at; - land subsidence - dewateing open pits - Consolidation of sediments Remembe the stoage of wate
More informationLiquid gas interface under hydrostatic pressure
Advances in Fluid Mechanics IX 5 Liquid gas inteface unde hydostatic pessue A. Gajewski Bialystok Univesity of Technology, Faculty of Civil Engineeing and Envionmental Engineeing, Depatment of Heat Engineeing,
More information( ) [ ] [ ] [ ] δf φ = F φ+δφ F. xdx.
9. LAGRANGIAN OF THE ELECTROMAGNETIC FIELD In the pevious section the Lagangian and Hamiltonian of an ensemble of point paticles was developed. This appoach is based on a qt. This discete fomulation can
More informationA Transport Equation Residual Model Incorporating a Damkohler Criterion for Predicting the Flame Propagation in Gasoline Direct Injection Engines
Eighteenth Intenational Multidimensional Engine Modeling Use s Goup Meeting at the SAE Congess, Apil 3, 8, Detoit, Michigan A anspot Equation Residual Model Incopoating a Damkohle Citeion fo Pedicting
More informationIn the previous section we considered problems where the
5.4 Hydodynamically Fully Developed and Themally Developing Lamina Flow In the pevious section we consideed poblems whee the velocity and tempeatue pofile wee fully developed, so that the heat tansfe coefficient
More informationPhysics 235 Chapter 5. Chapter 5 Gravitation
Chapte 5 Gavitation In this Chapte we will eview the popeties of the gavitational foce. The gavitational foce has been discussed in geat detail in you intoductoy physics couses, and we will pimaily focus
More informationElectromagnetism Physics 15b
lectomagnetism Physics 15b Lectue #20 Dielectics lectic Dipoles Pucell 10.1 10.6 What We Did Last Time Plane wave solutions of Maxwell s equations = 0 sin(k ωt) B = B 0 sin(k ωt) ω = kc, 0 = B, 0 ˆk =
More informationCurrent, Resistance and
Cuent, Resistance and Electomotive Foce Chapte 25 Octobe 2, 2012 Octobe 2, 2012 Physics 208 1 Leaning Goals The meaning of electic cuent, and how chages move in a conducto. What is meant by esistivity
More information22.615, MHD Theory of Fusion Systems Prof. Freidberg Lecture 4: Toroidal Equilibrium and Radial Pressure Balance
.615, MHD Theoy of Fusion Systems Pof. Feidbeg Lectue 4: Tooidal Equilibium and Radial Pessue Balance Basic Poblem of Tooidal Equilibium 1. Radial pessue balance. Tooidal foce balance Radial Pessue Balance
More informationAnalysis of high speed machining center spindle dynamic unit structure performance Yuan guowei
Intenational Confeence on Intelligent Systems Reseach and Mechatonics Engineeing (ISRME 0) Analysis of high speed machining cente spindle dynamic unit stuctue pefomance Yuan guowei Liaoning jidian polytechnic,dan
More informationPhysics Fall Mechanics, Thermodynamics, Waves, Fluids. Lecture 18: System of Particles II. Slide 18-1
Physics 1501 Fall 2008 Mechanics, Themodynamics, Waves, Fluids Lectue 18: System of Paticles II Slide 18-1 Recap: cente of mass The cente of mass of a composite object o system of paticles is the point
More informationVector Control. Application to Induction Motor Control. DSP in Motion Control - Seminar
Vecto Contol Application to Induction Moto Contol Vecto Contol - Pinciple The Aim of Vecto Contol is to Oient the Flux Poducing Component of the Stato Cuent to some Suitable Flux Vecto unde all Opeating
More informationModeling of the fermentation in an internal loop airlift reactor
