Partial differential equations Hyperbolic equations Theorem
d'Alembert's formula
Builds on Wave equation
Statement
Let , let and let . Define by Then , solves the wave equation on , and , for all . Moreover, is the only solution of this initial value problem.
Remarks
The change of variables , turns the equation into . Hence every solution has the form , and the two initial conditions determine and up to a constant that cancels. This argument also proves uniqueness. Example: with and , the formula gives , a standing wave. The value depends only on the data in the interval , which shows finite speed of propagation in one dimension. If is only continuous, the formula still defines a function, but it is a weak solution rather than a classical one.
Going deeper
For a student
d'Alembert's formula is the first explicit solution formula in a PDE course and the basis for the other dimensions. By the method of spherical means, it gives Kirchhoff's formula in dimension , and then by descent Poisson's formula in dimension . On the half line, the formula combined with an odd or even reflection of the data solves the problems with Dirichlet or Neumann boundary condition. For the inhomogeneous equation , Duhamel's principle adds the term .
Reading path
To understand this page from the ground up, read these 2 pages in order. The foundations come first.
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- Wave equation concept
- d'Alembert's formula statement
Further reading
About this page
| Tag | YVQRAPSF77 |
|---|---|
| URI | m2://YVQRAPSF77 |
| Kind | statement, theorem |
| Writing | W0 stub |
| MSC | 35L05, 35C05, 35L15 |
| Status | This copy of the site has no build data. Run m2 status YVQRAPSF77. |
| About | Wave equation |
| Uses | Wave equation |
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