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MEI ) AI XIE BEI LI ( Atef Elsherbeni )

ISBN 10: 7118080535 ISBN 13: 9787118080537

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From: liu xing (JiangSu, JS, China)

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About this Item: paperback. Condition: New. Ship out in 2 business day, And Fast shipping, Free Tracking number will be provided after the shipment.Paperback. Pub Date :2012-08-01 Pages: 374 Publisher: National Defence Industry Press title: high-tech Renditions: the electromagnetic hours MATLAB simulation domain finite difference method (with CD 1) List Price: 79.00 yuan Author: (Atef Elsherbeni) Press (U.S.) Aixiebeili: National Defense Industry Press Publication Date :2012-08-01ISBN: 9787118080537 words: Pages: 374 Edition: 1 Format: Folio: 16 Weight: Editor's Choice Executive Summary MATLAB language programming is simple and can be given a fine image features. it has become essential for college students of science and engineering system tools platform. Its complete toolbox functions. making the MATLAB increasingly loved by college students and engineers. The high-tech Renditions: MATLAB simulation of electromagnetic Hours domain finite difference method rapid development in recent years. the electromagnetic field finite-difference time-domain (FDTD) method MATLAB programming language points. with rich instance. It e class professional senior undergraduate or graduate study as a primer of the finite difference time domain method. other discipline engineers interested in the finite-difference time-domain method is also suitable for reading. Contents Chapter 1 the FDTD Introduction 1.1 1.2 derivative of the basic equations of the FDTD method difference approximation 1.3 three-dimensional problem FDTD update equations 1.4 the FDTD iteration equation of the two-dimensional problem 1.5 one-dimensional FDTD update equations 1.6 Exercises Chapter 2 numerically stable numerical stability and dispersion 2.1 2.1.1 2.1.2 FDTD method in the stability domain algorithm CFL stability conditions numerical dispersion 2.3 2.2 Exercises Chapter 3 Yee grid to create the definition of the goal of 3.1 goals 3.1.1 defined the parameters of the problem space defined in the problem space 3.1.2 target medium approximation 3.3 3.2 tangential and normal to the component sub-grid average program 3.4 defined target 3.5 to create a medium grid 3.6 improve 8 grid average 3.7 Exercises Chapter 4 active The FDTD modeling lumped elements and the passive lumped parameter circuit 4.1 FDTD update formula 4.1.1 voltage source 4.1.2 hard resistance current source excitation voltage source 4.1.3 4.1.4 4.1.5 capacitor FDTD modeling 4.1.6 inductor FDTD modeling lumped 4.2.1 4.1.7 4.1.8 diode FDTD simulation 4.1.9 summarizes 4.2 lumped elements located on the surface or volume of lumped elements defined initialization and simulation 4.2.2 FDTD of parameter elements of defined parameters and initialization of the array 4.2.3 lumped elements initialization 4.2.4 update coefficients initialization 4.2.5 electric and magnetic fields and the voltage and current sampling 4.2.6 output parameters defined with initialization 4.2.7 running FDTD simulation: the resistance into circulation 4.2.8 shows the FDTD simulation results the 4.3 simulation example 4.3.1 sine wave voltage source excitation 4.3.2 sine wave source excitation diode 4.3.3 to simulation waveforms 5.1.1 sine shaped 5.1.2 Gaussian waveform 5.1.3 Gaussian waveform derivative of the normalized waveform from the time domain to the frequency domain transform 5.1 Top FDTD excitation by a unit step voltage source capacitance 4.4 practice Chapter 5 excitation source 5.2 FDTD simulation a 5.1.4 cosine function modulated by Gaussian waveform excitation source definition and initialization of 5.3 from the time domain to the frequency domain transform 5.4 Simulation Examples 5.4.1 to regain time domain by the Fourier transform waveform 5.4. calculation of parameters of cosine modulated Gaussian waveform incentive RCL circuit 5.5 Exercises Chapter 6 the scattering parameters 6.1 S parameters and return loss definition 6.2 S 6.3 simulated examples 6.3.1 14 wavelength converter 6.4 Exercises Chapter 7 perfect matched layer absorbing the boundary of Chapter 8 Chapter 9. Seller Inventory # FX009147

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MEI ) AI XIE BEI LI DENG ZHU . YU ZHI YUAN YI

