A vibrating string fixed at x = 0 and x = L undergoes oscillations described by the wave equation 1 Pu %3D dx² c² Ət² where u(x, t) represents the displacement from equilibrium of the string. Initially the profile of the string is u(x, 0) = sin L (#) and its initial vertical velocity is du = 87 sin L It=0 (a) The four basic periodic solutions of the wave equation are A cos(kr) cos(kct) C sin(kæ) cos(kct) B cos(kr) sin(kct) D sin(kx) sin(kct) where k is a real constant and A, B,C and D are arbitrary constants. Use the boundary conditions to find the allowed values for the separation constant k. (b) Obtain the solution u(x,t) of the wave equation that also satisfies the initial conditions.

Advanced Engineering Mathematics
10th Edition
ISBN:9780470458365
Author:Erwin Kreyszig
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Chapter2: Second-order Linear Odes
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A vibrating string fixed at x = 0 and x =
equation
L undergoes oscillations described by the wave
Pu
1 d³u
dx²
c² Ət?
where u(x, t) represents the displacement from equilibrium of the string. Initially the profile
of the string is
47
= sin
L
(#)
u(x,0) =
and its initial vertical velocity is
(7)
du
877
= 8T sin
It=0
(a) The four basic periodic solutions of the wave equation are
A cos(kr) cos(kct)
B cos(kæ) sin(kct)
D sin(kæ) sin(kct)
C sin(kr) cos(kct)
where k is a real constant and A, B,C and D are arbitrary constants. Use the boundary
conditions to find the allowed values for the separation constant k.
(b) Obtain the solution u(x, t) of the wave equation that also satisfies the initial conditions.
Transcribed Image Text:A vibrating string fixed at x = 0 and x = equation L undergoes oscillations described by the wave Pu 1 d³u dx² c² Ət? where u(x, t) represents the displacement from equilibrium of the string. Initially the profile of the string is 47 = sin L (#) u(x,0) = and its initial vertical velocity is (7) du 877 = 8T sin It=0 (a) The four basic periodic solutions of the wave equation are A cos(kr) cos(kct) B cos(kæ) sin(kct) D sin(kæ) sin(kct) C sin(kr) cos(kct) where k is a real constant and A, B,C and D are arbitrary constants. Use the boundary conditions to find the allowed values for the separation constant k. (b) Obtain the solution u(x, t) of the wave equation that also satisfies the initial conditions.
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