Effects of 20-H Rule and Shielding Vias on Electromagnetic Radiation From Printed Circuit Boards
|
|
- Shanon Alexander
- 6 years ago
- Views:
Transcription
1 Effects of 20-H Rule an Shieling Vias on Electromagnetic Raiation From Printe Circuit Boars Huabo Chen, Stuent Member, IEEE, an Jiayuan Fang, Senior Member, IEEE Dept. of Electrical Engineering, University of California at Santa Cruz, Santa Cruz, CA Tel: (83) Fax: (83) Abstract: This paper investigates the effects of 20-H rule an shieling vias on electromagnetic raiation from the printe circuits boars. Introuction As the operating frequency of electronic circuits continues to increase, toay s package an printe circuit boar esigners face more raiation problem than ever before. The control of raiate emissions to make the package comply with raiation constraints is one of the most important aspects of the EMC stuy. Some rules-of-thumb are employe to help the esigners to reuce the raiation problems. This paper presents an investigation on the effects of the 20-H rule an the shieling vias on raiation from printe circuit boars. Effects of 20-H Rule The 20-H rule [][3] states that the groun planes are extene beyon the s by about 20 times the istance between the planes. Let us consier the simple structure consisting of one an one groun plane shown in Figure (a). The 20-H rule structure is shown in Figure. groun plane 20 groun plane (a) two planes are of the same size 20-H rule 20 2 groun plane image of Since the raiation is closely relate to reflection coefficient at the open en of the two planes, the reflection coefficient is then investigate. Assume the planes have zero thickness, the reflection coefficient at the open en of two parallel planes shown in Figure (a) can be foun in [2] where an (c) image of the in 20-H rule structure R R Figure jθ = R e, () πq = e, (2) 2 sin q = + 2m θ 2q C ln A2 m+ ( S 2m+ ) q, (3) q q m= q =, (4) λ
2 where C is Euler s constant, which is , λ is the wavelength an is the plane separation. A 2 m+ is the expansion coefficient of the function sin x, S2 m+ can be obtaine by sin 2m+ x = A2 m+ x. (5) m= 0 S 2m+ =. (6) 2m+ n= n The amplitue an phase of the reflection coefficient as functions of the plane separation are shown in Figure 2(a) an 2 respectively. It can be seen that the larger the separation between planes, the smaller the amplitue of the reflections coefficient an the larger the raiation. The reflection coefficient of the 20-H rule structure can be estimate by that of the an its image pair as shown in Figure (c). Because the separation between the an its image plane is twice as large as that of the structure shown in Figure (a), the reflection coefficient of the 20-H rule structure is smaller in the amplitue. Therefore, more raiation is expecte to come out of the eges of the boar implemente with 20-H rule. The test structure for the numerical computation is shown in Figure 3. The size of the groun plane is 0cm by 0cm an the plane separation is 0.5mm. The relative ielectric constant is 4.0. The of the 20-H rule structure is cm smaller than the groun plane on each sie. 3-D FDTD metho is use to compute the raiation. The raiation power is efine as the surface integration of the poynting vector v v v P t = E H s, (7) ( ) ( ) Enclose Surface where E v is the electric fiel an H v is the magnetic fiel, on an enclose surface of the boar structure. The raiation is compare between the 20-H rule structure an the normal structure where the groun plane an the are both of 0cm x 0cm. Figure 4(a) shows the raiation on the top an the bottom surfaces. The raiation of the 20-H rule structure is somewhat smaller on the bottom surface but increases significantly on the top surface. The total raiation on the enclose surface is shown in Figure 4, from which one can see the raiation from the 20-H rule boar is much stronger than that from the boar of the same size planes. This observation is consistent with the theoretical analysis presente above. Figure 3 two-plane test structure Figure 5 three-plane test structure Consier the case where the 20-H rule is applie to the three-plane structure shown in Figure 5. The top an bottom groun planes are of the same size. The at the mile is shrinke insie by the 20-H rule. Raiation is examine on the enclose surface. Figure 6(a) an compare the raiation of the normal structure an the 20-H rule structure on the top an the bottom surfaces. It is foun that for the more than two plane structure, there is no significant change in raiation if the in the mile is setback using 20-H rule.
