Lecture 26. Dielectric Slab Waveguides

Thick-Walled Cylinders and Press Fits. 2004 by W.H.Dornfeld PressCylinder:

Thck-Walled Cylndes and Pess Fts 004 by W.H.Dnfeld PessCylnde: 1 Stesses n Thck-Walled Cylndes Thck-Walled cylndes have an aveage adus less than 0 tmes the wall thckness. σ σl They ae essuzed ntenally

UIUC Physics 436 EM Fields & Sources II Fall Semester, 2015 Lect. Notes 10.5 Prof. Steven Errede LECTURE NOTES 10.5

UIUC Phscs 436 EM Felds & Suces II Fall Semeste, 5 Lect. Ntes.5 Pf. Steven Eede LECTURE NOTES.5 EM Standng Waves n Resnant Cavtes One can ceate a esnant cavt f EM waves b takng a wavegude (f abta shape)

α α λ α = = λ λ α ψ = = α α α λ λ ψ α = + β = > θ θ β > β β θ θ θ β θ β γ θ β = γ θ > β > γ θ β γ = θ β = θ β = θ β = β θ = β β θ = = = β β θ = + α α α α α = = λ λ λ λ λ λ λ = λ λ α α α α λ ψ + α =

Electric Potential. otherwise to move the object from initial point i to final point f

PHY2061 Enched Physcs 2 Lectue Notes Electc Potental Electc Potental Dsclame: These lectue notes ae not meant to eplace the couse textbook. The content may be ncomplete. Some topcs may be unclea. These

BARTON COLLEGE PRACTICE PLACEMENT TEST. a) 4 b) 4 c) 12 d) 10.5. a) 7a 11 b) a 17 c) a 11 d) 7a 17. a) 14 b) 1 c) 66 d) 81

. Simplify: 0 + 4 (! 8) 4 4 0.. Simplify: (a 4) + (a ) (a+) 7a a 7 a 7a 7. Evaluate the expessin: 4a! 4ab + b, when a = and b = 4 8 4. Fiefightes use the fmula S = 0.P + t cmpute the hizntal ange S in

Oblique incidence: Interface between dielectric media

lecrmagnec Felds Oblque ncdence: Inerface beween delecrc meda Cnsder a planar nerface beween w delecrc meda. A plane wave s ncden a an angle frm medum. The nerface plane defnes he bundary beween he meda.

Bending Stresses for Simple Shapes

-6 Bendng Stesses fo Smple Sapes In bendng, te maxmum stess and amount of deflecton can be calculated n eac of te followng stuatons. Addtonal examples ae avalable n an engneeng andbook. Secton Modulus

SOLID MECHANICS TUTORIAL FRICTION CLUTCHES

SOLI MECHANICS TUTORIAL FRICTION CLUTCHES Ths wrk cvers elements f the syllabus fr the Edexcel mdule 17P HNC/ Mechancal Prncples OUTCOME. On cmpletn f ths shrt tutral yu shuld be able t d the fllwng. escrbe

s s f h s s SPH3UW Unit 7.7 Concave Lens Page 1 of 7 Notes Properties of a Converging Lens

SPH3UW Unt 7.7 Cncave Lens Page 1 f 7 Ntes Physcs Tl bx Thn Lens s an ptcal system wth tw refractng surfaces. The mst smplest thn lens cntan tw sphercal surfaces that are clse enugh tgether that we can

High-frequency response of a CG amplifier

Hgh-requency respnse a G apler between surce & grund between dran & grund w-pass lter Md-band p w-pass lter db Input Ple Output Ple n sb Hgh- respnse a G apler Exact Slutn ( db sb ( / : Nde ( / : Nde n

Chapter 25 The Reflection of Light: Mirrors. The content contained in all sections of chapter 25 of the textbook is included on the AP Physics B exam.

