Difference between revisions of "Eikonal equation"
Ulf Rehmann (talk | contribs) m (MR/ZBL numbers added) |
(TeX) |
||
Line 1: | Line 1: | ||
+ | {{TEX|done}} | ||
A partial differential equation of the form | A partial differential equation of the form | ||
− | + | $$\sum_{i=1}^m\left(\frac{\partial\tau}{\partial x^i}\right)^2=\frac{1}{c^2(x^1,\dots,x^m)}.$$ | |
− | Here | + | Here $m$ is the dimension of the space and $c$ is a smooth function bounded away from zero. In applications $c$ is the speed of the wave, and the surfaces $\tau(x^1,\dots,x^m)=\mathrm{const}$ are the wave fronts. The rays (see [[Fermat principle|Fermat principle]]) are the characteristics of the eikonal equation. This equation has a number of generalizations and analogues. In particular, one such generalization is |
− | + | $$H\left(x^1,\dots,x^m,\frac{\partial\tau}{\partial x^1},\dots,\frac{\partial\tau}{\partial x^m}\right)=1,$$ | |
− | where the function | + | where the function $H$ is homogeneous of degree 1 with respect to $\partial\tau/\partial x^1,\dots,\partial\tau/\partial x^m$ and satisfies some additional restrictions. Of considerable interest is the non-stationary analogue |
− | + | $$-\frac{\partial\theta}{\partial t}+c(t,x^1,\ldots,x^m)\sqrt{\sum_{i=1}^m\left(\frac{\partial\theta}{\partial x^i}\right)^2}=0.$$ | |
This is a special case of the dispersion equations occurring in the theory of wave phenomena, which have the form | This is a special case of the dispersion equations occurring in the theory of wave phenomena, which have the form | ||
− | + | $$\frac{\partial\theta}{\partial t}=\omega(t,x^1,\dots,x^m,\theta_{x^1},\theta_{x^m}).$$ | |
− | Here | + | Here $\omega$ is a given function. |
The mathematical theory of geometrical optics can be regarded as the theory of the eikonal equation. All forms of the eikonal equation are first-order partial differential equations. The solution of the eikonal equation may have singularities. Their theory is part of that of the [[Singularities of differentiable mappings|singularities of differentiable mappings]] (see also [[Hamilton–Jacobi theory|Hamilton–Jacobi theory]]; [[Geometric approximation|Geometric approximation]], and [[Ray method|Ray method]]). | The mathematical theory of geometrical optics can be regarded as the theory of the eikonal equation. All forms of the eikonal equation are first-order partial differential equations. The solution of the eikonal equation may have singularities. Their theory is part of that of the [[Singularities of differentiable mappings|singularities of differentiable mappings]] (see also [[Hamilton–Jacobi theory|Hamilton–Jacobi theory]]; [[Geometric approximation|Geometric approximation]], and [[Ray method|Ray method]]). |
Revision as of 14:27, 19 August 2014
A partial differential equation of the form
$$\sum_{i=1}^m\left(\frac{\partial\tau}{\partial x^i}\right)^2=\frac{1}{c^2(x^1,\dots,x^m)}.$$
Here $m$ is the dimension of the space and $c$ is a smooth function bounded away from zero. In applications $c$ is the speed of the wave, and the surfaces $\tau(x^1,\dots,x^m)=\mathrm{const}$ are the wave fronts. The rays (see Fermat principle) are the characteristics of the eikonal equation. This equation has a number of generalizations and analogues. In particular, one such generalization is
$$H\left(x^1,\dots,x^m,\frac{\partial\tau}{\partial x^1},\dots,\frac{\partial\tau}{\partial x^m}\right)=1,$$
where the function $H$ is homogeneous of degree 1 with respect to $\partial\tau/\partial x^1,\dots,\partial\tau/\partial x^m$ and satisfies some additional restrictions. Of considerable interest is the non-stationary analogue
$$-\frac{\partial\theta}{\partial t}+c(t,x^1,\ldots,x^m)\sqrt{\sum_{i=1}^m\left(\frac{\partial\theta}{\partial x^i}\right)^2}=0.$$
This is a special case of the dispersion equations occurring in the theory of wave phenomena, which have the form
$$\frac{\partial\theta}{\partial t}=\omega(t,x^1,\dots,x^m,\theta_{x^1},\theta_{x^m}).$$
Here $\omega$ is a given function.
The mathematical theory of geometrical optics can be regarded as the theory of the eikonal equation. All forms of the eikonal equation are first-order partial differential equations. The solution of the eikonal equation may have singularities. Their theory is part of that of the singularities of differentiable mappings (see also Hamilton–Jacobi theory; Geometric approximation, and Ray method).
References
[1] | V.M. Babich, V.S. Buldyrev, "Asymptotic methods in problems of diffraction of short waves" , Moscow (1972) (In Russian) (Translation forthcoming: Springer) |
[2] | G.B. Whitham, "Linear and nonlinear waves" , Wiley (1974) MR0483954 Zbl 0373.76001 |
Comments
For a nice account of the theory of geometrical optics see [a3]; geometrical optics and pseudo-differential operator theory are treated in [a2].
References
[a1] | P.R. Garabedian, "Partial differential equations" , Wiley (1964) MR0162045 Zbl 0124.30501 |
[a2] | M.E. Taylor, "Pseudodifferential operators" , Princeton Univ. Press (1981) MR0618463 Zbl 0453.47026 |
[a3] | M. Kline, I.W. Kay, "Electromagnetic theory and geometrical optics" , Interscience (1965) MR0180094 Zbl 0123.23602 |
[a4] | L.B. Felsen, N. Marcuvitz, "Radiation and scattering of waves" , Prentice-Hall (1973) pp. Sect. 1.7 MR0471626 |
Eikonal equation. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Eikonal_equation&oldid=33013