Transmission Lines Embedded in Arbitrary Anisotropic Media
|
|
- Melanie Byrd
- 6 years ago
- Views:
Transcription
1 ECE 53 1 st Century Electromagnetics Instructor: Office: Phone: E Mail: Dr. Raymond C. Rumpf A 337 (915) rcrumpf@utep.edu Lecture #4 Transmission Lines Embedded in Arbitrary Anisotropic Media Lecture 4 1 Lecture Outline RF transmission lines Transmission lines embedded in anisotropic media Finite-difference analysis of transmission lines embedded in arbitrary anisotropic media Formulation Implementation Eample Generalization of the method Lecture 4 Slide 1
2 RF Transmission Lines What are Transmission Lines? Transmission lines are metallic structures that guide electromagnetic waes from DC to ery high frequencies. Microstrip Coaial Cable Stripline Slotline Lecture 4 Slide 4
3 Characteristic Impedance The ratio of the oltage to current as well as the electric to magnetic field is a constant along the length of the transmission line. This ratio is the characteristic impedance. L Zc C The alue of the characteristic impedance alone has little meaning. Reflections are caused wheneer the impedance changes. For small H/W, 377H H H H Zc 1 1 rln r r rw rw W W For large H/W, H 1 W ln 8 377H W 3 H Zc 1 r H W 1 r 1 W ln W H 161 r r H S. Y. Poh, W. C. Chew, J. A. Kong, Approimate Formulas for Line Capacitance and Characteristic Impedance Lecture 4 of Microstrip Line, IEEE Trans. Microwae Theory Tech., ol. MTT 9, no., pp , May Slide 5 1 Approimate Equations Coaial 60 b Z0 ln a r Twin Lead cosh d Z ab r Parallel Plate 10 d Z0 w r Microstrip 60 8d w ln 1 D 4d w d Z0 10 w 1 D 3ln w d1.393 w d d r 1 r 1 D 11d 1st Century Electromagnetics 6 3
4 Analysis: Electrostatic Approimation Transmission lines are waeguides. To be rigorous, they should be modeled as such. This can be rather computationally intensie. An alternatie is to analyze transmission lines using Laplace s equation. The dimensions of transmission lines are typically much smaller than the operating waelength so the wae nature of electromagnetics is less important to consider. Therefore, we are essentially soling Mawell s equations as 0. Setting =0 is called the electrostatic approimation and the solution approimates the TEM solution of a waeguide. B 0 B 0 All of the field components are separable. The transmission line D 0 D 0 is TEM. H J D t H J Rigorously, the transmission line E B t E 0 is quasi TEM. Lecture 4 Slide 7 Analysis: Inhomogeneous Isotropic Laplace s Equation The diergence condition for the electric field is D 0 Eq. (1) But, we know that D= r E, so this equation becomes E Eq. () r 0 The electric field E is related to the scalar potential V as follows. E V Eq. (3) The inhomogeneous Laplace s equation is deried by substituting Eq. (3) into Eq. (). V r r V Lecture 4 Slide 8 0 4
5 Analysis: Calculating Distributed Capacitance In the electrostatic approimation, the transmission line is a capacitor. The total energy stored in a capacitor is U DE da 1 A The integral is performed oer the entire cross section of deice. For open deices like microstrips, this is infinite area. In practice, we integrate oer a large enough area to incorporate as much of of the electric field as possible. This equation is alid in anisotropic media. The capacitance is related to the total stored energy through CV U 0 V 0 is the oltage across the capacitor. If we set the aboe equations equal and substitute E V into the epression, we derie the equation for the distributed capacitance. 1 C DEdA V 0 A Lecture 4 Slide 9 Analysis: Calculating Distributed Inductance The oltage along the transmission line traels at the same elocity as the electric field so we can write 1 1 r r V E LC LC c Assuming the surrounding medium is homogeneous, we can calculate the distributed inductance from the aboe equation as L This means that for the dielectric only case, we can calculate the cc distributed inductance directly from the distributed capacitance. r r 0 Dielectric materials should not alter the inductance. Howeer if we use the alue of C calculated preiously, it will. This is incorrect. The solution is to calculate capacitance with a homogeneous dielectric C h and then calculate inductance from this. It is simplest to use just air. 1 0 Lecture 4 Slide 10 0 L cch 5
6 Analysis: Calculating TL Parameters The characteristic impedance is calculated from the distributed inductance and capacitance through Z c L C The elocity of a signal traelling along the transmission line is 1 LC The effectie refractie inde n eff is therefore c0 neff c0 LC Both Z c and n eff are needed to analyze transmission line circuits using network theory. Lecture 4 Slide 11 Two Step Modeling Approach Homogeneous Case air outer conductor Step 1 inner conductor distributed inductance L air Inhomogeneous Case Step 1 outer conductor inner conductor distributed capacitance C air Lecture 4 Slide 1 6
7 How We Will Analyze Transmission Lines Step 1 Construct homogeneous TL Step 4 Construct inhomogeneous TL 1 air outer conductor inner conductor air outer conductor inner conductor Step Construct and sole matri equation Vh 0 L h h L h air Zc n c0 LC 1 L C src Lecture 4 Slide 13 src 1 h src Step 5 Construct and sole matri equation r V V0 r L src Step 3 Calculate distributed inductance C D E da 0 h h h V0 A 1 L cc 0 h Step 6 Calculate distributed capacitance C DEdA V 0 0 A Step 7 Calculate TL parameters L Transmission Lines Embedded in Anisotropic Media 7
8 Effect of Strength of Anisotropy Dielectric anisotropy has no effect on the distributed inductance. Capacitance increases and impedance lowers with increasing yy. Field deelops most strongly in the direction with highest permittiity. The degree to which field follows highest is proportional to the strength of the anisotropy. Lecture 4 15 Effect of Spatially Varying the Tensor Orientation Impedance changes in the presences of the anisotropic medium. Field actually follows the anisotropy. Impedance changes slightly with tilt. Impedance relatiely constant regardless of spatial ariance. Lecture