3 Effects of Shieling Vias The effects of shieling vias are also stuie using FDTD metho. Shieling vias are ae to connect the two groun planes on four eges of the three-plane structure shown in Figure 5. The raiation from the boar with ifferent numbers of shieling vias is compare in Figure 7. It can be seen that a small number of shieling vias can cut the raiation significantly. Conclusion This paper investigates the effects of 20-H rule an shieling vias on the raiation from the printe circuit boar. For the two-plane structure, 20-H rule yiels much more raiation than the normal structure. For the multiple plane case, no significant change in raiation is foun if the 20-H rule is applie to the internal planes. Also the numerical result shows that the usage of shieling vias woul cut own the raiation effectively. Reference [] Mark I. Montrose, Printe Circuit Boar Design Techniques for EMC Compliance, New York: IEEE Inc., 996. [2] I. A. Weinstein, The Theory of Diffraction an the Factorization Metho (Generalize Wiener-Hopf Technique), Bouler: Golem Press, 969. [3] Dr. Zorica Pantic-Tanner & Franz Gisin, Raiation from Ege Effects in Printe Circuit Boars (PCBs), presentation at the monthly chapter meeting of Santa Clara Valley Chapter of IEEE EMC Society, May, (a) Figure 2. Reflection coefficient at the open en of two parallel planes (a) amplitue phase
4 (a) Figure 4. Comparison of the raiation of two-plane structure on (a) top an bottom surface summation of all the surfaces (a) Figure 6. Comparison of the raiation of three-plane structure on (a) top surface bottom surface Figure 7. Raiation from the boar with shieling vias
5
Design and Analysis of Printed Circuit Boards Using FDTD Method for The 20-H Rule
Singapore-MIT Alliance Annual Symposium 22 Design and Analysis of Printed Circuit Boards Using FDTD Method for The 2-H Rule Jiang Yi, Le-Wei Li and Er-Ping Li Abstract--With the increasing demand of higher
More informationDay 4: Motion Along a Curve Vectors
Day 4: Motion Along a Curve Vectors I give my stuents the following list of terms an formulas to know. Parametric Equations, Vectors, an Calculus Terms an Formulas to Know: If a smooth curve C is given
More informationTEST 2 (PHY 250) Figure Figure P26.21
TEST 2 (PHY 250) 1. a) Write the efinition (in a full sentence) of electric potential. b) What is a capacitor? c) Relate the electric torque, exerte on a molecule in a uniform electric fiel, with the ipole
More information10. Magnetism. ) it is. S G appropriate to call the magnetic pole
10 agnetism The wor magnetism is erive from iron ore magnetite (Fe 3 O 4, which was foun in the islan of magnesia in Greece It is believe that the Chinese ha known the property of the magnet even in 000
More informationA Model of Electron-Positron Pair Formation
Volume PROGRESS IN PHYSICS January, 8 A Moel of Electron-Positron Pair Formation Bo Lehnert Alfvén Laboratory, Royal Institute of Technology, S-44 Stockholm, Sween E-mail: Bo.Lehnert@ee.kth.se The elementary
More informationNuclear Physics and Astrophysics
Nuclear Physics an Astrophysics PHY-302 Dr. E. Rizvi Lecture 2 - Introuction Notation Nuclies A Nuclie is a particular an is esignate by the following notation: A CN = Atomic Number (no. of Protons) A
More informationChapter 6. Electromagnetic Oscillations and Alternating Current
hapter 6 Electromagnetic Oscillations an Alternating urrent hapter 6: Electromagnetic Oscillations an Alternating urrent (hapter 31, 3 in textbook) 6.1. Oscillations 6.. The Electrical Mechanical Analogy
More informationIn the usual geometric derivation of Bragg s Law one assumes that crystalline
Diffraction Principles In the usual geometric erivation of ragg s Law one assumes that crystalline arrays of atoms iffract X-rays just as the regularly etche lines of a grating iffract light. While this
More informationPhysics for Scientists & Engineers 2
Capacitors Physics for Scientists & Engineers 2 Spring Semester 2005 Lecture 12 Capacitors are evices that can store electrical energy Capacitors are use in many every-ay applications Heart efibrillators
More informationA Quantitative Analysis of Coupling for a WPT System Including Dielectric/Magnetic Materials
