PLANAR MULTIBODY DYNAMICS Formulation, Programming, and Applications. Errata Last update: November 2014
|
|
- Paul Perry
- 6 years ago
- Views:
Transcription
1 PLANAR MULTIBODY DYNAMICS Formulation, Programming, and Applications Errata Last update: November 204 During the preparation of this tetbook, a great deal of attention was paid to minimize the number of errors that normall occur either in the preparation phase or in the publication phase of a book. Despite that effort, some errors in the manuscript were not detected, as well as other errors that appeared during the publication phase. As such errors become known, the will be reported in this document. This document will be updated as soon as new errors are found. A note to the reader: If ou come across an errors, please inform the author b sending an to pen@ .arizona.edu. Thank ou! Page 6; line 5 from the bottom Change O to B. Attaching a Cartesian reference frame - at B, Page 39; Eample 2.9, 4th line Replace the second equation with the following equation: Φ 2 = Page 44; Problem 2. Over-score. appears incorrectl on several Φ s. Make the following changes: In the problem statement: Φ = z + z 2 4z z z 2 (a)... Φ q... (c)... Φ = Φ q q. Page 45; Problem 2.22(a) Change q = { φ 2 2 to: { } q = φ 2 2 φ 2 Page 50; Figure 3.4 Change the vector component along the -ais from s (ξ) to: s () Page 77; 2nd line Change Fig. 3.5 to: Fig. 4.3
2 Page 94; line 3 % Define spring-damper-actiator constants % Define spring-damper-actuator constants Page 95; equation in the middle of the page Correct the number in (s,d,a) f = to: (s,d,a) f = Page 99; Equation (4.4), line following equation, and Eq. (4.42) Lambda should be in bold-face: (c) f = D λ (4.4) where λ is an (c) h = D λ (4.42) Page 32; in the middle of the page Revise the first line of the Jacobian matri in function D to: D = [ jac_j_aq z2 z2 Page 32; near the bottom Revise the first line of the MATLAB file to: function gamma = PC_MP_gamma(dees_d) Page 33; near the top Revise the entries for gamma arra to: gamma = Page 33; near the bottom Revise the first and the fourth lines of the MATLAB file to: % file name: PC_FS_A.m % Film Strip Advancer clear all addpath Basics PC_Basics PC_AA Page 36; Figure (d) for Problem 5.3 The distance b on the figure is misplaced. Replace the figure with the one shown here. b a Planar Multibod Dnamics: Errata 2
3 Page 45; Figure 6.2 Remove reaction force from (b). O O O (c) f A,B (c ) f B,A A B A B A (a) (b) (c) B Page 48; first line in the first program % Append to the file P_MP % Append to the file PC_MP Page 49; middle of the page Change the MATLAB statement M_diag = to: M = Page 77; second paragraph, first line Change joint-coordinate to: point-coordinate Page 26; line 6 in the M-file function Phi = BC_Phi Change the line d = r_p{3} - r_p{5}; to: d = r_p{4} - r_p{5}; Page 27; lines & 6 in the M-file function gamma = BC_MP_A_gamma Change the line function gamma = BC_MP_A_gamma to: function gamma = BC_gamma Change the line d = r_p{3} - r_p{5}; d_d = r_p_d{3} - r_p_d{5}; to: d = r_p{4} - r_p{5}; d_d = r_p_d{4} - r_p_d{5}; Page 226; Problem 7.9, (a) Change in term of to in terms of Page 234; middle of the page Change (Eqs. [4.22] to [5.25]) to (Eqs. [4.22] to [5.27]) Page 246; line following Eq. (8.25) Change are the sub-jacobians of to are the transpose of the sub-jacobians of Planar Multibod Dnamics: Errata 3
4 Page 25; Matri before Section 8.4 REMARKS Change the sign of one of the entries in the last column of the Jacobian transpose λ 0.25 λ λ λ 4 0 Page 255; Problem 8.8, first line Change a pin join to a pin joint Page 265; Figure 9.5(b) Add the - aes and the angle φ to the figure: A θ u ξ φ θ 2 ξ 2 Page 266; Equations (9.6) and (9.7) Both equations require correction. Correct the equations to: r r 0 r 0 r 0 φ 0 = θ r 2 r 2 u θ θ 2 r 2 u (9.6) B = 0 0 θ 2 (9.7) r 2 u φ Page 277; Equation (9.23) Second and fourth lines have errors. Correct the equation to: * Φ = * Dc + * Dc = * D(B θ + B θ) + * DBθ = D θ + ( * D B + * DB) θ = D θ + D θ = 0 Planar Multibod Dnamics: Errata 4
