Sommerfeld radiation condition

Arnold Sommerfeld defined the condition of radiation for a scalar field satisfying the Helmholtz equation as

"the sources must be sources, not sinks of energy. The energy which is radiated from the sources must scatter to infinity; no energy may be radiated from infinity into ... the field."^[1]

Mathematically, consider the inhomogeneous Helmholtz equation

(\nabla ^{2}+k^{2})u=-f{\mbox{ in }}{\mathbb R}^{n}

where $n=2,3$ is the dimension of the space, $f$ is a given function with compact support representing a bounded source of energy, and $k>0$ is a constant, called the wavenumber. A solution $u$ to this equation is called radiating if it satisfies the Sommerfeld radiation condition

\lim _{{|x|\to \infty }}|x|^{{{\frac {n-1}{2}}}}\left({\frac {\partial }{\partial |x|}}-ik\right)u(x)=0

uniformly in all directions

{\hat {x}}={\frac {x}{|x|}}

(above, $i$ is the imaginary unit and $|\cdot |$ is the Euclidean norm). Here, it is assumed that the time-harmonic field is $e^{{-i\omega t}}u.$ If the time-harmonic field is instead $e^{{i\omega t}}u,$ one should replace $-i$ with $+i$ in the Sommerfeld radiation condition.

The Sommerfeld radiation condition is used to solve uniquely the Helmholtz equation. For example, consider the problem of radiation due to a point source $x_{0}$ in three dimensions, so the function $f$ in the Helmholtz equation is $f(x)=\delta (x-x_{0}),$ where $\delta$ is the Dirac delta function. This problem has an infinite number of solutions, for example, any function of the form

u=cu_{+}+(1-c)u_{-}\,

where $c$ is a constant, and

u_{{\pm }}(x)={\frac {e^{{\pm ik|x-x_{0}|}}}{4\pi |x-x_{0}|}}.

Of all these solutions, only $u_{+}$ satisfies the Sommerfeld radiation condition and corresponds to a field radiating from $x_{0}.$ The other solutions are unphysical. For example, $u_{{-}}$ can be interpreted as energy coming from infinity and sinking at $x_{0}.$

References

↑ A. Sommerfeld, Partial Differential Equations in Physics, Academic Press, New York, New York, 1949.

Martin, P. A (2006). Multiple scattering: interaction of time-harmonic waves with N obstacles. Cambridge; New York: Cambridge University Press. ISBN 0-521-86554-9.
"Eighty years of Sommerfeld’s radiation condition", Steven H. Schot, Historia Mathematica 19, #4 (November 1992), pp. 385-401, doi:10.1016/0315-0860(92)90004-U.

External links

A.G. Sveshnikov (2001), "Radiation conditions", in Hazewinkel, Michiel, Encyclopedia of Mathematics, Springer, ISBN 978-1-55608-010-4

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