Dynamic Simulation of Electromagnets. European COMSOL Conference. 5 November 2008

Size: px
Start display at page:

Download "Dynamic Simulation of Electromagnets. European COMSOL Conference. 5 November 2008"

Transcription

1 Pesented at the COMSOL Confeence 28 Hannove Dynamic Simulation of Electomagnets Euopean COMSOL Confeence 5 Novembe 28 1 / D. Haald Bille / pinted 21 Octobe 28 Continental AG

2 Contents 1. Electonic bake systems by Continental Automotive Systems ABS ESC 2. COMSOL fo electomagnetic actuatos Magnetic foce Amatue movement by mesh defomation Fast calculation of system dynamics 3. Conclusion 2 / D. Haald Bille / pinted 21 Octobe 28 Continental AG

3 Contents 1. Electonic bake systems by Continental Automotive Systems ABS ESC 2. COMSOL fo electomagnetic actuatos Magnetic foce Amatue movement by mesh defomation Fast calculation of system dynamics 3. Conclusion 3 / D. Haald Bille / pinted 21 Octobe 28 Continental AG

4 Anti-lock bake system (ABS) contol slip between wheel and oad stick fiction > slip fiction maximie foce between wheel and oad maintain lateal guiding foce tagets: vehicle emains stable vehicle can be steeed shote stopping distance in most situations 1 / D. Haald Bille / pinted 21 Octobe 28 Continental AG

5 ABS components 11 / D. Haald Bille / pinted 21 Octobe 28 Continental AG

6 ABS hydaulic layout bake pedal, booste, maste cylinde outlet valve inlet valve wheel bake 12 / D. Haald Bille / pinted 21 Octobe 28 Continental AG

7 ABS active contol constant pessue phase pessue decease phase inlet valve closed outlet valve open 13 / D. Haald Bille / pinted 21 Octobe 28 Continental AG

8 Antilock Bake System ABS µ-split Baking with ABS 14 / D. Haald Bille / pinted 21 Octobe 28 Continental AG

9 Antilock Bake System ABS µ-split Baking without ABS 15 / D. Haald Bille / pinted 21 Octobe 28 Continental AG

10 Electonic Stability Contol ESC Active Yaw Contol 18 / D. Haald Bille / pinted 21 Octobe 28 Continental AG

11 Electonic Stability Contol ESC ABS: Anti-lock Bake System + EBD: Electonic Bake foce Distibution + TCS: Taction Contol System + AYC: Active Yaw Contol = ESC: Electonic Stability Contol 19 / D. Haald Bille / pinted 21 Octobe 28 Continental AG

12 Contents 1. Electonic bake systems by Continental Automotive Systems ABS ESC 2. COMSOL fo electomagnetic actuatos Magnetic foce Amatue movement by mesh defomation Fast calculation of system dynamics 3. Conclusion 2 / D. Haald Bille / pinted 21 Octobe 28 Continental AG

13 Electonic Stability Contol ESC Exploded View MK6 ESC 21 / D. Haald Bille / pinted 21 Octobe 28 Continental AG

14 Electomagnetic inlet valve 22 / D. Haald Bille / pinted 21 Octobe 28 Continental AG

15 Magnetiation of steel magnetic field H = µ 1 µ B magnetic flux density 2 COMSOL > Physics > Subdomain Settings flux density [T] magnetic field [ka/m] COMSOL > Physics > Equation System > Subdomain Settings nomb_qa = sqt( eps + abs(b_qa)^2 + abs(b_qa)^2 ) 23 / D. Haald Bille / pinted 21 Octobe 28 Continental AG

16 Mateials, mesh, solution satuation! foce : 23.1 N 24 / D. Haald Bille / pinted 21 Octobe 28 Continental AG

17 Contents 1. Electonic bake systems by Continental Automotive Systems ABS ESC 2. COMSOL fo electomagnetic actuatos Magnetic foce Amatue movement by mesh defomation Fast calculation of system dynamics 3. Conclusion 25 / D. Haald Bille / pinted 21 Octobe 28 Continental AG

18 Geomety and defomation domain simplified geomety amatue with defomation domain amatue with igid hull yoke coe amatue winding 26 / D. Haald Bille / pinted 21 Octobe 28 Continental AG

19 27 / D. Haald Bille / pinted 21 Octobe 28 Continental AG Idea of ALE ( abitay Lagangian-Euleian ) mesh defomation physical equation fo u(, ) patial diff l equation (PDE) fo U(R,): R R efeence coodinates space coodinates ), ( ), ( R R = = (, ) U u ), ( ), ( def u R U = R u R u R U + = u u U + = chain ule R R = with = R U R U u 1 + = R U R U u 1 solve system of equations inset into PDE fo u

20 Detemine the functions (R, ) and (R, ) 1. pescibed a) physical defomation (e.g. stuctual mechanics) b) explicit fomula ecommended hee (puely axial motion of igid pats) 2. fom bounday conditions a) Laplace smoothing: 2 2 R = b) Winslow smoothing: 2 R = 28 / D. Haald Bille / pinted 21 Octobe 28 Continental AG

21 Explicit defomation () ? / D. Haald Bille / pinted 21 Octobe 28 Continental AG

22 Continuous / diffeentiable defomations () / D. Haald Bille / pinted 21 Octobe 28 Continental AG

23 Continuous / diffeentiable defomations () / D. Haald Bille / pinted 21 Octobe 28 Continental AG

24 Continuous / diffeentiable defomations () / D. Haald Bille / pinted 21 Octobe 28 Continental AG

25 Continuous / diffeentiable defomations () / D. Haald Bille / pinted 21 Octobe 28 Continental AG

26 Continuous / diffeentiable defomations () / D. Haald Bille / pinted 21 Octobe 28 Continental AG

27 Continuous / diffeentiable defomations () / D. Haald Bille / pinted 21 Octobe 28 Continental AG

28 Continuous / diffeentiable defomations () / D. Haald Bille / pinted 21 Octobe 28 Continental AG

29 Continuous / diffeentiable defomations () / D. Haald Bille / pinted 21 Octobe 28 Continental AG

30 Continuous / diffeentiable defomations () / D. Haald Bille / pinted 21 Octobe 28 Continental AG

31 Continuous / diffeentiable defomations () / D. Haald Bille / pinted 21 Octobe 28 Continental AG

32 Continuous / diffeentiable defomations () / D. Haald Bille / pinted 21 Octobe 28 Continental AG

33 Continuous / diffeentiable defomations () 1.25 ecommended hee: linea defomation / D. Haald Bille / pinted 21 Octobe 28 Continental AG

