ROTATION IN 3D WORLD RIGID BODY MOTION

Similar documents
KINEMATICS OF RIGID BODIES

CET MATHEMATICS 2013

A little harder example. A block sits at rest on a flat surface. The block is held down by its weight. What is the interaction pair for the weight?

Families of Solutions to Bernoulli ODEs

MATRICES AND VECTORS SPACE

Matrix Eigenvalues and Eigenvectors September 13, 2017

KINEMATICS OF RIGID BODIES

Plate Theory. Section 11: PLATE BENDING ELEMENTS

Practice Problems for the First Midterm

Plate Theory. Section 13: PLATE BENDING ELEMENTS

2. VECTORS AND MATRICES IN 3 DIMENSIONS

Multiple Integrals. Review of Single Integrals. Planar Area. Volume of Solid of Revolution

set is not closed under matrix [ multiplication, ] and does not form a group.

A proof of the strong twin prime conjecture

PHYS 601 HW3 Solution

Lecture 8 Wrap-up Part1, Matlab

The Islamic University of Gaza Faculty of Engineering Civil Engineering Department. Numerical Analysis ECIV Chapter 11

Multiple Integrals. Review of Single Integrals. Planar Area. Volume of Solid of Revolution

Math 520 Final Exam Topic Outline Sections 1 3 (Xiao/Dumas/Liaw) Spring 2008

Numerical Linear Algebra Assignment 008

Differential Geometry: Conformal Maps

Multivariate problems and matrix algebra

63. Representation of functions as power series Consider a power series. ( 1) n x 2n for all 1 < x < 1

Lecture Note 9: Orthogonal Reduction

The Algebra (al-jabr) of Matrices

Miscellaneous Problems. pinned to the ground

Uses of transformations. 3D transformations. Review of vectors. Vectors in 3D. Points vs. vectors. Homogeneous coordinates S S [ H [ S \ H \ S ] H ]

September 13 Homework Solutions

Texture and Anisotroy. Part I: Chapter 2. Description of Orientation

7.3 Problem 7.3. ~B(~x) = ~ k ~ E(~x)=! but we also have a reected wave. ~E(~x) = ~ E 2 e i~ k 2 ~x i!t. ~B R (~x) = ~ k R ~ E R (~x)=!

Week 10: Line Integrals

Eigen Values and Eigen Vectors of a given matrix

Partial Differential Equations

Plates on elastic foundation

Chapter 2. Vectors. 2.1 Vectors Scalars and Vectors

Some Methods in the Calculus of Variations

Chapter 3 Polynomials

THREE-DIMENSIONAL KINEMATICS OF RIGID BODIES

Matrix Solution to Linear Equations and Markov Chains

CS434a/541a: Pattern Recognition Prof. Olga Veksler. Lecture 2

Chapter 4 Force and Newton s Laws of Motion

Best Approximation in the 2-norm

Quadratic Residues. Chapter Quadratic residues

Jackson 2.26 Homework Problem Solution Dr. Christopher S. Baird University of Massachusetts Lowell

x = a To determine the volume of the solid, we use a definite integral to sum the volumes of the slices as we let!x " 0 :

Chapter 3. Vector Spaces

Unit 1 Exponentials and Logarithms

5.4. The Fundamental Theorem of Calculus. 356 Chapter 5: Integration. Mean Value Theorem for Definite Integrals

k and v = v 1 j + u 3 i + v 2

PART 1 MULTIPLE CHOICE Circle the appropriate response to each of the questions below. Each question has a value of 1 point.

Physics 116C Solution of inhomogeneous ordinary differential equations using Green s functions

AN020. a a a. cos. cos. cos. Orientations and Rotations. Introduction. Orientations

DEFINITION OF ASSOCIATIVE OR DIRECT PRODUCT AND ROTATION OF VECTORS

Pre-Calculus TMTA Test 2018

Math 211A Homework. Edward Burkard. = tan (2x + z)

MTH 5102 Linear Algebra Practice Exam 1 - Solutions Feb. 9, 2016

1 Linear Least Squares

We divide the interval [a, b] into subintervals of equal length x = b a n

Operations with Matrices

ES.182A Topic 32 Notes Jeremy Orloff

Supplement 4 Permutations, Legendre symbol and quadratic reciprocity

Space Curves. Recall the parametric equations of a curve in xy-plane and compare them with parametric equations of a curve in space.

