Complex Eigenvalues. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB
|
|
- Roland Piers Cross
- 6 years ago
- Views:
Transcription
1 Pepaed by Vince Zaccone Fo ampus Leaning ssistance Sevices at USB
2 omplex Numbes When solving fo the oots of a quadatic equation, eal solutions can not be found when the disciminant is negative. In these cases we use complex numbes to wite down the solutions. Fo example, if we ty to solve x 2-2x+2=0 we un into touble: x 2 ( 2) 2 2() ()(2) x 2 2 x i With the definition i 2 =-, we can wite the solutions as OMPLEX numbes, with a REL pat and an IMGINRY pat. In geneal, complex numbes look like a+bi, whee a and b ae eal. We call a the eal pat and b the imaginay pat of the complex numbe. Evey complex numbe has a conjugate a-bi. Multiplying conjugates yields a eal numbe: (a+bi)(a-bi)=a 2 +b 2. This is a vey useful tick! Pepaed by Vince Zaccone Fo ampus Leaning ssistance Sevices at USB
3 When a matix has complex eigenvalues they will always come in conjugate pais. The effect of multiplying by the matix will be a stetch and a otation. The example below should help claify the situation: 8 5 We will find the eigenvalues fo this matix. Pepaed by Vince Zaccone Fo ampus Leaning ssistance Sevices at USB
4 When a matix has complex eigenvalues they will always come in conjugate pais. The effect of multiplying by the matix will be a stetch and a otation. The example below should help claify the situation: 8 5 We will find the eigenvalues fo this matix. 5 0 ( )(5 ) ( 2) ( 2) 2 2() i ()(7) Next we find eigenvectos fo the eigenvalues. Pepaed by Vince Zaccone Fo ampus Leaning ssistance Sevices at USB
5 When a matix has complex eigenvalues they will always come in conjugate pais. The effect of multiplying by the matix will be a stetch and a otation. The example below should help claify the situation: 8 5 i ( i) 5 8 ( 0 i) 0 i 8 i 0 0 i 2 i 0 0 Pepaed by Vince Zaccone Fo ampus Leaning ssistance Sevices at USB
6 When a matix has complex eigenvalues they will always come in conjugate pais. The effect of multiplying by the matix will be a stetch and a otation. The example below should help claify the situation: 8 5 i ( i) 5 8 ( 0 i) 0 i 8 i 0 0 i 2 i 0 0 t this point we can wite down the equation and find the vecto. We could do ow eduction but it s not eally necessay (multiplying one ow by the conjugate of its complex enty should make it clea that the ows ae multiples of each othe. Let s use the second ow: x ( i) x2 0 x ( i) x2 i Hee is an eigenvecto fo λ=+i Pepaed by Vince Zaccone Fo ampus Leaning ssistance Sevices at USB
7 When a matix has complex eigenvalues they will always come in conjugate pais. The effect of multiplying by the matix will be a stetch and a otation. The example below should help claify the situation: 8 5 We could epeat the same wok to find the othe eigenvecto, but we don t need to. Since the e-values ae conjugates, so ae thei eigenvectos. i i i i Hee ae the eigenvalues with thei eigenvectos. t this point we could use ou diagonalization technique to obtain a diagonal matix with the (complex) eigenvalues on the diagonal, just like we did when the eigenvalues wee eal. Instead, we will get a matix that shows the otation and stetch that we mentioned peviously. Pepaed by Vince Zaccone Fo ampus Leaning ssistance Sevices at USB
8 When a matix has complex eigenvalues they will always come in conjugate pais. The effect of multiplying by the matix will be a stetch and a otation. The example below should help claify the situation: 8 5 We fom matix P whose columns ae the eal and imaginay pats of the eigenvecto. P i i 0 Real 0 Imaginay i The book uses the e-value with the negative imaginay pat, so we will do the same. The pocess will also wok if you choose the othe e-value. When we use this matix to do a similaity tansfomation on the oiginal matix (just like we did fo diagonalization) we get a new matix that will have the stetch and otation popeties we ae looking fo. Pepaed by Vince Zaccone Fo ampus Leaning ssistance Sevices at USB
9 When a matix has complex eigenvalues they will always come in conjugate pais. The effect of multiplying by the matix will be a stetch and a otation. The example below should help claify the situation: 8 5 P 0 P 0 Use the shotcut fo 2x2 invese matices Pepaed by Vince Zaccone Fo ampus Leaning ssistance Sevices at USB
10 When a matix has complex eigenvalues they will always come in conjugate pais. The effect of multiplying by the matix will be a stetch and a otation. The example below should help claify the situation: 8 5 P 0 P 0 Use the shotcut fo 2x2 invese matices P P Fo eigenvalue a-bi, the matix will always take the fom a b b a Pepaed by Vince Zaccone Fo ampus Leaning ssistance Sevices at USB