5 Page 278; Equation (9.25) The equation is in error. Correct it to: D θ = γ Page 278; Equation (9.26) First, second and third lines have errors. Correct the equation to: γ = D θ = * D B θ * Dc = * D B θ + * γ Page 286; Equation (9.37) Missing dots. Correct the equation to: θ A A γ = D θ = r u 2 r 2 θ 2 θ 3 Page 298; Last equation B contains errors. Correct the equation to: r B = r 2 u 0 0 Page 299; Equation (0.9) This equation contains errors. Correct the equation to: h = B (h M B θ) f + w m r θ r r2 n = 0 0 u 0 f 2 + w 2 m 2 ( r 2 θ + u d2 ) 0 r (f + w m r θ ) + n + r 2 f 2 + w 2 m 2 ( r 2 θ + u d2 ( )) = u f 2 + w 2 m 2 ( ( r 2 θ + u d2 (0.9) )) Page 300; middle of the page Change the listed values for h_joint = to: h_joint = Page 324; following the first two lines Change record(:5,:) = to: record(:5,:6) Planar Multibod Dnamics: Errata 5
6 Page 335; Problem.8 Change the last line to: (c) Appl the bod coordinate Page 337; Problem.2, fourth line Change in Problem.9 to: in Problem.20. Page 344; third line Change Eqs. (2.6) and (2.9) to: Eqs. (2.6) and (2.9) Page 35; Problem 2., first line Change Refer to Problem.3 to: Refer to Problem.4. Page 35; Problem 2.2, first line Change Refer to Problem.4 to: Refer to Problem.5. Page 35; Problem 2.3, first line Change Refer to Problem.9 to: Refer to Problem.20. Page 35; Problem 2.4, first line Change Refer to Problem.20 to: Refer to Problem.2. Page 359; third M-file Change the first line of the MATLAB file to: function z_d = E_3_3(t, z) Pages ; the M-file that starts on page 367 There are several misprint and programming errors in this file. The last two lines that appear on page 367 should be removed. Change the global and the mass matri statements. Add the gravitational constant. There should be no separation line before the % Set time parameters statement. clear all addpath Basics PC_Basics global k_ L 0 d_c_ m_a m_b g r_o M M_arra % Define particle masses and spring-damper characteristics m_a = 3; m_b = 4; ; g = 9.8; k_ = 50; L 0 =.; d_c_ = 20; % Initial velues for coordinates and velocities r_a = [0.5; -]; r_a_d = [0.0; 0.0]; r_o = [0; 0]; r_b = [2; -]; r_b_d = [0.0; 0.0]; % Construct the mass matri (arra) Planar Multibod Dnamics: Errata 6
7 M_arra = [m_a; m_a; m_b; m_b]; M = diag(m_arra); % Initialize z arra z = [r_a; r_b; r_a_d; r_b_d]; % Set time parameters Tspan = [0.0:0.04:.0]; % Integrate [T, zt] = ode45(@e_3_6, Tspan, z); % Animation nt = size(t); plot_trace(nt, r_o, zt) Page 368; the second M-file Revise the global statement: function z_d = E_3_6(t, z) global k_ L 0 d_c_ m_a m_b g r_o M M_arra... Page 369; Figure 3.4 Due to the errors in the M-file as has been described in Corrections 2 and 3, the figure should be replaced. Page 372; middle of the page Add the following short phrase to the end of the paragraph before the M-file function h = BC_h:... b invoking the function BC_radial which is saved in the folder BC_Basics. Page 397; third line of the program Revise the line c_d = D_all\rhsv; to c_d = [D; D_driver]\rhsv; Planar Multibod Dnamics: Errata 7
PLANAR MULTIBODY DYNAMICS Formulation, Programming, and Applications. Errata Last update: August 2012
PLANAR MULTIBODY DYNAMICS Formulation, Programming, and Applications Errata Last update: August 202 During the preparation of this tetbook, a great deal of attention was paid to minimize the number of
More informationChapter 6: Structural Analysis
Chapter 6: Structural Analysis APPLICATIONS Trusses are commonly used to support a roof. For a given truss geometry and load, how can we determine the forces in the truss members and select their sizes?
More informationEngineering Mechanics: Statics STRUCTURAL ANALYSIS. by Dr. Ibrahim A. Assakkaf SPRING 2007 ENES 110 Statics
CHAPTER Engineering Mechanics: Statics STRUCTURAL ANALYSIS College of Engineering Department of Mechanical Engineering Tenth Edition 6a by Dr. Ibrahim A. Assakkaf SPRING 2007 ENES 110 Statics Department
More informationRigid Body Transforms-3D. J.C. Dill transforms3d 27Jan99
ESC 489 3D ransforms 1 igid Bod ransforms-3d J.C. Dill transforms3d 27Jan99 hese notes on (2D and) 3D rigid bod transform are currentl in hand-done notes which are being converted to this file from that
More informationLecture 5: 3-D Rotation Matrices.