Calculus 2: Integration. Differentiation. Integration

Math 32B Discussion Session Session 7 Notes August 28, 2018

Section 6.1 INTRO to LAPLACE TRANSFORMS

USA Mathematical Talent Search Round 1 Solutions Year 25 Academic Year

APPLICATIONS OF DEFINITE INTEGRALS

Machine Design II Prof. K.Gopinath & Prof. M.M.Mayuram. Drum Brakes. Among the various types of devices to be studied, based on their practical use,

LINEAR ALGEBRA APPLIED

x = b a n x 2 e x dx. cdx = c(b a), where c is any constant. a b

Exploring parametric representation with the TI-84 Plus CE graphing calculator

Thomas Whitham Sixth Form

Chapter 4 Contravariance, Covariance, and Spacetime Diagrams

LECTURE 10: JACOBI SYMBOL

Quantum Mechanics Qualifying Exam - August 2016 Notes and Instructions

( dg. ) 2 dt. + dt. dt j + dh. + dt. r(t) dt. Comparing this equation with the one listed above for the length of see that

Chapter 1 VECTOR ALGEBRA

in a uniform magnetic flux density B = Boa z. (a) Show that the electron moves in a circular path. (b) Find the radius r o

Taylor Polynomial Inequalities

SECTION 9-4 Translation of Axes

THE IMPORTANCE OF INCLUDING ELASTIC PROPERTY OF PENSTOCK IN THE EVALUATION OF STABILITY OF HYDROPOWEWR PLANTS

Lecture 6: Isometry. Table of contents

SCHOOL OF ENGINEERING & BUILT ENVIRONMENT

Problem set 1: Solutions Math 207B, Winter 2016

In Section 5.3 we considered initial value problems for the linear second order equation. y.a/ C ˇy 0.a/ D k 1 (13.1.4)

Counting intersections of spirals on a torus

Practice final exam solutions

CSCI 5525 Machine Learning

Polynomials and Division Theory

Jackson 2.7 Homework Problem Solution Dr. Christopher S. Baird University of Massachusetts Lowell

Improper Integrals, and Differential Equations

Main topics for the Second Midterm

Orthogonal Polynomials

ES.182A Topic 30 Notes Jeremy Orloff

CBSE-XII-2015 EXAMINATION. Section A. 1. Find the sum of the order and the degree of the following differential equation : = 0

INTRODUCTION TO LINEAR ALGEBRA

PRIMES AND QUADRATIC RECIPROCITY

Consider a potential problem in the half-space dened by z 0, with Dirichlet boundary conditions on the plane z = 0 (and at innity).

Abstract inner product spaces

Physics 712 Electricity and Magnetism Solutions to Final Exam, Spring 2016

Transcription:

OTATION IN 3D WOLD IGID BODY MOTION

igid Bod Motion Simultion igid bod motion Eqution of motion ff mmvv NN ddiiωω/dddd Angulr velocit Integrtion of rottion nd it s eression is necessr.

Simultion nd Eression of ottion igid bod movements cn be considered s combintion of trnsltion nd rottion. Ho to reresent the orienttion/rottion of rigid bod?

Toolog of rottion D osition One oint on line D rottion One oint on circle 3D osition One oint on 3D sce 3D rottion????

Eression of ottion ottion mtri Euler ngles Ais nd Angle Quternion There re mn eressions, becuse ech eression hs dvntges nd disdvntges. Let s see the rottion, differentil nd integrl.

Euler Angles For emle, rotte coordinte is in order of is 3 An orienttion cn be reresented b 3 ngles Order of rottions cn be vried. roll itch is one oulr order. Euler ngle cn be understood s joint ngles of mniultor nd orienttion of the end effector.

Euler Angles nd ottion Mtri The folloing three bsic rottion mtrices rotte vectors round the,, or is -- Euler ngles -- Euler ngles,,,, 3 3,, 3 3

ottion order is imortnt in 3D E.g., rotte Euler ngles ith the sme,, -- Euler ngles rottion: -- Euler ngles rottion: Comrison If the order is different, the result is different.

Chrcteristics of Mtri Multiliction ABC ABC in generl, it is correct, but AB BA is incorrect in most cses. The results deend on the rottion orders X is 3 Y is 3 Z is 3 Y is 3 X is 3 Z is 3 esult different orienttions

Problems on Mtri/Euler ngles bsed Eression Euler ngles hve some gulrities., 8, is sme orienttion for n b,, b is sme orienttion for n b. Comrison of orienttions re not es. E.g., 8, 3, 8, 3 6, 8, 6 33 mtri hs 9 elements nd inconvenient ottion is eressed not b ll 33 mtrices, but b 33 mtrices hose bsis re orthogonl ech other, sies re nd determinnt is. Comuttionl error m cuse violtion of these constrints. Differentil oertion is strnge form.