11 When a matix has complex eigenvalues they will always come in conjugate pais. The effect of multiplying by the matix will be a stetch and a otation. The example below should help claify the situation: 8 5 Matix is simila to Matix. It has the same eigenvalues. Matix splits into 2 pats. One is just a stetch (multiplication by the length of the eigenvalue). The othe pat is a otation. a b b 0 0 cos( ) sin( ) sin( ) cos( ) Pepaed by Vince Zaccone Fo ampus Leaning ssistance Sevices at USB
12 When a matix has complex eigenvalues they will always come in conjugate pais. The effect of multiplying by the matix will be a stetch and a otation. The example below should help claify the situation: 8 5 Matix is simila to Matix. It has the same eigenvalues. Matix splits into 2 pats. One is just a stetch (multiplication by the length of the eigenvalue). The othe pat is a otation. a b b 0 0 cos( ) sin( ) In ou example, the eigenvalue is +i, so = 7 sin( ) cos( ) Pepaed by Vince Zaccone Fo ampus Leaning ssistance Sevices at USB
13 When a matix has complex eigenvalues they will always come in conjugate pais. The effect of multiplying by the matix will be a stetch and a otation. The example below should help claify the situation: 8 5 Matix is simila to Matix. It has the same eigenvalues. Matix splits into 2 pats. One is just a stetch (multiplication by the length of the eigenvalue). The othe pat is a otation. a b b 0 0 cos( ) sin( ) In ou example, the eigenvalue is +i, so = sin( ) cos( ) Pepaed by Vince Zaccone Fo ampus Leaning ssistance Sevices at USB
14 When a matix has complex eigenvalues they will always come in conjugate pais. The effect of multiplying by the matix will be a stetch and a otation. The example below should help claify the situation: 8 5 Matix is simila to Matix. It has the same eigenvalues. Matix splits into 2 pats. One is just a stetch (multiplication by the length of the eigenvalue). The othe pat is a otation. a b b 0 0 cos( ) sin( ) In ou example, the eigenvalue is +i, so = cos( ) 7 sin( ) cos( ) 76 So matix will stetch a vecto by 7, and otate it counte-clockwise by 76. This will coespond to an outwad spial when we look at the effect of matix. Pepaed by Vince Zaccone Fo ampus Leaning ssistance Sevices at USB
A Crash Course in (2 2) Matrices
A Cash Couse in ( ) Matices Seveal weeks woth of matix algeba in an hou (Relax, we will only stuy the simplest case, that of matices) Review topics: What is a matix (pl matices)? A matix is a ectangula
More informationMAC Module 12 Eigenvalues and Eigenvectors
MAC 23 Module 2 Eigenvalues and Eigenvectos Leaning Objectives Upon completing this module, you should be able to:. Solve the eigenvalue poblem by finding the eigenvalues and the coesponding eigenvectos
More informationMODULE 5a and 5b (Stewart, Sections 12.2, 12.3) INTRO: In MATH 1114 vectors were written either as rows (a1, a2,..., an) or as columns a 1 a. ...
MODULE 5a and 5b (Stewat, Sections 2.2, 2.3) INTRO: In MATH 4 vectos wee witten eithe as ows (a, a2,..., an) o as columns a a 2... a n and the set of all such vectos of fixed length n was called the vecto
More informationPHYS 705: Classical Mechanics. Small Oscillations
PHYS 705: Classical Mechanics Small Oscillations Fomulation of the Poblem Assumptions: V q - A consevative system with depending on position only - The tansfomation equation defining does not dep on time
More informationADVANCED SUBSIDIARY (AS) General Certificate of Education Mathematics Assessment Unit F1. assessing. Module FP1: Further Pure Mathematics 1
ADVACED SUBSIDIARY (AS) Geneal Cetificate of Education 15 Mathematics Assessment Unit F1 assessing Module F1: Futhe ue Mathematics 1 [AMF11] WEDESDAY 4 UE, MRIG MAR SCHEME 958.1 F GCE ADVACED/ADVACED SUBSIDIARY
More informationMATH 220: SECOND ORDER CONSTANT COEFFICIENT PDE. We consider second order constant coefficient scalar linear PDEs on R n. These have the form
MATH 220: SECOND ORDER CONSTANT COEFFICIENT PDE ANDRAS VASY We conside second ode constant coefficient scala linea PDEs on R n. These have the fom Lu = f L = a ij xi xj + b i xi + c i whee a ij b i and
More informationSection 8.2 Polar Coordinates
Section 8. Pola Coodinates 467 Section 8. Pola Coodinates The coodinate system we ae most familia with is called the Catesian coodinate system, a ectangula plane divided into fou quadants by the hoizontal