9 Isolation of a Microstrip Ordinary microstrip with metal ball in proimity. Near field is perturbed affecting the signal in the line. Same microstrip embedded in an anisotropic material with dielectric tensor tilted away from ball. Nearfield is less perturbed, affecting the line much less. Lecture 4 17 Eperimental Results Ordinary Microstrip Embedded Microstrip Lecture
10 Finite-Difference Analysis of Transmission Lines Embedded in Arbitrary Anisotropic Media Formulation The Grid We hae two unknowns, V and E, so we adopt a staggered grid. We can use our yeeder() function to construct the deriatie operators. V E E y Lecture
11 Goerning Equations D D 0 D y 0 y z Dz D y z E D E D E y y yy yz y D z z zy zz E z E E V E y V y E z z Lecture 4 1 Reduction to Two Dimensions D 0 Dz D y 0 D y z 0 D D z y y D z 0 y z E E Dy y yy D yz E y y E D D z z zy zz Ez y y yy E y E Ey y V E z z E V E y y Transmission line properties are independent of z, yz, z, zy, and zz. Lecture 4 11
12 Finite-Difference Approimation D e e d 0 y y D D D 0 y d y D ye d ε εy e D y y yy E y d y εy εyyey E e D V E y y e y D y??? Lecture 4 3 The Problem with the Tensor D D E E ye D E D E E y y y y yy y y y yy y D D??? i, j i, j i, j i, j E y E i, j y??? i, j i, j i, j i, j i, j y y E yy Ey In the first finite difference equation, E y is in a physically different position than E and D. Similarly, in the second finite difference equation, E is in a physically different position than E y and D y. The finite difference equations aboe are incorrect because not all of the terms eist at the same position in space. Lecture 4 4 1
13 The Correction Recall the interpolation matrices R, R, R, R, R, and R Computational Electromagnetics. y z y z from Lecture 10 in D D E E E E E 4 E E E E i, j i, j i, j i, j i, j i1, j i1, j i, j1 i, j1 i1, j1 i1, j1 y y y y y y y y i, j i, j i1, j i1, j i, j1 i, j1 i1, j1 i1, j1 i, j y y y y i, j i, j y yy Ey 4 d ε e R R ε e y y y d R R ε e εyey y y y R a interpolation matri a ais along which aerage is taken direction of adjacent cell Lecture 4 5 Reised Finite-Difference Approimation We modify our tensor by incorporating the interpolation matrices. D e e d 0 y y D D D 0 y d y D y E d ε RRyε y e D y y yy E y dy RRε y y εyy ey E e D V E y y e y D y Lecture
14 Matri Form of the Inhomogeneous Laplace s Equation We now derie the matri form of the inhomogeneous Laplaces equation. Eq. 1 Eq. Eq. 3 e e d D D y 0 d y d ε R R ε e ey y y dy RRε y y εyy e D e y D y Step 1: Substitute Eq. () into Eq. (1) ε e e RRyεy e D D y 0 RRε y y εyy e y Step : Substitute Eq. (3) into the aboe ε e e RRyε y D D D y 0 RRε y y εyy Dy Step 3: Drop the negatie sign ε e e RRyε y D D D y 0 RRε y y εyy Dy Lecture 4 7 Matri Form of the Homogeneous Laplace s Equation For the homogeneous case, our tensor reduces to ε RRyε y I 0 RRε y y εyy 0 I Substituting this into the inhomogeneous Laplace s equation gies us e e I 0D D Dy 0 0 ID y D e e D Dy 0 D y Lecture
15 The Ecitation Vector b We hae L = 0. This is not solable because we hae not stated the applied potentials. When we do this, our equation becomes L = b.? V 0 + V z L 0 L b Lecture 4 9 Enforcing the Known Potentials It turns out we must also modify L in addition to constructing b. Each point on the grid containing a metal must be forced to some known potential. We do this by modifying the corresponding row in the matri as follows: 1. Replace entire row in L with all zeroes.. Place a 1 in the position along the center diagonal. 3. Place the alue of the applied potential in the same row in b. # # # # # # V1 0 # # # # # # V 0 metal applied metal applied V Vm Vm m Vm # # # # # # V NNy1 0 # # # # # # V N 0 Ny L' b Lecture
16 Fancy Way of Forcing Potentials We construct two terms: F Force matri f forced potentials Diagonal matri containing 1 s in the positions corresponding to alues we wish to force. Column ector containing the forced potentials. Numbers in positions not being forced are ignored. 1. Replace forced rows in L with all zeros. L IF L # # # # # # V1 0. Place a 1 in the diagonal element. # # # # # # V 0 metal applied metal applied L FIFL V Vm Vm m Vm. Place the forced potentials in b. # # # # # # V NNy1 0 # # # # # # V N 0 Ny b F Use same b for both f L' b homogeneous and inhomogeneous cases. Lecture 4 31 Calculating Transmission Line Parameters Calculate the field quantities e D e, h D e y Dy ey, h D y d ε RRyε y e dh, eh, dy RRε y y εyy ey dy, h ey, h C T d e 0y d y ey Calculate the transmission line parameters Z L C n c LC c eff 0 r,eff n eff Lecture 4 3 h T dh, eh, 1 Ch 0y L d yh, e yh, cc 0 h Note: we hae moed the constant 0 to the capacitance equation for conenience. Calculate the inductance and capacitance using numerical integration CAUTION: Be careful that you are consistent with your units. For eample, it is incorrect to set centimeters=1 and then set e0=8.854e-1 because 0 has units of F/m. 16
17 Finite-Difference Analysis of Transmission Lines Embedded in Arbitrary Anisotropic Media Implementation Step 1: Choose a Transmission Line We will choose to model a microstrip transmission line with the following parameters: r,sup r,sub w h r,sup r,sub air superstrate dielectric substrate w = 4.0 mm h = 3.0 mm Lecture
18 Step : Build Deice on Grid (1 of ) N unit cells N y unit cells We will use Dirichlet boundary conditions so there must be sufficient space between the microstrip and boundaries. Rule of Thumb: Spacer regions should be around three times the width of the line. Lecture 4 35 Step : Build Deice on Grid ( of ) We use si arrays to describe the transmission line. 1 grid ER ERy ERy ERyy grid 0 s 0 s 9 s 0 s 0 s 9 s We do not need to build ERz, ERyz, ERz, ERzy, or ERzz. Lecture
