Part V: Closed-form solutions to Loop Closure Equations

Size: px
Start display at page:

Download "Part V: Closed-form solutions to Loop Closure Equations"

Transcription

1 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 in the loop closue equation ) One unknown angle and one unknown length 3) Two unknown lengths. Review vecto notation and basic opeations y x ME 360 Couse Notes S. Canfield Pat V -

2 Table: D Vecto Desciptions and Opeations Catesian Complex Pola ME 360 Couse Notes S. Canfield Pat V -

3 Closed-Fom Solutions to the Vecto Loop Closue Equation A geneal loop closue equation may look something like: whee i ae vectos in the chain. The loop closue equation is a vecto equation (and epesents scala equations) and can be solved if only scala unknowns exist in the equation. Thee possible cases exist: case ) two unknown angles case ) one unknown angle, one unknown length case 3) two unknown lengths Solution fo case ) Two unknown angles: A geneal loop closue eq. with two unknown angles may look like: // // /? /? // 0 (c.) Hee the unknowns ae 3 and 4. Fo geneality, call the vectos with unknown angles ua and ua: // // /? /? // ua 0 (c.) ua 5 Step 0: Reaange to collect all the knowns into a single vecto: (c.) with: ME 360 Couse Notes S. Canfield Pat V -3

4 Step : Now, ewite Eq. c. with one of the unknown angles isolated on one side (c.3) Step : Expand Eq. c.3 into eal and x and y components (eal and imaginay pats) (c.4) Step 3: Squae and add Eq. c..4 to eliminate one unknown angle (ua) (c.5) Step 4: Use the tan ½ angle identity to yield an algebaic (quadatic) equation: t t cua, s, t tan ua ua (c.6) t t (c.7) (c.8) ME 360 Couse Notes S. Canfield Pat V -4

5 Step 5: Solve fo t: b b 4ac t (c.9) a Note: the two solutions yield the two banches of the mechanism. Step 6: Solve fo the unknown angle fom the tan-/ identity (ua) (c.0) Step 7: Solve fo the othe unknown angle, ua: Note: The use of an atan function (quadant sensitive) ensues solution of unique angle value. (c.) ME 360 Couse Notes S. Canfield Pat V -5

6 Discuss: Physical Intepetation of solutions: ) solutions: ) Valid solutions: 3 4 O O4 Othe notes: ) Assumes all vecto tavel in the same diection ) If you have a vecto taveling in the opposite diection, use these equations but include a negative on the associated vecto magnitude tem in the equations ME 360 Couse Notes S. Canfield Pat V -6

7 Example : Conside the fou-ba shown below as a schematic, with vecto model, loop closue equation and known 3 4 O O4 The loop closue equation becomes, // o // /? /? (c.) Knowns: ; 6; ua 8; ua 90 ; 40 ; 5; Fist (Step 0 above): Collect all knowns into a single vecto: ME 360 Couse Notes S. Canfield Pat V -7

8 Second: Solve fo a, b, c: (Step 4) Thid: Solve fo t: (Step 5) Fouth: Solve fo angle, 4: (Step 6) Fifth: Solve fo 3 (Step 7) ME 360 Couse Notes S. Canfield Pat V -8

9 Automating the solution pocess fo one common case of mechanisms, the fouba linkage. Since the fouba is such a common mechanism, automating the solution pocess is wothwhile. A few ways to do this might include: Wite a function that etuns the solution based on an input set of link lengths and diving angle Ceate a fouba class that has the functionality of solving the position poblem. An example of the fist of these methods is biefly descibed hee. The syntax is based on pogamming in Matlab. Fist, ceate a function in matlab that will be called to solve the fouba, (fo example, fba.m). This function will accept the link lengths, gound link angle, input angle and banch, and etun the unknown angles in the fouba. % fba.m (theta3, theta4) = fba(,,3,4,theta,theta,banch); theta3= theta4= etun ME 360 Couse Notes S. Canfield Pat V -9

10 Solution fo case ) One unknown angle, one unknown link length: Two possibilities exist in this case, the unknown angle and length exist in the same vecto, o they do not. In the fist case, the solution is tivial (unknown vecto esults fom vecto addition). In the second case, fo example as shown in the loop closue equation shown below, the pocedue is as follows.?/ // /? // (c.) with the fist tailing supescipt indicating known/unknown length, the second indicating known/unknown angle. Fo geneality, call the vecto with unknown length ul and the vecto with unknown angle ua:?/ // /? // ul 0 (c.) ua 4 Step 0: Collect knowns into a single vecto: With Step : Rewite the loop closue equation with the unknown angle isolated on one side of the equation. (c.) Step : Expand Eq. c.3 into eal and x and y components (eal and imaginay pats) (c.3) ME 360 Couse Notes S. Canfield Pat V -0