Progress In Electromagnetics Research Letters, Vol. 72, 127 134, 2018 A Quantitative Analysis of Coupling for a WPT System Incluing Dielectric/Magnetic Materials Yangjun Zhang *, Tatsuya Yoshiawa, an Taahiro
More informationV q.. REASONING The potential V created by a point charge q at a spot that is located at a
8. REASONING The electric potential at a istance r from a point charge q is given by Equation 9.6 as kq / r. The total electric potential at location P ue to the four point charges is the algebraic sum
More informationHomework 7 Due 18 November at 6:00 pm
Homework 7 Due 18 November at 6:00 pm 1. Maxwell s Equations Quasi-statics o a An air core, N turn, cylinrical solenoi of length an raius a, carries a current I Io cos t. a. Using Ampere s Law, etermine
More information3-dimensional Evolution of an Emerging Flux Tube in the Sun. T. Magara
3-imensional Evolution of an Emerging Flux Tube in the Sun T. Magara (Montana State University) February 6, 2002 Introuction of the stuy Dynamical evolution of emerging fiel lines Physical process working
More informationConservation laws a simple application to the telegraph equation
J Comput Electron 2008 7: 47 51 DOI 10.1007/s10825-008-0250-2 Conservation laws a simple application to the telegraph equation Uwe Norbrock Reinhol Kienzler Publishe online: 1 May 2008 Springer Scienceusiness
More informationWave Propagation in Grounded Dielectric Slabs with Double Negative Metamaterials
6 Progress In Electromagnetics Research Symposium 6, Cambrige, US, March 6-9 Wave Propagation in Groune Dielectric Slabs with Double Negative Metamaterials W. Shu an J. M. Song Iowa State University, US
More informationMATH , 06 Differential Equations Section 03: MWF 1:00pm-1:50pm McLaury 306 Section 06: MWF 3:00pm-3:50pm EEP 208
MATH 321-03, 06 Differential Equations Section 03: MWF 1:00pm-1:50pm McLaury 306 Section 06: MWF 3:00pm-3:50pm EEP 208 Instructor: Brent Deschamp Email: brent.eschamp@ssmt.eu Office: McLaury 316B Phone:
More informationThis section outlines the methodology used to calculate the wave load and wave wind load values.
COMPUTERS AND STRUCTURES, INC., JUNE 2014 AUTOMATIC WAVE LOADS TECHNICAL NOTE CALCULATION O WAVE LOAD VALUES This section outlines the methoology use to calculate the wave loa an wave win loa values. Overview
More informationThermal conductivity of graded composites: Numerical simulations and an effective medium approximation
JOURNAL OF MATERIALS SCIENCE 34 (999)5497 5503 Thermal conuctivity of grae composites: Numerical simulations an an effective meium approximation P. M. HUI Department of Physics, The Chinese University
More informationTable of Common Derivatives By David Abraham
Prouct an Quotient Rules: Table of Common Derivatives By Davi Abraham [ f ( g( ] = [ f ( ] g( + f ( [ g( ] f ( = g( [ f ( ] g( g( f ( [ g( ] Trigonometric Functions: sin( = cos( cos( = sin( tan( = sec
More informationHarmonic Modelling of Thyristor Bridges using a Simplified Time Domain Method
1 Harmonic Moelling of Thyristor Briges using a Simplifie Time Domain Metho P. W. Lehn, Senior Member IEEE, an G. Ebner Abstract The paper presents time omain methos for harmonic analysis of a 6-pulse
More informationCAPACITANCE: CHAPTER 24. ELECTROSTATIC ENERGY and CAPACITANCE. Capacitance and capacitors Storage of electrical energy. + Example: A charged spherical
CAPACITANCE: CHAPTER 24 ELECTROSTATIC ENERGY an CAPACITANCE Capacitance an capacitors Storage of electrical energy Energy ensity of an electric fiel Combinations of capacitors In parallel In series Dielectrics
More information3.7 Implicit Differentiation -- A Brief Introduction -- Student Notes
Fin these erivatives of these functions: y.7 Implicit Differentiation -- A Brief Introuction -- Stuent Notes tan y sin tan = sin y e = e = Write the inverses of these functions: y tan y sin How woul we
More informationx f(x) x f(x) approaching 1 approaching 0.5 approaching 1 approaching 0.
Engineering Mathematics 2 26 February 2014 Limits of functions Consier the function 1 f() = 1. The omain of this function is R + \ {1}. The function is not efine at 1. What happens when is close to 1?