Chapter 25 The Reflectn f Lght: Mrrrs Chapter 25 THE REFLECTION OF LIGHT: MIRRORS PREVIEW The ray mel f lght states that lght may be represente by a straght lne alng the rectn f mtn, an ray ptcs s the

Chapter 14, Problem 1. Find the transfer function V o. /V i. of the RC circuit in Fig. 14.68. Express it using ω = 1/RC. Figure 14.68 For Prob. 14.1.

Chapter 4, Prblem. Fnd the traner unctn V /V the C crcut n Fg. 4.68. Expre t ung /C. Fgure 4.68 Fr Prb. 4.. Chapter 4, Slutn. V H ( ) V H() jc jc jc j 0 j 0, where 0 C H 0 π - H ( ) φ H ( ) tan ( 0 ) 0

n + d + q = 24 and.05n +.1d +.25q = 2 { n + d + q = 24 (3) n + 2d + 5q = 40 (2)

MATH 16T Exam 1 : Part I (In-Class) Solutons 1. (0 pts) A pggy bank contans 4 cons, all of whch are nckels (5 ), dmes (10 ) or quarters (5 ). The pggy bank also contans a con of each denomnaton. The total

Gravitation. Definition of Weight Revisited. Newton s Law of Universal Gravitation. Newton s Law of Universal Gravitation. Gravitational Field

Defnton of Weght evsted Gavtaton The weght of an object on o above the eath s the gavtatonal foce that the eath exets on the object. The weght always ponts towad the cente of mass of the eath. On o above

The Full-Wave Rectifier

9/3/2005 The Full Wae ectfer.doc /0 The Full-Wae ectfer Consder the followng juncton dode crcut: s (t) Power Lne s (t) 2 Note that we are usng a transformer n ths crcut. The job of ths transformer s to

Luby s Alg. for Maximal Independent Sets using Pairwise Independence

Lecture Notes for Randomzed Algorthms Luby s Alg. for Maxmal Independent Sets usng Parwse Independence Last Updated by Erc Vgoda on February, 006 8. Maxmal Independent Sets For a graph G = (V, E), an ndependent

Green's function integral equation methods for plasmonic nanostructures

Geens functon ntegal equaton methods fo plasmonc nanostuctues (Ph Couse: Optcal at the Nanoscale) Thomas Søndegaad epatment of Phscs and Nanotechnolog, Aalbog Unvest, Senve 4A, K-9 Aalbog Øst, enma. Intoducton

Module 2. AC to DC Converters. Version 2 EE IIT, Kharagpur 1

Mdule AC t DC Cnverters Versn EE IIT, Kharagpur 1 Lessn 9 Sngle Phase Uncntrlled Rectfer Versn EE IIT, Kharagpur Operatn and Analyss f sngle phase uncntrlled rectfers Instructnal Objectves On cmpletn the

the role of angular momentum

Ultafast ast magnetization at dynamics: the ole of angula momentum Andei Kiilyuk, The Nethelands 1 Magnetization dynamics and switching N S enegy gain: E = M dl H toque: = T dt with damping: M γ = dm dt

Gauss Law. Physics 231 Lecture 2-1

Gauss Law Physics 31 Lectue -1 lectic Field Lines The numbe of field lines, also known as lines of foce, ae elated to stength of the electic field Moe appopiately it is the numbe of field lines cossing

!"#$%&'()%"*#%*+,-./-*+01.2(.*3+456789*!"#$%&"'()'*+,-."/01&2#."'3424,'

"#$()"*#*+,-./-*+01.2(.*3+456789* "#$"()*+,-."/012#."3424, Dr. Peter T. Gallagher Astrphysics Research Grup Trinity Cllege Dublin :2";,

Nanoscale Heat Transfer using Phonon Boltzmann Transport Equation

Presented at the COMSOL Cnference 9 Bstn Nanscale Heat Transfer usng Phnn Bltzmann Transprt Equatn Sangwk Shn Ar Frce Research Labratry, Materals and Manufacturng Drectrate, AFRL/RX, Wrght-Pattersn AFB,

We are now ready to answer the question: What are the possible cardinalities for finite fields?