More informationPart V: Closed-form solutions to Loop Closure Equations
Pat V: Closed-fom solutions to Loop Closue Equations This section will eview the closed-fom solutions techniques fo loop closue equations. The following thee cases will be consideed. ) Two unknown angles
More informationChapter 5 Linear Equations: Basic Theory and Practice
Chapte 5 inea Equations: Basic Theoy and actice In this chapte and the next, we ae inteested in the linea algebaic equation AX = b, (5-1) whee A is an m n matix, X is an n 1 vecto to be solved fo, and
More information18.06 Problem Set 4 Solution
8.6 Poblem Set 4 Solution Total: points Section 3.5. Poblem 2: (Recommended) Find the lagest possible numbe of independent vectos among ) ) ) v = v 4 = v 5 = v 6 = v 2 = v 3 =. Solution (4 points): Since
More informationWaves and Polarization in General
Waves and Polaization in Geneal Wave means a distubance in a medium that tavels. Fo light, the medium is the electomagnetic field, which can exist in vacuum. The tavel pat defines a diection. The distubance
More informationof the contestants play as Falco, and 1 6
JHMT 05 Algeba Test Solutions 4 Febuay 05. In a Supe Smash Bothes tounament, of the contestants play as Fox, 3 of the contestants play as Falco, and 6 of the contestants play as Peach. Given that thee
More informationMU+CU+KU=F MU+CU+KU=0
MEEN 67 Handout # MODAL ANALYSIS OF MDOF Systems with VISCOUS DAMPING ^ Symmetic he motion of a n-dof linea system is descibed by the set of 2 nd ode diffeential equations MU+CU+KU=F t whee U (t) and F
More informationTo Feel a Force Chapter 7 Static equilibrium - torque and friction
To eel a oce Chapte 7 Chapte 7: Static fiction, toque and static equilibium A. Review of foce vectos Between the eath and a small mass, gavitational foces of equal magnitude and opposite diection act on
More informationGraphs of Sine and Cosine Functions
Gaphs of Sine and Cosine Functions In pevious sections, we defined the tigonometic o cicula functions in tems of the movement of a point aound the cicumfeence of a unit cicle, o the angle fomed by the
More informationRigid Body Dynamics 2. CSE169: Computer Animation Instructor: Steve Rotenberg UCSD, Winter 2018
Rigid Body Dynamics 2 CSE169: Compute Animation nstucto: Steve Rotenbeg UCSD, Winte 2018 Coss Poduct & Hat Opeato Deivative of a Rotating Vecto Let s say that vecto is otating aound the oigin, maintaining
More informationPhysics 2B Chapter 22 Notes - Magnetic Field Spring 2018
Physics B Chapte Notes - Magnetic Field Sping 018 Magnetic Field fom a Long Staight Cuent-Caying Wie In Chapte 11 we looked at Isaac Newton s Law of Gavitation, which established that a gavitational field
More informationCS-184: Computer Graphics. Today
CS-184: Compute Gaphics Lectue #6: 3D Tansfomations and Rotations Pof. James O Bien Univesity of Califonia, Bekeley V2006-F-06-1.0 Today Tansfomations in 3D Rotations Matices Eule angles Eponential maps
More informationA Bijective Approach to the Permutational Power of a Priority Queue
A Bijective Appoach to the Pemutational Powe of a Pioity Queue Ia M. Gessel Kuang-Yeh Wang Depatment of Mathematics Bandeis Univesity Waltham, MA 02254-9110 Abstact A pioity queue tansfoms an input pemutation
More informationChapter 2: Introduction to Implicit Equations
Habeman MTH 11 Section V: Paametic and Implicit Equations Chapte : Intoduction to Implicit Equations When we descibe cuves on the coodinate plane with algebaic equations, we can define the elationship
More informationCALCULUS II Vectors. Paul Dawkins
CALCULUS II Vectos Paul Dawkins Table of Contents Peface... ii Vectos... 3 Intoduction... 3 Vectos The Basics... 4 Vecto Aithmetic... 8 Dot Poduct... 13 Coss Poduct... 21 2007 Paul Dawkins i http://tutoial.math.lama.edu/tems.aspx
More informationHomework # 3 Solution Key
PHYSICS 631: Geneal Relativity Homewok # 3 Solution Key 1. You e on you hono not to do this one by hand. I ealize you can use a compute o simply look it up. Please don t. In a flat space, the metic in
More informationOn a quantity that is analogous to potential and a theorem that relates to it
Su une quantité analogue au potential et su un théoème y elatif C R Acad Sci 7 (87) 34-39 On a quantity that is analogous to potential and a theoem that elates to it By R CLAUSIUS Tanslated by D H Delphenich
More informationPhysics 2A Chapter 10 - Moment of Inertia Fall 2018
Physics Chapte 0 - oment of netia Fall 08 The moment of inetia of a otating object is a measue of its otational inetia in the same way that the mass of an object is a measue of its inetia fo linea motion.