34 Geomety and defomation domain simplified geomety amatue with defomation domain amatue with igid hull yoke coe amatue winding 42 / D. Haald Bille / pinted 21 Octobe 28 Continental AG

35 Voltage step esponse mesh defomation and magnetic field 43 / D. Haald Bille / pinted 21 Octobe 28 Continental AG

36 Voltage step esponse eddy cuents 44 / D. Haald Bille / pinted 21 Octobe 28 Continental AG

37 Voltage step esponse amatue motion solenoid cuent [A] with eddy cuents without eddy cuents magnetic foce [N] eddy cuent powe [W] amatue coe yoke total time [ms] 45 / D. Haald Bille / pinted 21 Octobe 28 Continental AG

38 Voltage step esponse amatue motion gap [mm].5 with eddy cuents without eddy cuents velocity [m / s] time [ms] 46 / D. Haald Bille / pinted 21 Octobe 28 Continental AG

39 Compaison to expeiment 16 Inlet valve - foce vesus gap fo 25 ampee tuns 14 COMSOL test bench 12 foce [N] gap [mm] 47 / D. Haald Bille / pinted 21 Octobe 28 Continental AG

40 Contents 1. Electonic bake systems by Continental Automotive Systems ABS ESC 2. COMSOL fo electomagnetic actuatos Magnetic foce Amatue movement by mesh defomation Fast calculation of system dynamics 3. Conclusion 48 / D. Haald Bille / pinted 21 Octobe 28 Continental AG

41 49 / D. Haald Bille / pinted 21 Octobe 28 Continental AG Static dependence of field on solenoid cuent (up to eddy cuents) coil ext ot S e I n B e v H E ϕ σ σ = + A ot = (neglect eddy cuents fom field change) t A E = J H = ot coil ext ot ot 1 ot S e I n A e v A t A ϕ σ µ µ σ = + ),, ( x v I A A ext = coil ext ) ( S e I n B e v E ϕ σ + + = ext ) ( J B v E + + = σ B H = µ µ

42 Dynamics of solenoid cuent: integal paamete magnetic flux 1 I ext = ( Uext + U R ind ) 1 n = U + ext 2 π R S coil Scoil E d d 1 d n = U ext 2 π A d d R dt S coil S coil Ψ I 1 = U R d Ψ, dt = Ψ(A ext ext ) Ψ = Ψ( A( I, v, x) ) ext 5 / D. Haald Bille / pinted 21 Octobe 28 Continental AG

43 System dynamics I 1 = U R d Ψ, dt Ψ = Ψ ext ext ( I ext, v, x) I ext = I ext COMSOL solves fo I ext ( Ψ, v, x) Ψ( I = Ψ ext ) look-up table / intepolation pesc Ψ [mvs] m/s 2 2 m/s m/s 1-2 m/s -4 m/s I [A] ext d Ψ dt = U ext R I ext ( Ψ, v, x) + amatue equation of motion + simple effective eddy cuent model 51 / D. Haald Bille / pinted 21 Octobe 28 Continental AG

44 Effective eddy cuent model I stat ( Ψ) effective eddy cuent inductance L eddy extenal voltage U ext (t) i eddy effective eddy cuent esistance R eddy solenoid esistance R Ψ' ( t) = U ext ( t) R ( I ( Ψ( t) + ψ (t) ) + i eddy ( t) ) stat L eddy i eddy '( t) = L Ψ'( t) Reddy ieddy( t) eddy 1 ms Reddy τ1 ψ '( t) = τ 2 Ψ'( t) ψ ( t) ( τ 1.2 ms) detemine L eddy, R eddy, τ 1,τ 2 fom least squaes fit to Comsol esult 52 / D. Haald Bille / pinted 21 Octobe 28 Continental AG

45 Geneation of small systems of odinay diffeential equations look-up table y & = f ( u, y) paamete fit u u y 1/s y y f(u, y) Integato educed linea model dynamic system (e.g. Simulink) fast solution field poblem (e.g. COMSOL) paamete vaiation integation into compehensive model 53 / D. Haald Bille / pinted 21 Octobe 28 Continental AG

46 Conclusion simulation in industial development 1. efficiency fewe pototypes bette expeiments 2. poduct pefomance moe vaiants automatic optimiation functional insight obseve new quantities isolate paamete influence 3. obust poducts ceate limit configuations study toleances statistically 54 / D. Haald Bille / pinted 21 Octobe 28 Continental AG

J. Electrical Systems 1-3 (2005): Regular paper

J. Electrical Systems 1-3 (2005): Regular paper K. Saii D. Rahem S. Saii A Miaoui Regula pape Coupled Analytical-Finite Element Methods fo Linea Electomagnetic Actuato Analysis JES Jounal of Electical Systems In this pape, a linea electomagnetic actuato

More information

Review: Electrostatics and Magnetostatics

Review: Electrostatics and Magnetostatics Review: Electostatics and Magnetostatics In the static egime, electomagnetic quantities do not vay as a function of time. We have two main cases: ELECTROSTATICS The electic chages do not change postion

More information

Finite Element Computational Model for Defect Simulation and Detection by Eddy Currents Non Destructive Testing

Finite Element Computational Model for Defect Simulation and Detection by Eddy Currents Non Destructive Testing Finite Element Computational Model fo Defect Simulation and Detection by Eddy Cuents Non Destuctive Testing M. RACHEK, M. ZAOUA, H. DENOUN, C. BROUCHE Faculté de Génie Electique et de l nfomatique. Dépatement