17 th Euopean Symposium on Compute Aided Pocess Engineeing ESCAPE17 V. Plesu and P.S. Agachi (Editos) 7 Elsevie B.V. All ights eseved. 1 Modeling of the fementation in an intenal loop ailift eacto Ivan
More informationA new class of exact solutions of the Navier Stokes equations for swirling flows in porous and rotating pipes
Advances in Fluid Mechanics VIII 67 A new class of exact solutions of the Navie Stokes equations fo swiling flows in poous and otating pipes A. Fatsis1, J. Stathaas2, A. Panoutsopoulou3 & N. Vlachakis1
More informationEffects of Fines on Undrained Behaviour of Sands. Misko Cubrinovski 1 and Sean Rees 2
Effects of Fines on Undained Behaviou of Sands Misko Cubinovski 1 and Sean Rees 2 1 Associate Pofesso, Depatment of Civil and Natual Resouces Engineeing, Univesity of Cantebuy, New Zealand; misko.cubinovski@cantebuy.ac.nz
More informationNon-Ideal Gas Behavior P.V.T Relationships for Liquid and Solid:
hemodynamis Non-Ideal Gas Behavio.. Relationships fo Liquid and Solid: An equation of state may be solved fo any one of the thee quantities, o as a funtion of the othe two. If is onsideed a funtion of
More informationResearch Article EXPERIMENTAL STUDY OF HEAT TRANSFER CHARACTERISTICS OF STAINLESS STEEL FIBROUS FLOW INSULATOR
Tansactions of the TSME (16) Vol. 4, No. 2, 148 155 Jounal of seach and Applications in Mechanical Engineeing Copyight 16 by TSME ISSN 2229-2152 pint DOI: 1.14456/jame.16.15 seach Aticle EXPERIMENTAL STUDY
More informationThe Combined Effect of Chemical reaction, Radiation, MHD on Mixed Convection Heat and Mass Transfer Along a Vertical Moving Surface
Available at http://pvamu.edu/aam Appl. Appl. Math. ISSN: 93-966 Vol. 5, Issue (Decembe ), pp. 53 53 (Peviously, Vol. 5, Issue, pp. 63 6) Applications and Applied Mathematics: An Intenational Jounal (AAM)
More informationApplied Aerodynamics
Applied Aeodynamics Def: Mach Numbe (M), M a atio of flow velocity to the speed of sound Compessibility Effects Def: eynolds Numbe (e), e ρ c µ atio of inetial foces to viscous foces iscous Effects If
More informationChapter 2: Basic Physics and Math Supplements
Chapte 2: Basic Physics and Math Supplements Decembe 1, 215 1 Supplement 2.1: Centipetal Acceleation This supplement expands on a topic addessed on page 19 of the textbook. Ou task hee is to calculate
More informationInstitute of Fundamental Sciences-Mathematics,Massey University, Palmerston North,NZ
Poceedings20th NZ Geothemal Wokshop 1998 FLUID FLOW A FLASHING CYCLONE SEPARATOR Institute of Fundamental SciencesMathematics,Massey Univesity, Palmeston Noth,NZ SUMMARY In geothemal steamgatheingsystems
More informationT. Raja Rani. Military Technological College, Muscat, Oman. Abstract
ISSN: 78-8 Vol. Issue, Octobe - Fee Convection ove a Vaying all Vetical Cylinde embedded in a Poous medium ith effect of Radiation, Vaiable Fluid Popeties and Statification. T. Raja Rani Militay Technological
More informationImproved Dielectric Model for Polyvinyl Alcohol-Water Hydrogel at Microwave Frequencies
Ameican Jounal of Applied Sciences 7 (2): 270-276, 2010 ISSN 1546-9239 2010 Science Publications Impoved Dielectic Model fo Polyvinyl Alcohol-Wate Hydogel at Micowave Fequencies 1 You Kok Yeow, 2 Zulkifly
More informationLecture 24 Stability of Molecular Clouds
Lectue 4 Stability of Molecula Clouds 1. Stability of Cloud Coes. Collapse and Fagmentation of Clouds 3. Applying the iial Theoem Refeences Oigins of Stas & Planetay Systems eds. Lada & Kylafis http://cfa-www.havad.edu/cete
More informationMobility of atoms and diffusion. Einstein relation.