More informationConjugate Gradient Methods. Michael Bader. Summer term 2012
Gadient Methods Outlines Pat I: Quadatic Foms and Steepest Descent Pat II: Gadients Pat III: Summe tem 2012 Pat I: Quadatic Foms and Steepest Descent Outlines Pat I: Quadatic Foms and Steepest Descent
More informationMath 124B February 02, 2012
Math 24B Febuay 02, 202 Vikto Gigoyan 8 Laplace s equation: popeties We have aleady encounteed Laplace s equation in the context of stationay heat conduction and wave phenomena. Recall that in two spatial
More informationCh 8 Alg 2 Note Sheet Key
Ch 8 Alg Note Sheet Key Chapte 8: Eponential and Logaithmic Functions 8. Eploing Eponential Models Fo some data, the est model is a function that uses the independent vaiale as an eponent. An eponential
More informationON THE TWO-BODY PROBLEM IN QUANTUM MECHANICS
ON THE TWO-BODY PROBLEM IN QUANTUM MECHANICS L. MICU Hoia Hulubei National Institute fo Physics and Nuclea Engineeing, P.O. Box MG-6, RO-0775 Buchaest-Maguele, Romania, E-mail: lmicu@theoy.nipne.o (Received
More informationsinγ(h y > ) exp(iωt iqx)dωdq
Lectue 9/28/5 Can we ecove a ay pictue fom the above G fo a membane stip? Such a pictue would be complementay to the above expansion in a seies of integals along the many banches of the dispesion elation.
More informationMATH 417 Homework 3 Instructor: D. Cabrera Due June 30. sin θ v x = v r cos θ v θ r. (b) Then use the Cauchy-Riemann equations in polar coordinates
MATH 417 Homewok 3 Instucto: D. Cabea Due June 30 1. Let a function f(z) = u + iv be diffeentiable at z 0. (a) Use the Chain Rule and the fomulas x = cosθ and y = to show that u x = u cosθ u θ, v x = v
More informationChapter 4. Newton s Laws of Motion
Chapte 4 Newton s Laws of Motion 4.1 Foces and Inteactions A foce is a push o a pull. It is that which causes an object to acceleate. The unit of foce in the metic system is the Newton. Foce is a vecto
More informationEEO 401 Digital Signal Processing Prof. Mark Fowler
EEO 41 Digital Signal Pocessing Pof. Mak Fowle Note Set #31 Linea Phase FIR Design Optimum Equiipple (Paks-McClellan) Reading: Sect. 1.2.4 1.2.6 of Poakis & Manolakis 1/2 Motivation The window method and
More informationCS-184: Computer Graphics. Today. Lecture #5: 3D Transformations and Rotations. Wednesday, September 7, 11. Transformations in 3D Rotations
CS-184: Compute Gaphics Lectue #5: D Tansfomations and Rotations Pof. James O Bien Univesity of Califonia, Bekeley V011-F-05-1.0 Today Tansfomations in D Rotations Matices Eule angles Eponential maps Quatenions
More information2 x 8 2 x 2 SKILLS Determine whether the given value is a solution of the. equation. (a) x 2 (b) x 4. (a) x 2 (b) x 4 (a) x 4 (b) x 8
5 CHAPTER Fundamentals When solving equations that involve absolute values, we usually take cases. EXAMPLE An Absolute Value Equation Solve the equation 0 x 5 0 3. SOLUTION By the definition of absolute
More informationMath 301: The Erdős-Stone-Simonovitz Theorem and Extremal Numbers for Bipartite Graphs
Math 30: The Edős-Stone-Simonovitz Theoem and Extemal Numbes fo Bipatite Gaphs May Radcliffe The Edős-Stone-Simonovitz Theoem Recall, in class we poved Tuán s Gaph Theoem, namely Theoem Tuán s Theoem Let
More informationDonnishJournals
DonnishJounals 041-1189 Donnish Jounal of Educational Reseach and Reviews. Vol 1(1) pp. 01-017 Novembe, 014. http:///dje Copyight 014 Donnish Jounals Oiginal Reseach Pape Vecto Analysis Using MAXIMA Savaş
More informationWhat to Expect on the Placement Exam
What to Epect on the Placement Eam Placement into: MTH o MTH 44 05 05 The ACCUPLACER placement eam is an adaptive test ceated by the College Boad Educational Testing Sevice. This document was ceated to
More informationOSCILLATIONS AND GRAVITATION
1. SIMPLE HARMONIC MOTION Simple hamonic motion is any motion that is equivalent to a single component of unifom cicula motion. In this situation the velocity is always geatest in the middle of the motion,
More informationMATH 300: Solutions for Problem Set 1
Question.a: The de is MATH 300: Solutions fo Poblem Set 2u 4u 4u u 0: So a 2, b 2 and c 4. Hence b 2 ac 4 < 0. The de is ellitic. Question.b: The de is u 2u u u 0: So a, b and c. Hence b 2 ac 2. The de
More informationLecture 7: Angular Momentum, Hydrogen Atom
