Math 2.0

Partial differential equations Hyperbolic equations Theorem

d'Alembert's formula

Builds on Wave equation

Statement

Let c>0c > 0, let g∈C2(ℝ)g \in C^2(\R) and let h∈C1(ℝ)h \in C^1(\R). Define u ⁣:ℝ×[0,∞)→ℝu \colon \R \times [0, \infty) \to \R by u(x,t)=g(x+ct)+g(x−ct)2+12c∫x−ctx+cth(s) ds.u(x, t) = \frac{g(x + ct) + g(x - ct)}{2} + \frac{1}{2c} \int_{x - ct}^{x + ct} h(s)\, ds. Then u∈C2(ℝ×[0,∞))u \in C^2(\R \times [0, \infty)), uu solves the wave equation utt=c2uxxu_{tt} = c^2 u_{xx} on ℝ×(0,∞)\R \times (0, \infty), and u(x,0)=g(x)u(x, 0) = g(x), ut(x,0)=h(x)u_t(x, 0) = h(x) for all x∈ℝx \in \R. Moreover, uu is the only C2C^2 solution of this initial value problem.

Remarks

The change of variables ξ=x+ct\xi = x + ct, η=x−ct\eta = x - ct turns the equation into uξη=0u_{\xi\eta} = 0. Hence every C2C^2 solution has the form u=F(x+ct)+G(x−ct)u = F(x + ct) + G(x - ct), and the two initial conditions determine FF and GG up to a constant that cancels. This argument also proves uniqueness. Example: with g=0g = 0 and h=cos⁡h = \cos, the formula gives u(x,t)=12c(sin⁡(x+ct)−sin⁡(x−ct))=1ccos⁡xsin⁡(ct)u(x, t) = \frac{1}{2c}\big(\sin(x + ct) - \sin(x - ct)\big) = \frac{1}{c}\cos x \sin(ct), a standing wave. The value u(x,t)u(x, t) depends only on the data in the interval [x−ct,x+ct][x - ct, x + ct], which shows finite speed of propagation in one dimension. If gg 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 33, and then by descent Poisson's formula in dimension 22. 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 utt−c2uxx=fu_{tt} - c^2 u_{xx} = f, Duhamel's principle adds the term 12c∫0t∫x−c(t−s)x+c(t−s)f(y,s) dy ds\frac{1}{2c}\int_0^t \int_{x - c(t - s)}^{x + c(t - s)} f(y, s)\, dy\, ds.

Reading path

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  1. Wave equation concept
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Further reading

  1. Web https://en.wikipedia.org/wiki/D%27Alembert%27s_formula
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Kindstatement, theorem
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MSC35L05, 35C05, 35L15
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AboutWave equation
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