19 Step 3: Construct Matri Operators We use yeeder() to calculate the deriatie operators. % CALL FUNCTION TO CONSTRUCT DERIVATIVE OPERATORS NS = [N Ny]; %grid size RES = [d dy]; %grid resolution BC = [0 0]; %Dirichlet BCs [DVX,DVY,DEX,DEY] = yeeder(ns,res,bc); %Build matrices Since we are using Dirichlet boundary conditions, we can construct our interpolation matrices directly from the deriatie operators. y e R D R D R R R y y y f f f f i 1 i i1 i % FORM INTERPOLATION MATRIX FROM DERIVATIVE OPERATORS RXP = (d/)*abs(dvx); RYM = (dy/)*abs(dey); R = RXP*RYM; Lecture 4 37 Step 4: Construct Diagonalized Tensor Step 1: Parse materials from grid to 1 grid. ER = ER(::N,1::Ny); ERy = ERy(1::N,::Ny); ERy = ERy(::N,1::Ny); ERyy = ERyy(1::N,::Ny); Step : Diagonalize all four tensor elements. ER = diag(sparse(er(:))); ERy = diag(sparse(ery(:))); ERy = diag(sparse(ery(:))); ERyy = diag(sparse(eryy(:))); Step 3: Construct composite tensor ER = [ ER, R*ERy ; R *ERy, ERyy ]; Note the comple transpose here. Lecture
20 Step 5: Build L and L h Step 1. Build the inhomogeneous matri L L = [ DEX DEY ] * ER * [ DVX ; DVY ]; Step. Build the homogeneous matri L h Lh = [ DEX DEY ] * [ DVX ; DVY ]; L Lecture 4 39 Step 6: Force Known Potentials Step 1. Build the force matri F that identifies the locations of the forced potentials. F = SIG GND; F = diag(sparse(f(:))); Step : Build the column ector containing the alues of the forced potentials. f = 1*SIG + 0*GND; For two conductors 1 olt applied to SIG f = 0.5*SIG1 0.5*SIG + 0*GND; Step 3: Force the known potentials. L = (I - F)*L + F; Lh = (I - F)*Lh + F; b = F*f(:); For multiple conductors F = SIG1 SIG GND; Lecture
21 Step 7: Compute the Fields Step 1. Compute the potentials. BIG COMPUTATIONAL STEP!!!! 1 L b h L b 1 h Step : Calculate the E fields. e D e e y D y Step 3: Compute the D fields. d ε Rεy e d H dy R εy εyy ey e h d h e D h, e yh, D y d, h e, h d e yh, yh, h Lecture 4 41 Step 8: Compute TL Parameters Step 1. Compute the distributed capacitance C. 1 C DEdA V 0 A Step : Calculate the distributed inductance L. C = (e0*d*dy)*dy'*ey; Ch = (e0*d*dy)*dyh'*eyh; 1 C D E da h h h V0 A 1 c0ch L Step 3: Calculate characteristic impedance impedance L = 1/(c0^*Ch); Recall that we moed the 0 term to this equation for conenience. Z 0 L C Be sure you are consistent with your units! Lecture 4 4 1
22 Step 9: Visualize the Fields Step 1. Etract the and y components of E. e E = ey(1:m); e Ey = ey(m+1:*m); e y Step : Reshape from column ectors to D arrays. = reshape(,n,ny); E = reshape(e,n,ny); Ey = reshape(ey,n,ny); Step 3: Visualize in MATLAB using imagesc(), pcolor(), and/or quier(). For day to day data analysis, I use imagesc(). For generating pictures for publications and presentations, I use pcolor(). Lecture 4 43 Finite-Difference Analysis of Transmission Lines Embedded in Arbitrary Anisotropic Media Eamples
23 Eample #1: Ordinary Microstrip (1 of ) r,sup r,sub w h w = 4.0 mm h = 3.0 mm r,sup r,sub air dielectric Lecture 4 45 Eample #1: Ordinary Microstrip ( of ) N = 00 Ny = 150 d = dy = Z0 = ohms Lecture
24 Eample #: Anisotropic Microstrip (1 of 3) z y r,sup r,sub w h w = 4.0 mm h = 3.0 mm r,sup r,sub Lecture 4 47 Eample #: Anisotropic Microstrip ( of 3) To generate correct tensors, we start with the diagonalized tensor and the angle that it should be rotated around the z ais r z The rotation matri is cos 30 sin R R 30 sin 30 cos 30 0 z The rotated tensor is then R R r 1 z y z Lecture
25 Eample #: Anisotropic Microstrip (3 of 3) N = 00 Ny = 150 d = dy = Z0 = ohms Lecture 4 49 Generalization of the Method 5
26 Method Can Do More than Transmission Lines! The model we just deeloped simply calculates the potential in the icinity of multiple forced potentials. We used it to model a transmission line, but the method has other applications. V1 5 V V 7 V 5 V 7 V Potential V 0 V 0 V Lecture 4 51 Think of Laplace s Equation as a Linear Number Filler Inner Gien known alues at certain points (boundary conditions), Laplace s equation calculates the numbers eerywhere else so they ary linearly. Map of known alues (boundary alues) Laplace s equation is soled to fill in the alues away from the boundaries. Lecture 4 5 6
Topic 7e Finite Difference Analysis of Transmission Lines
Course Instructor r. Raymond C. Rumpf Office: A 337 Phone: (915) 747 6958 Mail: rcrumpf@utep.edu Topic 7e Finite ifference Analysis of Transmission Lines 4386/531 Computational Methods in 1 Outline Introduction
More informationNumerical Implementation of Transformation Optics
ECE 5322 21 st Century Electromagnetics Instructor: Office: Phone: E Mail: Dr. Raymond C. Rumpf A 337 (915) 747 6958 rcrumpf@utep.edu Lecture #16b Numerical Implementation of Transformation Optics Lecture
More informationTransmission lines using a distributed equivalent circuit
Cambridge Uniersity Press 978-1-107-02600-1 - Transmission Lines Equialent Circuits, Electromagnetic Theory, and Photons Part 1 Transmission lines using a distributed equialent circuit in this web serice
More informationElectrostatics: Energy in Electrostatic Fields
7/4/08 Electrostatics: Energy in Electrostatic Fields EE33 Electromagnetic Field Theory Outline Energy in terms of potential Energy in terms of the field Power and energy in conductors Electrostatics --
More informationElectrostatics: Electrostatic Devices
Electrostatics: Electrostatic Devices EE331 Electromagnetic Field Theory Outline Laplace s Equation Derivation Meaning Solving Laplace s equation Resistors Capacitors Electrostatics -- Devices Slide 1
More informationMagnetic Fields Part 3: Electromagnetic Induction
