Efficiently Solve u_xx = u_tt with D'Lambert Method | Detailed Guide

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  • Thread starter Hurry
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In summary, we can solve the given partial differential equation using the d'Alembert's solution, which involves taking the average of the initial conditions and integrating over the appropriate intervals. There are five possible cases, depending on the values of \(x\) and \(t\), which result in different solutions for \(U(x,t)\).
  • #1
Hurry
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Consider

$\begin{align*}
& {{u}_{tt}}={{u}_{xx}},\text{ }x\in \mathbb{R},\text{ }t>0 \\
& u(x,0)=0,\text{ }x\in \mathbb{R} \\
& {{u}_{t}}(x,0)=\left\{ \begin{matrix}
\sin x,\text{ }\left| x \right|\le \pi \\
0,\text{ }x\notin [-\pi ,\pi ] \\
\end{matrix} \right.
\end{align*}
$

How can I solve this by using D'Lambert method?
 
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  • #2
Hurry said:
Consider

$\begin{align*}
& {{u}_{tt}}={{u}_{xx}},\text{ }x\in \mathbb{R},\text{ }t>0 \\
& u(x,0)=0,\text{ }x\in \mathbb{R} \\
& {{u}_{t}}(x,0)=\left\{ \begin{matrix}
\sin x,\text{ }\left| x \right|\le \pi \\
0,\text{ }x\notin [-\pi ,\pi ] \\
\end{matrix} \right.
\end{align*}
$

How can I solve this by using D'Lambert method?

Hi Hurry,

The d'Alembert's Solution for the given partial differential equation is, (Refer this or this.)

\[U(x,\,t)=\frac{1}{2}U(x-t,\,0)+\frac{1}{2}U(x+t,\,0)+\frac{1}{2}\int_{x-t}^{x+t}U_{t}(s,\,0)\,ds\]

Since \(U(x,\,0)=0~\forall~x\in\Re\) we get,

\begin{eqnarray}

U(x,\,t)&=&\frac{1}{2}\int_{x-t}^{x+t}U_{t}(s,\,0)\,ds\\

\end{eqnarray}

Case I: When, \(x-t\leq-\pi\mbox{ and }x+t\geq\pi\)

\begin{eqnarray}

U(x,\,t)&=&\frac{1}{2}\int_{-\pi}^{\pi}\sin(s)\,ds\\

&=&0

\end{eqnarray}

Case II: When, \(-\pi<x-t<\pi\mbox{ and }x+t\geq\pi\)

\begin{eqnarray}

U(x,\,t)&=&\frac{1}{2}\int_{x-t}^{\pi}\sin(s)\,ds\\

&=&\frac{1}{2}[1+\cos(x-t)]

\end{eqnarray}Case III: When, \(-\pi<x-t<\pi\mbox{ and }-\pi<x+t<\pi\)

\begin{eqnarray}

U(x,\,t)&=&\frac{1}{2}\int_{x-t}^{x+t}\sin(s)\,ds\\

&=&\frac{1}{2}[-cos(x+t)+\cos(x-t)]

\end{eqnarray}

By the Sum to product identity we get,

\[U(x,\,t)=\sin(x)\sin(t)\]

Case IV: When, \(x-t\leq-\pi\mbox{ and }-\pi<x+t<\pi\)

\begin{eqnarray}

U(x,\,t)&=&\frac{1}{2}\int_{-\pi}^{x+t}\sin(s)\,ds\\

&=&\frac{1}{2}[-1-\cos(x+t)]

\end{eqnarray}

Case V: Otherwise. (\([-\pi,\pi]\cap[x-t,x+t]=\varnothing\))

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

Kind Regards,
Sudharaka.
 

FAQ: Efficiently Solve u_xx = u_tt with D'Lambert Method | Detailed Guide

What is the D'Lambert problem?

The D'Lambert problem is a mathematical problem that involves finding the trajectory of a spacecraft from one point in space to another, while taking into account the gravitational pull of multiple celestial bodies. It is often used in space mission planning and navigation.

How is the D'Lambert problem solved?

The D'Lambert problem is typically solved using numerical methods, such as the Lambert's method or the Gauss's method. These methods involve solving a system of equations to determine the spacecraft's trajectory and flight path.

What are the main challenges of the D'Lambert problem?

The main challenges of the D'Lambert problem include accurately modeling the gravitational forces of multiple celestial bodies, accounting for perturbations in the spacecraft's trajectory, and ensuring the spacecraft reaches its desired destination with the desired velocity.

How is the D'Lambert problem used in real-world applications?

The D'Lambert problem is used in a variety of real-world applications, such as space mission planning and navigation, satellite orbit determination, and interplanetary trajectory design. It is also used in the aerospace industry for spacecraft and satellite mission planning.

What are some potential future developments in solving the D'Lambert problem?

Some potential future developments in solving the D'Lambert problem include the use of artificial intelligence and machine learning algorithms to improve the accuracy and efficiency of the solutions, as well as the development of new numerical methods to handle more complex scenarios, such as multiple spacecraft or non-gravitational forces.

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