11 Step 3: Use the squae and add technique to emove the unknown angle. (c.4) Step 4: This equation is now quadatic in the emaining unknown (), solve fo the two oots. Note, the two oots coespond to the two possible banches of this loop. (c.5) Step 5: Finally, solve fo the emaining unknown angle using the atan function as befoe. ME 360 Couse Notes S. Canfield Pat V -

12 Discuss: Physical Intepetation of solutions: ) solutions: ) Valid solutions: ME 360 Couse Notes S. Canfield Pat V -

13 Example of Solution fo case : The figue below shows a linkage schematic with vecto model, loop closue equation and known paametes. Solve fo the unknowns in this model The loop closue equation becomes, // // /??/ // // /??/ o ua ul 0 5; 3; 3 ua 8; Knowns: 50 ; 0 ; (c.) (c.) Fist (Step 0 above): Collect all knowns into a single vecto: Second: Solve fo a, b, c: (Step 4) ME 360 Couse Notes S. Canfield Pat V -3

14 Thid: Solve fo ul: (Step 4, second pat) Fouth: Solve fo angle, 3: (Step 5) ME 360 Couse Notes S. Canfield Pat V -4

15 Solution fo case 3) Two unknown lengths: In case 3, the unknown lengths in the loop closue equation esult in a set of two linea scala equations and can be solved diectly with linea algeba. The following example demonstates this case. The vecto loop equation is,?/?/ // // (c3.) with the unknowns hee in and. Fo geneality, call the vectos with unknown length ul, ul.?/?/ // // ul ul Step 0: Collect the knowns into a single vecto:?/ // /? ul ul k 0 with cos cos kx ky 3 sin 3 k k sin 3 kx 4 a tan ky ky, kx 4 (c3.) Step : Isolate the unknowns on one side of the equation the knowns on the othe;?/?/ // (c3.3) ul ul k Step : Expand this equation into its scala components, c c c ul ul s ul ul ul ul s ul ul k s Step 3: Cast these equations into matix fom, cul culul k ck s ul sul ul k sk o Ax b k k k (c3.4) (c3.5) ME 360 Couse Notes S. Canfield Pat V -5

Section 8.2 Polar Coordinates

Section 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 information

Tutorial Exercises: Central Forces

Tutorial Exercises: Central Forces Tutoial Execises: Cental Foces. Tuning Points fo the Keple potential (a) Wite down the two fist integals fo cental motion in the Keple potential V () = µm/ using J fo the angula momentum and E fo the total

More information

SHORT ANSWER. Write the word or phrase that best completes each statement or answers the question.

SHORT ANSWER. Write the word or phrase that best completes each statement or answers the question. Chapte 7-8 Review Math 1316 Name SHORT ANSWER. Wite the wod o phase that best completes each statement o answes the question. Solve the tiangle. 1) B = 34.4 C = 114.2 b = 29.0 1) Solve the poblem. 2) Two

More information

Physics Tutorial V1 2D Vectors

Physics Tutorial V1 2D Vectors Physics Tutoial V1 2D Vectos 1 Resolving Vectos & Addition of Vectos A vecto quantity has both magnitude and diection. Thee ae two ways commonly used to mathematically descibe a vecto. y (a) The pola fom:,

More information

As is natural, our Aerospace Structures will be described in a Euclidean three-dimensional space R 3.

As is natural, our Aerospace Structures will be described in a Euclidean three-dimensional space R 3. Appendix A Vecto Algeba As is natual, ou Aeospace Stuctues will be descibed in a Euclidean thee-dimensional space R 3. A.1 Vectos A vecto is used to epesent quantities that have both magnitude and diection.

More information

MAC Module 12 Eigenvalues and Eigenvectors

MAC 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 information

Appendix A. Appendices. A.1 ɛ ijk and cross products. Vector Operations: δ ij and ɛ ijk

Appendix 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 information

A Crash Course in (2 2) Matrices

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 information

DonnishJournals

DonnishJournals 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 information

Reading Assignment. Problem Description for Homework #9. Read Chapters 29 and 30.