Chapter 3 Fnte felds We have seen, n the prevous chapters, some examples of fnte felds. For example, the resdue class rng Z/pZ (when p s a prme) forms a feld wth p elements whch may be dentfed wth the

Simple Interest Loans (Section 5.1) :

Chapter 5 Fnance The frst part of ths revew wll explan the dfferent nterest and nvestment equatons you learned n secton 5.1 through 5.4 of your textbook and go through several examples. The second part

CHAPTER 8 Potential Energy and Conservation of Energy

CHAPTER 8 Potental Energy and Conservaton o Energy One orm o energy can be converted nto another orm o energy. Conservatve and non-conservatve orces Physcs 1 Knetc energy: Potental energy: Energy assocated

CITY AND GUILDS 9210 Level 6 Module - Unit 129 FLUID MECHANICS

ITY AND GUILDS 90 Level 6 Mdule - Unt 9 FLUID MEHANIS OUTOME - TUTOIAL FLUID FLOW ALULATIONS Ths mdule has Leanng Outcmes. Ths s the secnd tutal utcme Outcme Pem lud lw calculatns The leane can:. Slve

>

Energies of Network Nastsemble

Supplementary materal: Assessng the relevance of node features for network structure Gnestra Bancon, 1 Paolo Pn,, 3 and Matteo Marsl 1 1 The Abdus Salam Internatonal Center for Theoretcal Physcs, Strada

Voltage ( = Electric Potential )

V-1 Voltage ( = Electic Potential ) An electic chage altes the space aound it. Thoughout the space aound evey chage is a vecto thing called the electic field. Also filling the space aound evey chage is

An Algorithm For Factoring Integers

An Algothm Fo Factong Integes Yngpu Deng and Yanbn Pan Key Laboatoy of Mathematcs Mechanzaton, Academy of Mathematcs and Systems Scence, Chnese Academy of Scences, Bejng 100190, People s Republc of Chna

Network Theorems - Alternating Current examples - J. R. Lucas

Netwrk Therems - lternating urrent examples - J. R. Lucas n the previus chapter, we have been dealing mainly with direct current resistive circuits in rder t the principles f the varius therems clear.

1240 ev nm 2.5 ev. (4) r 2 or mv 2 = ke2

Chapte 5 Example The helium atom has 2 electonic enegy levels: E 3p = 23.1 ev and E 2s = 20.6 ev whee the gound state is E = 0. If an electon makes a tansition fom 3p to 2s, what is the wavelength of the

Rotation Kinematics, Moment of Inertia, and Torque

Rotaton Knematcs, Moment of Inerta, and Torque Mathematcally, rotaton of a rgd body about a fxed axs s analogous to a lnear moton n one dmenson. Although the physcal quanttes nvolved n rotaton are qute

B A S I C S C I E N C E S

B A S I C S C I E N C E S 10 B A S I C S C I E N C E S F I R S T S E M E S T E R C O U R S E S : H U M A N S T R U C T U R E A N D F U N C T I O N [ H S F I ] M O L E C U L A R B A S I S O F M E D I C

VRT012 User s guide V0.1. Address: Žirmūnų g. 27, Vilnius LT-09105, Phone: (370-5) 2127472, Fax: (370-5) 276 1380, Email: info@teltonika.

VRT012 User s gude V0.1 Thank you for purchasng our product. We hope ths user-frendly devce wll be helpful n realsng your deas and brngng comfort to your lfe. Please take few mnutes to read ths manual

So far circuit analysis has been performed on single-

Three phase systems ntrdctn S far crct analyss has been perfrmed n sngle- phase crcts,.e. there has been ne crct wth a nmber f dfferent vltage and crrent srces whch were nt synchrnsed n any prpsefl way.