3.7 Transformation Matri and Stiffness Matri in Three- Dimensional Space. The displacement vector d is a real vector entit. It is independent of the frame used to define it. d = d i + d j + d k = dˆ iˆ+
More informationKinematics. Félix Monasterio-Huelin, Álvaro Gutiérrez & Blanca Larraga. September 5, Contents 1. List of Figures 1.
Kinematics Féli Monasterio-Huelin, Álvaro Gutiérre & Blanca Larraga September 5, 2018 Contents Contents 1 List of Figures 1 List of Tables 2 Acronm list 3 1 Degrees of freedom and kinematic chains of rigid
More information1 HOMOGENEOUS TRANSFORMATIONS
HOMOGENEOUS TRANSFORMATIONS Purpose: The purpose of this chapter is to introduce ou to the Homogeneous Transformation. This simple 4 4 transformation is used in the geometr engines of CAD sstems and in
More informationRobotics I June 11, 2018
Exercise 1 Robotics I June 11 018 Consider the planar R robot in Fig. 1 having a L-shaped second link. A frame RF e is attached to the gripper mounted on the robot end effector. A B y e C x e Figure 1:
More informationINSTRUCTIONS TO CANDIDATES:
NATIONAL NIVERSITY OF SINGAPORE FINAL EXAMINATION FOR THE DEGREE OF B.ENG ME 444 - DYNAMICS AND CONTROL OF ROBOTIC SYSTEMS October/November 994 - Time Allowed: 3 Hours INSTRCTIONS TO CANDIDATES:. This
More informationExercise 1b: Differential Kinematics of the ABB IRB 120
Exercise 1b: Differential Kinematics of the ABB IRB 120 Marco Hutter, Michael Blösch, Dario Bellicoso, Samuel Bachmann October 5, 2016 Abstract The aim of this exercise is to calculate the differential
More informationNumerical Methods for Engineers, Second edition: Chapter 1 Errata
Numerical Methods for Engineers, Second edition: Chapter 1 Errata 1. p.2 first line, remove the Free Software Foundation at 2. p.2 sixth line of the first proper paragraph, fe95.res should be replaced
More informationON THE INTERPRETATION OF THE LAGRANGE MULTIPLIERS IN THE CONSTRAINT FORMULATION OF CONTACT PROBLEMS; OR WHY ARE SOME MULTIPLIERS ALWAYS ZERO?
Proceedings of the ASME 214 International Design Engineering Technical Conferences & Computers and Information in Engineering Conference IDETC/CIE 214 August 17-2, 214, Buffalo, New York, USA DETC214-3479
More informationMoving Reference Frame Kinematics Homework
Chapter 3 Moving Reference Frame Kinematics Homework Freeform c 2016 3-1 3-2 Freeform c 2016 Homework 3. Given: n L-shaped telescoping arm is pinned to ground at point. The arm is rotating counterclockwise
More information7. FORCE ANALYSIS. Fundamentals F C
ME 352 ORE NLYSIS 7. ORE NLYSIS his chapter discusses some of the methodologies used to perform force analysis on mechanisms. he chapter begins with a review of some fundamentals of force analysis using
More informationENGR-1100 Introduction to Engineering Analysis. Lecture 19
ENGR-1100 Introduction to Engineering Analysis Lecture 19 SIMPLE TRUSSES, THE METHOD OF JOINTS, & ZERO-FORCE MEMBERS Today s Objectives: Students will be able to: In-Class Activities: a) Define a simple
More informationME751 Advanced Computational Multibody Dynamics
ME751 Advanced Computational Multibody Dynamics Inverse Dynamics Equilibrium Analysis Various Odd Ends March 18, 2010 Dan Negrut, 2010 ME751, UW-Madison Action speaks louder than words but not nearly as
More informationLinear Algebra II (finish from last time) Root finding
Lecture 5: Topics: Linear lgebra II (finish from last time) Root finding -Cross product of two vectors -Finding roots of linear equations -Finding roots of nonlinear equations HW: HW 1, Part 3-4 given
More informationErrata Dynamic General Equilibrium Modelling, Springer: Berlin August 2015
Errata Dynamic General Equilibrium Modelling, Springer: Berlin 2005 17 August 2015 Chapter 1.1 p. 9/10: Figure 1.1 was computed for the parameter values T = 59, α = 0.50, and ρ = 0.35 and not as stated
More informationTransformation of kinematical quantities from rotating into static coordinate system
Transformation of kinematical quantities from rotating into static coordinate sstem Dimitar G Stoanov Facult of Engineering and Pedagog in Sliven, Technical Universit of Sofia 59, Bourgasko Shaussee Blvd,
More informationKevin James. MTHSC 3110 Section 2.1 Matrix Operations
MTHSC 3110 Section 2.1 Matrix Operations Notation Let A be an m n matrix, that is, m rows and n columns. We ll refer to the entries of A by their row and column indices. The entry in the i th row and j
More informationCS-184: Computer Graphics. Today
CS-184: Computer Graphics Lecture #3: 2D Transformations Prof. James O Brien Universit of California, Berkele V2006-S-03-1.0 Toda 2D Transformations Primitive Operations Scale, Rotate, Shear, Flip, Translate
More informationTo show how to determine the forces in the members of a truss using the method of joints and the method of sections.