More informationLie symmetry and Mei conservation law of continuum system
Chin. Phys. B Vol. 20, No. 2 20 020 Lie symmetry an Mei conservation law of continuum system Shi Shen-Yang an Fu Jing-Li Department of Physics, Zhejiang Sci-Tech University, Hangzhou 3008, China Receive
More informationDiophantine Approximations: Examining the Farey Process and its Method on Producing Best Approximations
Diophantine Approximations: Examining the Farey Process an its Metho on Proucing Best Approximations Kelly Bowen Introuction When a person hears the phrase irrational number, one oes not think of anything
More informationMath 1B, lecture 8: Integration by parts
Math B, lecture 8: Integration by parts Nathan Pflueger 23 September 2 Introuction Integration by parts, similarly to integration by substitution, reverses a well-known technique of ifferentiation an explores
More informationThe Principle of Least Action
Chapter 7. The Principle of Least Action 7.1 Force Methos vs. Energy Methos We have so far stuie two istinct ways of analyzing physics problems: force methos, basically consisting of the application of
More informationLinear First-Order Equations
5 Linear First-Orer Equations Linear first-orer ifferential equations make up another important class of ifferential equations that commonly arise in applications an are relatively easy to solve (in theory)
More informationStudy on aero-acoustic structural interactions in fan-ducted system
Stuy on aero-acoustic structural interactions in fan-ucte system Yan-kei CHIANG 1 ; Yat-sze CHOY ; Li CHENG 3 ; Shiu-keung TANG 4 1,, 3 Department of Mechanical Engineering, The Hong Kong Polytechnic University,
More informationSOLUTION & ANSWER FOR KCET-2009 VERSION A1 [PHYSICS]
SOLUTION & ANSWER FOR KCET-009 VERSION A [PHYSICS]. The number of significant figures in the numbers.8000 ---- 5 an 7.8000 5 significant igits 8000.50 7 significant igits. β-ecay means emission of electron
More informationOptimization of Geometries by Energy Minimization
Optimization of Geometries by Energy Minimization by Tracy P. Hamilton Department of Chemistry University of Alabama at Birmingham Birmingham, AL 3594-140 hamilton@uab.eu Copyright Tracy P. Hamilton, 1997.
More informationDue to Sun s (and rest of solar system s) motion [Fig 16-3, relative_motion.avi]
Chapter 6: Basic Properties of Stars Star Names Ancient Arabic, Greek or Latin names By constellation, ecreasing orer of brightness α alpha, β beta, γ gamma... Stellar istances Pre-telescope Observations
More informationTRACKING CONTROL OF MULTIPLE MOBILE ROBOTS: A CASE STUDY OF INTER-ROBOT COLLISION-FREE PROBLEM
265 Asian Journal of Control, Vol. 4, No. 3, pp. 265-273, September 22 TRACKING CONTROL OF MULTIPLE MOBILE ROBOTS: A CASE STUDY OF INTER-ROBOT COLLISION-FREE PROBLEM Jurachart Jongusuk an Tsutomu Mita
More informationd dx But have you ever seen a derivation of these results? We ll prove the first result below. cos h 1
Lecture 5 Some ifferentiation rules Trigonometric functions (Relevant section from Stewart, Seventh Eition: Section 3.3) You all know that sin = cos cos = sin. () But have you ever seen a erivation of
More informationPERMANENT MAGNETS CHAPTER MAGNETIC POLES AND BAR MAGNETS
CHAPTER 6 PERAET AGET 6. AGETIC POLE AD BAR AGET We have seen that a small current-loop carrying a current i, prouces a magnetic fiel B o 4 ji ' at an axial point. Here p ia is the magnetic ipole moment
More informationLecture XII. where Φ is called the potential function. Let us introduce spherical coordinates defined through the relations
Lecture XII Abstract We introuce the Laplace equation in spherical coorinates an apply the metho of separation of variables to solve it. This will generate three linear orinary secon orer ifferential equations:
More informationLecture 2 Lagrangian formulation of classical mechanics Mechanics
Lecture Lagrangian formulation of classical mechanics 70.00 Mechanics Principle of stationary action MATH-GA To specify a motion uniquely in classical mechanics, it suffices to give, at some time t 0,
More informationOn Ruby s solid angle formula and some of its generalizations
On Ruby s soli angle formula an some of its generalizations Samuel Friot arxiv:4.3985v [nucl-ex] 5 Oct 4 Abstract Institut e Physique Nucléaire Orsay Université Paris-Su, INP3-NRS, F-945 Orsay eex, France
More informationTHE USE OF KIRCHOFF S CURRENT LAW AND CUT-SET EQUATIONS IN THE ANALYSIS OF BRIDGES AND TRUSSES
Session TH US O KIRCHO S CURRNT LAW AND CUT-ST QUATIONS IN TH ANALYSIS O BRIDGS AND TRUSSS Ravi P. Ramachanran an V. Ramachanran. Department of lectrical an Computer ngineering, Rowan University, Glassboro,
More informationLagrangian and Hamiltonian Mechanics
Lagrangian an Hamiltonian Mechanics.G. Simpson, Ph.. epartment of Physical Sciences an Engineering Prince George s Community College ecember 5, 007 Introuction In this course we have been stuying classical
More informationAIEEE Physics Model Question Paper
IEEE Physics Moel Question Paper ote: Question o. 11 to 1 an 1 to consist of Eight (8) marks each for each correct response an remaining questions consist of Four (4) marks. ¼ marks will be eucte for inicating
More informationTAYLOR S POLYNOMIAL APPROXIMATION FOR FUNCTIONS
MISN-0-4 TAYLOR S POLYNOMIAL APPROXIMATION FOR FUNCTIONS f(x ± ) = f(x) ± f ' (x) + f '' (x) 2 ±... 1! 2! = 1.000 ± 0.100 + 0.005 ±... TAYLOR S POLYNOMIAL APPROXIMATION FOR FUNCTIONS by Peter Signell 1.