Reading Assignment. Problem Description for Homework #9. Read Chapters 29 and 30. Reading Assignment Read Chaptes 29 and 30. Poblem Desciption fo Homewok #9 In this homewok, you will solve the inhomogeneous Laplace s equation to calculate the electic scala potential that exists between

More information

PHYS 110B - HW #7 Spring 2004, Solutions by David Pace Any referenced equations are from Griffiths Problem statements are paraphrased

PHYS 110B - HW #7 Spring 2004, Solutions by David Pace Any referenced equations are from Griffiths Problem statements are paraphrased PHYS 0B - HW #7 Sping 2004, Solutions by David Pace Any efeenced euations ae fom Giffiths Poblem statements ae paaphased. Poblem 0.3 fom Giffiths A point chage,, moves in a loop of adius a. At time t 0

More information

B da = 0. Q E da = ε. E da = E dv

B da = 0. Q E da = ε. E da = E dv lectomagnetic Theo Pof Ruiz, UNC Asheville, doctophs on YouTube Chapte Notes The Maxwell quations in Diffeential Fom 1 The Maxwell quations in Diffeential Fom We will now tansfom the integal fom of the

More information

Chapter 9 Dynamic stability analysis III Lateral motion (Lectures 33 and 34)

Chapter 9 Dynamic stability analysis III Lateral motion (Lectures 33 and 34) Pof. E.G. Tulapukaa Stability and contol Chapte 9 Dynamic stability analysis Lateal motion (Lectues 33 and 34) Keywods : Lateal dynamic stability - state vaiable fom of equations, chaacteistic equation

More information

3.6 Applied Optimization

3.6 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 information

Physics 111 Lecture 5 (Walker: 3.3-6) Vectors & Vector Math Motion Vectors Sept. 11, 2009

Physics 111 Lecture 5 (Walker: 3.3-6) Vectors & Vector Math Motion Vectors Sept. 11, 2009 Physics 111 Lectue 5 (Walke: 3.3-6) Vectos & Vecto Math Motion Vectos Sept. 11, 2009 Quiz Monday - Chap. 2 1 Resolving a vecto into x-component & y- component: Pola Coodinates Catesian Coodinates x y =

More information

MONTE CARLO SIMULATION OF FLUID FLOW

MONTE CARLO SIMULATION OF FLUID FLOW MONTE CARLO SIMULATION OF FLUID FLOW M. Ragheb 3/7/3 INTRODUCTION We conside the situation of Fee Molecula Collisionless and Reflective Flow. Collisionless flows occu in the field of aefied gas dynamics.

More information

An Application of Fuzzy Linear System of Equations in Economic Sciences

An Application of Fuzzy Linear System of Equations in Economic Sciences Austalian Jounal of Basic and Applied Sciences, 5(7): 7-14, 2011 ISSN 1991-8178 An Application of Fuzzy Linea System of Equations in Economic Sciences 1 S.H. Nassei, 2 M. Abdi and 3 B. Khabii 1 Depatment

More information

18.06 Problem Set 4 Solution

18.06 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 information

Now we just need to shuffle indices around a bit. The second term is already of the form

Now we just need to shuffle indices around a bit. The second term is already of the form Depatment of Physics, UCSD Physics 5B, Geneal Relativity Winte 05 Homewok, solutions. (a) Fom the Killing equation, ρ K σ ` σ K ρ 0 taking one deivative, µ ρ K σ ` µ σ K ρ 0 σ µ K ρ σ ρ K µ 0 ρ µ K σ `

More information

Right-handed screw dislocation in an isotropic solid

Right-handed screw dislocation in an isotropic solid Dislocation Mechanics Elastic Popeties of Isolated Dislocations Ou study of dislocations to this point has focused on thei geomety and thei ole in accommodating plastic defomation though thei motion. We

More information

Physics 2B Chapter 22 Notes - Magnetic Field Spring 2018

Physics 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 information

1D2G - Numerical solution of the neutron diffusion equation

1D2G - Numerical solution of the neutron diffusion equation DG - Numeical solution of the neuton diffusion equation Y. Danon Daft: /6/09 Oveview A simple numeical solution of the neuton diffusion equation in one dimension and two enegy goups was implemented. Both

More information

Quaternion Based Inverse Kinematics for Industrial Robot Manipulators with Euler Wrist

Quaternion Based Inverse Kinematics for Industrial Robot Manipulators with Euler Wrist Quatenion Based Invese Kinematics fo Industial Robot Manipulatos with Eule Wist Yavuz Aydın Electonics and Compute Education Kocaeli Univesity Umuttepe Kocaeli Tukey yavuz_98@hotmailcom Seda Kucuk Electonics

