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Problem 1: Greens Functions In class on Wednesday we found that we could solve the position, r(t), of a mass and spring when an arbitrary force is applied using Greens Functions, r(t)= | G(t,T)f(r)dr and that the particular Greens Function for this case is Gu.T)--sin ) wo where w, h/m and Θ(p) is a step function at p = 0. A: Find the position of the mass as a function of time if a force fo is applied for a short time Δι << T where T is the period of the mass-spring system. 2π Check that your answer has sensible physical units B Imagine the force on a mass spring system is 0, then is constant for the ime of one natural period, and then is 0 again.0 Otherwise. Find (t) for all time. Is it what you expected?

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Answer #1

The position is given by
x(t)=int G(t, au)f( au)~d au
where, the Green's function is given by
G(t, au)=rac{1}{omega_0}Theta(t- au)sin(omega_0(t- au))

A)

Now for
f(r) = fo, for 0 < τ < M where. Δt << T
we get
  r(t)-:/ ef (rje (t-r)sin(o(t_r)) dr
zitー:/ar(r) sini! (t-r)) dr
fo wo o sin(wo(t -T)) dT
t) = for sin(uo(t-At)) r(

B)

And for
f(r)-,fo, for 0 < T <T 0, otherwise
where,
omega_0 T = 2pi .
So, we get
  
  zitー:/ar(r) sini! (t-r)) dr
  fo wo o r(t)-- sin(wo(t - T)) dT
Rightarrow x(t)=rac{f_0}{omega_0}int_{0}^{T} ig[sinomega_0 t cosomega_0 au -cosomega_0 t sinomega_0 auig]~d au
Rightarrow x(t)=rac{f_0}{omega_0} ig[sinomega_0 t int_{0}^{T}cosomega_0 au~d au -cosomega_0 t int_{0}^{T}sinomega_0 au~d auig]
We now use the result
int_{0}^{T}cosomega_0 au~d au =int_{0}^{T}sinomega_0 au~d au=0
So, we get
  (t)0

This is the averaged value.
  
  

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