5 Chapter Objectives To show how to determine the forces in the members of a truss using the method of joints and the method of sections. To analyze the forces acting on the members of frames and machines
More informationReview of Linear Algebra
Review of Linear Algebra Dr Gerhard Roth COMP 40A Winter 05 Version Linear algebra Is an important area of mathematics It is the basis of computer vision Is very widely taught, and there are many resources
More informationPROJECT 1 DYNAMICS OF MACHINES 41514
PROJECT DYNAMICS OF MACHINES 454 Theoretical and Experimental Modal Analysis and Validation of Mathematical Models in Multibody Dynamics Ilmar Ferreira Santos, Professor Dr.-Ing., Dr.Techn., Livre-Docente
More informationErrata for Instructor s Solutions Manual for Gravity, An Introduction to Einstein s General Relativity 1st printing
Errata for Instructor s Solutions Manual for Gravity, An Introduction to Einstein s General Relativity st printing Updated 7/7/003 (hanks to Scott Fraser who provided almost all of these.) Statement of
More informationk is a product of elementary matrices.
Mathematics, Spring Lecture (Wilson) Final Eam May, ANSWERS Problem (5 points) (a) There are three kinds of elementary row operations and associated elementary matrices. Describe what each kind of operation
More informationDealing with Rotating Coordinate Systems Physics 321. (Eq.1)
Dealing with Rotating Coordinate Systems Physics 321 The treatment of rotating coordinate frames can be very confusing because there are two different sets of aes, and one set of aes is not constant in
More informationStatics: Lecture Notes for Sections
Chapter 6: Structural Analysis Today s Objectives: Students will be able to: a) Define a simple truss. b) Determine the forces in members of a simple truss. c) Identify zero-force members. READING QUIZ
More informationCS 335 Graphics and Multimedia. 2D Graphics Primitives and Transformation
C 335 Graphics and Multimedia D Graphics Primitives and Transformation Basic Mathematical Concepts Review Coordinate Reference Frames D Cartesian Reference Frames (a) (b) creen Cartesian reference sstems
More informationErrata (Includes critical corrections only for the 1 st, 2 nd & 3 rd reprints)
Page Number Errata (Includes critical corrections only for the 1 st, 2 nd & 3 rd reprints) Description of Correction Mechanics of Materials, 8e James M. Gere & Barry J. Goodno ISBN: 9781111577735 11 Figure
More informationConservation of Linear Momentum for a Differential Control Volume
Conservation of Linear Momentum for a Differential Control Volume When we applied the rate-form of the conservation of mass equation to a differential control volume (open sstem in Cartesian coordinates,
More informationMatrix Mathematics. Errata and Addenda for the Second Edition. Dennis S. Bernstein February 13, 2014
Matrix Mathematics Errata and Addenda for the Second Edition Dennis S. Bernstein dsbaero@umich.edu February 13, 2014 This document contains an updated list of errata for the second edition of Matrix Mathematics.