More information

Chapter 2: Introduction to Implicit Equations

Chapter 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 information

Introduction and Vectors

Introduction and Vectors SOLUTIONS TO PROBLEMS Intoduction and Vectos Section 1.1 Standads of Length, Mass, and Time *P1.4 Fo eithe sphee the volume is V = 4! and the mass is m =!V =! 4. We divide this equation fo the lage sphee

More information

Absolute Specifications: A typical absolute specification of a lowpass filter is shown in figure 1 where:

Absolute 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 information

Complex Eigenvalues. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB

Complex Eigenvalues. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB Pepaed by Vince Zaccone Fo ampus Leaning ssistance Sevices at USB omplex Numbes When solving fo the oots of a quadatic equation, eal solutions can not be found when the disciminant is negative. In these

More information

Many Electron Atoms. Electrons can be put into approximate orbitals and the properties of the many electron systems can be catalogued

Many Electron Atoms. Electrons can be put into approximate orbitals and the properties of the many electron systems can be catalogued Many Electon Atoms The many body poblem cannot be solved analytically. We content ouselves with developing appoximate methods that can yield quite accuate esults (but usually equie a compute). The electons

More information

INTRODUCTION. 2. Vectors in Physics 1

INTRODUCTION. 2. Vectors in Physics 1 INTRODUCTION Vectos ae used in physics to extend the study of motion fom one dimension to two dimensions Vectos ae indispensable when a physical quantity has a diection associated with it As an example,

More information

2 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

2 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 information

Phys 201A. Homework 5 Solutions

Phys 201A. Homework 5 Solutions Phys 201A Homewok 5 Solutions 3. In each of the thee cases, you can find the changes in the velocity vectos by adding the second vecto to the additive invese of the fist and dawing the esultant, and by

More information

ME 3600 Control Systems Frequency Domain Analysis

ME 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 information

AST 121S: The origin and evolution of the Universe. Introduction to Mathematical Handout 1

AST 121S: The origin and evolution of the Universe. Introduction to Mathematical Handout 1 Please ead this fist... AST S: The oigin and evolution of the Univese Intoduction to Mathematical Handout This is an unusually long hand-out and one which uses in places mathematics that you may not be

More information

ENGI 4430 Non-Cartesian Coordinates Page xi Fy j Fzk from Cartesian coordinates z to another orthonormal coordinate system u, v, ˆ i ˆ ˆi

ENGI 4430 Non-Cartesian Coordinates Page xi Fy j Fzk from Cartesian coordinates z to another orthonormal coordinate system u, v, ˆ i ˆ ˆi ENGI 44 Non-Catesian Coodinates Page 7-7. Conesions between Coodinate Systems In geneal, the conesion of a ecto F F xi Fy j Fzk fom Catesian coodinates x, y, z to anothe othonomal coodinate system u,,

More information

School of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007

School of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007 School of Electical and Compute Engineeing, Conell Univesity ECE 303: Electomagnetic Fields and Waves Fall 007 Homewok 8 Due on Oct. 19, 007 by 5:00 PM Reading Assignments: i) Review the lectue notes.

More information

Physics 121 Hour Exam #5 Solution

Physics 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 information

Liquid gas interface under hydrostatic pressure

Liquid gas interface under hydrostatic pressure Advances in Fluid Mechanics IX 5 Liquid gas inteface unde hydostatic pessue A. Gajewski Bialystok Univesity of Technology, Faculty of Civil Engineeing and Envionmental Engineeing, Depatment of Heat Engineeing,

More information

PHYS 705: Classical Mechanics. Small Oscillations

PHYS 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 information

Vectors Serway and Jewett Chapter 3

Vectors Serway and Jewett Chapter 3 Vectos Sewa and Jewett Chapte 3 Scalas and Vectos Vecto Components and Aithmetic Vectos in 3 Dimensions Unit vectos i, j, k Pactice Poblems: Chapte 3, poblems 9, 19, 31, 45, 55, 61 Phsical quantities ae

More information

MCV4U Final Exam Review. 1. Consider the function f (x) Find: f) lim. a) lim. c) lim. d) lim. 3. Consider the function: 4. Evaluate. lim. 5. Evaluate.

