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Lab Room | Theory Map | Forced Vibration | Forced Vibration Equation Solution

Forced Vibration Equation Solution

Presented here is the solution to the second order differential equation that governs the behavior of the forced vibration mode of our apparatus.

If there is a periodic forcing function [F(t) = A sin t], the beam will experience a forced vibration response, or periodic response.

This is modelled by:

(1)     

It can be shown that the steady state solution for an underdamped system is given by:

(2)     

where:
D is the amplitude of the response and
is the phase response (shift).

The amplitude response, D, can be written as:

(3)     

The phase response (shift), , is given by:

(5)     
where
is the ratio of the forcing frequency to the phase shift.

This ratio is defined as:

(6)     

The response of the spring-mass-dashpot system to an instantaneously applied forcing function includes both a transient adjustment to the forcing function plus a steady-state response. When taking data, be sure to sample for a long enough time to allow the transient response to approach zero.


Last Updated: January 16, 2000, beam@bits.me.berkeley.edu
Copyright © 1993-1995, 2000, Pamela A. Eibeck and Brandon Muramatsu
Original WWW Conversion by Winston Wang, 1994
WWW ReConversion by Brandon Muramtasu, 2000