Mobility of atoms and diffusion. Einstein elation. In M simulation we can descibe the mobility of atoms though the mean squae displacement that can be calculated as N 1 MS ( t ( i ( t i ( 0 N The MS contains
More informationNATURAL CONVECTION HEAT TRANSFER WITHIN VERTICALLY ECCENTRIC DOMED SKYLIGHTS CAVITIES
Poceedings: Building Simulation 007 NATURAL CONVECTION HEAT TRANSFER WITHIN VERTICALLY ECCENTRIC DOMED SKYLIGHTS CAVITIES A. Satipi, A. Laouadi, D. Naylo 3, R. Dhib 4 Depatment of Mechanical and Industial
More informationx 1 b 1 Consider the midpoint x 0 = 1 2
1 chapte 2 : oot-finding def : Given a function f(), a oot is a numbe satisfying f() = 0. e : f() = 2 3 = ± 3 question : How can we find the oots of a geneal function f()? 2.1 bisection method idea : Find
More informationABSTRACT SIMULATION OF DYNAMIC PRESSURE- Professor Timothy A. Barbari Department of Chemical Engineering
ABSTRACT Title: SIMULATION OF DYNAMIC PRESSURE- SWING GAS SORPTION IN POLYMERS Heathe Jane St. Piee, Maste of Science, 2005 Diected By: Pofesso Timothy A. Babai Depatment of Chemical Engineeing A tanspot
More informationPearson s Chi-Square Test Modifications for Comparison of Unweighted and Weighted Histograms and Two Weighted Histograms
Peason s Chi-Squae Test Modifications fo Compaison of Unweighted and Weighted Histogams and Two Weighted Histogams Univesity of Akueyi, Bogi, v/noduslód, IS-6 Akueyi, Iceland E-mail: nikolai@unak.is Two
More informationPhysics 2212 GH Quiz #2 Solutions Spring 2016
Physics 2212 GH Quiz #2 Solutions Sping 216 I. 17 points) Thee point chages, each caying a chage Q = +6. nc, ae placed on an equilateal tiangle of side length = 3. mm. An additional point chage, caying
More informationSynthesis of Epichlorohydrin from Glycerol. Hydrochlorination of Glycerol
Synthesis of Epichloohydin fom yceol. Hydochloination of yceol Geogy Dmitiev S.*, Leonid Zanaveskin N. Fedeation State Unitay Oganization "Kapov Institute of Physical hemisty" Russia, Moscow, Minusinskaya
More informationV7: Diffusional association of proteins and Brownian dynamics simulations
V7: Diffusional association of poteins and Bownian dynamics simulations Bownian motion The paticle movement was discoveed by Robet Bown in 1827 and was intepeted coectly fist by W. Ramsay in 1876. Exact
More informationSEARCH-BASED DYNAMIC IDENTIFICATION OF INDUCTION MOTORS
SEARCH-BASED DYNAMIC IDENTIFICATION OF INDUCTION MOTORS Alexande Vladimiovich Nesteovskiy Veniamin Geogievich ashiskikh Valey Mihailovich Zavyalov and Iina Yuyevna Semykina uzbass State Technical Univesity
More informationThe Catalytic Hydrogenation of Aromatic Nitro Ketone in a Microreactor: Reactor Performance and Kinetic Studies
TERATOAL JOURAL OF EMAL REATOR EGEERG Volume 6 008 Aticle A The atalytic ydogenation of Aomatic ito etone in a Micoeacto: Reacto Pefomance and inetic Studies Sunitha Tadepalli Adeniyi Lawal Stevens nstitute
More informationPower efficiency and optimum load formulas on RF rectifiers featuring flow-angle equations
LETTE IEICE Electonics Expess, Vol.10, No.11, 1 9 Powe efficiency and optimum load fomulas on F ectifies featuing flow-angle equations Takashi Ohia a) Toyohashi Univesity of Technology, 1 1 Hibaigaoka,
More informationAPPLICATION OF MAC IN THE FREQUENCY DOMAIN
PPLICION OF MC IN HE FREQUENCY DOMIN D. Fotsch and D. J. Ewins Dynamics Section, Mechanical Engineeing Depatment Impeial College of Science, echnology and Medicine London SW7 2B, United Kingdom BSRC he
More informationGalilean Transformation vs E&M y. Historical Perspective. Chapter 2 Lecture 2 PHYS Special Relativity. Sep. 1, y K K O.