MCV4U Final Exam Review. 1. Consider the function f (x) Find: f) lim. a) lim. c) lim. d) lim. 3. Consider the function: 4. Evaluate. lim. 5. Evaluate. MCVU Final Eam Review Answe (o Solution) Pactice Questions Conside the function f () defined b the following gaph Find a) f ( ) c) f ( ) f ( ) d) f ( ) Evaluate the following its a) ( ) c) sin d) π / π

More information

15 Solving the Laplace equation by Fourier method

15 Solving the Laplace equation by Fourier method 5 Solving the Laplace equation by Fouie method I aleady intoduced two o thee dimensional heat equation, when I deived it, ecall that it taes the fom u t = α 2 u + F, (5.) whee u: [0, ) D R, D R is the

More information

Math 2263 Solutions for Spring 2003 Final Exam

Math 2263 Solutions for Spring 2003 Final Exam Math 6 Solutions fo Sping Final Exam ) A staightfowad appoach to finding the tangent plane to a suface at a point ( x, y, z ) would be to expess the cuve as an explicit function z = f ( x, y ), calculate

More information

10.2 Parametric Calculus

10.2 Parametric Calculus 10. Paametic Calculus Let s now tun ou attention to figuing out how to do all that good calculus stuff with a paametically defined function. As a woking eample, let s conside the cuve taced out by a point

More information

PROBLEM SET #1 SOLUTIONS by Robert A. DiStasio Jr.

PROBLEM 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 information

MODULE 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 (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 information

Non-Linear Dynamics Homework Solutions Week 2

Non-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 information

ME 210 Applied Mathematics for Mechanical Engineers

ME 210 Applied Mathematics for Mechanical Engineers Tangent and Ac Length of a Cuve The tangent to a cuve C at a point A on it is defined as the limiting position of the staight line L though A and B, as B appoaches A along the cuve as illustated in the

More information

radians). Figure 2.1 Figure 2.2 (a) quadrant I angle (b) quadrant II angle is in standard position Terminal side Terminal side Terminal side

radians). Figure 2.1 Figure 2.2 (a) quadrant I angle (b) quadrant II angle is in standard position Terminal side Terminal side Terminal side . TRIGONOMETRIC FUNCTIONS OF GENERAL ANGLES In ode to etend the definitions of the si tigonometic functions to geneal angles, we shall make use of the following ideas: In a Catesian coodinate sstem, an

More information

KEPLER S LAWS OF PLANETARY MOTION

KEPLER S LAWS OF PLANETARY MOTION EPER S AWS OF PANETARY MOTION 1. Intoduction We ae now in a position to apply what we have leaned about the coss poduct and vecto valued functions to deive eple s aws of planetay motion. These laws wee

More information

REVIEW Polar Coordinates and Equations

REVIEW Polar Coordinates and Equations REVIEW 9.1-9.4 Pola Coodinates and Equations You ae familia with plotting with a ectangula coodinate system. We ae going to look at a new coodinate system called the pola coodinate system. The cente of

More information

Chapter 5 Linear Equations: Basic Theory and Practice

Chapter 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 information

1 Spherical multipole moments

1 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 information

Physics 11 Chapter 3: Vectors and Motion in Two Dimensions. Problem Solving

Physics 11 Chapter 3: Vectors and Motion in Two Dimensions. Problem Solving Physics 11 Chapte 3: Vectos and Motion in Two Dimensions The only thing in life that is achieved without effot is failue. Souce unknown "We ae what we epeatedly do. Excellence, theefoe, is not an act,

More information

Physics 2020, Spring 2005 Lab 5 page 1 of 8. Lab 5. Magnetism

Physics 2020, Spring 2005 Lab 5 page 1 of 8. Lab 5. Magnetism Physics 2020, Sping 2005 Lab 5 page 1 of 8 Lab 5. Magnetism PART I: INTRODUCTION TO MAGNETS This week we will begin wok with magnets and the foces that they poduce. By now you ae an expet on setting up

More information

Relating Branching Program Size and. Formula Size over the Full Binary Basis. FB Informatik, LS II, Univ. Dortmund, Dortmund, Germany

Relating Branching Program Size and. Formula Size over the Full Binary Basis. FB Informatik, LS II, Univ. Dortmund, Dortmund, Germany Relating Banching Pogam Size and omula Size ove the ull Binay Basis Matin Saueho y Ingo Wegene y Ralph Wechne z y B Infomatik, LS II, Univ. Dotmund, 44 Dotmund, Gemany z ankfut, Gemany sauehof/wegene@ls.cs.uni-dotmund.de

