One end of a tightly stretched flexible thin string of length l is fixed at the origin and the other at x=l. It is plucked at x=l/3 so that it assumes initially the shape of a triangle of height h in the x-y plane. Find the displacement y at any distance x and at any time t after the string is released from rest. Take mass per unit lengthhorizontal tension=c2.
Technique
d’Alembert/Fourier (separation of variables); cosine-in-time modes for the rest condition; half-range sine coefficients of the triangular initial profile.
Solution
Step 1 — Governing equation and boundary/initial conditions
The transverse displacement satisfies the one-dimensional wave equation
∂t2∂2y=c2∂x2∂2y,0<x<l,
with
y(0,t)=0,y(l,t)=0(fixed ends),∂t∂y(x,0)=0(released from rest),
Carrying out the integration (integration by parts),
bn=π2n29hsin3nπ.
(Equivalently, the standard plucked-string result bn=π2n2a(l−a)2hl2sinlnπa with a=l/3.) Note sin3nπ=0 for n=3,6,9,…, so every third harmonic is absent.