PHYS-2402 Chapte 2 Lectue 2 Special Relativity 1. Basic Ideas Sep. 1, 2016 Galilean Tansfomation vs E&M y K O z z y K In 1873, Maxwell fomulated Equations of Electomagnetism. v Maxwell s equations descibe
More informationVoltage ( = Electric Potential )
V-1 of 10 Voltage ( = lectic Potential ) An electic chage altes the space aound it. Thoughout the space aound evey chage is a vecto thing called the electic field. Also filling the space aound evey chage
More informationInseting this into the left hand side of the equation of motion above gives the most commonly used algoithm in classical molecula dynamics simulations
Chem465 in 2000 Univesity of Washington Lectue notes Hannes Jonsson Classical dynamics When we ae dealing with heavy atoms and high enough enegy o tempeatue, it is often suciently accuate to neglect quantum
More informationQuantum Mechanics and the Cool Science of Hydrogen. drogen roperties for nergy esearch
Quantum Mechanics and the Cool Science of Hydogen H H Y P E R dogen opeties fo negy eseach In this talk: 1. An intoduction. Why hydogen? 3. Quantum Mechanics 4. Equations of State 5. Mixtues Jacob Leachman,
More informationBlack Body Radiation and Radiometric Parameters:
Black Body Radiation and Radiometic Paametes: All mateials absob and emit adiation to some extent. A blackbody is an idealization of how mateials emit and absob adiation. It can be used as a efeence fo
More informationPotential Energy and Conservation of Energy
Potential Enegy and Consevation of Enegy Consevative Foces Definition: Consevative Foce If the wok done by a foce in moving an object fom an initial point to a final point is independent of the path (A
More informationOSCILLATIONS AND GRAVITATION
1. SIMPLE HARMONIC MOTION Simple hamonic motion is any motion that is equivalent to a single component of unifom cicula motion. In this situation the velocity is always geatest in the middle of the motion,
More informationPhysics 2020, Spring 2005 Lab 5 page 1 of 8. Lab 5. Magnetism
Physics 2020, Sping 2005 Lab 5 page 1 of 8 Lab 5. Magnetism PART I: INTRODUCTION TO MAGNETS This week we will begin wok with magnets and the foces that they poduce. By now you ae an expet on setting up
More informationMolecular dynamics simulation of ultrafast laser ablation of fused silica
IOP Publishing Jounal of Physics: Confeence Seies 59 (27) 1 14 doi:1.188/1742-6596/59/1/22 Eighth Intenational Confeence on Lase Ablation Molecula dynamics simulation of ultafast lase ablation of fused
More informationTitle :THERMAL TRANSFER AND FLUID MECHANICS IN THE THEORY OF ETHER Author:Thierry DELORT Date:1 st May 2013
Title :THERMAL TRANSFER AND FLUID MECHANICS IN THE THEORY OF ETHER Autho:Thiey DELORT Date: st May 03 Email:tdelot@yahoo.f Abstact: In a pevious aticle (), we pesented a vey complete cosmological theoy
More informationEmpirical Prediction of Fitting Densities in Industrial Workrooms for Ray Tracing. 1 Introduction. 2 Ray Tracing using DRAYCUB
Empiical Pediction of Fitting Densities in Industial Wokooms fo Ray Tacing Katina Scheebnyj, Muay Hodgson Univesity of Bitish Columbia, SOEH-MECH, Acoustics and Noise Reseach Goup, 226 East Mall, Vancouve,
More informationNumerical simulation of velocity and temperature fields in natural circulation loop
Jounal of Physics: Confeence Seies PAPER OPEN ACCESS Numeical simulation of velocity and tempeatue fields in natual ciculation loop To cite this aticle: L A Sukomel and O N Kaban kov 2017 J. Phys.: Conf.
More informationTransverse Wakefield in a Dielectric Tube with Frequency Dependent Dielectric Constant
ARDB-378 Bob Siemann & Alex Chao /4/5 Page of 8 Tansvese Wakefield in a Dielectic Tube with Fequency Dependent Dielectic Constant This note is a continuation of ARDB-368 that is now extended to the tansvese
More informationSo, if we are finding the amount of work done over a non-conservative vector field F r, we do that long ur r b ur =
3.4 Geen s Theoem Geoge Geen: self-taught English scientist, 793-84 So, if we ae finding the amount of wok done ove a non-consevative vecto field F, we do that long u b u 3. method Wok = F d F( () t )
More informationWhat molecular weight polymer is necessary to provide steric stabilization? = [1]
1/7 What molecula weight polyme is necessay to povide steic stabilization? The fist step is to estimate the thickness of adsobed polyme laye necessay fo steic stabilization. An appoximation is: 1 t A d
More information