More informationAnalytic Scaling Formulas for Crossed Laser Acceleration in Vacuum
October 6, 4 ARDB Note Analytic Scaling Formulas for Crosse Laser Acceleration in Vacuum Robert J. Noble Stanfor Linear Accelerator Center, Stanfor University 575 San Hill Roa, Menlo Park, California 945
More informationA simple model for the small-strain behaviour of soils
A simple moel for the small-strain behaviour of soils José Jorge Naer Department of Structural an Geotechnical ngineering, Polytechnic School, University of São Paulo 05508-900, São Paulo, Brazil, e-mail:
More informationPhysics 505 Electricity and Magnetism Fall 2003 Prof. G. Raithel. Problem Set 3. 2 (x x ) 2 + (y y ) 2 + (z + z ) 2
Physics 505 Electricity an Magnetism Fall 003 Prof. G. Raithel Problem Set 3 Problem.7 5 Points a): Green s function: Using cartesian coorinates x = (x, y, z), it is G(x, x ) = 1 (x x ) + (y y ) + (z z
More informationLectures - Week 10 Introduction to Ordinary Differential Equations (ODES) First Order Linear ODEs
Lectures - Week 10 Introuction to Orinary Differential Equations (ODES) First Orer Linear ODEs When stuying ODEs we are consiering functions of one inepenent variable, e.g., f(x), where x is the inepenent
More informationPARALLEL-PLATE CAPACITATOR
Physics Department Electric an Magnetism Laboratory PARALLEL-PLATE CAPACITATOR 1. Goal. The goal of this practice is the stuy of the electric fiel an electric potential insie a parallelplate capacitor.
More informationPH 132 Exam 1 Spring Student Name. Student Number. Lab/Recitation Section Number (11,,36)
PH 13 Exam 1 Spring 010 Stuent Name Stuent Number ab/ecitation Section Number (11,,36) Instructions: 1. Fill out all of the information requeste above. Write your name on each page.. Clearly inicate your
More informationEXPONENTIAL FOURIER INTEGRAL TRANSFORM METHOD FOR STRESS ANALYSIS OF BOUNDARY LOAD ON SOIL
Tome XVI [18] Fascicule 3 [August] 1. Charles Chinwuba IKE EXPONENTIAL FOURIER INTEGRAL TRANSFORM METHOD FOR STRESS ANALYSIS OF BOUNDARY LOAD ON SOIL 1. Department of Civil Engineering, Enugu State University
More informationFINAL EXAM 1 SOLUTIONS Below is the graph of a function f(x). From the graph, read off the value (if any) of the following limits: x 1 +
FINAL EXAM 1 SOLUTIONS 2011 1. Below is the graph of a function f(x). From the graph, rea off the value (if any) of the following its: x 1 = 0 f(x) x 1 + = 1 f(x) x 0 = x 0 + = 0 x 1 = 1 1 2 FINAL EXAM
More informationProblem Set 2: Solutions
UNIVERSITY OF ALABAMA Department of Physics an Astronomy PH 102 / LeClair Summer II 2010 Problem Set 2: Solutions 1. The en of a charge rubber ro will attract small pellets of Styrofoam that, having mae
More informationand from it produce the action integral whose variation we set to zero:
Lagrange Multipliers Monay, 6 September 01 Sometimes it is convenient to use reunant coorinates, an to effect the variation of the action consistent with the constraints via the metho of Lagrange unetermine
More informationSimulation of Angle Beam Ultrasonic Testing with a Personal Computer
Key Engineering Materials Online: 4-8-5 I: 66-9795, Vols. 7-73, pp 38-33 oi:.48/www.scientific.net/kem.7-73.38 4 rans ech ublications, witzerlan Citation & Copyright (to be inserte by the publisher imulation
More informationA Path Planning Method Using Cubic Spiral with Curvature Constraint
A Path Planning Metho Using Cubic Spiral with Curvature Constraint Tzu-Chen Liang an Jing-Sin Liu Institute of Information Science 0, Acaemia Sinica, Nankang, Taipei 5, Taiwan, R.O.C., Email: hartree@iis.sinica.eu.tw
More informationBoth the ASME B and the draft VDI/VDE 2617 have strengths and
Choosing Test Positions for Laser Tracker Evaluation an Future Stanars Development ala Muralikrishnan 1, Daniel Sawyer 1, Christopher lackburn 1, Steven Phillips 1, Craig Shakarji 1, E Morse 2, an Robert