Largest Fixed-Aspect, Axis-Aligned Rectangle

Largest Fixed-Aspect, Axis-Aligned Rectangle David Eberly Geometric Tools, LLC http://www.geometrictools.com/ Copyright c 1998-2016. All Rights Reserved. Created: February 21, 2004 Last Modified: February

NMT EE 589 & UNM ME 482/582 ROBOT ENGINEERING. Dr. Stephen Bruder NMT EE 589 & UNM ME 482/582

NMT EE 589 & UNM ME 482/582 ROBOT ENGINEERING Dr. Stephen Bruder NMT EE 589 & UNM ME 482/582 7. Root Dynamcs 7.2 Intro to Root Dynamcs We now look at the forces requred to cause moton of the root.e. dynamcs!!

The Electric Potential, Electric Potential Energy and Energy Conservation. V = U/q 0. V = U/q 0 = -W/q 0 1V [Volt] =1 Nm/C

Geneal Physics - PH Winte 6 Bjoen Seipel The Electic Potential, Electic Potential Enegy and Enegy Consevation Electic Potential Enegy U is the enegy of a chaged object in an extenal electic field (Unit

AREA COVERAGE SIMULATIONS FOR MILLIMETER POINT-TO-MULTIPOINT SYSTEMS USING STATISTICAL MODEL OF BUILDING BLOCKAGE

Radoengneeng Aea Coveage Smulatons fo Mllmete Pont-to-Multpont Systems Usng Buldng Blockage 43 Vol. 11, No. 4, Decembe AREA COVERAGE SIMULATIONS FOR MILLIMETER POINT-TO-MULTIPOINT SYSTEMS USING STATISTICAL

gloser og kommentarer til Macbeth ( sidetal henviser til "Illustrated Shakespeare") GS 96

side 1! " # $ % &! " '! ( $ ) *! " & +! '!, $ #! "! - % " "! &. / 0 1 & +! '! ' & ( ' 2 ) % $ 2 3 % # 2! &. 2! ' 2! '! $ $! " 2! $ ( ' 4! " 3 & % / ( / ( ' 5! * ( 2 & )! 2 5! 2 &! # '! " & +! '! ' & &!

PCA vs. Varimax rotation

PCA vs. Vamax otaton The goal of the otaton/tansfomaton n PCA s to maxmze the vaance of the new SNP (egensnp), whle mnmzng the vaance aound the egensnp. Theefoe the dffeence between the vaances captued

Bipolar-Junction (BJT) transistors

Bplar-Junctn (BJT) transstrs References: Barbw (Chapter 7), Hayes & Hrwtz (pp 84-4), Rzzn (Chapters 8 & 9) A bplar junctn transstr s frmed by jnng three sectns f semcnductrs wth alternately dfferent dpngs.

YOU ARE RECEIVING THIS NOTICE AS REQUIRED BY THE NEW NATIONAL HEALTH REFORM LAW (ALSO KNOWN AS THE AFFORDABLE CARE ACT OR ACA)

YOU ARE RECEIVING THIS NOTICE AS REQUIRED BY THE NEW NATIONAL HEALTH REFORM LAW (ALSO KNOWN AS THE AFFORDABLE CARE ACT OR ACA) On January 1, 2014, the Affrdable Care Act (ACA) wll be mplemented n Massachusetts

Institute of Informatics, Faculty of Business and Management, Brno University of Technology,Czech Republic

Lagrange Multplers as Quanttatve Indcators n Economcs Ivan Mezník Insttute of Informatcs, Faculty of Busness and Management, Brno Unversty of TechnologCzech Republc Abstract The quanttatve role of Lagrange

Electric Circuits II. More about Mutual Inductance. Lecture #22

EE 05 Dr. A. Ziduri Electric Circuits II Mre abut Mutual Inductance Lecture # - - EE 05 Dr. A. Ziduri The material t be cvered in this lecture is as fllws: Mutual Inductance in Terms f Self Inductance

s i æ I N D h / i E l f w g u v b s Z b S p U m z ts n z ˆ k Z ç w o R U h E D d d æ T S

s i æ I N D h / i E l f w g u v b s Z b S p U m z ts n z ˆ k Z ç w o R U h E D d d æ T S T g z l A i ˆ ç z R ts m o m p o j g h v S i n d w b j n s T I A N ç / t U æ k h ts S dz u A j i ç v / T I e v h

