King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 28.

Slides:



Advertisements
Similar presentations
Kinematics of Rigid Bodies
Advertisements

Chapter 15 KINEMATICS OF RIGID BODIES
Kinematics of Particles
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 9.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 3.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 25.
ME Robotics Dynamics of Robot Manipulators Purpose: This chapter introduces the dynamics of mechanisms. A robot can be treated as a set of linked.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 40.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 7.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 16.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 27.
King Fahd University of Petroleum & Minerals
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 21.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 6.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 39.
Mechanics of rigid body StaticsDynamics Equilibrium Galilei Newton Lagrange Euler KinematicsKinetics v=ds/dt a=dv/dt Σ F = 0 Σ F = m a mechanics of rigid.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 32.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 8.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 17.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 20.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 38.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 16.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 29.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 27.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 11.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 35.
Kinematics of Rigid Bodies
RELATIVE MOTION ANALYSIS: ACCELERATION
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 13.
Objective Rectangular Components Normal and Tangential Components
Copyright Kaplan AEC Education, 2005 Dynamics Outline Overview DYNAMICS, p. 193 KINEMATICS OF A PARTICLE, p. 194 Relating Distance, Velocity and the Tangential.
ESC020: Rigid Body Mechanics
King Fahd University of Petroleum & Minerals
MAE 242 Dynamics – Section I Dr. Kostas Sierros.
INTRODUCTION TO DYNAMICS ANALYSIS OF ROBOTS (Part 3)
5.Kinematics of Particles
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 5.
Rotational Motion Comparison of Angular Motion with One-dimensional Horizontal Motion Distance traveled is replaced by the angle traveled around the circle.
MOTION RELATIVE TO ROTATING AXES
MAE 242 Dynamics – Section I Dr. Kostas Sierros. Problem 1.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 30.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 18.
DYNAMICS CONTENTS.
CHAPTER 11 Kinematics of Particles INTRODUCTION TO DYNAMICS Galileo and Newton (Galileo’s experiments led to Newton’s laws) Galileo and Newton (Galileo’s.
Static Equilibrium Physics 150/250 Center of Mass Types of Motion
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 21.
THREE-DIMENSIONAL KINEMATICS OF RIGID BODIES
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 15.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 10.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 37.
VECTOR MECHANICS FOR ENGINEERS: DYNAMICS Seventh Edition Ferdinand P. Beer E. Russell Johnston, Jr. Lecture Notes: J. Walt Oler Texas Tech University CHAPTER.
Acceleration Analysis
Vector-Valued Functions and Motion in Space
KINEMATICS OF RIGID BODY
King Fahd University of Petroleum & Minerals
King Fahd University of Petroleum & Minerals
King Fahd University of Petroleum & Minerals
King Fahd University of Petroleum & Minerals
King Fahd University of Petroleum & Minerals
King Fahd University of Petroleum & Minerals
King Fahd University of Petroleum & Minerals
King Fahd University of Petroleum & Minerals
King Fahd University of Petroleum & Minerals
King Fahd University of Petroleum & Minerals
King Fahd University of Petroleum & Minerals
King Fahd University of Petroleum & Minerals
King Fahd University of Petroleum & Minerals
King Fahd University of Petroleum & Minerals
King Fahd University of Petroleum & Minerals
Presentation transcript:

King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 28

Examples of relative motions “ motion of one part lead to the motion of other parts ” (pin-connected rigid body)

Relative-Motion Analysis : Relative Velocity Relative Acceleration Instantaneous Center of Zero Velocity

Examples of Non-Relative-Motions )sliding connections and has two independent motion)

Position Rotating axes

Velocity Rotating axes & translating object  r + v

Velocity V C = Velocity of the Collar, measured from the X, Y, Z reference V O = Velocity of the origin O of the x,y,z reference measured from the X,Y,Z reference (V C/O ) xyz = relative velocity of “ C with respect to O ” observer attached to the rotating x,y,z reference  = angular velocity of the x,y,z reference, measured from the X,Y,Z reference r C/O = relative position of “ C with respect to O ”

Acceleration Acceleration is the time derivative of velocity Rotating axes & translating object  r + v)

Rotating axes & translating object  r + v)  r Tangential acceleration  2 r Normal acceleration Coriolis acceleration Acceleration of the object Acceleration of origin

Coriolis acceleration Whenever a point is moving on a path and the path is rotating, there is an extra component of the acceleration due to coupling between the motion of the point on the path and the rotation of the path. This component is called Coriolis acceleration. First measured by the French engineer G.C. Coriolis Important in studying the effect “ force and acceleration ” of earth rotation on the rockets and long-range projectiles

Recall cylindrical coordinate Compare ! Rearrange

Recall – Cylindrical coordinate Coriolis acceleration

Example 16-20a C/D = ?  DE = ?  DE = ?