Lectue 7: Angula Momentum, Hydogen Atom Vecto Quantization of Angula Momentum and Nomalization of 3D Rigid Roto wavefunctions Conside l, so L 2 2 2. Thus, we have L 2. Thee ae thee possibilities fo L z
More informationQuantum Fourier Transform
Chapte 5 Quantum Fouie Tansfom Many poblems in physics and mathematics ae solved by tansfoming a poblem into some othe poblem with a known solution. Some notable examples ae Laplace tansfom, Legende tansfom,
More informationInformation Retrieval Advanced IR models. Luca Bondi
Advanced IR models Luca Bondi Advanced IR models 2 (LSI) Pobabilistic Latent Semantic Analysis (plsa) Vecto Space Model 3 Stating point: Vecto Space Model Documents and queies epesented as vectos in the
More informationDynamic Visualization of Complex Integrals with Cabri II Plus
Dynamic Visualiation of omplex Integals with abi II Plus Sae MIKI Kawai-juu, IES Japan Email: sand_pictue@hotmailcom Abstact: Dynamic visualiation helps us undestand the concepts of mathematics This pape
More information1 Spherical multipole moments
Jackson notes 9 Spheical multipole moments Suppose we have a chage distibution ρ (x) wheeallofthechageiscontained within a spheical egion of adius R, as shown in the diagam. Then thee is no chage in the
More informationThen the number of elements of S of weight n is exactly the number of compositions of n into k parts.
Geneating Function In a geneal combinatoial poblem, we have a univee S of object, and we want to count the numbe of object with a cetain popety. Fo example, if S i the et of all gaph, we might want to
More informationPhysics 121 Hour Exam #5 Solution
Physics 2 Hou xam # Solution This exam consists of a five poblems on five pages. Point values ae given with each poblem. They add up to 99 points; you will get fee point to make a total of. In any given
More informationOn the integration of the equations of hydrodynamics
Uebe die Integation de hydodynamischen Gleichungen J f eine u angew Math 56 (859) -0 On the integation of the equations of hydodynamics (By A Clebsch at Calsuhe) Tanslated by D H Delphenich In a pevious
More informationH.W.GOULD West Virginia University, Morgan town, West Virginia 26506
A F I B O N A C C I F O R M U L A OF LUCAS A N D ITS SUBSEQUENT M A N I F E S T A T I O N S A N D R E D I S C O V E R I E S H.W.GOULD West Viginia Univesity, Mogan town, West Viginia 26506 Almost eveyone
More informationQuantum Mechanics I - Session 5
Quantum Mechanics I - Session 5 Apil 7, 015 1 Commuting opeatos - an example Remine: You saw in class that Â, ˆB ae commuting opeatos iff they have a complete set of commuting obsevables. In aition you
More informationCOORDINATE TRANSFORMATIONS - THE JACOBIAN DETERMINANT
COORDINATE TRANSFORMATIONS - THE JACOBIAN DETERMINANT Link to: phsicspages home page. To leave a comment o epot an eo, please use the auilia blog. Refeence: d Inveno, Ra, Intoducing Einstein s Relativit
More informationTANTON S TAKE ON CONTINUOUS COMPOUND INTEREST
CURRICULUM ISPIRATIOS: www.maa.og/ci www.theglobalmathpoject.og IOVATIVE CURRICULUM OLIE EXPERIECES: www.gdaymath.com TATO TIDBITS: www.jamestanton.com TATO S TAKE O COTIUOUS COMPOUD ITEREST DECEMBER 208
More information11.2 Proving Figures are Similar Using Transformations
Name lass ate 11. Poving igues ae Simila Using Tansfomations ssential Question: How can similait tansfomations be used to show two figues ae simila? esouce ocke ploe onfiming Similait similait tansfomation
More informationCS-184: Computer Graphics. Today. Lecture #5: 3D Transformations and Rotations. 05-3DTransformations.key - September 21, 2016
1 CS-184: Compute Gaphics Lectue #5: D Tansfomations and Rotations Pof. James O Bien Univesity of Califonia, Bekeley V016-S-05-1.0 Today Tansfomations in D Rotations Matices Eule angles Eponential maps
More informationA Hartree-Fock Example Using Helium
Univesity of Connecticut DigitalCommons@UConn Chemisty Education Mateials Depatment of Chemisty June 6 A Hatee-Fock Example Using Helium Cal W. David Univesity of Connecticut, Cal.David@uconn.edu Follow
More informationMonotonluğu Koruyan Matrisler. Monotonicity Preserving Matrices
SAKARYA ÜNİVERSİTESİ FEN BİLİMLERİ ENSTİTÜSÜ DERGİSİ SAKARYA UNIVERSITY JOURNAL OF SCIENCE e-issn: 2147-835X Degi sayfası: http://degipa.gov.t/saufenbilde Geliş/Received 15.02.2016 Kabul/Accepted 27.03.2017
