Prepared by Dr. Hassan Fadag.

Slides:



Advertisements
Similar presentations
Mechanics of Rigid Body. C
Advertisements

Physics 111: Mechanics Lecture 5
Kinetics of Particles Impulse and Momentum.
Work & Energy Principles
Kinematics of Particles
Force Scenario Solutions
MAE 242 Dynamics – Section I Dr. Kostas Sierros. Problem 1.
Relative Motion & Constrained Motion
ABSOLUTE DEPENDENT MOTION ANALYSIS OF TWO PARTICLES (Section 12.9)
ABSOLUTE DEPENDENT MOTION ANALYSIS OF TWO PARTICLES
RIGID BODY MOTION: TRANSLATION & ROTATION (Sections )
PLANAR RIGID BODY MOTION: TRANSLATION & ROTATION
RIGID BODY MOTION: TRANSLATION & ROTATION (Sections )
RIGID BODY MOTION: TRANSLATION & ROTATION
Kinematics of Particles
KINETICS of PARTICLES Newton’s 2nd Law & The Equation of Motion
KINETICS of PARTICLES Newton’s 2nd Law & The Equation of Motion
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 7.
Normal-Tangential coordinates
Normal-Tangential coordinates
ENGR 215 ~ Dynamics Sections 16.4
Prepared by Dr. Hassan Fadag.
KINEMATICS OF PARTICLES PLANE CURVILINEAR MOTION
MAE 242 Dynamics – Section I Dr. Kostas Sierros. Problem.
MAE 242 Dynamics – Section I Dr. Kostas Sierros.
Newton’s Laws (cont…) Blocks, ramps, pulleys and other problems
ABSOLUTE DEPENDENT MOTION ANALYSIS OF TWO PARTICLES Today’s Objectives: Students will be able to: 1.Relate the positions, velocities, and accelerations.
ENGR 214 Chapter 15 Kinematics of Rigid Bodies
Projectiles Horizontal Projection Horizontally: Vertically: Vertical acceleration g  9.8 To investigate the motion of a projectile, its horizontal and.
ABSOLUTE DEPENDENT MOTION ANALYSIS OF TWO PARTICLES Today’s Objectives: Students will be able to: 1.Relate the positions, velocities, and accelerations.
MOTION RELATIVE TO ROTATING AXES
PLANAR KINEMATICS OF A RIGID BODY
11.3 Principle of Virtual Work for a System of Connected Rigid Bodies Method of virtual work most suited for solving equilibrium problems involving a system.
ABSOLUTE DEPENDENT MOTION ANALYSIS OF TWO PARTICLES
Kinematics of Particles Lecture II. Subjects Covered in Kinematics of Particles Rectilinear motion Curvilinear motion Rectangular coords n-t coords Polar.
DYNAMICS VECTOR MECHANICS FOR ENGINEERS: DYNAMICS Tenth Edition Ferdinand P. Beer E. Russell Johnston, Jr. Phillip J. Cornwell Lecture Notes: Brian P.
1 Applying Newton’s Laws Assumptions Assumptions Objects behave as particles Objects behave as particles can ignore rotational motion (for now) can ignore.
KINEMATICS OF PARTICLES
Apply the three equations of motion for a rigid body in planar motion. Analyze problems involving translational motion. PLANAR KINETIC EQUATIONS OF MOTION:
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lectures 16, 17, 18.
KINEMATICS OF PARTICLES RELATIVE MOTION WITH RESPECT TO TRANSLATING AXES.
Work & Energy Principles
Plane Dynamics of Rigid Bodies
Objectives: Write the equation of motion for an accelerating body.
Normal-Tangential coordinates
ABSOLUTE DEPENDENT MOTION ANALYSIS OF TWO PARTICLES
Work & Energy Principles
KINETICS of PARTICLES Newton’s 2nd Law & The Equation of Motion
Instructor: Dr. Tatiana Erukhimova
PRINCIPLE OF LINEAR IMPULSE AND MOMENTUM
University Physics: Mechanics
RIGID BODY MOTION: TRANSLATION & ROTATION (Sections )
Problem In the position shown, collar B moves A
POWER AND EFFICIENCY Today’s Objectives: Students will be able to:
ABSOLUTE DEPENDENT MOTION ANALYSIS OF TWO PARTICLES
PRINCIPLE OF LINEAR IMPULSE AND MOMENTUM
Conceptual Dynamics Part II: Kinematics of Particles Chapter 3
FRICTION.
RIGID BODY MOTION: TRANSLATION & ROTATION (Sections )
Kinematics of Particles
FRICTION.
ABSOLUTE DEPENDENT MOTION ANALYSIS OF TWO PARTICLES
Friction.
University Physics: Mechanics
FRICTION.
Chapter 14 : Kinematics Of A Particle – Work and Energy
A block of mass m resting on a horizontal
PRINCIPLE OF LINEAR IMPULSE AND MOMENTUM
Simple Lifting Machines
King Fahd University of Petroleum & Minerals
Presentation transcript:

Prepared by Dr. Hassan Fadag. Lecture III Dependent Motion

Prepared by Dr. Hassan Fadag. Dependent Motion Here, motions of more than one particle are interrelated because of the constraints imposed by the interconnecting members. In such problems, it is necessary to account for these constraints in order to determine the respective motions of the particles.

Dependent Motion (Cont.) Prepared by Dr. Hassan Fadag. Dependent Motion (Cont.) + Datum + One Degree of Freedom System Notes: Horizontal motion of A is twice the vertical motion of B. The motion of B is the same as that of the center of its pulley, so we establish position coordinates x and y measured from a convenient fixed datum. The system is one degree of freedom, since only one variable, either x or y, is needed to specify the positions of all parts of the system. L, r1, r2, and b are constants Differentiating once and twice gives:

Dependent Motion (Cont.) Prepared by Dr. Hassan Fadag. Dependent Motion (Cont.) Datum Datum + + + + Two Degree of Freedom System Note: The positions of the lower pulley C depend on the separate specifications of the two coordinates yA & yB. It is impossible for the signs of all three terms to be +ve simultaneously. Differentiating once gives: Differentiating once gives: Eliminating the terms in gives:

Dependent Motion Exercises Prepared by Dr. Hassan Fadag. Dependent Motion Exercises

Exercise # 1 Determine the speed of block A if block B has an upward speed of 2 m/s.

Exercise # 2 The crate is being lifted up the inclined plane using the motor M and the rope and pulley arrangement shown. Determine the speed at which the cable must be taken up by the motor in order to move the crate up the plane with a constant speed of 1.2 m/s.

Exercise # 3 Determine the constraint equation which relates the accelerations of bodies A and B. Assume that the upper surface of A remains horizontal.

Exercise # 4 The power winches on the industrial scaffold enable it to be raised or lowered. For rotation in the senses indicated, the scaffold is being raised. If each drum has a diameter of 200 mm and turns at the rate of 40 rev/min. determine the upward velocity v of the scaffold.

Exercise # 5 Block C starts from rest and moves down with a constant acceleration. Knowing that after block A has moved 0.5 m its velocity is 0.2 m/s, determine (a) the accelerations of A and C, (b) the velocity and the change in position of block B after 2 s.

Exercise # 6 The crate C is being lifted by moving the roller at A downward with a constant speed of v = 2 m/s along the guide. Determine the velocity and acceleration of the crate at the instant s = 1 m. When the roller is at B, the crate rests on the ground. Neglect the size of the pulley in the calculation. Hint: Relate the coordinates xC and xA using the problem geometry, then take the first and second time derivatives.