More information

Designing a Sine-Coil for Measurement of Plasma Displacements in IR-T1 Tokamak

Designing 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 information

6.641 Electromagnetic Fields, Forces, and Motion Spring 2005

6.641 Electromagnetic Fields, Forces, and Motion Spring 2005 MIT OpenouseWae http://ocw.mit.edu 6.641 Electomagnetic Fields, Foces, and Motion Sping 2005 Fo infomation about citing these mateials o ou Tems of Use, visit: http://ocw.mit.edu/tems. 6.641 Electomagnetic

More information

TUTORIAL 9. Static magnetic field

TUTORIAL 9. Static magnetic field TUTOIAL 9 Static magnetic field Vecto magnetic potential Null Identity % & %$ A # Fist postulation # " B such that: Vecto magnetic potential Vecto Poisson s equation The solution is: " Substitute it into

More information

Spring 2001 Physics 2048 Test 3 solutions

Spring 2001 Physics 2048 Test 3 solutions Sping 001 Physics 048 Test 3 solutions Poblem 1. (Shot Answe: 15 points) a. 1 b. 3 c. 4* d. 9 e. 8 f. 9 *emembe that since KE = ½ mv, KE must be positive Poblem (Estimation Poblem: 15 points) Use momentum-impulse

More information

Numerical Integration

Numerical Integration MCEN 473/573 Chapte 0 Numeical Integation Fall, 2006 Textbook, 0.4 and 0.5 Isopaametic Fomula Numeical Integation [] e [ ] T k = h B [ D][ B] e B Jdsdt In pactice, the element stiffness is calculated numeically.

More information

MAGNETIC FIELD AROUND TWO SEPARATED MAGNETIZING COILS

MAGNETIC FIELD AROUND TWO SEPARATED MAGNETIZING COILS The 8 th Intenational Confeence of the Slovenian Society fo Non-Destuctive Testing»pplication of Contempoay Non-Destuctive Testing in Engineeing«Septembe 1-3, 5, Potoož, Slovenia, pp. 17-1 MGNETIC FIELD

More information

Magnetic Field and Inductance Calculations in Theta-Pinch and Z-Pinch Geometries

Magnetic Field and Inductance Calculations in Theta-Pinch and Z-Pinch Geometries Magnetic Field and Inductance Calculations in Theta-Pinch and Z-Pinch Geometies T.J. Awe, R.E. Siemon, B.S. Baue, S. Fuelling, V. Makhin, Univesity of Nevada, Reno, NV 89557 S.C. Hsu, T.P. Intato Los Alamos

More information

A Double Exponential Function Fitting Algorithm for Optimize Parameter of µh Curve

A Double Exponential Function Fitting Algorithm for Optimize Parameter of µh Curve Advanced Mateials Reseach Online: 214-6-18 ISSN: 1662-8985, Vols. 96-961, pp 1146-115 doi:1.428/www.scientific.net/amr.96-961.1146 214 Tans Tech Publications, Switzeland A Double Exponential Function Fitting

More information

Conservative Averaging Method and its Application for One Heat Conduction Problem

Conservative Averaging Method and its Application for One Heat Conduction Problem Poceedings of the 4th WSEAS Int. Conf. on HEAT TRANSFER THERMAL ENGINEERING and ENVIRONMENT Elounda Geece August - 6 (pp6-) Consevative Aveaging Method and its Application fo One Heat Conduction Poblem

More information

Clutches and Brakes Des Mach Elem Mech. Eng. Department Chulalongkorn University

Clutches and Brakes Des Mach Elem Mech. Eng. Department Chulalongkorn University Clutches and Bakes 0330 Des Mach Elem Mech. Eng. Depatment Chulalongkon Univesity ntoduction ( Clutch and bake ae the machine elements used in tansmission and otation contol. Hee only clutch and bake using

More information

Analysis of high speed machining center spindle dynamic unit structure performance Yuan guowei

Analysis 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 information

Physics 2020, Spring 2005 Lab 5 page 1 of 8. Lab 5. Magnetism

Physics 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 information

Compactly Supported Radial Basis Functions

Compactly Supported Radial Basis Functions Chapte 4 Compactly Suppoted Radial Basis Functions As we saw ealie, compactly suppoted functions Φ that ae tuly stictly conditionally positive definite of ode m > do not exist The compact suppot automatically

More information

[2007] IEEE. Reprinted, with permission, from [Jiaxin Chen, Jianguo Zhu, Youguang Guo, A 2-D nonlinear FEA tool embedded in Matlab/Simulink

[2007] IEEE. Reprinted, with permission, from [Jiaxin Chen, Jianguo Zhu, Youguang Guo, A 2-D nonlinear FEA tool embedded in Matlab/Simulink [2007] IEEE. Repinted, with pemission, fom [Jiaxin Chen, Jianguo Zhu, Youguang Guo, A 2-D nonlinea FEA tool embedded in Matlab/Simulin suounding fo application of electomagnetic field analysis in powe

More information

Right-handed screw dislocation in an isotropic solid

Right-handed screw dislocation in an isotropic solid Dislocation Mechanics Elastic Popeties of Isolated Dislocations Ou study of dislocations to this point has focused on thei geomety and thei ole in accommodating plastic defomation though thei motion. We

More information

ELASTIC ANALYSIS OF CIRCULAR SANDWICH PLATES WITH FGM FACE-SHEETS

ELASTIC ANALYSIS OF CIRCULAR SANDWICH PLATES WITH FGM FACE-SHEETS THE 9 TH INTERNATIONAL CONFERENCE ON COMPOSITE MATERIALS ELASTIC ANALYSIS OF CIRCULAR SANDWICH PLATES WITH FGM FACE-SHEETS R. Sbulati *, S. R. Atashipou Depatment of Civil, Chemical and Envionmental Engineeing,

More information

Unit 7: Sources of magnetic field

Unit 7: Sources of magnetic field Unit 7: Souces of magnetic field Oested s expeiment. iot and Savat s law. Magnetic field ceated by a cicula loop Ampèe s law (A.L.). Applications of A.L. Magnetic field ceated by a: Staight cuent-caying

More information

THE INFLUENCE OF THE MAGNETIC NON-LINEARITY ON THE MAGNETOSTATIC SHIELDS DESIGN

THE INFLUENCE OF THE MAGNETIC NON-LINEARITY ON THE MAGNETOSTATIC SHIELDS DESIGN THE INFLUENCE OF THE MAGNETIC NON-LINEARITY ON THE MAGNETOSTATIC SHIELDS DESIGN LIVIU NEAMŢ 1, ALINA NEAMŢ, MIRCEA HORGOŞ 1 Key wods: Magnetostatic shields, Magnetic non-lineaity, Finite element method.