More informationChapter 3: Theory of Modular Arithmetic 38
Chapte 3: Theoy of Modula Aithmetic 38 Section D Chinese Remainde Theoem By the end of this section you will be able to pove the Chinese Remainde Theoem apply this theoem to solve simultaneous linea conguences
More informationA Relativistic Electron in a Coulomb Potential
A Relativistic Electon in a Coulomb Potential Alfed Whitehead Physics 518, Fall 009 The Poblem Solve the Diac Equation fo an electon in a Coulomb potential. Identify the conseved quantum numbes. Specify
More informationSOME GENERAL NUMERICAL RADIUS INEQUALITIES FOR THE OFF-DIAGONAL PARTS OF 2 2 OPERATOR MATRICES
italian jounal of pue and applied mathematics n. 35 015 (433 44) 433 SOME GENERAL NUMERICAL RADIUS INEQUALITIES FOR THE OFF-DIAGONAL PARTS OF OPERATOR MATRICES Watheq Bani-Domi Depatment of Mathematics
More informationWhen two numbers are written as the product of their prime factors, they are in factored form.
10 1 Study Guide Pages 420 425 Factos Because 3 4 12, we say that 3 and 4 ae factos of 12. In othe wods, factos ae the numbes you multiply to get a poduct. Since 2 6 12, 2 and 6 ae also factos of 12. The
More informationHopefully Helpful Hints for Gauss s Law
Hopefully Helpful Hints fo Gauss s Law As befoe, thee ae things you need to know about Gauss s Law. In no paticula ode, they ae: a.) In the context of Gauss s Law, at a diffeential level, the electic flux
More informationGreen s Identities and Green s Functions
LECTURE 7 Geen s Identities and Geen s Functions Let us ecall The ivegence Theoem in n-dimensions Theoem 7 Let F : R n R n be a vecto field ove R n that is of class C on some closed, connected, simply
More informationSo, if we are finding the amount of work done over a non-conservative vector field F r, we do that long ur r b ur =
3.4 Geen s Theoem Geoge Geen: self-taught English scientist, 793-84 So, if we ae finding the amount of wok done ove a non-consevative vecto field F, we do that long u b u 3. method Wok = F d F( () t )
More information33. 12, or its reciprocal. or its negative.
Page 6 The Point is Measuement In spite of most of what has been said up to this point, we did not undetake this poject with the intent of building bette themometes. The point is to measue the peson. Because
More informationAPPLICATION OF MAC IN THE FREQUENCY DOMAIN
PPLICION OF MC IN HE FREQUENCY DOMIN D. Fotsch and D. J. Ewins Dynamics Section, Mechanical Engineeing Depatment Impeial College of Science, echnology and Medicine London SW7 2B, United Kingdom BSRC he
More informationGeometry of the homogeneous and isotropic spaces
Geomety of the homogeneous and isotopic spaces H. Sonoda Septembe 2000; last evised Octobe 2009 Abstact We summaize the aspects of the geomety of the homogeneous and isotopic spaces which ae most elevant
More informationHW Solutions # MIT - Prof. Please study example 12.5 "from the earth to the moon". 2GmA v esc
HW Solutions # 11-8.01 MIT - Pof. Kowalski Univesal Gavity. 1) 12.23 Escaping Fom Asteoid Please study example 12.5 "fom the eath to the moon". a) The escape velocity deived in the example (fom enegy consevation)
More informationMA557/MA578/CS557. Lecture 14. Prof. Tim Warburton. Spring
MA557/MA578/CS557 Lectue 4 Sping 3 Pof. Tim Wabuton timwa@math.unm.edu Matlab Notes To ceate a symbolic vaiable (say theta) use the command: theta = sym( theta ); Example manipulation: Matlab cont To evaluate
More informationA STUDY OF HAMMING CODES AS ERROR CORRECTING CODES
AGU Intenational Jounal of Science and Technology A STUDY OF HAMMING CODES AS ERROR CORRECTING CODES Ritu Ahuja Depatment of Mathematics Khalsa College fo Women, Civil Lines, Ludhiana-141001, Punjab, (India)
More informationQuestion 1: The dipole
Septembe, 08 Conell Univesity, Depatment of Physics PHYS 337, Advance E&M, HW #, due: 9/5/08, :5 AM Question : The dipole Conside a system as discussed in class and shown in Fig.. in Heald & Maion.. Wite
More informationClassical Worm algorithms (WA)
Classical Wom algoithms (WA) WA was oiginally intoduced fo quantum statistical models by Pokof ev, Svistunov and Tupitsyn (997), and late genealized to classical models by Pokof ev and Svistunov (200).