MATHEMATICS FOR ENGINEERING TRIGONOMETRY TUTORIAL 1 TRIGONOMETRIC RATIOS, TRIGONOMETRIC TECHNIQUES AND GRAPHICAL METHODS

MATHEMATICS FOR ENGINEERING TRIGONOMETRY TUTORIAL 1 TRIGONOMETRIC RATIOS, TRIGONOMETRIC TECHNIQUES AND GRAPHICAL METHODS This is the ne f a series f basic tutrials in mathematics aimed at beginners r anyne

2 r2 θ = r2 t. (3.59) The equal area law is the statement that the term in parentheses,

3.4. KEPLER S LAWS 145 3.4 Keple s laws You ae familia with the idea that one can solve some mechanics poblems using only consevation of enegy and (linea) momentum. Thus, some of what we see as objects

A Neural Network and Web-Based Decision Support System for Forex Forecasting and Trading

A Neural Network and Web-Based Decision Support System for Forex Forecasting and Trading K.K. Lai 1, Lean Yu 2,3, and Shouyang Wang 2,4 1 Department of Management Sciences, City University of Hong Kong,

Finite Math Chapter 10: Study Guide and Solution to Problems

Fnte Math Chapter 10: Study Gude and Soluton to Problems Basc Formulas and Concepts 10.1 Interest Basc Concepts Interest A fee a bank pays you for money you depost nto a savngs account. Prncpal P The amount

Additional File 1 - A model-based circular binary segmentation algorithm for the analysis of array CGH data

1 Addtonal Fle 1 - A model-based ccula bnay segmentaton algothm fo the analyss of aay CGH data Fang-Han Hsu 1, Hung-I H Chen, Mong-Hsun Tsa, Lang-Chuan La 5, Ch-Cheng Huang 1,6, Shh-Hsn Tu 6, Ec Y Chuang*

Vector Calculus: Are you ready? Vectors in 2D and 3D Space: Review

Vecto Calculus: Ae you eady? Vectos in D and 3D Space: Review Pupose: Make cetain that you can define, and use in context, vecto tems, concepts and fomulas listed below: Section 7.-7. find the vecto defined

Lecture 10: TEM, TE, and TM Modes for Waveguides. Rectangular Waveguide.

Whites, EE 481/581 Lecture 10 Page 1 of 10 Lecture 10: TEM, TE, and TM Modes for Waveguides. Rectangular Waveguide. We will now generalie our discussion of transmission lines by considering EM waveguides.

Orbit dynamics and kinematics with full quaternions

bt dynamcs and knematcs wth full quatenons Davde Andes and Enco S. Canuto, Membe, IEEE Abstact Full quatenons consttute a compact notaton fo descbng the genec moton of a body n the space. ne of the most

The Bridge Rectifier

9/4/004 The Brdge ectfer.doc 1/9 The Brdge ectfer Now consder ths juncton dode rectfer crcut: 1 Lne (t) - O (t) _ 4 3 We call ths crcut the brdge rectfer. Let s analyze t and see what t does! Frst, we

TUTORIAL No. 1 FLUID FLOW THEORY

TUTOIAL N. FLUID FLOW THEOY In de t cmlete ths tutal yu shuld aleady have cmleted level have a gd basc knwledge lud mechancs equvalent t the Engneeng Cuncl at eamnatn 03. When yu have cmleted ths tutal,

SMA5101 Thermodynamics of Materials Ceder 2001

SMA5101 Thermdynamcs f Materals Ceder 2001 Chapter 4 Slutn Thery In the frst chapters we dealt prmarly wth clsed systems fr whch nly heat and wrk s transferred between the system and the envrnment. In

