A critically damped, driven oscillator’s displacement x(t) satisfies the equation of motion
x¨ + 2ω0x˙ + ω
2
0x = f0 cos ωt (1)
where ω0 is the natural frequency, and ω is the “driving frequency”.
(i) Find the particular solution to the above equation, in the form xp(t) = A cos(ωt + φ).
Your answer should clearly give the expressions for A and φ.
(ii) The homogeneous equation ¨x + 2ω0x˙ + ω
2
0x = 0 has e
−ω0t as one solution. Show, by
substitution, that the function te−βt can be the second solution. Find β in terms of ω0.
(iii) Use the above results to construct the complete solution to Eq. 1, subject to the initial
conditions x(0) = 0 = ˙x(0). (3 MARKS)
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