MHB Wave equation and multiple boundary conditions

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To solve the wave equation \(u_{tt}=c^2u_{xx}\) on a semi-infinite interval with given boundary and initial conditions, d'Alembert's method can be applied. The solution is expressed as \(u(x,t)=\frac{1}{2}u(x-ct,0)+\frac{1}{2}u(x+ct,0)\) since the initial velocity \(u_t(x,0)=0\). For the specified initial conditions, the solution evaluates to zero when \(0<x-ct<2\) or \(x-ct>3\), and equals one when \(2<x-ct<3\). This approach effectively captures the behavior of the wave under the defined constraints. The method provides a clear framework for analyzing wave propagation in this context.
Markov2
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I need to apply D'Lembert's method but in this case I don't know how. How to proceed?

Determine the solution of the wave equation on a semi-infinite interval $u_{tt}=c^2u_{xx},$ $0<x<\infty,$ $t>0,$ where $u(0,t)=0$ and the initial conditions:

$\begin{aligned} & u(x,0)=\left\{ \begin{align}
& 0,\text{ }0<x<2 \\
& 1,\text{ }2<x<3 \\
& 0,\text{ }x>3 \\
\end{align} \right. \\
& {{u}_{t}}(x,0)=0. \\
\end{aligned}$
 
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Markov said:
I need to apply D'Lembert's method but in this case I don't know how. How to proceed?

Determine the solution of the wave equation on a semi-infinite interval $u_{tt}=c^2u_{xx},$ $0<x<\infty,$ $t>0,$ where $u(0,t)=0$ and the initial conditions:

$\begin{aligned} & u(x,0)=\left\{ \begin{align}
& 0,\text{ }0<x<2 \\
& 1,\text{ }2<x<3 \\
& 0,\text{ }x>3 \\
\end{align} \right. \\
& {{u}_{t}}(x,0)=0. \\
\end{aligned}$

Hi Markov, :)

The d'Alembert's solution for the wave equation, \(u_{tt}=c^2u_{xx}\) can be written as,

\[u(x,t)=\frac{1}{2}u(x-ct,\,0)+\frac{1}{2}u(x+ct,\,0)-\frac{1}{2c}\int_{x-ct}^{x+ct}u_{t}(s,\,0)\,ds\]

Since, \(u_{t}(x,0)=0\) we get,

\[u(x,t)=\frac{1}{2}u(x-ct,\,0)+\frac{1}{2}u(x+ct,\,0)\]

Case I: When \(0<x-ct<2\mbox{ or }x-ct>3\)

\[u(x,t)=0\]

Case II: When \(2<x-ct<3\)

\[u(x,t)=1\]

Kind Regards,
Sudharaka.
 

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