From Quantum to Matter 2006

From Quantum to Matter 006 Why such a course? Ronald Griessen Vrije Universiteit, Amsterdam AMOLF, May 4, 004 vrije Universiteit amsterdam Why study quantum mechanics? From Quantum to Matter: The main

(Semi)Parametric Models vs Nonparametric Models

buay, 2003 Pobablty Models (Sem)Paametc Models vs Nonpaametc Models I defne paametc, sempaametc, and nonpaametc models n the two sample settng My defnton of sempaametc models s a lttle stonge than some

Lecture 16: 11.04.05 Single-Component phase diagrams continued; Thermodynamics of solutions

Lecture 16: 11.04.05 Single-Cmpnent phase diagrams cntinued; Thermdynamics f slutins Tday: LAST TIME...2 Single-cmpnent phase diagrams and the Gibbs phase rule...2 Cnstraints n the shape f phase bundaries

x o R n a π(a, x o ) A R n π(a, x o ) π(a, x o ) A R n a a x o x o x n X R n δ(x n, x o ) d(a, x n ) d(, ) δ(, ) R n x n X d(a, x n ) δ(x n, x o ) a = a A π(a, xo ) a a A = X = R π(a, x o ) = (x o + ρ)

Ring structure of splines on triangulations

www.oeaw.ac.at Rng structure of splnes on trangulatons N. Vllamzar RICAM-Report 2014-48 www.rcam.oeaw.ac.at RING STRUCTURE OF SPLINES ON TRIANGULATIONS NELLY VILLAMIZAR Introducton For a trangulated regon

Voltage ( = Electric Potential )

V-1 of 9 Voltage ( = lectic Potential ) An electic chage altes the space aound it. Thoughout the space aound evey chage is a vecto thing called the electic field. Also filling the space aound evey chage

6.2 Permutations continued

6.2 Permutations continued Theorem A permutation on a finite set A is either a cycle or can be expressed as a product (composition of disjoint cycles. Proof is by (strong induction on the number, r, of

Problem Set 3. a) We are asked how people will react, if the interest rate i on bonds is negative.

Queston roblem Set 3 a) We are asked how people wll react, f the nterest rate on bonds s negatve. When

Addendum to: Importing Skill-Biased Technology

Addendum to: Importng Skll-Based Technology Arel Bursten UCLA and NBER Javer Cravno UCLA August 202 Jonathan Vogel Columba and NBER Abstract Ths Addendum derves the results dscussed n secton 3.3 of our

Description of the Force Method Procedure. Indeterminate Analysis Force Method 1. Force Method con t. Force Method con t

Indeternate Analyss Force Method The force (flexblty) ethod expresses the relatonshps between dsplaceents and forces that exst n a structure. Prary objectve of the force ethod s to deterne the chosen set

Chapter 8 Atomic Electronic Configurations and Periodicity

Chapter 8 Electron Configurations Page 1 Chapter 8 Atomic Electronic Configurations and Periodicity 8-1. Substances that are weakly attracted to a magnetic field but lose their magnetism when removed from

Series Solutions of ODEs 2 the Frobenius method. The basic idea of the Frobenius method is to look for solutions of the form 3

Royal Holloway Unversty of London Department of Physs Seres Solutons of ODEs the Frobenus method Introduton to the Methodology The smple seres expanson method works for dfferental equatons whose solutons

Faraday's Law of Induction

Introducton Faraday's Law o Inducton In ths lab, you wll study Faraday's Law o nducton usng a wand wth col whch swngs through a magnetc eld. You wll also examne converson o mechanc energy nto electrc energy

Lecture 16: Color and Intensity. and he made him a coat of many colours. Genesis 37:3

Lectue 16: Colo and Intensity and he made him a coat of many colous. Genesis 37:3 1. Intoduction To display a pictue using Compute Gaphics, we need to compute the colo and intensity of the light at each

Chapter 6. Work and Energy

Chapter 6 Wrk and Energy 6. Wrk Dne by a Cnstant Frce Wrk invlves frce and displacement. W = Fs N! m = jule ( J) 6. Wrk Dne by a Cnstant Frce 6. Wrk Dne by a Cnstant Frce Mre general definitin f the wrk