More information

, and the curve BC is symmetrical. Find also the horizontal force in x-direction on one side of the body. h C

, and the curve BC is symmetrical. Find also the horizontal force in x-direction on one side of the body. h C Umeå Univesitet, Fysik 1 Vitaly Bychkov Pov i teknisk fysik, Fluid Dynamics (Stömningsläa), 2013-05-31, kl 9.00-15.00 jälpmedel: Students may use any book including the textbook Lectues on Fluid Dynamics.

More information

An Exact Solution of Navier Stokes Equation

An Exact Solution of Navier Stokes Equation An Exact Solution of Navie Stokes Equation A. Salih Depatment of Aeospace Engineeing Indian Institute of Space Science and Technology, Thiuvananthapuam, Keala, India. July 20 The pincipal difficulty in

More information

Solutions. V in = ρ 0. r 2 + a r 2 + b, where a and b are constants. The potential at the center of the atom has to be finite, so a = 0. r 2 + b.

Solutions. V in = ρ 0. r 2 + a r 2 + b, where a and b are constants. The potential at the center of the atom has to be finite, so a = 0. r 2 + b. Solutions. Plum Pudding Model (a) Find the coesponding electostatic potential inside and outside the atom. Fo R The solution can be found by integating twice, 2 V in = ρ 0 ε 0. V in = ρ 0 6ε 0 2 + a 2

More information

Proposal of Impedance Control for Electric Vehicles with Wheel Resolver - Application to Hand Assisted Parking and Position Adjustment -

Proposal of Impedance Control for Electric Vehicles with Wheel Resolver - Application to Hand Assisted Parking and Position Adjustment - Poposal of Impedance Contol fo Electic ehicles with Wheel Resolve - Application to Hand Assisted Paking and Position Adjustment - T. Enmei*, H.Fujimoto**, Y. Hoi*** The Univesity of Tokyo --, Kashiwanoha,

More information

On the integration of the equations of hydrodynamics

On the integration of the equations of hydrodynamics Uebe die Integation de hydodynamischen Gleichungen J f eine u angew Math 56 (859) -0 On the integation of the equations of hydodynamics (By A Clebsch at Calsuhe) Tanslated by D H Delphenich In a pevious

More information

Description of TEAM Workshop Problem 33.b: Experimental Validation of Electric Local Force Formulations.

Description of TEAM Workshop Problem 33.b: Experimental Validation of Electric Local Force Formulations. 1 Desciption of TEAM Wokshop Poblem 33.b: Expeimental Validation of Electic Local Foce Fomulations. Olivie Baé, Pascal Bochet, Membe, IEEE Abstact Unde extenal stesses, the esponse of any mateial is a

More information

Magnetic Fields Due to Currents

Magnetic Fields Due to Currents PH -C Fall 1 Magnetic Fields Due to Cuents Lectue 14 Chapte 9 (Halliday/esnick/Walke, Fundamentals of Physics 8 th edition) 1 Chapte 9 Magnetic Fields Due to Cuents In this chapte we will exploe the elationship

More information

Antennas & Propagation

Antennas & Propagation Antennas & Popagation 1 Oveview of Lectue II -Wave Equation -Example -Antenna Radiation -Retaded potential THE KEY TO ANY OPERATING ANTENNA ot H = J +... Suppose: 1. Thee does exist an electic medium,

More information

LINEAR AND NONLINEAR ANALYSES OF A WIND-TUNNEL BALANCE

LINEAR AND NONLINEAR ANALYSES OF A WIND-TUNNEL BALANCE LINEAR AND NONLINEAR ANALYSES O A WIND-TUNNEL INTRODUCTION BALANCE R. Kakehabadi and R. D. Rhew NASA LaRC, Hampton, VA The NASA Langley Reseach Cente (LaRC) has been designing stain-gauge balances fo utilization

More information

Faraday s Law. Faraday s Law. Faraday s Experiments. Faraday s Experiments. Magnetic Flux. Chapter 31. Law of Induction (emf( emf) Faraday s Law

Faraday s Law. Faraday s Law. Faraday s Experiments. Faraday s Experiments. Magnetic Flux. Chapter 31. Law of Induction (emf( emf) Faraday s Law Faaday s Law Faaday s Epeiments Chapte 3 Law of nduction (emf( emf) Faaday s Law Magnetic Flu Lenz s Law Geneatos nduced Electic fields Michael Faaday discoeed induction in 83 Moing the magnet induces

More information

Phys-272 Lecture 18. Mutual Inductance Self-Inductance R-L Circuits

Phys-272 Lecture 18. Mutual Inductance Self-Inductance R-L Circuits Phys-7 ectue 8 Mutual nductance Self-nductance - Cicuits Mutual nductance f we have a constant cuent i in coil, a constant magnetic field is ceated and this poduces a constant magnetic flux in coil. Since

More information

15 Solving the Laplace equation by Fourier method

15 Solving the Laplace equation by Fourier method 5 Solving the Laplace equation by Fouie method I aleady intoduced two o thee dimensional heat equation, when I deived it, ecall that it taes the fom u t = α 2 u + F, (5.) whee u: [0, ) D R, D R is the

More information

Passivity-Based Control of Saturated Induction Motors

Passivity-Based Control of Saturated Induction Motors Passivity-Base Contol of Satuate Inuction otos Levent U. Gökee, embe, IEEE, awan A. Simaan, Fellow, IEEE, an Chales W. Bice, Senio embe, IEEE Depatment of Electical Engineeing Univesity of South Caolina

More information

A dual-reciprocity boundary element method for axisymmetric thermoelastodynamic deformations in functionally graded solids

A dual-reciprocity boundary element method for axisymmetric thermoelastodynamic deformations in functionally graded solids APCOM & ISCM 11-14 th Decembe, 013, Singapoe A dual-ecipocity bounday element method fo axisymmetic themoelastodynamic defomations in functionally gaded solids *W. T. Ang and B. I. Yun Division of Engineeing

More information

11) A thin, uniform rod of mass M is supported by two vertical strings, as shown below.