Magnetic Fields Part 3: Electromagnetic Induction Last modified: 15/12/2017 Contents Links Electromagnetic Induction Induced EMF Induced Current Induction & Magnetic Flux Magnetic Flux Change in Flux Faraday
More informationLecture Outline 9/27/2017. EE 4347 Applied Electromagnetics. Topic 4a
9/7/17 Course Instructor Dr. Raymond C. Rumpf Office: A 337 Phone: (915) 747 6958 E Mail: rcrumpf@utep.edu EE 4347 Applied Electromagnetics Topic 4a Transmission Lines Transmission These Lines notes may
More informationСollisionless damping of electron waves in non-maxwellian plasma 1
http:/arxi.org/physics/78.748 Сollisionless damping of electron waes in non-mawellian plasma V. N. Soshnio Plasma Physics Dept., All-Russian Institute of Scientific and Technical Information of the Russian
More informationTransmission Line Transients
8 5 Transmission Line Transients CHAPTER OBJECTIES After reading this chapter, you should be able to: Proide an analysis of traelling waes on transmission lines Derie a wae equation Understand the effect
More informationMaxwell s Equations:
Course Instructor Dr. Raymond C. Rumpf Office: A-337 Phone: (915) 747-6958 E-Mail: rcrumpf@utep.edu Maxwell s Equations: Physical Interpretation EE-3321 Electromagnetic Field Theory Outline Maxwell s Equations
More informationDynamics ( 동역학 ) Ch.2 Motion of Translating Bodies (2.1 & 2.2)
Dynamics ( 동역학 ) Ch. Motion of Translating Bodies (. &.) Motion of Translating Bodies This chapter is usually referred to as Kinematics of Particles. Particles: In dynamics, a particle is a body without
More informationE : Ground-penetrating radar (GPR)
Geophysics 3 March 009 E : Ground-penetrating radar (GPR) The EM methods in section D use low frequency signals that trael in the Earth by diffusion. These methods can image resistiity of the Earth on
More informationDepartment of Physics PHY 111 GENERAL PHYSICS I
EDO UNIVERSITY IYAMHO Department o Physics PHY 111 GENERAL PHYSICS I Instructors: 1. Olayinka, S. A. (Ph.D.) Email: akinola.olayinka@edouniersity.edu.ng Phone: (+234) 8062447411 2. Adekoya, M. A Email:
More informationTASK A. TRANSMISSION LINE AND DISCONTINUITIES
TASK A. TRANSMISSION LINE AND DISCONTINUITIES Task A. Transmission Line and Discontinuities... 1 A.I. TEM Transmission Line... A.I.1. Circuit Representation of a Uniform Transmission Line... A.I.. Time
More informationLECTURE 2: CROSS PRODUCTS, MULTILINEARITY, AND AREAS OF PARALLELOGRAMS
LECTURE : CROSS PRODUCTS, MULTILINEARITY, AND AREAS OF PARALLELOGRAMS MA1111: LINEAR ALGEBRA I, MICHAELMAS 016 1. Finishing up dot products Last time we stated the following theorem, for which I owe you
More informationLecture #16. Spatial Transforms. Lecture 16 1
ECE 53 1 st Century Electromagnetics Instructor: Office: Phone: E Mail: Dr. Raymond C. Rumpf A 337 (915) 747 6958 rcrumpf@utep.edu Lecture #16 Spatial ransforms Lecture 16 1 Lecture Outline ransformation
More informationSection 6: PRISMATIC BEAMS. Beam Theory
Beam Theory There are two types of beam theory aailable to craft beam element formulations from. They are Bernoulli-Euler beam theory Timoshenko beam theory One learns the details of Bernoulli-Euler beam
More informationLecture Outline. Maxwell s Equations Predict Waves Derivation of the Wave Equation Solution to the Wave Equation 8/7/2018
Course Instructor Dr. Raymond C. Rumpf Office: A 337 Phone: (915) 747 6958 E Mail: rcrumpf@utep.edu EE 4347 Applied Electromagnetics Topic 3a Electromagnetic Waves Electromagnetic These notes Waves may
More informationChapter 24 Capacitance and Dielectrics
Chapter 24 Capacitance and Dielectrics Lecture by Dr. Hebin Li Goals for Chapter 24 To understand capacitors and calculate capacitance To analyze networks of capacitors To calculate the energy stored in
More informationPH213 Chapter 24 Solutions
PH213 Chapter 24 Solutions 24.12. IDENTIFY and S ET UP: Use the expression for derived in Example 24.4. Then use Eq. (24.1) to calculate Q. E XECUTE: (a) From Example 24.4, The conductor at higher potential
More informationGeneral Lorentz Boost Transformations, Acting on Some Important Physical Quantities
General Lorentz Boost Transformations, Acting on Some Important Physical Quantities We are interested in transforming measurements made in a reference frame O into measurements of the same quantities as
More informationMaxwell s Equations:
Course Instructor Dr. Raymond C. Rumpf Office: A-337 Phone: (915) 747-6958 E-Mail: rcrumpf@utep.edu Maxwell s Equations: Terms & Definitions EE-3321 Electromagnetic Field Theory Outline Maxwell s Equations
More informationKinetic plasma description
Kinetic plasma description Distribution function Boltzmann and Vlaso equations Soling the Vlaso equation Examples of distribution functions plasma element t 1 r t 2 r Different leels of plasma description
More informationElectromagnetic Properties of Materials Part 2
ECE 5322 21 st Century Electromagnetics Instructor: Office: Phone: E Mail: Dr. Raymond C. Rumpf A 337 (915) 747 6958 rcrumpf@utep.edu Lecture #3 Electromagnetic Properties of Materials Part 2 Nonlinear
More informationChapter 1: Kinematics of Particles
Chapter 1: Kinematics of Particles 1.1 INTRODUCTION Mechanics the state of rest of motion of bodies subjected to the action of forces Static equilibrium of a body that is either at rest or moes with constant
More informationChapter 24 Capacitance and Dielectrics
Chapter 24 Capacitance and Dielectrics 1 Capacitors and Capacitance A capacitor is a device that stores electric potential energy and electric charge. The simplest construction of a capacitor is two parallel
More information1. The figure shows two long parallel wires carrying currents I 1 = 15 A and I 2 = 32 A (notice the currents run in opposite directions).