More informationKinetic Energy Is Important in the Nanoscale World
Kinetic Energy Is Important in the Nanoscale Worl Frank Riou Department of Chemistry College of St. Beneict & St. John's University St. Joseph, MN 56374 Most eplanations of atomic an molecular phenomena
More informationExtension of de Weger s Attack on RSA with Large Public Keys
Extension of e Weger s Attack on RSA with Large Public Keys Nicolas T. Courtois, Theoosis Mourouzis an Pho V. Le Department of Computer Science, University College Lonon, Gower Street, Lonon, U.K. {n.courtois,
More informationMATHEMATICS BONUS FILES for faculty and students
MATHMATI BONU FIL for faculty an stuents http://www.onu.eu/~mcaragiu1/bonus_files.html RIVD: May 15, 9 PUBLIHD: May 5, 9 toffel 1 Maxwell s quations through the Major Vector Theorems Joshua toffel Department
More informationCOMPACT BANDPASS FILTERS UTILIZING DIELECTRIC FILLED WAVEGUIDES
Progress In Electromagnetics Research B, Vol. 7, 105 115, 008 COMPACT BADPASS FILTERS UTILIZIG DIELECTRIC FILLED WAVEGUIDES H. Ghorbanineja an M. Khalaj-Amirhosseini College of Electrical Engineering Iran
More informationSemiclassical analysis of long-wavelength multiphoton processes: The Rydberg atom
PHYSICAL REVIEW A 69, 063409 (2004) Semiclassical analysis of long-wavelength multiphoton processes: The Ryberg atom Luz V. Vela-Arevalo* an Ronal F. Fox Center for Nonlinear Sciences an School of Physics,
More informationStatics, Quasistatics, and Transmission Lines
CHAPTER 6 Statics, Quasistatics, an Transmission Lines In the preceing chapters, we learne that the phenomenon of wave propagation is base upon the interaction between the time-varying or ynamic electric
More informationQubit channels that achieve capacity with two states
Qubit channels that achieve capacity with two states Dominic W. Berry Department of Physics, The University of Queenslan, Brisbane, Queenslan 4072, Australia Receive 22 December 2004; publishe 22 March
More informationLecture 6: Control of Three-Phase Inverters
Yoash Levron The Anrew an Erna Viterbi Faculty of Electrical Engineering, Technion Israel Institute of Technology, Haifa 323, Israel yoashl@ee.technion.ac.il Juri Belikov Department of Computer Systems,
More informationθ x = f ( x,t) could be written as
9. Higher orer PDEs as systems of first-orer PDEs. Hyperbolic systems. For PDEs, as for ODEs, we may reuce the orer by efining new epenent variables. For example, in the case of the wave equation, (1)
More informationMicrowave Reflection from the Region of Electron Cyclotron Resonance Heating in the L-2M Stellarator )
Microwave Reflection from the Region of Electron Cyclotron Resonance Heating in the L-2M Stellarator German M. BATANOV, Valentin D. BORZOSEKOV, Nikolay K. KHARCHEV, Leoni V. KOLIK, Eugeny M. KONCHEKOV,
More informationVariational principle for limit cycles of the Rayleigh van der Pol equation
PHYICAL REVIEW E VOLUME 59, NUMBER 5 MAY 999 Variational principle for limit cycles of the Rayleigh van er Pol equation R. D. Benguria an M. C. Depassier Faculta e Física, Pontificia Universia Católica
More information6.003 Homework #7 Solutions
6.003 Homework #7 Solutions Problems. Secon-orer systems The impulse response of a secon-orer CT system has the form h(t) = e σt cos(ω t + φ)u(t) where the parameters σ, ω, an φ are relate to the parameters
More informationElectromagnet Gripping in Iron Foundry Automation Part II: Simulation
www.ijcsi.org 238 Electromagnet Gripping in Iron Founry Automation Part II: Simulation Rhythm-Suren Wahwa Department of Prouction an Quality Engineering, NTNU Tronheim, 7051, Norway Abstract This paper
More informationThe dynamics of the simple pendulum
.,, 9 G. Voyatzis, ept. of Physics, University of hessaloniki he ynamics of the simple penulum Analytic methos of Mechanics + Computations with Mathematica Outline. he mathematical escription of the moel.