More informationExam 2 October 17, 2013
Exam 2 Instructions: You have 60 minutes to complete this exam. This is a closed-book, closed-notes exam. You are allowed to use an approved calculator during the exam. Usage of mobile phones and other
More informationMulti-body Singularity Equations IRI Technical Report
IRI-TR-10-02 Multi-body Singularity Equations IRI Technical Report On how to obtain the equations for computation with CUIK O. Bohigas-Nadal L. Ros Abstract This technical report explains how to obtain
More informationFigure 1. A planar mechanism. 1
ME 352 - Machine Design I Summer Semester 201 Name of Student Lab Section Number EXAM 1. OPEN BOOK AND CLOSED NOTES. Wednesday, July 2nd, 201 Use the blank paper provided for your solutions. Write on one
More informationMEAM 520. More Velocity Kinematics
MEAM 520 More Velocity Kinematics Katherine J. Kuchenbecker, Ph.D. General Robotics, Automation, Sensing, and Perception Lab (GRASP) MEAM Department, SEAS, University of Pennsylvania Lecture 12: October
More informationAE/ME 339. K. M. Isaac Professor of Aerospace Engineering. December 21, 2001 topic13_grid_generation 1
AE/ME 339 Professor of Aerospace Engineering December 21, 2001 topic13_grid_generation 1 The basic idea behind grid generation is the creation of the transformation laws between the phsical space and the
More informationANALYTICAL GEOMETRY Revision of Grade 10 Analytical Geometry
ANALYTICAL GEOMETRY Revision of Grade 10 Analtical Geometr Let s quickl have a look at the analtical geometr ou learnt in Grade 10. 8 LESSON Midpoint formula (_ + 1 ;_ + 1 The midpoint formula is used
More informationI xx + I yy + I zz = (y 2 + z 2 )dm + (x 2 + y 2 )dm. (x 2 + z 2 )dm + (x 2 + y 2 + z 2 )dm = 2
9196_1_s1_p095-0987 6/8/09 1:09 PM Page 95 010 Pearson Education, Inc., Upper Saddle River, NJ. ll rights reserved. This material is protected under all copright laws as the currentl 1 1. Show that the
More informationMiscellaneous (dimension, angle, etc.) - black [pencil] Use different colors in diagrams. Body outline - blue [black] Vector
1. Sstems of orces & s 2142111 Statics, 2011/2 Department of Mechanical Engineering, Chulalongkorn Uniersit bjecties Students must be able to Course bjectie Analze a sstem of forces and moments Chapter
More informationME451 Kinematics and Dynamics of Machine Systems
ME451 Kinematics and Dynamics of Machine Systems Cam-Follower Constraints 3.3 Driving Constraints 3.5 October 11, 2011 Dan Negrut, 2011 ME451, UW-Madison "Computers are useless. They can only give you
More informationAPPLIED MECHANICS I Resultant of Concurrent Forces Consider a body acted upon by co-planar forces as shown in Fig 1.1(a).
PPLIED MECHNICS I 1. Introduction to Mechanics Mechanics is a science that describes and predicts the conditions of rest or motion of bodies under the action of forces. It is divided into three parts 1.
More informationDynamics of multiple pendula without gravity
Chaotic Modeling and Simulation (CMSIM) 1: 57 67, 014 Dnamics of multiple pendula without gravit Wojciech Szumiński Institute of Phsics, Universit of Zielona Góra, Poland (E-mail: uz88szuminski@gmail.com)
More informationRigid and Braced Frames
RH 331 Note Set 12.1 F2014abn Rigid and raced Frames Notation: E = modulus of elasticit or Young s modulus F = force component in the direction F = force component in the direction FD = free bod diagram
More information11. Prove that the Missing Strip Plane is an. 12. Prove the above proposition.
10 Pasch Geometries Definition (Pasch s Postulate (PP)) A metric geometry satisfies Pasch s Postulate (PP) if for any line l, any triangle ABC, and any point D l such that A D B, then either l AC or l
More informationErrata for Robot Vision
Errata for Robot Vision This is a list of known nontrivial bugs in Robot Vision 1986 by B.K.P. Horn, MIT Press, Cambridge, MA ISBN 0-262-08159-8 and McGraw-Hill, New York, NY ISBN 0-07-030349-5. If you
More informationDYNAMICS OF MACHINERY 41514
DYNAMICS OF MACHINERY 454 PROJECT : Theoretical and Experimental Modal Analysis and Validation of Mathematical Models in Multibody Dynamics Holistic Overview of the Project Steps & Their Conceptual Links
More informationSRSD 2093: Engineering Mechanics 2SRRI SECTION 19 ROOM 7, LEVEL 14, MENARA RAZAK
SRSD 2093: Engineering Mechanics 2SRRI SECTION 19 ROOM 7, LEVEL 14, MENARA RAZAK SIMPLE TRUSSES, THE METHOD OF JOINTS, & ZERO-FORCE MEMBERS Today s Objectives: Students will be able to: a) Define a simple
More informationChapter 5 Equilibrium of a Rigid Body Objectives
Chapter 5 Equilibrium of a Rigid Bod Objectives Develop the equations of equilibrium for a rigid bod Concept of the free-bod diagram for a rigid bod Solve rigid-bod equilibrium problems using the equations
More informationIdentifying second degree equations
Chapter 7 Identifing second degree equations 71 The eigenvalue method In this section we appl eigenvalue methods to determine the geometrical nature of the second degree equation a 2 + 2h + b 2 + 2g +
More informationMidterm 1 revision source for MATH 227, Introduction to Linear Algebra
Midterm revision source for MATH 227, Introduction to Linear Algebra 5 March 29, LJB page 2: Some notes on the Pearson correlation coefficient page 3: Practice Midterm Exam page 4: Spring 27 Midterm page
More informationWarner, R. M. (2008). Applied Statistics: From bivariate through multivariate techniques. Thousand Oaks: Sage.
