mass Q(x, t), so that the resulting vertical displacement u(x, t) satisfies
J²u
21²
and the initial conditions are
J²u
əx²
(1)
where e is a constant. The ends of the string are looped around and free to slide on vertical
frictionless wires so that the boundary conditions are
+ Q(x, t)
Ju(0, 1) — 0, Ju(π, l)
Әх
ər
u(x,0) = 0,
Ju
ƏL
=
0.
(x,0) = Vo
where Vo is a constant.
(a) In (1), what are the dimensions of c? What does e represent physically?
Next, seek a solution to (1-3) in the form
u(x, t) = Σan (1)on(x)
n=0
(2)
(3)
(4)
by following the steps below:
(b) Assume a separable solution to the homogeneous version of the PDE and boundary con-
ditions (1)-(2) of the form u = o(r)h(t). Write down or find the eigenvalues An and
eigenfunctions on(r) of the homogeneous problem.
(c) Using the eigenfunction expansion (4) and your results from (b), find the second-order
ODEs satisfied by each unknown time-dependent amplitude an (1) for Q(x, t) in (1) given
by
Q(x, t) = cos + et cos(2x)
(5)
where is a constant.
(d) Find the initial conditions for an (l) for all n = 0, 1, 2....
(e) Using the ODEs and initial conditions found in (c) and (d), obtain the general solution
for an (1) for all n = 0, 1, 2....
(f) Write the final expression for u(x, t).
Fig: 1