Approximate the solution to the wave equation: a'u d'u (x.t) (x.t)-0 for 0 0 (x.t)-0 for 00 (0.1)- u(1.1) –0 for 1>0 suhject to u(x.0)= sin 2.zx for 0srs1 g(x)= (x.0)= 27 sin 2zx for 0sxs1 Delta x=0.2, Delta t=0.1 using the Finite-Differenee Method with h- 0.2 and k - 0.1. Comparc your results to the actual solution u(x.t) = sin 2zx (cos 2m + sin 27) at i= 0.2.

Introductory Circuit Analysis (13th Edition)
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Author:Robert L. Boylestad
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Approximate the solution to the wave equation:
d'u
ar: (x.1)-0 for 0 <x<1 and 1>0
u(0,1) - u(1.1)-0 for 1>0
suhject to u(x.0)= sin 2.zx for 0srs1
g(x)=
(x.0)%3D27 sin 2zm for 0sxs1
Delta x=0.2, Delta t=0.1
using the Finite-Difference Method with h- 0.2 and k - 0.1. Comparc your results to the
actual solution u(x.t) = sin 2zx (cos 2m + sin 2m) at 1 = 0.2.
Transcribed Image Text:Approximate the solution to the wave equation: d'u ar: (x.1)-0 for 0 <x<1 and 1>0 u(0,1) - u(1.1)-0 for 1>0 suhject to u(x.0)= sin 2.zx for 0srs1 g(x)= (x.0)%3D27 sin 2zm for 0sxs1 Delta x=0.2, Delta t=0.1 using the Finite-Difference Method with h- 0.2 and k - 0.1. Comparc your results to the actual solution u(x.t) = sin 2zx (cos 2m + sin 2m) at 1 = 0.2.
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