Errata for Warner, R. M. (2008). Applied Statistics: From bivariate through multivariate techniques. Thousand Oaks: Sage. Most recent update: March 4, 2009 Please send information about any errors in the
More informationExample: Inverted pendulum on cart
Chapter 11 Eample: Inverted pendulum on cart The figure to the right shows a rigid body attached by an frictionless pin (revolute) joint to a cart (modeled as a particle). Thecart slides on a horizontal
More informationTENSOR TRANSFORMATION OF STRESSES
GG303 Lecture 18 9/4/01 1 TENSOR TRANSFORMATION OF STRESSES Transformation of stresses between planes of arbitrar orientation In the 2-D eample of lecture 16, the normal and shear stresses (tractions)
More informationErrata list for An Introduction to Modern Astrophysics, c2007 Second Edition (second printing or later) February 23, 2010
Errata list for An Introduction to Modern Astrophysics, c2007 Second Edition (second printing or later) February 23, 2010 To determine the printing of your text, look on page ii (the page following the
More informationROBOTICS Laboratory Problem 02
ROBOTICS 2015-2016 Laboratory Problem 02 Basilio Bona DAUIN PoliTo Problem formulation The planar system illustrated in Figure 1 consists of a cart C sliding with or without friction along the horizontal
More informationCh. 5: Jacobian. 5.1 Introduction
5.1 Introduction relationship between the end effector velocity and the joint rates differentiate the kinematic relationships to obtain the velocity relationship Jacobian matrix closely related to the
More information6.2 Truss - Two Dimensions
6.2 Truss - Two Dimensions Trusses make it easy to carry heavy loads. A bridge over the river, roof over your house, the giant crane used in construction or unloading heavy cargo from a ship are some of
More informationSTATICS. Equivalent Systems of Forces. Vector Mechanics for Engineers: Statics VECTOR MECHANICS FOR ENGINEERS: Contents & Objectives.
3 Rigid CHATER VECTOR ECHANICS FOR ENGINEERS: STATICS Ferdinand. Beer E. Russell Johnston, Jr. Lecture Notes: J. Walt Oler Teas Tech Universit Bodies: Equivalent Sstems of Forces Contents & Objectives
More informationME451 Kinematics and Dynamics of Machine Systems
ME451 Kinematics and Dynamics of Machine Systems Introduction to Dynamics 6.1 October 30, 2014 Dan Negrut ME451, Fall 2014 University of Wisconsin-Madison Quote of the day: Computer science education cannot
More informationEngineering Mathematics 2018 : MA6151
Engineering Mathematics 08 NAME OF THE SUBJECT : Mathematics I SUBJECT CODE : MA65 NAME OF THE METERIAL : Part A questions REGULATION : R 03 WEBSITE : wwwhariganeshcom UPDATED ON : November 07 TEXT BOOK
More information2D Geometric Transformations. (Chapter 5 in FVD)
2D Geometric Transformations (Chapter 5 in FVD) 2D geometric transformation Translation Scaling Rotation Shear Matri notation Compositions Homogeneous coordinates 2 2D Geometric Transformations Question:
More informationAtomic Physics: an exploration through problems and solutions (2nd edition)
Atomic Physics: an exploration through problems and solutions (2nd edition) We would be greatly indebted to our readers for informing us of errors and misprints in the book by sending an e-mail to: budker@berkeley.edu.
More informationModeling and Solving Constraints. Erin Catto Blizzard Entertainment
Modeling and Solving Constraints Erin Catto Blizzard Entertainment Basic Idea Constraints are used to simulate joints, contact, and collision. We need to solve the constraints to stack boxes and to keep
More informationSIMPLE TRUSSES, THE METHOD OF JOINTS, & ZERO-FORCE MEMBERS
SIMPLE TRUSSES, THE METHOD OF JOINTS, & ZERO-FORCE MEMBERS Today s Objectives: Students will be able to: a) Define a simple truss. b) Determine the forces in members of a simple truss. c) Identify zero-force
More information1.1 The Equations of Motion
1.1 The Equations of Motion In Book I, balance of forces and moments acting on an component was enforced in order to ensure that the component was in equilibrium. Here, allowance is made for stresses which
More informationMatrix Arithmetic. a 11 a. A + B = + a m1 a mn. + b. a 11 + b 11 a 1n + b 1n = a m1. b m1 b mn. and scalar multiplication for matrices via.