More informationME 3600 Control Systems Frequency Domain Analysis
ME 3600 Contol Systems Fequency Domain Analysis The fequency esponse of a system is defined as the steady-state esponse of the system to a sinusoidal (hamonic) input. Fo linea systems, the esulting steady-state
More informationn 1 Cov(X,Y)= ( X i- X )( Y i-y ). N-1 i=1 * If variable X and variable Y tend to increase together, then c(x,y) > 0
Covaiance and Peason Coelation Vatanian, SW 540 Both covaiance and coelation indicate the elationship between two (o moe) vaiables. Neithe the covaiance o coelation give the slope between the X and Y vaiable,
More informationI. CONSTRUCTION OF THE GREEN S FUNCTION
I. CONSTRUCTION OF THE GREEN S FUNCTION The Helmohltz equation in 4 dimensions is 4 + k G 4 x, x = δ 4 x x. In this equation, G is the Geen s function and 4 efes to the dimensionality. In the vey end,
More informationAuchmuty High School Mathematics Department Advanced Higher Notes Teacher Version
The Binomial Theoem Factoials Auchmuty High School Mathematics Depatment The calculations,, 6 etc. often appea in mathematics. They ae called factoials and have been given the notation n!. e.g. 6! 6!!!!!
More information8 Separation of Variables in Other Coordinate Systems
8 Sepaation of Vaiables in Othe Coodinate Systems Fo the method of sepaation of vaiables to succeed you need to be able to expess the poblem at hand in a coodinate system in which the physical boundaies
More informationIntroduction to Arrays
Intoduction to Aays Page 1 Intoduction to Aays The antennas we have studied so fa have vey low diectivity / gain. While this is good fo boadcast applications (whee we want unifom coveage), thee ae cases
More informationLinear Systems With Coeæcient Matrices. Having Fields of Values. Ren-Cang Li. Department of Mathematics. University of California at Berkeley
Linea Systems With Coeæcient Matices Having Fields of Values Not Containing The Oigin æ Ren-Cang Li Depatment of Mathematics Univesity of Califonia at Bekeley Bekeley, Califonia 9470 Mach 9, 994 Compute
More informationDouble-angle & power-reduction identities. Elementary Functions. Double-angle & power-reduction identities. Double-angle & power-reduction identities
Double-angle & powe-eduction identities Pat 5, Tigonomety Lectue 5a, Double Angle and Powe Reduction Fomulas In the pevious pesentation we developed fomulas fo cos( β) and sin( β) These fomulas lead natually
More informationRelated Rates - the Basics
Related Rates - the Basics In this section we exploe the way we can use deivatives to find the velocity at which things ae changing ove time. Up to now we have been finding the deivative to compae the
More information3.6 Applied Optimization
.6 Applied Optimization Section.6 Notes Page In this section we will be looking at wod poblems whee it asks us to maimize o minimize something. Fo all the poblems in this section you will be taking the
More informationMultiple Experts with Binary Features
Multiple Expets with Binay Featues Ye Jin & Lingen Zhang Decembe 9, 2010 1 Intoduction Ou intuition fo the poect comes fom the pape Supevised Leaning fom Multiple Expets: Whom to tust when eveyone lies
More informationInformation Filtering and Retrieval lecture SS 2007
Infomation Filteing and Retieval lectue SS 7 D. Dominik Kuopka Pof. D. Mathias Weske Repetition: limitations of models without tem intedependency Real Wold usage, poblems appea Mophology? Synonymy? adaptation
More informationAnalytic Evaluation of two-electron Atomic Integrals involving Extended Hylleraas-CI functions with STO basis
Analytic Evaluation of two-electon Atomic Integals involving Extended Hylleaas-CI functions with STO basis B PADHY (Retd.) Faculty Membe Depatment of Physics, Khalikote (Autonomous) College, Behampu-760001,
More informationAP Physics - Coulomb's Law
AP Physics - oulomb's Law We ve leaned that electons have a minus one chage and potons have a positive one chage. This plus and minus one business doesn t wok vey well when we go in and ty to do the old
More informationScattering in Three Dimensions
Scatteing in Thee Dimensions Scatteing expeiments ae an impotant souce of infomation about quantum systems, anging in enegy fom vey low enegy chemical eactions to the highest possible enegies at the LHC.