8.5 UNITARY AND HERMITIAN MATRICES. The conjugate transpose of a complex matrix A, denoted by A*, is given by

6 CHAPTER 8 COMPLEX VECTOR SPACES 5. Fnd the kernel of the lnear transformaton gven n Exercse 5. In Exercses 55 and 56, fnd the mage of v, for the ndcated composton, where and are gven by the followng

21 Vectors: The Cross Product & Torque

21 Vectors: The Cross Product & Torque Do not use our left hand when applng ether the rght-hand rule for the cross product of two vectors dscussed n ths chapter or the rght-hand rule for somethng curl

5.74 Introductory Quantum Mechanics II

MIT OpenCourseWare http://ocw.mt.edu 5.74 Introductory Quantum Mechancs II Sprng 9 For nformaton about ctng these materals or our Terms of Use, vst: http://ocw.mt.edu/terms. 4-1 4.1. INTERACTION OF LIGHT

Using Sentry-go Enterprise/ASPX for Sentry-go Quick & Plus! monitors

Using Sentry-g Enterprise/ASPX fr Sentry-g Quick & Plus! mnitrs 3Ds (UK) Limited, February, 2014 http://www.sentry-g.cm Be Practive, Nt Reactive! Intrductin Sentry-g Enterprise Reprting is a self-cntained

Goals Rotational quantities as vectors. Math: Cross Product. Angular momentum

Physcs 106 Week 5 Torque and Angular Momentum as Vectors SJ 7thEd.: Chap 11.2 to 3 Rotatonal quanttes as vectors Cross product Torque expressed as a vector Angular momentum defned Angular momentum as a

Questions & Answers Chapter 10 Software Reliability Prediction, Allocation and Demonstration Testing

M13914 Questions & Answes Chapte 10 Softwae Reliability Pediction, Allocation and Demonstation Testing 1. Homewok: How to deive the fomula of failue ate estimate. λ = χ α,+ t When the failue times follow

Time-Domain Analysis of Transmission Line Circuits (Part 3)

igna Integrity an High-pee Intercnnects Time-Dmain Anaysis f Transmissin Line Circuits (Part 3) Dr. Jsé Ernest Rayas ánchez 1 Outine Buncing iagrams fr TLs with iea ecitatin puses an resistive terminatins

Solution Derivations for Capa #8

Solution Deivations fo Capa #8 1) A ass spectoete applies a voltage of 2.00 kv to acceleate a singly chaged ion (+e). A 0.400 T field then bends the ion into a cicula path of adius 0.305. What is the ass

4. How many integers between 2004 and 4002 are perfect squares?

5 is 0% of what number? What is the value of + 3 4 + 99 00? (alternating signs) 3 A frog is at the bottom of a well 0 feet deep It climbs up 3 feet every day, but slides back feet each night If it started

Drag force acting on a bubble in a cloud of compressible spherical bubbles at large Reynolds numbers

Euopean Jounal of Mechancs B/Fluds 24 2005 468 477 Dag foce actng on a bubble n a cloud of compessble sphecal bubbles at lage Reynolds numbes S.L. Gavlyuk a,b,,v.m.teshukov c a Laboatoe de Modélsaton en

Operational Amplifier Circuits Comparators and Positive Feedback

Operatinal Amplifier Circuits Cmparatrs and Psitive Feedback Cmparatrs: Open Lp Cnfiguratin The basic cmparatr circuit is an p-amp arranged in the pen-lp cnfiguratin as shwn n the circuit f Figure. The

GED MATH STUDY GUIDE. Last revision July 15, 2011

GED MATH STUDY GUIDE Last revisin July 15, 2011 General Instructins If a student demnstrates that he r she is knwledgeable n a certain lessn r subject, yu can have them d every ther prblem instead f every

T ( a i x i ) = a i T (x i ).