Matrix Arithmetic There is an arithmetic for matrices that can be viewed as extending the arithmetic we have developed for vectors to the more general setting of rectangular arrays: if A and B are m n
More informationErrata for Amacher, Ollikainen, and Koskela, Economics of Forest Resources, The MIT Press, 2009
Errata for Amacher, Ollikainen, and Koskela, Economics of Forest Resources, he MI Press, 9 Chapters 6, 8, his will be a continuously evolving document Please send queries to either Greg Amacher (gamacher@vtedu
More information3. ANALYTICAL KINEMATICS
In planar mechanisms, kinematic analysis can be performed either analytically or graphically In this course we first discuss analytical kinematic analysis nalytical kinematics is based on projecting the
More informationAnalog Circuit Design Discrete & Integrated
This document contains the Errata for the textbook Analog Circuit Design Discrete & Integrated The Hardcover Edition (shown below at the left and published by McGraw-Hill Education) was preceded by a Spiral-Bound
More informationDynamics and control of mechanical systems
JU 18/HL Dnamics and control of mechanical sstems Date Da 1 (3/5) 5/5 Da (7/5) Da 3 (9/5) Da 4 (11/5) Da 5 (14/5) Da 6 (16/5) Content Revie of the basics of mechanics. Kinematics of rigid bodies coordinate
More informationIdentification of muscle forces in human lower limbs during sagittal plane movements Part I: Human body modelling
Acta of ioenineerin and iomechanics Vol. No. 00 Identification of muscle forces in human lower limbs durin saittal plane movements Part I: uman bod modellin WOJCIEC LAJER KRZYSZOF DZIEWIECKI ZENON MAZUR
More informationx 1 To help us here we invoke MacLaurin, 1 + t = 1 + t/2 + O(t 2 ) for small t, and write
On the Deormation o an Elastic Fiber We consider the case illustrated in Figure. The bold solid line is a iber in its reerence state. When we subject its two ends to the two orces, (, ) and (, ) the respective
More informationCHAPTER 8: Matrices and Determinants
(Exercises for Chapter 8: Matrices and Determinants) E.8.1 CHAPTER 8: Matrices and Determinants (A) means refer to Part A, (B) means refer to Part B, etc. Most of these exercises can be done without a
More informationStatics and Strength of Materials For Architecture and Building Construction
Insstructor s Manual to accompan Statics and Strength of Materials For rchitecture and Building Construction Fourth Edition Barr S. Onoue Upper Saddle River, New Jerse Columbus, Ohio Copright 2012 b Pearson
More informationA MULTI-BODY ALGORITHM FOR WAVE ENERGY CONVERTERS EMPLOYING NONLINEAR JOINT REPRESENTATION
Proceedings of the ASME 2014 33rd International Conference on Ocean, Offshore and Arctic Engineering OMAE2014 June 8-13, 2014, San Francisco, California, USA OMAE2014-23864 A MULTI-BODY ALGORITHM FOR WAVE
More informationhwhat is mechanics? hscalars and vectors hforces are vectors htransmissibility of forces hresolution of colinear forces hmoments and couples
orces and Moments CIEG-125 Introduction to Civil Engineering all 2005 Lecture 3 Outline hwhat is mechanics? hscalars and vectors horces are vectors htransmissibilit of forces hresolution of colinear forces
More informationPlane Trusses Trusses
TRUSSES Plane Trusses Trusses- It is a system of uniform bars or members (of various circular section, angle section, channel section etc.) joined together at their ends by riveting or welding and constructed
More informationMedical Imaging Signals and Systems Jerry L. Prince and Jonathan M. Links Upper Saddle River, NJ: Pearson Prentice Hall, 2006
i Medical Imaging Signals and Systems Jerry L. Prince and Jonathan M. Links Upper Saddle River, NJ: Pearson Prentice Hall, 2006 Errata, Version 1.02, August 8, 2006 This errata applies to the first printing
More informationME 101: Engineering Mechanics
ME 0: Engineering Mechanics Rajib Kumar Bhattacharja Department of Civil Engineering ndian nstitute of Technolog Guwahati M Block : Room No 005 : Tel: 8 www.iitg.ernet.in/rkbc Area Moments of nertia Parallel
More information5. Nonholonomic constraint Mechanics of Manipulation
5. Nonholonomic constraint Mechanics of Manipulation Matt Mason matt.mason@cs.cmu.edu http://www.cs.cmu.edu/~mason Carnegie Mellon Lecture 5. Mechanics of Manipulation p.1 Lecture 5. Nonholonomic constraint.