More informationDeriving ARX Models for Synchronous Generators
Deriving AR Moels for Synchronous Generators Yangkun u, Stuent Member, IEEE, Zhixin Miao, Senior Member, IEEE, Lingling Fan, Senior Member, IEEE Abstract Parameter ientification of a synchronous generator
More informationThe Exact Form and General Integrating Factors
7 The Exact Form an General Integrating Factors In the previous chapters, we ve seen how separable an linear ifferential equations can be solve using methos for converting them to forms that can be easily
More informationLecture 12. Energy, Force, and Work in Electro- and Magneto-Quasistatics
Lecture 1 Energy, Force, an ork in Electro an MagnetoQuasistatics n this lecture you will learn: Relationship between energy, force, an work in electroquasistatic an magnetoquasistatic systems ECE 303
More informationarxiv: v1 [physics.class-ph] 20 Dec 2017
arxiv:1712.07328v1 [physics.class-ph] 20 Dec 2017 Demystifying the constancy of the Ermakov-Lewis invariant for a time epenent oscillator T. Pamanabhan IUCAA, Post Bag 4, Ganeshkhin, Pune - 411 007, Inia.
More informationAPPROXIMATE SOLUTION FOR TRANSIENT HEAT TRANSFER IN STATIC TURBULENT HE II. B. Baudouy. CEA/Saclay, DSM/DAPNIA/STCM Gif-sur-Yvette Cedex, France
APPROXIMAE SOLUION FOR RANSIEN HEA RANSFER IN SAIC URBULEN HE II B. Bauouy CEA/Saclay, DSM/DAPNIA/SCM 91191 Gif-sur-Yvette Ceex, France ABSRAC Analytical solution in one imension of the heat iffusion equation
More informationSIMULATION OF POROUS MEDIUM COMBUSTION IN ENGINES
SIMULATION OF POROUS MEDIUM COMBUSTION IN ENGINES Jan Macek, Miloš Polášek Czech Technical University in Prague, Josef Božek Research Center Introuction Improvement of emissions from reciprocating internal
More informationExperimental Studies and Parametric Modeling of Ionic Flyers
1 Experimental Stuies an Parametric Moeling of Ionic Flyers Chor Fung Chung an Wen J. Li* Centre for Micro an Nano Systems, Faculty of Engineering The Chinese University of Hong Kong *Contact Author: wen@mae.cuhk.eu.hk
More informationMath 1271 Solutions for Fall 2005 Final Exam
Math 7 Solutions for Fall 5 Final Eam ) Since the equation + y = e y cannot be rearrange algebraically in orer to write y as an eplicit function of, we must instea ifferentiate this relation implicitly
More informationDT7: Implicit Differentiation
Differentiation Techniques 7: Implicit Differentiation 143 DT7: Implicit Differentiation Moel 1: Solving for y Most of the functions we have seen in this course are like those in Table 1 (an the first
More information1 Heisenberg Representation
1 Heisenberg Representation What we have been ealing with so far is calle the Schröinger representation. In this representation, operators are constants an all the time epenence is carrie by the states.
More informationThe derivative of a function f(x) is another function, defined in terms of a limiting expression: f(x + δx) f(x)
Y. D. Chong (2016) MH2801: Complex Methos for the Sciences 1. Derivatives The erivative of a function f(x) is another function, efine in terms of a limiting expression: f (x) f (x) lim x δx 0 f(x + δx)
More information1 The Derivative of ln(x)
Monay, December 3, 2007 The Derivative of ln() 1 The Derivative of ln() The first term or semester of most calculus courses will inclue the it efinition of the erivative an will work out, long han, a number
More informationSecond Major Solution Q1. The three capacitors in the figure have an equivalent capacitance of 2.77 µf. What is C 2?
Secon Major Solution Q1. The three capacitors in the figure have an equivalent capacitance of.77 µf. What is C? C 4.0 µf.0 µf A) 7 µf B) µf C) 4 µf D) 3 µf E) 6 µf Q. When the potential ifference across
More informationUpper and Lower Bounds on ε-approximate Degree of AND n and OR n Using Chebyshev Polynomials
Upper an Lower Bouns on ε-approximate Degree of AND n an OR n Using Chebyshev Polynomials Mrinalkanti Ghosh, Rachit Nimavat December 11, 016 1 Introuction The notion of approximate egree was first introuce
More information'HVLJQ &RQVLGHUDWLRQ LQ 0DWHULDO 6HOHFWLRQ 'HVLJQ 6HQVLWLYLW\,1752'8&7,21
Large amping in a structural material may be either esirable or unesirable, epening on the engineering application at han. For example, amping is a esirable property to the esigner concerne with limiting
More informationA Course in Machine Learning
A Course in Machine Learning Hal Daumé III 12 EFFICIENT LEARNING So far, our focus has been on moels of learning an basic algorithms for those moels. We have not place much emphasis on how to learn quickly.