Is integrtion ossible? Integrl of elements is meningless, becuse ddition is not lloed. t t t t t t dt dt dt dt dt dt t ω ω ω ω ω ω, t if ω integrl t t t : t comosite:

Comrison of Position nd ottion osition: velocit: v direction: 3 d dt 3D Vector SO3 ngulr velocit : ω d dt ω ω ω ω ω ω 3 3 3 rottion 3 ω mtri Secil orthogonl orthonormlied mtri ith determinnt of t t ω t t d t t t t dt

Ais nd Angle bsed Eression As n intuitive rottion eression; otte rd round this is Cn eressed b 3D vector 3 : rottion ngle : direction of rottion is

Ais nd Angle bsed Eression The rnge of is vector is ~π π π - Inside of bll ith rdius π Normlition of vector if eceeds π ' ', ' hen ' ', ' hen ', hich stisfis ' Find l l l l l l Z n n l l < < π π π π π

Ais nd Angle bsed Eression Angulr velocit is differentil of the is nd the ngle. d ω dt The integrl of ngulr velocit is meningless. ngulr velocit : ω t ngulr velocit integrl: I ω if ω t ω t <, t < t ω t dt do not eress orienttion of t ωdt Addition hs no mening!, fter rottion of ω t

Ais nd Angle bsed Eression Addition of is nd ngle is imossible drn for 9 nd 9

Ais nd Angle bsed Eression Norml differentil is ngulr velocit. Addition hs no menings, comosition is troublesome For comosition, Find corresonding rottion mtri nd multil them. Integrl hs no mening

Quternion Quternion Euler rmeter Euler ngles Eress ngle ith four rel numbers Quternion for rottion round is u u ngle is q q,, u. Also cn be ritten in q v u, v

Quternion s oertion Tke ijk s n ension of imginr unit i Multiliction ijk k j i k j i q kk kj ki k jk jj ji j ik ij ii i k j i k j i k j i q q This is the rel form of quternion

Quternion s oertion Multiliction k j i kk kj ki k jk jj ji j ik ij ii i k j i q q - -k k Multiliction of quternion results in comosition of rottion q q q

Quternion s oertion ottion of osition vector k j i k j i ˆ The quternion hich corresonds * ˆ ' ˆ q q q k j i q k j i q * q q quternion the conjugtion of is * ' is

Quternion nd ottion Ais For quternion,,, v u Comre to Ais ngle reresenttion,, ' ' ' u Their forms re similr. But in quternion; Comosition of to rottions rottion of oint ottion is unit vector re done b the four rules of rithmetic ithout clculting trigonometric functions.

Quternion nd ottion For q v Quternion ith rottion round is, v u * q qq v u The rottion quternion sie is. u u is Shericl shell ith rdius of in 4,,, dimensionl sce

Quternion nd ottion q v,, v u u u nd < π cn eress n rottion. <, < cn eress n rottion. v q nd q eress the sme rottion. ight hemishere cn eress n rottion Comosition of quternion m result in left hemishere. Such quternions hve different quternions in left hemishere. Sme rottion eressed b different quternions cn led bugs. -q q

Summr of ottion Eression Ais nd Angle Differentil is ngulr velocit vector. Quternion Comuttion is fst onl bsic rithmetic oertion is needed for comosition nd rottion of oints. The rottion is is embedded. Euler ngles Es to understnd. Singulrit: one orienttion is reresented b infinite Euler ngles. ottion Mtri Clcultion is es. Corresond to bsis vectors.

Trnsformtion ithout She Chnge ottion ottion mtri orthonormlied mtri ith determinnt of three bsis vectors re orthogonl ech other nd sie is The determinnt of orthonormlied mtri is or - Set of 3D rottion mtri is nmed secil orthogonl grou SO3 SO is set of rottion mtri in D Confirmtion rottion mtri rottion round n is Confirm. n rottion round n is cn be eressed b rottion mtri.. An rottion eressed b rottion mtri cn be reresented b rottion round n is. ottion round n is ottion mtri A mtri hich eresses rottion round is ngle Proof is in the net ge You cn confirm tht this mtri is orthonormlied nd determinnt

Trnsformtion ithout She Chnge ottion Point is the result of rotting, in the ngle, round n is. O v Define v to stisf,v nd re orthogonl ech other. ' v v v Thus, e cn mke 33 rottion mtri b rotting three bsis vectors.

Trnsformtion ithout She Chnge ottion ottion mtri ottion round n is A quternion is ner to rottion mtri thn is nd ngle. So, e strt from quternion.

Quternion Mtri ottion mtri for rottion,in ngle, round is Quternion for rottion,in ngle, round is E:, element of the mtri α α α α α α The rottion mtri cn be eressed s は

Mtri Quternion m m m 3 m m m 3 m m m 3 3 33 m m m m m 33 3 4 m 33 3 4 m3 m3 m 3 m3 4, 4, cn be found in the sme 4 There should be ±. Hoever, in quternion, -q eress the sme rottion to q. So e choose onl. To quternions re corresond to one rottion mtri m m 3 m m 3 m Finll, checking m3 m3 m3 m3 m m m m m33 4 m m m33 4 comes to hen the mtri belongs SO3 33

Mtri Quternion With constrints of rottion mtri orthonormlied nd determinnt, e cn sho the sie of the quternion is. Quternion hve is nd ngle. So, trnsformtion of n rottion mtri cn be eressed b rottion round n is.