Final Eam Physics 222 7/29/211 NAME Use o = 8.85 1-12 C 2 /N.m 2, o = 9 1 9 N.m 2 /C 2, o/= 1-7 T m/a There are additional formulas in the final page of this eam. 1. The figure shows two long parallel
More informationElectric Motor and Dynamo the Hall effect
Electric Motor and Dynamo the Hall effect Frits F.M. de Mul Motor and Dynamo; Hall effect 1 Presentations: Electromagnetism: History Electromagnetism: Electr. topics Electromagnetism: Magn. topics Electromagnetism:
More information0 a 3 a 2 a 3 0 a 1 a 2 a 1 0
Chapter Flow kinematics Vector and tensor formulae This introductory section presents a brief account of different definitions of ector and tensor analysis that will be used in the following chapters.
More informationPHYS 1443 Section 004 Lecture #4 Thursday, Sept. 4, 2014
PHYS 1443 Section 004 Lecture #4 Thursday, Sept. 4, 014 One Dimensional Motion Motion under constant acceleration One dimensional Kinematic Equations How do we sole kinematic problems? Falling motions
More informationElectromagnetic Waves
Electromagnetic Waves Our discussion on dynamic electromagnetic field is incomplete. I H E An AC current induces a magnetic field, which is also AC and thus induces an AC electric field. H dl Edl J ds
More information10. Yes. Any function of (x - vt) will represent wave motion because it will satisfy the wave equation, Eq
CHAPER 5: Wae Motion Responses to Questions 5. he speed of sound in air obeys the equation B. If the bulk modulus is approximately constant and the density of air decreases with temperature, then the speed
More informationValidity of expressions
E&M Lecture 8 Topics: (1)Validity of expressions ()Electrostatic energy (in a capacitor?) (3)Collection of point charges (4)Continuous charge distribution (5)Energy in terms of electric field (6)Energy
More informationTransmission Line Basics
Transmission Line Basics Prof. Tzong-Lin Wu NTUEE 1 Outlines Transmission Lines in Planar structure. Key Parameters for Transmission Lines. Transmission Line Equations. Analysis Approach for Z and T d
More informationChapter 2: 1D Kinematics Tuesday January 13th
Chapter : D Kinematics Tuesday January 3th Motion in a straight line (D Kinematics) Aerage elocity and aerage speed Instantaneous elocity and speed Acceleration Short summary Constant acceleration a special
More informationLESSON 4: INTEGRATION BY PARTS (I) MATH FALL 2018
LESSON 4: INTEGRATION BY PARTS (I) MATH 6 FALL 8 ELLEN WELD. Integration by Parts We introduce another method for ealuating integrals called integration by parts. The key is the following : () u d = u
More informationChapter 24 Capacitance and Dielectrics
Chapter 24 Capacitance and Dielectrics 1 Capacitors and Capacitance A capacitor is a device that stores electric potential energy and electric charge. The simplest construction of a capacitor is two parallel
More informationECE 546 Lecture 13 Scattering Parameters
ECE 546 Lecture 3 Scattering Parameters Spring 08 Jose E. Schutt-Aine Electrical & Computer Engineering University of Illinois jesa@illinois.edu ECE 546 Jose Schutt Aine Transfer Function Representation
More informationChap. 1 Fundamental Concepts
NE 2 Chap. 1 Fundamental Concepts Important Laws in Electromagnetics Coulomb s Law (1785) Gauss s Law (1839) Ampere s Law (1827) Ohm s Law (1827) Kirchhoff s Law (1845) Biot-Savart Law (1820) Faradays
More informationa) (4 pts) What is the magnitude and direction of the acceleration of the electron?