More informationImproving the Lorentz Force Amplitude of an EMAT Using Stacked Coil Configuration
Sensors & Transucers, Vol. 155, Issue 8, August 213, pp. 262-27 Sensors & Transucers 213 by IFSA http://www.sensorsportal.com Improving the Lorentz Force Amplitue of an MAT Using Stacke Coil Configuration
More informationAdaptive Optimal Path Following for High Wind Flights
Milano (Italy) August - September, 11 Aaptive Optimal Path Following for High Win Flights Ashwini Ratnoo P.B. Sujit Mangal Kothari Postoctoral Fellow, Department of Aerospace Engineering, Technion-Israel
More informationELECTRON DIFFRACTION
ELECTRON DIFFRACTION Electrons : wave or quanta? Measurement of wavelength an momentum of electrons. Introuction Electrons isplay both wave an particle properties. What is the relationship between the
More informationAppendix A: Mathematical Formulae
Appenix A: Mathematical Formulae A.1 Introuction Mathematical formulae are very important to o in etail analysis of electromagnetic fiels an waves. These formulae are mainly trigonometry, ifferentiation
More informationPhysics 2212 K Quiz #2 Solutions Summer 2016
Physics 1 K Quiz # Solutions Summer 016 I. (18 points) A positron has the same mass as an electron, but has opposite charge. Consier a positron an an electron at rest, separate by a istance = 1.0 nm. What
More informationA note on asymptotic formulae for one-dimensional network flow problems Carlos F. Daganzo and Karen R. Smilowitz
A note on asymptotic formulae for one-imensional network flow problems Carlos F. Daganzo an Karen R. Smilowitz (to appear in Annals of Operations Research) Abstract This note evelops asymptotic formulae
More informationCHAPTER: 2 ELECTROSTATIC POTENTIAL AND CAPACITANCE
CHAPTER: 2 ELECTROSTATIC POTENTIAL AND CAPACITANCE. Define electric potential at a point. *Electric potential at a point is efine as the work one to bring a unit positive charge from infinity to that point.
More informationVehicle Stability Improvement Based on Electronic Differential Using Sliding Mode Control
7th WSEAS International Conference on Electric Power Systems, High Voltages, Electric Machines, Venice, Italy, November 1-3, 007 331 Vehicle Stability Improvement Base on Electronic Differential Using
More informationSwitching Time Optimization in Discretized Hybrid Dynamical Systems
Switching Time Optimization in Discretize Hybri Dynamical Systems Kathrin Flaßkamp, To Murphey, an Sina Ober-Blöbaum Abstract Switching time optimization (STO) arises in systems that have a finite set
More informationConstruction of the Electronic Radial Wave Functions and Probability Distributions of Hydrogen-like Systems
Construction of the Electronic Raial Wave Functions an Probability Distributions of Hyrogen-like Systems Thomas S. Kuntzleman, Department of Chemistry Spring Arbor University, Spring Arbor MI 498 tkuntzle@arbor.eu
More informationSensors & Transducers 2015 by IFSA Publishing, S. L.
Sensors & Transucers, Vol. 184, Issue 1, January 15, pp. 53-59 Sensors & Transucers 15 by IFSA Publishing, S. L. http://www.sensorsportal.com Non-invasive an Locally Resolve Measurement of Soun Velocity
More informationImplicit Differentiation
Implicit Differentiation Thus far, the functions we have been concerne with have been efine explicitly. A function is efine explicitly if the output is given irectly in terms of the input. For instance,
More informationv r 1 E β ; v r v r 2 , t t 2 , t t 1 , t 1 1 v 2 v (3) 2 ; v χ αβγδ r 3 dt 3 , t t 3 ) βγδ [ R 3 ] exp +i ω 3 [ ] τ 1 exp i k v [ ] χ αβγ , τ 1 dτ 3
ON CLASSICAL ELECTROMAGNETIC FIELDS PAGE 58 VII. NONLINEAR OPTICS -- CLASSICAL PICTURE: AN EXTENDED PHENOMENOLOGICAL MODEL OF POLARIZATION : As an introuction to the subject of nonlinear optical phenomena,
More information( ) Energy storage in CAPACITORs. q C
Energy storage in CAPACITORs Charge capacitor by transferring bits of charge q at a time from bottom to top plate. Can use a battery to o this. Battery oes work which increase potential energy of capacitor.
More informationDifferentiability, Computing Derivatives, Trig Review. Goals:
Secants vs. Derivatives - Unit #3 : Goals: Differentiability, Computing Derivatives, Trig Review Determine when a function is ifferentiable at a point Relate the erivative graph to the the graph of an
More information