More informationApproach based on Cartesian coordinates
GraSMech course 2005-2006 Computer-aided analysis of rigid and flexible multibody systems Approach based on Cartesian coordinates Prof. O. Verlinden Faculté polytechnique de Mons Olivier.Verlinden@fpms.ac.be
More informationEngineering Dynamics: A Comprehensive Introduction Errata. N. Jeremy Kasdin & Derek A. Paley
Engineering Dynamics: A Comprehensive Introduction Errata N. Jeremy Kasdin & Derek A. Paley Last updated November 10, 2017 PRINCETON UNIVERSITY PRESS PRINCETON AND OXFORD Chapter 2: i) [First printing
More informationMath Theory of Number Homework 1
Math 4050 Theory of Number Homework 1 Due Wednesday, 015-09-09, in class Do 5 of the following 7 problems. Please only attempt 5 because I will only grade 5. 1. Find all rational numbers and y satisfying
More informationIntroduction to Mechanics Vectors in 2 Dimensions
Introduction to Mechanics Vectors in 2 Dimensions Lana heridan De Anza College Jan 29, 2018 Last time inertia freel falling objects acceleration due to gravit verview vectors in 2 dimensions some trigonometr
More informationME5286 Robotics Spring 2017 Quiz 2
Page 1 of 5 ME5286 Robotics Spring 2017 Quiz 2 Total Points: 30 You are responsible for following these instructions. Please take a minute and read them completely. 1. Put your name on this page, any other
More informationPROBLEMS In each of Problems 1 through 12:
6.5 Impulse Functions 33 which is the formal solution of the given problem. It is also possible to write y in the form 0, t < 5, y = 5 e (t 5/ sin 5 (t 5, t 5. ( The graph of Eq. ( is shown in Figure 6.5.3.
More informationMATHEMATICS. r Statement I Statement II p q ~p ~q ~p q q p ~(p ~q) F F T T F F T F T T F T T F T F F T T T F T T F F F T T
MATHEMATICS Directions : Questions number to 5 are Assertion-Reason type questions. Each of these questions contains two statements : Statement- (Assertion) and Statement- (Reason). Each of these questions
More informationwe must pay attention to the role of the coordinate system w.r.t. which we perform a tform
linear SO... we will want to represent the geometr of points in space we will often want to perform (rigid) transformations to these objects to position them translate rotate or move them in an animation
More informationErrata for Gravity: An Introduction to Einstein s General Relativity, Printings 1-3, B: typos, etc.
Errata for Gravity: An Introduction to Einstein s General Relativity, Printings 1-3, B: typos, etc. Updated 11/18/2004 The errata that were not corrected in the in the first three printings have been divided
More informationErrata for Robot Vision
Errata for Robot Vision This is a list of known nontrivial bugs in Robot Vision 1986) by B.K.P. Horn, MIT Press, Cambridge, MA ISBN 0-6-08159-8 and McGraw-Hill, New York, NY ISBN 0-07-030349-5. Thanks
More informationPage Points Score Total: 100
Math 1130 Spring 2019 Sample Midterm 3c 4/11/19 Name (Print): Username.#: Lecturer: Rec. Instructor: Rec. Time: This exam contains 10 pages (including this cover page) and 10 problems. Check to see if
More informationErrata for Robot Vision
Errata for Robot Vision This is a list of known nontrivial bugs in Robot Vision 1986) by B.K.P. Horn, MIT Press, Cambridge, MA ISBN 0-6-08159-8 and McGraw-Hill, New York, NY ISBN 0-07-030349-5. If you
More informationME751 Advanced Computational Multibody Dynamics
ME751 Advanced Computational Multibody Dynamics Review: Elements of Linear Algebra & Calculus September 9, 2016 Dan Negrut University of Wisconsin-Madison Quote of the day If you can't convince them, confuse
More informationERRATA MATHEMATICS FOR THE INTERNATIONAL STUDENT MATHEMATICS HL (CORE) (2nd edition)
ERRATA MATHEMATICS FOR THE INTERNATIONAL STUDENT MATHEMATICS HL (CORE) (nd edition) Second edition - 010 reprint page 95 TEXT last paragraph on the page should read: e is a special number in mathematics.
More informationRobotics I. Test November 29, 2013
Exercise 1 [6 points] Robotics I Test November 9, 013 A DC motor is used to actuate a single robot link that rotates in the horizontal plane around a joint axis passing through its base. The motor is connected
More informationIntroduction to 3D Game Programming with DirectX 9.0c: A Shader Approach
Introduction to 3D Game Programming with DirectX 90c: A Shader Approach Part I Solutions Note : Please email to frank@moon-labscom if ou find an errors Note : Use onl after ou have tried, and struggled
More informationCartesian Coordinates, Points, and Transformations
Cartesian Coordinates, Points, and Transformations CIS - 600.445 Russell Taylor Acknowledgment: I would like to thank Ms. Sarah Graham for providing some of the material in this presentation Femur Planned
More informationEquilibrium Equilibrium and Trusses Trusses
Equilibrium and Trusses ENGR 221 February 17, 2003 Lecture Goals 6-4 Equilibrium in Three Dimensions 7-1 Introduction to Trusses 7-2Plane Trusses 7-3 Space Trusses 7-4 Frames and Machines Equilibrium Problem
More informationICS 6N Computational Linear Algebra Matrix Algebra
ICS 6N Computational Linear Algebra Matrix Algebra Xiaohui Xie University of California, Irvine xhx@uci.edu February 2, 2017 Xiaohui Xie (UCI) ICS 6N February 2, 2017 1 / 24 Matrix Consider an m n matrix
More information