PHYSCS 22 Fall 2010 - MDTERM #3 SHOW ALL WORK & REASONNG FOR FULL PONTS Question 1. (5 pts): Accurately show or state the direction of the force that is felt by the following charges or currents. +q -q
More informationLecture Outline. Attenuation Coefficient and Phase Constant Characteristic Impedance, Z 0 Special Cases of Transmission Lines
Course Instructor Dr. Raymond C. Rumpf Office: A 337 Phone: (915) 747 6958 E Mail: rcrumpf@utep.edu EE 4347 Applied Electromagnetics Topic 4b Transmission Line Parameters Transmission These Line notes
More informationv v Downloaded 01/11/16 to Redistribution subject to SEG license or copyright; see Terms of Use at
The pseudo-analytical method: application of pseudo-laplacians to acoustic and acoustic anisotropic wae propagation John T. Etgen* and Serre Brandsberg-Dahl Summary We generalize the pseudo-spectral method
More informationTransmission-Line Essentials for Digital Electronics
C H A P T E R 6 Transmission-Line Essentials for Digital Electronics In Chapter 3 we alluded to the fact that lumped circuit theory is based on lowfrequency approximations resulting from the neglect of
More informationReview of Linear Algebra
Review of Linear Algebra Dr Gerhard Roth COMP 40A Winter 05 Version Linear algebra Is an important area of mathematics It is the basis of computer vision Is very widely taught, and there are many resources
More informationDisplacement, Time, Velocity
Lecture. Chapter : Motion along a Straight Line Displacement, Time, Velocity 3/6/05 One-Dimensional Motion The area of physics that we focus on is called mechanics: the study of the relationships between
More informationLAB 5. INTRODUCTION Finite Difference Method
LAB 5 In previous two computer labs, you have seen how the analytical techniques for solving electrostatic problems can be approximately solved using numerical methods. For example, you have approximated
More informationFeb 6, 2013 PHYSICS I Lecture 5
95.141 Feb 6, 213 PHYSICS I Lecture 5 Course website: faculty.uml.edu/pchowdhury/95.141/ www.masteringphysics.com Course: UML95141SPRING213 Lecture Capture h"p://echo36.uml.edu/chowdhury213/physics1spring.html
More informationComplex Wave Parameters Visualization of EM Waves Complex Wave Parameters for Special Cases
Course Instructor Dr. Ramond C. Rumpf Office: A 337 Phone: (915) 747 6958 E Mail: rcrumpf@utep.edu EE 4347 Applied Electromagnetics Topic 3d Waves in Loss Dielectrics Loss Dielectrics These notes ma contain
More informationDynamic potentials and the field of the moving charges
Dynamic potentials and the field of the moing charges F. F. Mende http://fmnauka.narod.ru/works.html mende_fedor@mail.ru Abstract Is deeloped the concept of scalar-ector potential, in which within the
More informationEE243 Advanced Electromagnetic Theory Lec # 15 Plasmons. Reading: These PPT notes and Harrington on corrugated surface 4.8.
EE Applied EM Fall 6, Neureuther Lecture #5 Ver //6 EE43 Adanced Electromagnetic Theory Lec # 5 Plasmons Fixed Slides 6, (Group and Phase Velocity for Guided Waes) (Sign Reersals for Propagation Direction
More informationElectromagnetic Waves & Polarization
Course Instructor Dr. Raymond C. Rumpf Office: A 337 Phone: (915) 747 6958 E Mail: rcrumpf@utep.edu EE 4347 Applied Electromagnetics Topic 3a Electromagnetic Waves & Polarization Electromagnetic These
More informationCourse no. 4. The Theory of Electromagnetic Field
Cose no. 4 The Theory of Electromagnetic Field Technical University of Cluj-Napoca http://www.et.utcluj.ro/cs_electromagnetics2006_ac.htm http://www.et.utcluj.ro/~lcret March 19-2009 Chapter 3 Magnetostatics
More informationUNDERSTAND MOTION IN ONE AND TWO DIMENSIONS
SUBAREA I. COMPETENCY 1.0 UNDERSTAND MOTION IN ONE AND TWO DIMENSIONS MECHANICS Skill 1.1 Calculating displacement, aerage elocity, instantaneous elocity, and acceleration in a gien frame of reference
More informationLecture #8-6 Waves and Sound 1. Mechanical Waves We have already considered simple harmonic motion, which is an example of periodic motion in time.
Lecture #8-6 Waes and Sound 1. Mechanical Waes We hae already considered simple harmonic motion, which is an example of periodic motion in time. The position of the body is changing with time as a sinusoidal
More informationPower Engineering II. Power System Transients
Power System Transients Oeroltage Maximum supply oltage U m the maximum effectie alue of line oltage that can occur at any time or place under normal operating conditions Rated oltage (k) 6 10 22 35 110
More informationChapter 6: Operational Amplifiers
Chapter 6: Operational Amplifiers Circuit symbol and nomenclature: An op amp is a circuit element that behaes as a VCVS: The controlling oltage is in = and the controlled oltage is such that 5 5 A where
More informationLecture Outline. Scattering at an Impedance Discontinuity Power on a Transmission Line Voltage Standing Wave Ratio (VSWR) 8/10/2018
Course Instructor Dr. Raymond C. Rumpf Office: A 337 Phone: (95) 747 6958 E Mail: rcrumpf@utep.edu EE 4347 Applied Electromagnetics Topic 4d Scattering on a Transmission Line Scattering These on a notes
More informationbe ye transformed by the renewing of your mind Romans 12:2
Lecture 12: Coordinate Free Formulas for Affine and rojectie Transformations be ye transformed by the reing of your mind Romans 12:2 1. Transformations for 3-Dimensional Computer Graphics Computer Graphics
More informationLecture Outline. Scattering at an Interface Sunrises & Sunsets Rainbows Polarized Sunglasses 8/9/2018. EE 4347 Applied Electromagnetics.
