The motion of an overdamped harmonic oscillator subject to an impulsive force is described by the equation x^(¨)+2gamma x^(˙)+p^(2)x=delta (t) for a function x(t) and constants gamma >p>0. Given that x=0 for t<0, show by Fourier transform methods that for t>0
x(t)=(e^(-gamma t))/(sqrt(gamma ^(2)-p^(2)))sinh(sqrt(gamma ^(2)-p^(2))t)
12. The motion of an overdamped harmonic oscillator subject to an impulsive force is described by the equation i+ 2i + px = &(t) for a function x(t) and constants > p > 0. Given that x =0 for t < 0, show by Fourier transform methods that for O<7 -Y c(t) sinh (V2-p2 t)