At a given instant the body of mass m has an angular velocity V and its mass center has a velocity vG. Show that its kinetic energy can be represented as T = 1 2 IICv2 , where IIC is the moment of inertia of the body determined about the instantaneous axis of zero velocity, located a distance rG>IC from the mass center as shown.
Read moreTable of Contents
1
General Principles
2
Force Vectors
3
Equilibrium of a Particle
4
Force System Resultants
5
Equilibrium of a Rigid Body
6
Structural Analysis
7
Internal Forces
8
Friction
9
Center of Gravity and Centroid
10
Moments of Inertia
11
Virtual Work
12
Kinematics of a Particle
13
Kinetics of a Particle: Force and Acceleration
14
Kinetics of a Particle: Work and Energy
15
Kinetics of a Particle: Impulse and Momentum
16
Planar Kinematics of a Rigid Body
17
Planar Kinematics of a Rigid Body: Force and Acceleration
18
Planar Kinetics of a Rigid Body: Work and Energy
19
Planar Kinetics of a Rigid Body: Impulse and Momentum
20
Three-dimensional Kinematics of a Rigid Body
21
Three-dimensional Kinetics of a Rigid Body
22
Vibrations
Textbook Solutions for Engineering Mechanics: Statics & Dynamics
Chapter 18 Problem 18-15
Question
The pendulum consists of a 10-kg uniform disk and a 3-kg uniform slender rod. If it is released from rest in the position shown, determine its angular velocity when it rotates clockwise 90.
Solution
The first step in solving 18 problem number 15 trying to solve the problem we have to refer to the textbook question: The pendulum consists of a 10-kg uniform disk and a 3-kg uniform slender rod. If it is released from rest in the position shown, determine its angular velocity when it rotates clockwise 90.
From the textbook chapter Planar Kinetics of a Rigid Body: Work and Energy you will find a few key concepts needed to solve this.
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full solution
full solution
Title
Engineering Mechanics: Statics & Dynamics 14
Author
Russell C. Hibbeler
ISBN
9780133951929