Chapter 2 Defn 1. (p. 65) Let V and W be vector spaces (over F ). We call a function T : V W a linear transformation form V to W if, for all x, y V and c F, we have (a) T (x + y) = T (x) + T (y) and (b)

Chem 115 POGIL Worksheet - Week 4 Moles & Stoichiometry

Chem 115 POGIL Worksheet - Week 4 Moles & Stoichiometry Why? Chemists are concerned with mass relationships in chemical reactions, usually run on a macroscopic scale (grams, kilograms, etc.). To deal with

Carter-Penrose diagrams and black holes

Cate-Penose diagams and black holes Ewa Felinska The basic intoduction to the method of building Penose diagams has been pesented, stating with obtaining a Penose diagam fom Minkowski space. An example

University Physics AI No. 11 Kinetic Theory

Unersty hyscs AI No. 11 Knetc heory Class Number Name I.Choose the Correct Answer 1. Whch type o deal gas wll hae the largest alue or C -C? ( D (A Monatomc (B Datomc (C olyatomc (D he alue wll be the same

MACHINE SHOP. Course Design 2005-2006. MET231 to ASU, DEC to NAU, NT to UofA Activity Course

MACHINE SHOP Curse Design 2005-2006 Curse Infrmatin Organizatin Eastern Arizna Cllege Divisin Industrial Technlgy Educatin Curse Number MSP 104 Title Machine Shp Credits 4 Develped by Dryden Lecture/Lab

The OC Curve of Attribute Acceptance Plans

The OC Curve of Attrbute Acceptance Plans The Operatng Characterstc (OC) curve descrbes the probablty of acceptng a lot as a functon of the lot s qualty. Fgure 1 shows a typcal OC Curve. 10 8 6 4 1 3 4

Section 5.4 Annuities, Present Value, and Amortization

Secton 5.4 Annutes, Present Value, and Amortzaton Present Value In Secton 5.2, we saw that the present value of A dollars at nterest rate per perod for n perods s the amount that must be deposted today

1 Example 1: Axis-aligned rectangles

COS 511: Theoretcal Machne Learnng Lecturer: Rob Schapre Lecture # 6 Scrbe: Aaron Schld February 21, 2013 Last class, we dscussed an analogue for Occam s Razor for nfnte hypothess spaces that, n conjuncton

Multiple choice questions [60 points]

1 Multiple choice questions [60 points] Answe all o the ollowing questions. Read each question caeully. Fill the coect bubble on you scanton sheet. Each question has exactly one coect answe. All questions

Support Vector Machines

Support Vector Machnes Max Wellng Department of Computer Scence Unversty of Toronto 10 Kng s College Road Toronto, M5S 3G5 Canada wellng@cs.toronto.edu Abstract Ths s a note to explan support vector machnes.

Fraser Surrey Docks Adds Compliance System to the Container Gate Reservation System (GRS)

July 20 th, 2009 Fraser Surrey Dcks Adds Cmpliance System t the Cntainer Gate Reservatin System (GRS) In an effrt t increase cmpliance with the GRS, we have implemented a system t mnitr cmpliance s that

Financing Terms in the EOQ Model

Financing Tems in the EOQ Model Habone W. Stuat, J. Columbia Business School New Yok, NY 1007 hws7@columbia.edu August 6, 004 1 Intoduction This note discusses two tems that ae often omitted fom the standad

The Greedy Method. Introduction. 0/1 Knapsack Problem

The Greedy Method Introducton We have completed data structures. We now are gong to look at algorthm desgn methods. Often we are lookng at optmzaton problems whose performance s exponental. For an optmzaton

benefit is 2, paid if the policyholder dies within the year, and probability of death within the year is ).

REVIEW OF RISK MANAGEMENT CONCEPTS LOSS DISTRIBUTIONS AND INSURANCE Loss and nsurance: When someone s subject to the rsk of ncurrng a fnancal loss, the loss s generally modeled usng a random varable or