More information

2. Plane Elasticity Problems

2. Plane Elasticity Problems S0 Solid Mechanics Fall 009. Plane lasticity Poblems Main Refeence: Theoy of lasticity by S.P. Timoshenko and J.N. Goodie McGaw-Hill New Yok. Chaptes 3..1 The plane-stess poblem A thin sheet of an isotopic

More information

The Substring Search Problem

The Substring Search Problem The Substing Seach Poblem One algoithm which is used in a vaiety of applications is the family of substing seach algoithms. These algoithms allow a use to detemine if, given two chaacte stings, one is

More information

dq 1 (5) q 1 where the previously mentioned limit has been taken.

dq 1 (5) q 1 where the previously mentioned limit has been taken. 1 Vecto Calculus And Continuum Consevation Equations In Cuvilinea Othogonal Coodinates Robet Maska: Novembe 25, 2008 In ode to ewite the consevation equations(continuit, momentum, eneg) to some cuvilinea

More information

Lecture 1a: Satellite Orbits

Lecture 1a: Satellite Orbits Lectue 1a: Satellite Obits Outline 1. Newton s Laws of Motion 2. Newton s Law of Univesal Gavitation 3. Calculating satellite obital paametes (assuming cicula motion) Scala & Vectos Scala: a physical quantity

More information

arxiv: v1 [physics.pop-ph] 3 Jun 2013

arxiv: v1 [physics.pop-ph] 3 Jun 2013 A note on the electostatic enegy of two point chages axiv:1306.0401v1 [physics.pop-ph] 3 Jun 013 A C Tot Instituto de Física Univesidade Fedeal do io de Janeio Caixa Postal 68.58; CEP 1941-97 io de Janeio,

More information

Pushdown Automata (PDAs)

Pushdown Automata (PDAs) CHAPTER 2 Context-Fee Languages Contents Context-Fee Gammas definitions, examples, designing, ambiguity, Chomsky nomal fom Pushdown Automata definitions, examples, euivalence with context-fee gammas Non-Context-Fee

More information

Cartesian Coordinate System and Vectors

Cartesian Coordinate System and Vectors Catesian Coodinate System and Vectos Coodinate System Coodinate system: used to descibe the position of a point in space and consists of 1. An oigin as the efeence point 2. A set of coodinate axes with

More information

Question 1: The dipole

Question 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 information

Classical Mechanics Homework set 7, due Nov 8th: Solutions

Classical Mechanics Homework set 7, due Nov 8th: Solutions Classical Mechanics Homewok set 7, due Nov 8th: Solutions 1. Do deivation 8.. It has been asked what effect does a total deivative as a function of q i, t have on the Hamiltonian. Thus, lets us begin with

More information

When two numbers are written as the product of their prime factors, they are in factored form.

When 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 information

6.4 Period and Frequency for Uniform Circular Motion

6.4 Period and Frequency for Uniform Circular Motion 6.4 Peiod and Fequency fo Unifom Cicula Motion If the object is constained to move in a cicle and the total tangential foce acting on the total object is zeo, F θ = 0, then (Newton s Second Law), the tangential

More information

Computational Methods of Solid Mechanics. Project report

Computational Methods of Solid Mechanics. Project report Computational Methods of Solid Mechanics Poject epot Due on Dec. 6, 25 Pof. Allan F. Bowe Weilin Deng Simulation of adhesive contact with molecula potential Poject desciption In the poject, we will investigate

More information

Practice Integration Math 120 Calculus I Fall 2015

Practice Integration Math 120 Calculus I Fall 2015 Pactice Integation Math 0 Calculus I Fall 05 Hee s a list of pactice eecises. Thee s a hint fo each one as well as an answe with intemediate steps... ( + d. Hint. Answe. ( 8 t + t + This fist set of indefinite

More information

Inverse Square Law and Polarization

Inverse Square Law and Polarization Invese Squae Law and Polaization Objectives: To show that light intensity is invesely popotional to the squae of the distance fom a point light souce and to show that the intensity of the light tansmitted

More information

MATH 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. 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 information

EFFECTS OF FRINGING FIELDS ON SINGLE PARTICLE DYNAMICS. M. Bassetti and C. Biscari INFN-LNF, CP 13, Frascati (RM), Italy

