Top Banner
Vibrations Free Forced Undamped Damped Undamped Damped
12
Welcome message from author
This document is posted to help you gain knowledge. Please leave a comment to let me know what you think about it! Share it to your friends and learn new things together.
Transcript
Page 1: Vibrations FreeForced UndampedDampedUndampedDamped.

Vibrations

Free Forced

Undamped Damped Undamped Damped

Page 2: Vibrations FreeForced UndampedDampedUndampedDamped.

Transient Vibrations of

Single Degree of Freedom Systems

Single Degree of Freedom System with an applied force f(t):

where f(t) can be of any form.

Page 3: Vibrations FreeForced UndampedDampedUndampedDamped.

Equation of Motion:

Solution:

Page 4: Vibrations FreeForced UndampedDampedUndampedDamped.

Solution for a General Force F(t):

Page 5: Vibrations FreeForced UndampedDampedUndampedDamped.

Example:

Page 6: Vibrations FreeForced UndampedDampedUndampedDamped.
Page 7: Vibrations FreeForced UndampedDampedUndampedDamped.

Excitations Changing at Discrete Times:

A step force f(t) starting at t = 0:

Page 8: Vibrations FreeForced UndampedDampedUndampedDamped.

A step force f(t) starting at t = t0:

In general, we have the convolution integral:

Page 9: Vibrations FreeForced UndampedDampedUndampedDamped.

Some Excitations Given in Figure 4.5:

Page 10: Vibrations FreeForced UndampedDampedUndampedDamped.

Response of an Undamped Single-Degree-of-Freedom System:

Page 11: Vibrations FreeForced UndampedDampedUndampedDamped.

Transient Motion due to Base Excitation:

x: Displacement of system

y: Displacement of base

Equation of Motion :

Defining z = x y, we get

Or,

Page 12: Vibrations FreeForced UndampedDampedUndampedDamped.

Solution with Convolution Integral :