Lecture 9 Time Domain Vibration Flashcards

1
Q

What does force generally do in real life

A

vary with time

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2
Q

What are the four methods for predicting time domain forced response

A

analytical methods - trail solution and laplace transform

Time domain Numerical Methods - Convolution Integral and Time Marching calculations

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3
Q

Where is the convolution integral applied

A

linear systems,

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4
Q

issues with convolution integral

A

analytical form can be cumbersome

discrete form very useful

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5
Q

what does the convolution integral do

A

break arbitrary force history up into many impulse measures
calculate impulse response
sum up responses to individual impulses

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6
Q

What does an impulse reponse look like

A

initial motion follow by free vibration

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7
Q

For a unit impulse the chance in velocity is

A

x.t1 - x.t0 = 1/m

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8
Q

initial conditions for free vibrations after impulse is applied

A
x(t=0) = 0 insufficient time to move
x.(t=0) = 1/m from unit impulse chance in velocity when DETLA T is small
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9
Q

equation of all impulse response

A

x(t) = Sum from 0 to t, f(tau)h(t-tau)DELTAtau

where tau is time shifted to allow initial momentum change

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10
Q

derive convolution integral from x(t) = Sum from 0 to t, f(tau)h(t-tau)DELTAtau

A

DETLAtau -> 0 becomes integral 0 to t of f(tau)h(t-tau) dtau
substitute theta = t - tau
x(t) = integral from - inf to t of f(t-theta)
h(theta)*dtheta

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11
Q

Fourier transform of the impulse response

A

H(w) = integral -inf to +inf of h(t) exp(-jwt) dt

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12
Q

impulse reponse from steady state freq response

A

h(t) = 1/2Pi() * integral from -inf to + inf H(w)*exp(jwt)dw

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