ISBN 10: 7118080535 ISBN 13: 9787118080537

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About this Item: paperback. Condition: New. Ship out in 2 business day, And Fast shipping, Free Tracking number will be provided after the shipment.Paperback. Pub Date :2012-08-01 Pages: 374 Publisher: National Defence Industry Press title: MATLAB simulation electromagnetics domain finite difference method - (with CD-ROM) List Price: 79 yuan Author: Yi Xiebei (U.S.) inside waiting for. Yu Zhiyuan Translation Publishing House: National Defense Industry Press Publication Date :2012-8-1ISBN: 9787118080537 Words: 554.000 yards: 374 Edition: 1 Binding: Paperback: 16 open size and weight of the product: Editor's Choice SUMMARY MATLAB language programming is simple and can be given a fine image features. it has become essential for college students of science and engineering system tools platform. Its complete toolbox functions. making the MATLAB increasingly loved by college students and engineers. MATLAB simulation of electromagnetic Hours domain finite difference method developed rapidly in recent years. the electromagnetic field of the finite-difference time-domain (FDTD) method MATLAB programming language points. with rich instance. It e class professional senior undergraduate or graduate study as a primer of the finite difference time domain method. other discipline engineers interested in the finite-difference time-domain method is also suitable for reading. The fdtd iteration of the basic equation 1.2 Matlab simulation of electromagnetic hours FDTD method Chapter 1 the fdtd Introduction 1.1 FDTD method of derivative differential approximation 1.3 three-dimensional problem the fdtd update equation 1.4 two-dimensional problem directory directory top the numerical stability of the update equation 1.6 Exercises Chapter 2 of the equation 1.5 one-dimensional the fdtd problem of numerical stability and dispersion 2.1 2.1.1 when the method stability 2.1.2fdtd domain algorithm. cfl stable condition practice numerical dispersion 2.3 2.2 Chapter 3 yee grid to create the definition of the goal of 3.1 goals 3.1.1 defined problem space parameters 3.1.2 define the problem space target medium approximation 3.3 3.2 tangential and normal to the component sub-grid the average programs .3.4 defined target 3.5 create medium improve eight grid Grid 3.6 average 3.7 Exercises Chapter 4 of active and passive lumped parameter circuit 4.1fdtd 4.1.1 update formula lumped elements voltage source 4.1.2 Hard 4.1.3 current source excitation voltage source the fdtd modeling 4.1.7 4.1.4 resistance fdtd the fdtd modeling 4.1.5 capacitance modeling 4.1.6 inductor located on the surface or volume of lumped elements 4.1.8 diode fdtd simulation 4.1.9 Summary 4.2 set the definition of the parameter elements 4.2.1 lumped parameter initialization and simulation the elements defined 4.2.2fdtd parameters and array initialization 4.2.3 lumped elements initialization 4.2.4 update coefficients of the initialization 4.2.5 electric field and magnetic field. as well as voltage and current sampling 4.2.6 output parameters defined with initialization run fdtd simulation 4.2.7: 4.2.8 show fdtd simulation results into circulation the 4.3 simulation example 4.3.1 sine wave voltage source incentive resistance 4.3.2 sine wave source excitation diode 4.3.3 by the unit step excitation voltage source capacitance 4.4 Exercises Chapter 5 excitation source waveform commonly 5.1 fdtd transformation from the time domain to the frequency domain simulation waveform 5.1.1 Gaussian waveform. sinusoidal waveform 5.1.2 5.1.3 Gaussian waveform derivative of normalization 5.1.4 cosine function modulated Gaussian waveform 5.2fdtd analog excitation source definition and initialization of 5.3 from the time domain to the frequency domain transform 5.4 Simulation Examples 5.4.1 Fourier transform regain rcl circuit 5.5 Exercises Chapter 6 the scattering parameter 6.1s parameters and return loss defined the 6.2s parameters of the time-domain waveform 5.4.2 cosine modulated Gaussian waveform incentive calculation 6.3 simulated examples 6.3 the Chap. Seller Inventory # FV071037

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BEN SHE

ISBN 10: 7118080535 ISBN 13: 9787118080537

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From: liu xing (JiangSu, JS, China)