11) A thin, uniform rod of mass M is supported by two vertical strings, as shown below. Fall 2007 Qualifie Pat II 12 minute questions 11) A thin, unifom od of mass M is suppoted by two vetical stings, as shown below. Find the tension in the emaining sting immediately afte one of the stings

More information

FI 2201 Electromagnetism

FI 2201 Electromagnetism FI 2201 Electomagnetism Alexande A. Iskanda, Ph.D. Physics of Magnetism and Photonics Reseach Goup Electodynamics ELETROMOTIVE FORE AND FARADAY S LAW 1 Ohm s Law To make a cuent flow, we have to push the

More information

Phys-272 Lecture 17. Motional Electromotive Force (emf) Induced Electric Fields Displacement Currents Maxwell s Equations

Phys-272 Lecture 17. Motional Electromotive Force (emf) Induced Electric Fields Displacement Currents Maxwell s Equations Phys-7 Lectue 17 Motional Electomotive Foce (emf) Induced Electic Fields Displacement Cuents Maxwell s Equations Fom Faaday's Law to Displacement Cuent AC geneato Magnetic Levitation Tain Review of Souces

More information

FE FORMULATIONS FOR PLASTICITY

FE FORMULATIONS FOR PLASTICITY G These slides ae designed based on the book: Finite Elements in Plasticity Theoy and Pactice, D.R.J. Owen and E. Hinton, 970, Pineidge Pess Ltd., Swansea, UK. Couse Content: A INTRODUCTION AND OVERVIEW

More information

The physics of induction stoves

The physics of induction stoves The physics of uction stoves This is an aticle fom my home page: www.olewitthansen.dk Contents 1. What is an uction stove...1. Including self-uctance...4 3. The contibution fom the magnetic moments...6

More information

3. Magnetostatic fields

3. Magnetostatic fields 3. Magnetostatic fields D. Rakhesh Singh Kshetimayum 1 Electomagnetic Field Theoy by R. S. Kshetimayum 3.1 Intoduction to electic cuents Electic cuents Ohm s law Kichoff s law Joule s law Bounday conditions

More information

On the Sun s Electric-Field

On the Sun s Electric-Field On the Sun s Electic-Field D. E. Scott, Ph.D. (EE) Intoduction Most investigatos who ae sympathetic to the Electic Sun Model have come to agee that the Sun is a body that acts much like a esisto with a

More information

Vector Control. Application to Induction Motor Control. DSP in Motion Control - Seminar

Vector 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 information

2. Electrostatics. Dr. Rakhesh Singh Kshetrimayum 8/11/ Electromagnetic Field Theory by R. S. Kshetrimayum

2. Electrostatics. Dr. Rakhesh Singh Kshetrimayum 8/11/ Electromagnetic Field Theory by R. S. Kshetrimayum 2. Electostatics D. Rakhesh Singh Kshetimayum 1 2.1 Intoduction In this chapte, we will study how to find the electostatic fields fo vaious cases? fo symmetic known chage distibution fo un-symmetic known

More information

A NEW VARIABLE STIFFNESS SPRING USING A PRESTRESSED MECHANISM

A 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 information

Qualifying Examination Electricity and Magnetism Solutions January 12, 2006

Qualifying Examination Electricity and Magnetism Solutions January 12, 2006 1 Qualifying Examination Electicity and Magnetism Solutions Januay 12, 2006 PROBLEM EA. a. Fist, we conside a unit length of cylinde to find the elationship between the total chage pe unit length λ and

More information

COUPLED MODELS OF ROLLING, SLIDING AND WHIRLING FRICTION

COUPLED MODELS OF ROLLING, SLIDING AND WHIRLING FRICTION ENOC 008 Saint Petesbug Russia June 30-July 4 008 COUPLED MODELS OF ROLLING SLIDING AND WHIRLING FRICTION Alexey Kieenkov Ins ti tu te fo P ob le ms in Me ch an ic s Ru ss ia n Ac ad em y of Sc ie nc es

More information

Coarse Mesh Radiation Transport Code COMET Radiation Therapy Application*

Coarse Mesh Radiation Transport Code COMET Radiation Therapy Application* Coase Mesh Radiation Tanspot Code COMT Radiation Theapy Application* Fazad Rahnema Nuclea & Radiological ngineeing and Medical Physics Pogams Geogia Institute of Technology Computational Medical Physics

More information

ASTR415: Problem Set #6

ASTR415: Problem Set #6 ASTR45: Poblem Set #6 Cuan D. Muhlbege Univesity of Mayland (Dated: May 7, 27) Using existing implementations of the leapfog and Runge-Kutta methods fo solving coupled odinay diffeential equations, seveal

More information

A Robust Wheel Slip Controller for a Hybrid Braking System

A Robust Wheel Slip Controller for a Hybrid Braking System Wold Academy of Science, Engineeing and Technology 59 0 A Robust Wheel Slip Contolle fo a Hybid Baking System Matin Ringdofe and Matin Hon, Membe, IEEE Abstact A obust wheel slip contolle fo electic vehicles

More information

( ) Make-up Tests. From Last Time. Electric Field Flux. o The Electric Field Flux through a bit of area is

( ) Make-up Tests. From Last Time. Electric Field Flux. o The Electric Field Flux through a bit of area is Mon., 3/23 Wed., 3/25 Thus., 3/26 Fi., 3/27 Mon., 3/30 Tues., 3/31 21.4-6 Using Gauss s & nto to Ampee s 21.7-9 Maxwell s, Gauss s, and Ampee s Quiz Ch 21, Lab 9 Ampee s Law (wite up) 22.1-2,10 nto to