EFFECTS OF FRINGING FIELDS ON SINGLE PARTICLE DYNAMICS. M. Bassetti and C. Biscari INFN-LNF, CP 13, Frascati (RM), Italy Fascati Physics Seies Vol. X (998), pp. 47-54 4 th Advanced ICFA Beam Dynamics Wokshop, Fascati, Oct. -5, 997 EFFECTS OF FRININ FIELDS ON SINLE PARTICLE DYNAMICS M. Bassetti and C. Biscai INFN-LNF, CP

More information

Describing Circular motion

Describing Circular motion Unifom Cicula Motion Descibing Cicula motion In ode to undestand cicula motion, we fist need to discuss how to subtact vectos. The easiest way to explain subtacting vectos is to descibe it as adding a

More information

Practice Integration Math 120 Calculus I D Joyce, Fall 2013

Practice Integration Math 120 Calculus I D Joyce, Fall 2013 Pactice Integation Math 0 Calculus I D Joyce, Fall 0 This fist set of indefinite integals, that is, antideivatives, only depends on a few pinciples of integation, the fist being that integation is invese

More information

MATH 415, WEEK 3: Parameter-Dependence and Bifurcations

MATH 415, WEEK 3: Parameter-Dependence and Bifurcations MATH 415, WEEK 3: Paamete-Dependence and Bifucations 1 A Note on Paamete Dependence We should pause to make a bief note about the ole played in the study of dynamical systems by the system s paametes.

More information

Math Notes on Kepler s first law 1. r(t) kp(t)

Math Notes on Kepler s first law 1. r(t) kp(t) Math 7 - Notes on Keple s fist law Planetay motion and Keple s Laws We conside the motion of a single planet about the sun; fo simplicity, we assign coodinates in R 3 so that the position of the sun is

More information

Graphs of Sine and Cosine Functions

Graphs 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 information

FW Laboratory Exercise. Survival Estimation from Banded/Tagged Animals. Year No. i Tagged

FW Laboratory Exercise. Survival Estimation from Banded/Tagged Animals. Year No. i Tagged FW66 -- Laboatoy Execise uvival Estimation fom Banded/Tagged Animals Conside a geogaphically closed population of tout (Youngs and Robson 97). The adults ae tagged duing fall spawning, and subsequently

More information

Homework # 3 Solution Key

Homework # 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 information

Conjugate Gradient Methods. Michael Bader. Summer term 2012

Conjugate 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 information

SHORT ANSWER. Write the word or phrase that best completes each statement or answers the question.

SHORT ANSWER. Write the word or phrase that best completes each statement or answers the question. Math Pecalculus Ch. 6 Review Name SHORT ANSWER. Wite the wod o phase that best completes each statement o answes the question. Solve the tiangle. ) ) 6 7 0 Two sides and an angle (SSA) of a tiangle ae

More information

Polar Coordinates. a) (2; 30 ) b) (5; 120 ) c) (6; 270 ) d) (9; 330 ) e) (4; 45 )

Polar Coordinates. a) (2; 30 ) b) (5; 120 ) c) (6; 270 ) d) (9; 330 ) e) (4; 45 ) Pola Coodinates We now intoduce anothe method of labelling oints in a lane. We stat by xing a oint in the lane. It is called the ole. A standad choice fo the ole is the oigin (0; 0) fo the Catezian coodinate

More information

Research Design - - Topic 17 Multiple Regression & Multiple Correlation: Two Predictors 2009 R.C. Gardner, Ph.D.

Research Design - - Topic 17 Multiple Regression & Multiple Correlation: Two Predictors 2009 R.C. Gardner, Ph.D. Reseach Design - - Topic 7 Multiple Regession & Multiple Coelation: Two Pedictos 009 R.C. Gadne, Ph.D. Geneal Rationale and Basic Aithmetic fo two pedictos Patial and semipatial coelation Regession coefficients

More information

COMPUTATIONS OF ELECTROMAGNETIC FIELDS RADIATED FROM COMPLEX LIGHTNING CHANNELS

COMPUTATIONS OF ELECTROMAGNETIC FIELDS RADIATED FROM COMPLEX LIGHTNING CHANNELS Pogess In Electomagnetics Reseach, PIER 73, 93 105, 2007 COMPUTATIONS OF ELECTROMAGNETIC FIELDS RADIATED FROM COMPLEX LIGHTNING CHANNELS T.-X. Song, Y.-H. Liu, and J.-M. Xiong School of Mechanical Engineeing