More informationThe Divergence Theorem
13.8 The ivegence Theoem Back in 13.5 we ewote Geen s Theoem in vecto fom as C F n ds= div F x, y da ( ) whee C is the positively-oiented bounday cuve of the plane egion (in the xy-plane). Notice this
More informationAppendix B The Relativistic Transformation of Forces
Appendix B The Relativistic Tansfomation of oces B. The ou-foce We intoduced the idea of foces in Chapte 3 whee we saw that the change in the fou-momentum pe unit time is given by the expession d d w x
More informationNon-Linear Dynamics Homework Solutions Week 2
Non-Linea Dynamics Homewok Solutions Week Chis Small Mach, 7 Please email me at smach9@evegeen.edu with any questions o concens eguading these solutions. Fo the ececises fom section., we sketch all qualitatively
More informationPDF Created with deskpdf PDF Writer - Trial ::
A APPENDIX D TRIGONOMETRY Licensed to: jsamuels@bmcc.cun.edu PDF Ceated with deskpdf PDF Wite - Tial :: http://www.docudesk.com D T i g o n o m e t FIGURE a A n g l e s Angles can be measued in degees
More informationMAGNETIC FIELD AROUND TWO SEPARATED MAGNETIZING COILS
The 8 th Intenational Confeence of the Slovenian Society fo Non-Destuctive Testing»pplication of Contempoay Non-Destuctive Testing in Engineeing«Septembe 1-3, 5, Potoož, Slovenia, pp. 17-1 MGNETIC FIELD
More informationLinear Algebra Math 221
Linea Algeba Math Open Book Eam Open Notes Sept Calculatos Pemitted Sho all ok (ecept #). ( pts) Gien the sstem of equations a) ( pts) Epess this sstem as an augmented mati. b) ( pts) Bing this mati to
More information30 The Electric Field Due to a Continuous Distribution of Charge on a Line
hapte 0 The Electic Field Due to a ontinuous Distibution of hage on a Line 0 The Electic Field Due to a ontinuous Distibution of hage on a Line Evey integal ust include a diffeential (such as d, dt, dq,
More informationPROBLEM SET #1 SOLUTIONS by Robert A. DiStasio Jr.
POBLM S # SOLUIONS by obet A. DiStasio J. Q. he Bon-Oppenheime appoximation is the standad way of appoximating the gound state of a molecula system. Wite down the conditions that detemine the tonic and
More informationA NEW VARIABLE STIFFNESS SPRING USING A PRESTRESSED MECHANISM
Poceedings of the ASME 2010 Intenational Design Engineeing Technical Confeences & Computes and Infomation in Engineeing Confeence IDETC/CIE 2010 August 15-18, 2010, Monteal, Quebec, Canada DETC2010-28496
More informationAppendix A. Appendices. A.1 ɛ ijk and cross products. Vector Operations: δ ij and ɛ ijk
Appendix A Appendices A1 ɛ and coss poducts A11 Vecto Opeations: δ ij and ɛ These ae some notes on the use of the antisymmetic symbol ɛ fo expessing coss poducts This is an extemely poweful tool fo manipulating
More informationRotational Motion. Lecture 6. Chapter 4. Physics I. Course website:
Lectue 6 Chapte 4 Physics I Rotational Motion Couse website: http://faculty.uml.edu/andiy_danylov/teaching/physicsi Today we ae going to discuss: Chapte 4: Unifom Cicula Motion: Section 4.4 Nonunifom Cicula
More informationCompactly Supported Radial Basis Functions
Chapte 4 Compactly Suppoted Radial Basis Functions As we saw ealie, compactly suppoted functions Φ that ae tuly stictly conditionally positive definite of ode m > do not exist The compact suppot automatically
More informationAbsolute Specifications: A typical absolute specification of a lowpass filter is shown in figure 1 where:
FIR FILTER DESIGN The design of an digital filte is caied out in thee steps: ) Specification: Befoe we can design a filte we must have some specifications. These ae detemined by the application. ) Appoximations
More informationScientific Computing II
Scientific Computing II Conjugate Gadient Methods Michael Bade Summe 2014 Conjugate Gadient Methods, Summe 2014 1 Families of Iteative Solves elaxation methods: Jacobi-, Gauss-Seidel-Relaxation,... Ove-Relaxation-Methods
More informationSection 26 The Laws of Rotational Motion
Physics 24A Class Notes Section 26 The Laws of otational Motion What do objects do and why do they do it? They otate and we have established the quantities needed to descibe this motion. We now need to
More information