More information

SOLVING THE VISCOUS COMPOSITE CYLINDER PROBLEM BY SOKOLOV S METHOD

SOLVING THE VISCOUS COMPOSITE CYLINDER PROBLEM BY SOKOLOV S METHOD 1 SOLVING THE VISCOUS COMPOSITE CYLINDER PROBLEM BY SOKOLOV S METHOD NGO By CO. H. TRAN, PHONG. T. Faculty of Mathematics & Infomatics, Univesity of Natual Sciences VNU-HCM Abstact : The pape pesents some

More information

PHY 114 A General Physics II 11 AM-12:15 PM TR Olin 101

PHY 114 A General Physics II 11 AM-12:15 PM TR Olin 101 PHY 114 A Geneal Physics II 11 AM-1:15 PM TR Olin 11 Plan fo Lectue 1 Chaptes 3): Souces of Magnetic fields 1. Pemanent magnets.biot-savat Law; magnetic fields fom a cuent-caying wie 3.Ampee Law 4.Magnetic

More information

Insulated Bearings MEGAOHM TM Series

Insulated Bearings MEGAOHM TM Series Fo ew Technology etwok copoation R Insulated eaings MEGAOHM TM Seies Insulated eaings MEGAOHM TM Seies : Offeing Enhanced Safety and Reliability eaings used in electical equipment such as motos and powe

More information

ELECTRON ENERGY DISTRIBUTIONS AND NON-COLLISIONAL HEATING IN MAGNETICALLY ENHANCED INDUCTIVELY COUPLED PLASMAS*

ELECTRON ENERGY DISTRIBUTIONS AND NON-COLLISIONAL HEATING IN MAGNETICALLY ENHANCED INDUCTIVELY COUPLED PLASMAS* ELECTRON ENERGY DISTRIUTIONS AND NON-COLLISIONAL HEATING IN MAGNETICALLY ENHANCED INDUCTIVELY COUPLED PLASMAS* Ronald L. Kinde and Mak J. Kushne Depatment of Electical and Compute Engineeing Ubana, IL

More information

Australian Journal of Basic and Applied Sciences

Australian Journal of Basic and Applied Sciences Austalian Jounal of Basic and Applied Sciences, 7(14) Decembe 13, Pages: 5-58 AENSI Jounals Austalian Jounal of Basic and Applied Sciences Jounal home page: www.ajbasweb.com Development of Induction Moto

More information

Construction Figure 10.1: Jaw clutches

Construction Figure 10.1: Jaw clutches CHAPTER TEN FRICTION CLUTCHES The wod clutch is a geneic tem descibing any one wide vaiety of devices that is capable of causing a machine o mechanism to become engaged o disengaged. Clutches ae of thee

More information

Reasons to Build a Hydraulic Model

Reasons to Build a Hydraulic Model Reasons to Build a Hydaulic Model Detemine dischage coefficient fo lage flow measuement stuctue (spillway o wei) Develop effective method fo enegy dissipation at outlet of hydaulic stuctue Development

More information

Numerical solution of diffusion mass transfer model in adsorption systems. Prof. Nina Paula Gonçalves Salau, D.Sc.

Numerical 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 information

Aspects of Modelling: Examples from Consideration of Unusual Movements. in Crash Simulation

Aspects of Modelling: Examples from Consideration of Unusual Movements. in Crash Simulation Examples fom Consideation of Unusual Movements Univ.-Pof. D.-Ing. Matin Meywek Depatment of Automotive and Powe Tain Engineeing Helmut-Schmidt-Univesity Univesity of the Fedeal Amed Foces, Hambug 1/17

More information

An Adaptive Neural-Network Model-Following Speed Control of PMSM Drives for Electric Vehicle Applications

An Adaptive Neural-Network Model-Following Speed Control of PMSM Drives for Electric Vehicle Applications Poceedings of the 9th WSEAS Intenational Confeence on Applied Mathematics, Istanbul, Tuey, May 27-29, 2006 (pp412-417) An Adaptive Neual-Netwo Model-Following Speed Contol of PMSM Dives fo Electic Vehicle

More information

EM Boundary Value Problems

EM Boundary Value Problems EM Bounday Value Poblems 10/ 9 11/ By Ilekta chistidi & Lee, Seung-Hyun A. Geneal Desciption : Maxwell Equations & Loentz Foce We want to find the equations of motion of chaged paticles. The way to do

More information

This gives rise to the separable equation dr/r = 2 cot θ dθ which may be integrated to yield r(θ) = R sin 2 θ (3)

This gives rise to the separable equation dr/r = 2 cot θ dθ which may be integrated to yield r(θ) = R sin 2 θ (3) Physics 506 Winte 2008 Homewok Assignment #10 Solutions Textbook poblems: Ch. 12: 12.10, 12.13, 12.16, 12.19 12.10 A chaged paticle finds itself instantaneously in the equatoial plane of the eath s magnetic

More information

High precision computer simulation of cyclotrons KARAMYSHEVA T., AMIRKHANOV I. MALININ V., POPOV D.

High precision computer simulation of cyclotrons KARAMYSHEVA T., AMIRKHANOV I. MALININ V., POPOV D. High pecision compute simulation of cyclotons KARAMYSHEVA T., AMIRKHANOV I. MALININ V., POPOV D. Abstact Effective and accuate compute simulations ae highly impotant in acceleatos design and poduction.