More information

Chapter 4. Newton s Laws of Motion

Chapter 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 information

A Power Method for Computing Square Roots of Complex Matrices

A Power Method for Computing Square Roots of Complex Matrices JOURNAL OF MATHEMATICAL ANALYSIS AND APPLICATIONS 13, 39345 1997 ARTICLE NO. AY975517 A Powe Method fo Computing Squae Roots of Complex Matices Mohammed A. Hasan Depatment of Electical Engineeing, Coloado

More information

S7: Classical mechanics problem set 2

S7: Classical mechanics problem set 2 J. Magoian MT 9, boowing fom J. J. Binney s 6 couse S7: Classical mechanics poblem set. Show that if the Hamiltonian is indepdent of a genealized co-odinate q, then the conjugate momentum p is a constant

More information

Simulation of a 2-link Brachiating Robot with Open-Loop Controllers

Simulation of a 2-link Brachiating Robot with Open-Loop Controllers Simulation of a -link Bachiating Robot with Open-oop Contolles David Uffod Nothwesten Univesit June 009 . Poject Oveview The goal of this poject was to wite a complete simulation of a -link swinging obot

More information

Assignment solution

Assignment solution Assignment 04 solution Theodoe S. Novell 689DueOct04 Q0 [4](Read all pats befoe attempting any.) Supposeaisanaayofnumbesoflengthn,andxholdsanumbe. (a)[4]witeacontact(specification)focomputing i {0,..n}

More information

EM Boundary Value Problems

EM Boundary Value Problems EM Bounday Value Poblems 10/ 9 11/ By Ilekta chistidi & Lee, Seung-Hyun A. Geneal Desciption : Maxwell Equations & Loentz Foce We want to find the equations of motion of chaged paticles. The way to do

More information

MU+CU+KU=F MU+CU+KU=0

MU+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 information

Quantum Mechanics II

Quantum Mechanics II Quantum Mechanics II Pof. Bois Altshule Apil 25, 2 Lectue 25 We have been dicussing the analytic popeties of the S-matix element. Remembe the adial wave function was u kl () = R kl () e ik iπl/2 S l (k)e

More information

CALCULUS II Vectors. Paul Dawkins

CALCULUS 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 information

Newton s Laws, Kepler s Laws, and Planetary Orbits

Newton s Laws, Kepler s Laws, and Planetary Orbits Newton s Laws, Keple s Laws, and Planetay Obits PROBLEM SET 4 DUE TUESDAY AT START OF LECTURE 28 Septembe 2017 ASTRONOMY 111 FALL 2017 1 Newton s & Keple s laws and planetay obits Unifom cicula motion

More information

Physics for Scientists and Engineers

Physics for Scientists and Engineers Phsics 111 Sections 003 and 005 Instucto: Pof. Haimin Wang E-mail: haimin@flae.njit.edu Phone: 973-596-5781 Office: 460 Tienan Hall Homepage: http://sola.njit.edu/~haimin Office Hou: 2:30 to 3:50 Monda

More information

Physics 11 Chapter 4: Forces and Newton s Laws of Motion. Problem Solving

Physics 11 Chapter 4: Forces and Newton s Laws of Motion. Problem Solving Physics 11 Chapte 4: Foces and Newton s Laws of Motion Thee is nothing eithe good o bad, but thinking makes it so. William Shakespeae It s not what happens to you that detemines how fa you will go in life;

More information

Using Laplace Transform to Evaluate Improper Integrals Chii-Huei Yu

Using Laplace Transform to Evaluate Improper Integrals Chii-Huei Yu Available at https://edupediapublicationsog/jounals Volume 3 Issue 4 Febuay 216 Using Laplace Tansfom to Evaluate Impope Integals Chii-Huei Yu Depatment of Infomation Technology, Nan Jeon Univesity of

More information

MATH 300: Solutions for Problem Set 1

MATH 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 information

Chapter 13 Gravitation

Chapter 13 Gravitation Chapte 13 Gavitation In this chapte we will exploe the following topics: -Newton s law of gavitation, which descibes the attactive foce between two point masses and its application to extended objects

More information

MATH 155/GRACEY CH. 10 PRACTICE. SHORT ANSWER. Write the word or phrase that best completes each statement or answers the question.

MATH 155/GRACEY CH. 10 PRACTICE. SHORT ANSWER. Write the word or phrase that best completes each statement or answers the question. MATH /GRACEY CH. PRACTICE Name SHORT ANSWER. Wite the wod o phase that best completes each statement o answes the question. At the given point, find the line that is nomal to the cuve at the given point.

More information

I. CONSTRUCTION OF THE GREEN S FUNCTION

I. 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 information