Course Instructor Dr. Raymond C. Rumpf Office: A 337 Phone: (915) 747 6958 E Mail: rcrumpf@utep.edu EE 4347 Applied Electromagnetics Topic 3i Scattering at an Interface: Examples Examples These notes may
More informationChapter 16. Kinetic Theory of Gases. Summary. molecular interpretation of the pressure and pv = nrt
Chapter 16. Kinetic Theory of Gases Summary molecular interpretation of the pressure and pv = nrt the importance of molecular motions elocities and speeds of gas molecules distribution functions for molecular
More informationEffective mass: from Newton s law. Effective mass. I.2. Bandgap of semiconductors: the «Physicist s approach» - k.p method
Lecture 4 1/10/011 Effectie mass I.. Bandgap of semiconductors: the «Physicist s approach» - k.p method I.3. Effectie mass approximation - Electrons - Holes I.4. train effect on band structure - Introduction:
More informationProgress In Electromagnetics Research Symposium 2005, Hangzhou, China, August
Progress In Electromagnetics Research Symposium 2005, Hangzhou, China, August 22-26 115 A Noel Technique for Localizing the Scatterer in Inerse Profiling of Two Dimensional Circularly Symmetric Dielectric
More informationS 1 S 2 A B C. 7/25/2006 Superposition ( F.Robilliard) 1
P S S S 0 x S A B C 7/5/006 Superposition ( F.Robilliard) Superposition of Waes: As we hae seen preiously, the defining property of a wae is that it can be described by a wae function of the form - y F(x
More informationBoundary and Excitation Training February 2003
Boundary and Excitation Training February 2003 1 Why are They Critical? For most practical problems, the solution to Maxwell s equations requires a rigorous matrix approach such as the Finite Element Method
More informationCS205b/CME306. Lecture 4. x v. + t
CS05b/CME306 Lecture 4 Time Integration We now consider seeral popular approaches for integrating an ODE Forward Euler Forward Euler eolution takes on the form n+ = n + Because forward Euler is unstable
More informationPhysics 11 Chapter 15/16 HW Solutions
Physics Chapter 5/6 HW Solutions Chapter 5 Conceptual Question: 5, 7 Problems:,,, 45, 50 Chapter 6 Conceptual Question:, 6 Problems:, 7,, 0, 59 Q5.5. Reason: Equation 5., string T / s, gies the wae speed
More informationIntroduction to RF Design. RF Electronics Spring, 2016 Robert R. Krchnavek Rowan University
Introduction to RF Design RF Electronics Spring, 2016 Robert R. Krchnavek Rowan University Objectives Understand why RF design is different from lowfrequency design. Develop RF models of passive components.
More informationStatus: Unit 2, Chapter 3
1 Status: Unit, Chapter 3 Vectors and Scalars Addition of Vectors Graphical Methods Subtraction of Vectors, and Multiplication by a Scalar Adding Vectors by Components Unit Vectors Vector Kinematics Projectile
More informationLesson 3: Free fall, Vectors, Motion in a plane (sections )
Lesson 3: Free fall, Vectors, Motion in a plane (sections.6-3.5) Last time we looked at position s. time and acceleration s. time graphs. Since the instantaneous elocit is lim t 0 t the (instantaneous)
More informationLect-19. In this lecture...
19 1 In this lecture... Helmholtz and Gibb s functions Legendre transformations Thermodynamic potentials The Maxwell relations The ideal gas equation of state Compressibility factor Other equations of
More informationAnisotropic Design Considerations for 28 Gbps Via to Stripline Transitions
DesignCon 2015 Anisotropic Design Considerations for 28 Gbps Via to Stripline Transitions Scott McMorrow, Teraspeed Consulting A Division of Samtec Ed Sayre, Teraspeed Consulting A Division of Samtec Chudy
More informationDoppler shifts in astronomy
7.4 Doppler shift 253 Diide the transformation (3.4) by as follows: = g 1 bck. (Lorentz transformation) (7.43) Eliminate in the right-hand term with (41) and then inoke (42) to yield = g (1 b cos u). (7.44)
More informationDO PHYSICS ONLINE. WEB activity: Use the web to find out more about: Aristotle, Copernicus, Kepler, Galileo and Newton.
DO PHYSICS ONLINE DISPLACEMENT VELOCITY ACCELERATION The objects that make up space are in motion, we moe, soccer balls moe, the Earth moes, electrons moe, - - -. Motion implies change. The study of the
More informationMicrowave Engineering 3e Author - D. Pozar
Microwave Engineering 3e Author - D. Pozar Sections 3.6 3.8 Presented by Alex Higgins 1 Outline Section 3.6 Surface Waves on a Grounded Dielectric Slab Section 3.7 Stripline Section 3.8 Microstrip An Investigation
More informationMon Apr dot product, length, orthogonality, projection onto the span of a single vector. Announcements: Warm-up Exercise:
Math 2270-004 Week 2 notes We will not necessarily finish the material from a gien day's notes on that day. We may also add or subtract some material as the week progresses, but these notes represent an
More informationA-level Mathematics. MM03 Mark scheme June Version 1.0: Final
-leel Mathematics MM0 Mark scheme 660 June 0 Version.0: Final Mark schemes are prepared by the Lead ssessment Writer and considered, together with the releant questions, by a panel of subject teachers.
More informationPHYS 212 Final Exam (Old Material) Solutions - Practice Test
PHYS 212 Final Exam (Old Material) Solutions - Practice Test 1E If the ball is attracted to the rod, it must be made of a conductive material, otherwise it would not have been influenced by the nearby
More informationPhysics 111. Help sessions meet Sunday, 6:30-7:30 pm in CLIR Wednesday, 8-9 pm in NSC 098/099
ics Announcements day, ember 7, 2007 Ch 2: graphing - elocity s time graphs - acceleration s time graphs motion diagrams - acceleration Free Fall Kinematic Equations Structured Approach to Problem Soling
More informationRelativistic Energy Derivation
Relatiistic Energy Deriation Flamenco Chuck Keyser //4 ass Deriation (The ass Creation Equation ρ, ρ as the initial condition, C the mass creation rate, T the time, ρ a density. Let V be a second mass
More informationI.3.5 Ringing. Ringing=Unwanted oscillations of voltage and/or current
I.3.5 Ringing Ringing=Unwanted oscillations of voltage and/or current Ringing is caused b multiple reflections. The original wave is reflected at the load, this reflection then gets reflected back at the
More informationLecture Outline. Shorted line (Z L = 0) Open circuit line (Z L = ) Matched line (Z L = Z 0 ) 9/28/2017. EE 4347 Applied Electromagnetics.