More information

A MICRODISCHARGE BASED PRESURE SENSOR*

A MICRODISCHARGE BASED PRESURE SENSOR* A MICRODISCHARGE BASED PRESURE SENSOR* Jun-Chieh Wang a), Zhongmin Xiong a), Chistine Eun a), Xin Luo a), Yogesh Gianchandani a) and Mak J. Kushne a) a), Ann Abo, MI 48109 USA unchwan@umich.edu, zxiong@umich.edu,

More information

3-7 FLUIDS IN RIGID-BODY MOTION

3-7 FLUIDS IN RIGID-BODY MOTION 3-7 FLUIDS IN IGID-BODY MOTION S-1 3-7 FLUIDS IN IGID-BODY MOTION We ae almost eady to bein studyin fluids in motion (statin in Chapte 4), but fist thee is one cateoy of fluid motion that can be studied

More information

is the instantaneous position vector of any grid point or fluid

is 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 information

Uncertainty in Operational Modal Analysis of Hydraulic Turbine Components

Uncertainty in Operational Modal Analysis of Hydraulic Turbine Components Intenational Jounal of Fluid Machiney and Systems Vol. 2, No. 4, Octobe-Decembe 2009 Oiginal Pape (Invited) Uncetainty in Opeational Modal Analysis of Hydaulic Tubine Components Matin Gagnon 1, S.-Antoine

More information

A moving charged particle creates a magnetic field vector at every point in space except at its position.

A moving charged particle creates a magnetic field vector at every point in space except at its position. 1 Pat 3: Magnetic Foce 3.1: Magnetic Foce & Field A. Chaged Paticles A moving chaged paticle ceates a magnetic field vecto at evey point in space ecept at its position. Symbol fo Magnetic Field mks units

More information

PERFORMANCE ANALYSIS OF FUZZY BASED FIELD ORIENTED CONTROL OF

PERFORMANCE ANALYSIS OF FUZZY BASED FIELD ORIENTED CONTROL OF PERFORMANCE ANALYSIS OF FUZZY BASED FIELD ORIENTED CONTROL OF INDUCTION MOTOR DRIVES FOR HYBRID ELECTRIC VEHICLES ABSTRACT 1 Maiam Khan, Student Membe, IEEE and 2 Naayan C. Ka, Membe, IEEE Electical Machine

More information

Today in Physics 218: radiation from moving charges

Today in Physics 218: radiation from moving charges Today in Physics 218: adiation fom moving chages Poblems with moving chages Motion, snapshots and lengths The Liénad-Wiechet potentials Fields fom moving chages Radio galaxy Cygnus A, obseved by Rick Peley

More information

Magnetostatics. Magnetic Forces. = qu. Biot-Savart Law H = Gauss s Law for Magnetism. Ampere s Law. Magnetic Properties of Materials. Inductance M.

Magnetostatics. Magnetic Forces. = qu. Biot-Savart Law H = Gauss s Law for Magnetism. Ampere s Law. Magnetic Properties of Materials. Inductance M. Magnetic Foces Biot-Savat Law Gauss s Law fo Magnetism Ampee s Law Magnetic Popeties of Mateials nductance F m qu d B d R 4 R B B µ 0 J Magnetostatics M. Magnetic Foces The electic field E at a point in

More information

Computational Methods of Solid Mechanics. Project report

Computational Methods of Solid Mechanics. Project report Computational Methods of Solid Mechanics Poject epot Due on Dec. 6, 25 Pof. Allan F. Bowe Weilin Deng Simulation of adhesive contact with molecula potential Poject desciption In the poject, we will investigate

More information

Ch 30 - Sources of Magnetic Field! The Biot-Savart Law! = k m. r 2. Example 1! Example 2!

Ch 30 - Sources of Magnetic Field! The Biot-Savart Law! = k m. r 2. Example 1! Example 2! Ch 30 - Souces of Magnetic Field 1.) Example 1 Detemine the magnitude and diection of the magnetic field at the point O in the diagam. (Cuent flows fom top to bottom, adius of cuvatue.) Fo staight segments,

More information

Steady State and Transient Performance Analysis of Three Phase Induction Machine using MATLAB Simulations

Steady State and Transient Performance Analysis of Three Phase Induction Machine using MATLAB Simulations Intenational Jounal of Recent Tends in Engineeing, Vol, No., May 9 Steady State and Tansient Pefomance Analysis of Thee Phase Induction Machine using MATAB Simulations Pof. Himanshu K. Patel Assistant

More information

General Railgun Function

General Railgun Function Geneal ailgun Function An electomagnetic ail gun uses a lage Loentz foce to fie a pojectile. The classic configuation uses two conducting ails with amatue that fits between and closes the cicuit between

More information

The Poisson bracket and magnetic monopoles

The Poisson bracket and magnetic monopoles FYST420 Advanced electodynamics Olli Aleksante Koskivaaa Final poject ollikoskivaaa@gmail.com The Poisson backet and magnetic monopoles Abstact: In this wok magnetic monopoles ae studied using the Poisson

More information

A method for solving dynamic problems for cylindrical domains

A method for solving dynamic problems for cylindrical domains Tansactions of NAS of Azebaijan, Issue Mechanics, 35 (7), 68-75 (016). Seies of Physical-Technical and Mathematical Sciences. A method fo solving dynamic poblems fo cylindical domains N.B. Rassoulova G.R.

More information

1D2G - Numerical solution of the neutron diffusion equation

1D2G - Numerical solution of the neutron diffusion equation DG - Numeical solution of the neuton diffusion equation Y. Danon Daft: /6/09 Oveview A simple numeical solution of the neuton diffusion equation in one dimension and two enegy goups was implemented. Both

More information

ScienceDirect. Hybrid Bearing with Actively Adjustable Radial Gap of Gas Foil Bearing

ScienceDirect. Hybrid Bearing with Actively Adjustable Radial Gap of Gas Foil Bearing Aailable online at.sciencediect.com ScienceDiect Pocedia Engineeing 06 (05 ) 3 0 Dynamics and Viboacoustics of Machines (DVM0) Hybid Beaing ith Actiely Adjustable Radial Gap of Gas Foil Beaing Roman Polyako*,

More information

Chapter Introduction to Finite Element Methods

Chapter Introduction to Finite Element Methods Chapte 1.4 Intoduction to Finite Element Methods Afte eading this chapte, you should e ale to: 1. Undestand the asics of finite element methods using a one-dimensional polem. In the last fifty yeas, the

More information

How Electric Currents Interact with Magnetic Fields

How Electric Currents Interact with Magnetic Fields How Electic Cuents nteact with Magnetic Fields 1 Oested and Long Wies wote these notes to help ou with vaious diectional ules, and the equivalence between the magnetism of magnets and the magnets of electic