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About this Item: paperback. Condition: New. Ship out in 2 business day, And Fast shipping, Free Tracking number will be provided after the shipment.Paperback. Pub Date: Unknown in Publisher: National Defence Industry Press List Price: 79.00 yuan Author: Publisher: National Defense Industry Press ISBN: 9787118080537 Yema: Revision: Binding: Folio: Published :2012 -8-1 printing time: words: Product ID: 22887936 About MATLAB language programming is simple. and can be given a fine image features. it has become essential for college students of science and engineering system tools platform. Its complete toolbox functions. making the MATLAB increasingly loved by college students and engineers. MATLAB simulation of electromagnetic Hours domain finite difference method developed rapidly in recent years. the electromagnetic field of the finite-difference time-domain (FDTD) method MATLAB programming language points. with rich instance. It e class professional senior undergraduate or graduate study as a primer of the finite difference time domain method. other discipline engineers interested in the finite-difference time-domain method is also suitable for reading. About the author catalog directory top 1.4 two-dimensional problem matlab simulation of electromagnetic hours FDTD method Chapter 1 the fdtd Introduction 1.1 difference approximation of the derivative of the basic equations of the FDTD method 1.2 1.3 three-dimensional problem the fdtd update equation the numerical stability of the update equation 1.6 Exercises Chapter 2 of the the fdtd iterative equation 1.5 one-dimensional the fdtd problem of numerical stability and dispersion 2.1 2.1.1 when the method stability 2.1.2fdtd domain algorithm. cfl stable condition 2.2 numerical dispersion 2.3 practice Chapter 3 yee grid to create the definition of the objectives of the target 3.1 3.1.1 define the problem space parameters defined in the problem space 3.1.2 target medium approximation 3.3 3.2 tangential and normal to the component sub-grid average program .3.4 defined objectives 3.5 improve eight grid to create a medium grid 3.6 average 3.7 update formula Exercises Chapter 4 of active and passive lumped parameter circuit 4.1fdtd of lumped parameter elements 4.1.1 voltage source 4.1.2 hard excitation voltage source 4.1.3 4.1.4 resistance of the current source the fdtd modeling 4.1.5 the fdtd modeling 4.1.6 inductance capacitance the fdtd modeling 4.1.7 in the surface or volume lumped elements 4.1.8 diode fdtd simulation 4.1.9 summarizes 4.2 lumped elements defined initialization and simulation 4.2.1 lumped elements of the definition 4.2.2fdtd parameters and array initialization 4.2.3 lumped elements initialized 4.2.4 update coefficient early initialization 4.2.5 electric and magnetic fields as well as voltage and current sampling 4.2.6 Output parameters defined initialization 4.2.7 running the fdtd analog: 4.3.1 sine wave cycle 4.2.8 displays the fdtd analog results into 4.3 analog example voltage source resistance incentive 4.3.2 excited by a sine wave source diode 4.3.3 by the unit step excitation voltage source capacitance of 4.4 Exercises Chapter 5 excitation source waveform commonly 5.1 fdtd transformation from the time domain to the frequency domain simulation waveform 5.1 .1 sine waveform 5.1.2 and Gaussian waveforms derivative of Gaussian waveform 5.1.3 normalization 5.1.4 cosine function modulation a Gaussian waveform 5.2fdtd analog definition and initialization of the excitation source from the time domain to the frequency domain transform 5.3 5.4 simulation example 5.4.1 regained by the Fourier transform rcl circuit 5.5 Exercises Chapter 6 time-domain waveform 5.4.2 excited by the cosine modulated Gaussian waveform the scattering parameter 6.1s parameters and return loss defined 6.2s parameters calculated 6.3 analog example 6.3.11 / 4 wavelength converter the theory perfect matched layer absorbing boundary 7.1pml 6.4 Exercises Chapter 7 7.1.1pml 7.2 of pml and real-space interface the theory 7.1.2pml in pml-pml inte. Seller Inventory # EJ010812

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MEI AI XIE BEI LI Atef Elsherbeni MEI DE MI ER Veysel Demir

ISBN 10: 7118080535 ISBN 13: 9787118080537

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From: liu xing (JiangSu, JS, China)

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About this Item: paperback. Condition: New. Paperback. Pub Date: 2012 08 Pages: 374 Language: Chinese in Publisher: National Defense Industry Press MATLAB language with simple programming. and exquisite image features can be given. it has become the science and engineering students must system tools platform. Its complete toolbox functions. making the MATLAB increasingly loved by college students and engineers. The high-tech Renditions: MATLAB simulation of electromagnetic Hours domain finite difference method rapid development in rece. Seller Inventory # CD023660

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