9/8/17 Course Instructor Dr. Raymond C. Rumpf Office: A 337 Phone: (915) 747 6958 E Mail: rcrumpf@utep.edu EE 4347 Applied Electromagnetics Topic 4b Transmission ine Behavior Transmission These ine notes
More informationYour Comments. I don't understand how to find current given the velocity and magnetic field. I only understand how to find external force
Your Comments CONFUSED! Especially with the direction of eerything The rotating loop checkpoint question is incredibly difficult to isualize. All of this is pretty confusing, but 'm especially confused
More informationWould you risk your live driving drunk? Intro
Martha Casquete Would you risk your lie driing drunk? Intro Motion Position and displacement Aerage elocity and aerage speed Instantaneous elocity and speed Acceleration Constant acceleration: A special
More informationSpectral Domain Analysis of Open Planar Transmission Lines
Mikrotalasna revija Novembar 4. Spectral Domain Analysis of Open Planar Transmission Lines Ján Zehentner, Jan Mrkvica, Jan Macháč Abstract The paper presents a new code calculating the basic characteristics
More informationECE 497 JS Lecture -03 Transmission Lines
ECE 497 JS Lecture -03 Transmission Lines Spring 2004 Jose E. Schutt-Aine Electrical & Computer Engineering University of Illinois jose@emlab.uiuc.edu 1 MAXWELL S EQUATIONS B E = t Faraday s Law of Induction
More informationFigure 1: Left: Image from A new era: Nanotube displays (Nature Photonics), Right: Our approximation of a single subpixel
MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Electrical Engineering and Computer Science 6.007 Electromagnetic Energy: From Motors to Lasers Spring 2011 Problem Set 2: Energy and Static Fields Due
More informationLECTURE 3 3.1Rules of Vector Differentiation
LETURE 3 3.1Rules of Vector Differentiation We hae defined three kinds of deriaties inoling the operator grad( ) i j k, x y z 1 3 di(., x y z curl( i x 1 j y k z 3 d The good news is that you can apply
More informationEE 5337 Computational Electromagnetics (CEM) Introduction to CEM
Instructor Dr. Raymond Rumpf (915) 747 6958 rcrumpf@utep.edu EE 5337 Computational Electromagnetics (CEM) Lecture #1 Introduction to CEM Lecture 1These notes may contain copyrighted material obtained under
More informationINTRODUCTION TO TRANSMISSION LINES DR. FARID FARAHMAND FALL 2012
INTRODUCTION TO TRANSMISSION LINES DR. FARID FARAHMAND FALL 2012 http://www.empowermentresources.com/stop_cointelpro/electromagnetic_warfare.htm RF Design In RF circuits RF energy has to be transported
More informationConventional Paper-I Solutions:(ECE)
Conentional Paper-- 13 olutions:(ece) ol. 1(a)(i) n certain type of polar dielectric materials permanent electric diploes are oriented in specific direction een in absence of external electric field. o
More informationPhysics 212. Lecture 7. Conductors and Capacitance. Physics 212 Lecture 7, Slide 1
Physics 212 Lecture 7 Conductors and Capacitance Physics 212 Lecture 7, Slide 1 Conductors The Main Points Charges free to move E = 0 in a conductor Surface = Equipotential In fact, the entire conductor
More informationPrediction of anode arc root position in a DC arc plasma torch
Prediction of anode arc root position in a DC arc plasma torch He-Ping Li 1, E. Pfender 1, Xi Chen 1 Department of Mechanical Engineering, Uniersity of Minnesota, Minneapolis, MN 55455, USA Department
More informationKINGS COLLEGE OF ENGINEERING DEPARTMENT OF ELECTRONICS AND COMMUNICATION ENGINEERING QUESTION BANK
KINGS COLLEGE OF ENGINEERING DEPARTMENT OF ELECTRONICS AND COMMUNICATION ENGINEERING QUESTION BANK SUB.NAME : ELECTROMAGNETIC FIELDS SUBJECT CODE : EC 2253 YEAR / SEMESTER : II / IV UNIT- I - STATIC ELECTRIC
More informationAntennas and Propagation. Chapter 2: Basic Electromagnetic Analysis
Antennas and Propagation : Basic Electromagnetic Analysis Outline Vector Potentials, Wave Equation Far-field Radiation Duality/Reciprocity Transmission Lines Antennas and Propagation Slide 2 Antenna Theory
More information4-vectors. Chapter Definition of 4-vectors
Chapter 12 4-ectors Copyright 2004 by Daid Morin, morin@physics.harard.edu We now come to a ery powerful concept in relatiity, namely that of 4-ectors. Although it is possible to derie eerything in special
More information4. A Physical Model for an Electron with Angular Momentum. An Electron in a Bohr Orbit. The Quantum Magnet Resulting from Orbital Motion.
4. A Physical Model for an Electron with Angular Momentum. An Electron in a Bohr Orbit. The Quantum Magnet Resulting from Orbital Motion. We now hae deeloped a ector model that allows the ready isualization
More informationAssignment 4 (Solutions) NPTEL MOOC (Bayesian/ MMSE Estimation for MIMO/OFDM Wireless Communications)
Assignment 4 Solutions NPTEL MOOC Bayesian/ MMSE Estimation for MIMO/OFDM Wireless Communications The system model can be written as, y hx + The MSE of the MMSE estimate ĥ of the aboe mentioned system
More informationA Brief Revision of Vector Calculus and Maxwell s Equations
A Brief Revision of Vector Calculus and Maxwell s Equations Debapratim Ghosh Electronic Systems Group Department of Electrical Engineering Indian Institute of Technology Bombay e-mail: dghosh@ee.iitb.ac.in
More informationECE 6340 Intermediate EM Waves. Fall 2016 Prof. David R. Jackson Dept. of ECE. Notes 15
ECE 634 Intermediate EM Waves Fall 6 Prof. David R. Jackson Dept. of ECE Notes 5 Attenuation Formula Waveguiding system (WG or TL): S z Waveguiding system Exyz (,, ) = E( xye, ) = E( xye, ) e γz jβz αz
More informationGravitational Poynting theorem: interaction of gravitation and electromagnetism
Graitational Poynting theorem 433 Journal of Foundations of Physics and Chemistry, 0, ol. (4) 433 440 Graitational Poynting theorem: interaction of graitation and electromagnetism M.W. Eans Alpha Institute
More information