More information

Dynamic Performances of Self-Excited Induction Generator Feeding Different Static Loads

Dynamic Performances of Self-Excited Induction Generator Feeding Different Static Loads SERBIAN JOURNAL OF ELECTRICAL ENGINEERING Vol. 3, No. 1, June 2006, 63-76 Dynamic Pefomances of Self-Excited Induction Geneato Feeding Diffeent Static Loads Ali Nesba 1, Rachid Ibtiouen 2, Oma Touhami

More information

Geometry and statistics in turbulence

Geometry and statistics in turbulence Geomety and statistics in tubulence Auoe Naso, Univesity of Twente, Misha Chetkov, Los Alamos, Bois Shaiman, Santa Babaa, Alain Pumi, Nice. Tubulent fluctuations obey a complex dynamics, involving subtle

More information

Applied Aerodynamics

Applied 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 information

Current, Resistance and

Current, 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 information

The evolution of the phase space density of particle beams in external fields

The evolution of the phase space density of particle beams in external fields The evolution of the phase space density of paticle beams in extenal fields E.G.Bessonov Lebedev Phys. Inst. RAS, Moscow, Russia, COOL 09 Wokshop on Beam Cooling and Related Topics August 31 Septembe 4,

More information

Magnetic Field. Conference 6. Physics 102 General Physics II

Magnetic Field. Conference 6. Physics 102 General Physics II Physics 102 Confeence 6 Magnetic Field Confeence 6 Physics 102 Geneal Physics II Monday, Mach 3d, 2014 6.1 Quiz Poblem 6.1 Think about the magnetic field associated with an infinite, cuent caying wie.

More information

Ferrite Loss Measurement and Models in Half Bridge and Full Bridge Waveforms

Ferrite Loss Measurement and Models in Half Bridge and Full Bridge Waveforms Feite Loss Measuement and Models in Half idge and Full idge Wavefoms Alex P. an den ossche Ghent Univesity, EELA SINT-PIETERSNIEUWSTRAAT 4 ELGIUM, 9 GENT David M. an de Sype Ghent Univesity, EELA SINT-PIETERSNIEUWSTRAAT

More information

In the previous section we considered problems where the

In 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 information

Rigid Body Dynamics 2. CSE169: Computer Animation Instructor: Steve Rotenberg UCSD, Winter 2018

Rigid Body Dynamics 2. CSE169: Computer Animation Instructor: Steve Rotenberg UCSD, Winter 2018 Rigid Body Dynamics 2 CSE169: Compute Animation nstucto: Steve Rotenbeg UCSD, Winte 2018 Coss Poduct & Hat Opeato Deivative of a Rotating Vecto Let s say that vecto is otating aound the oigin, maintaining

More information

Multiphase Flow and Heat Transfer

Multiphase 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 information

Magneto-Elastic Analysis of an Annular FGM Plate Based on Classical Plate Theory Using GDQ Method

Magneto-Elastic Analysis of an Annular FGM Plate Based on Classical Plate Theory Using GDQ Method 736 Magneto-Elastic Analysis of an Annula FGM Plate Based on Classical Plate Theoy Using GDQ Method Abstact Using GDQ method, the adial and cicumfeential stesses in an annula FGM plate with a unifom thickness

More information

To Feel a Force Chapter 7 Static equilibrium - torque and friction

To Feel a Force Chapter 7 Static equilibrium - torque and friction To eel a oce Chapte 7 Chapte 7: Static fiction, toque and static equilibium A. Review of foce vectos Between the eath and a small mass, gavitational foces of equal magnitude and opposite diection act on

More information

1) Consider an object of a parabolic shape with rotational symmetry z

1) Consider an object of a parabolic shape with rotational symmetry z Umeå Univesitet, Fysik 1 Vitaly Bychkov Pov i teknisk fysik, Fluid Mechanics (Stömningsläa), 01-06-01, kl 9.00-15.00 jälpmedel: Students may use any book including the tetbook Lectues on Fluid Dynamics.

More information

Multiphysics Simulation of Microwave Sintering in a Monomode Cavity

Multiphysics Simulation of Microwave Sintering in a Monomode Cavity Multiphysics Simulation of Micowave Sinteing in a Monomode Cavity Didie Bouvad, Sylvain Chamond and Claude P. Cay Laboatoie SIMAP, Genoble INP, Saint Matin d Hèes, Fance The simulation of sinteing of a

More information

Electrodynamic Forces in Steel Strip during Induction Heating

Electrodynamic Forces in Steel Strip during Induction Heating Intenational Scientific Colloquium Modelling fo Electomagnetic Pocessing Hannove, Mach 4-6, 3 Electodynamic Foces in Steel Stip duing Induction Heating H. Kasjanow, H. Schülbe,. Nikanoov bstact Tangential

More information

Yuvraj B. Jadhava, Abhijeet P. Shahb IJSER

Yuvraj B. Jadhava, Abhijeet P. Shahb IJSER Intenational Jounal of Scientific & Engineeing Reseach, Volume 8, Issue 4, Apil-07 ISSN 9-558 Mathematical modeling & design of wom and wom gea pai fo detemining the suface stess acting on the tooth of

More information

Gaussian beam propagation through a metamaterial lens

Gaussian beam propagation through a metamaterial lens Calhoun: The NPS Institutional Achive Faculty and Reseache Publications Faculty and Reseache Publications 4 Gaussian beam popagation though a metamateial lens Zhou, Hong Gaussian beam popagation though

More information

Mach-Zehnder Interferometer Sensor for Acoustic Detection with Optimal Performance

Mach-Zehnder Interferometer Sensor for Acoustic Detection with Optimal Performance IOSR Jounal of Electonics and Communication Engineeing (IOSRJECE) ISSN : 78-834 Volume, Issue 5 (Sep-Oct 01), PP 9-33 Mach-Zehnde Intefeomete Senso fo Acoustic Detection with Optimal Pefomance 1 Pashil

More information