KNOWPIA
WELCOME TO KNOWPIA

In mathematics, the eigenvalue problem for the Laplace operator is known as the **Helmholtz equation**. It corresponds to the linear partial differential equation

where ∇

The Helmholtz equation often arises in the study of physical problems involving partial differential equations (PDEs) in both space and time. The Helmholtz equation, which represents a **time-independent** form of the wave equation, results from applying the technique of separation of variables to reduce the complexity of the analysis.

For example, consider the wave equation

Separation of variables begins by assuming that the wave function *u*(**r**, *t*) is in fact separable:

Substituting this form into the wave equation and then simplifying, we obtain the following equation:

Notice that the expression on the left side depends only on **r**, whereas the right expression depends only on t. As a result, this equation is valid in the general case if and only if both sides of the equation are equal to the same constant value. This argument is key in the technique of solving linear partial differential equations by separation of variables. From this observation, we obtain two equations, one for *A*(**r**), the other for *T*(*t*):

where we have chosen, without loss of generality, the expression −*k*^{2} for the value of the constant. (It is equally valid to use any constant k as the separation constant; −*k*^{2} is chosen only for convenience in the resulting solutions.)

Rearranging the first equation, we obtain the Helmholtz equation:

Likewise, after making the substitution *ω* = *kc*, where k is the wave number, and ω is the angular frequency (assuming a monochromatic field), the second equation becomes

We now have Helmholtz's equation for the spatial variable **r** and a second-order ordinary differential equation in time. The solution in time will be a linear combination of sine and cosine functions, whose exact form is determined by initial conditions, while the form of the solution in space will depend on the boundary conditions. Alternatively, integral transforms, such as the Laplace or Fourier transform, are often used to transform a hyperbolic PDE into a form of the Helmholtz equation.

Because of its relationship to the wave equation, the Helmholtz equation arises in problems in such areas of physics as the study of electromagnetic radiation, seismology, and acoustics.

The solution to the spatial Helmholtz equation:

The two-dimensional analogue of the vibrating string is the vibrating membrane, with the edges clamped to be motionless. The Helmholtz equation was solved for many basic shapes in the 19th century: the rectangular membrane by Siméon Denis Poisson in 1829, the equilateral triangle by Gabriel Lamé in 1852, and the circular membrane by Alfred Clebsch in 1862. The elliptical drumhead was studied by Émile Mathieu, leading to Mathieu's differential equation.

If the edges of a shape are straight line segments, then a solution is integrable or knowable in closed-form only if it is expressible as a finite linear combination of plane waves that satisfy the boundary conditions (zero at the boundary, i.e., membrane clamped).

If the domain is a circle of radius a, then it is appropriate to introduce polar coordinates r and θ. The Helmholtz equation takes the form

We may impose the boundary condition that A vanishes if *r* = *a*; thus

the method of separation of variables leads to trial solutions of the form

It follows from the periodicity condition that

The general solution A then takes the form of a generalized Fourier series of terms involving products of *J _{n}*(

In spherical coordinates, the solution is:

This solution arises from the spatial solution of the wave equation and diffusion equation. Here *j _{ℓ}*(

Writing **r**_{0} = (*x*, *y*, *z*) function *A*(*r*_{0}) has asymptotics

where function f is called scattering amplitude and *u*_{0}(*r*_{0}) is the value of A at each boundary point *r*_{0}.

In the paraxial approximation of the Helmholtz equation,^{[1]} the complex amplitude A is expressed as

This equation has important applications in the science of optics, where it provides solutions that describe the propagation of electromagnetic waves (light) in the form of either paraboloidal waves or Gaussian beams. Most lasers emit beams that take this form.

The assumption under which the paraxial approximation is valid is that the z derivative of the amplitude function u is a slowly varying function of z:

This condition is equivalent to saying that the angle θ between the wave vector **k** and the optical axis z is small: *θ* ≪ 1.

The paraxial form of the Helmholtz equation is found by substituting the above-stated expression for the complex amplitude into the general form of the Helmholtz equation as follows:

Expansion and cancellation yields the following:

Because of the paraxial inequality stated above, the ∂^{2}*u*/∂*z*^{2} term is neglected in comparison with the *k*·∂*u*/∂*z* term. This yields the paraxial Helmholtz equation. Substituting *u*(**r**) = *A*(**r**) *e*^{−ikz} then gives the paraxial equation for the original complex amplitude A:

The Fresnel diffraction integral is an exact solution to the paraxial Helmholtz equation.^{[2]}

The **inhomogeneous Helmholtz equation** is the equation

In order to solve this equation uniquely, one needs to specify a boundary condition at infinity, which is typically the Sommerfeld radiation condition

in spatial dimensions, for all angles (i.e. any value of ). Here where are the coordinates of the vector .

With this condition, the solution to the inhomogeneous Helmholtz equation is

(notice this integral is actually over a finite region, since f has compact support). Here, G is the Green's function of this equation, that is, the solution to the inhomogeneous Helmholtz equation with *f* equaling the Dirac delta function, so G satisfies

The expression for the Green's function depends on the dimension n of the space. One has

Finally, for general n,

where and ,^{[3]}.

- Laplace's equation (a particular case of the Helmholtz equation)
- Weyl expansion

**^**J. W. Goodman.*Introduction to Fourier Optics*(2nd ed.). pp. 61–62.**^**Grella, R. (1982). "Fresnel propagation and diffraction and paraxial wave equation".*Journal of Optics*.**13**(6): 367–374. Bibcode:1982JOpt...13..367G. doi:10.1088/0150-536X/13/6/006.**^**https://ww3.math.ucla.edu/camreport/cam14-71.pdf

- Abramowitz, Milton; Stegun, Irene, eds. (1964).
*Handbook of Mathematical functions with Formulas, Graphs and Mathematical Tables*. New York: Dover Publications. ISBN 978-0-486-61272-0.

- Riley, K. F.; Hobson, M. P.; Bence, S. J. (2002). "Chapter 19".
*Mathematical methods for physics and engineering*. New York: Cambridge University Press. ISBN 978-0-521-89067-0.

- Riley, K. F. (2002). "Chapter 16".
*Mathematical Methods for Scientists and Engineers*. Sausalito, California: University Science Books. ISBN 978-1-891389-24-5.

- Saleh, Bahaa E. A.; Teich, Malvin Carl (1991). "Chapter 3".
*Fundamentals of Photonics*. Wiley Series in Pure and Applied Optics. New York: John Wiley & Sons. pp. 80–107. ISBN 978-0-471-83965-1.

- Sommerfeld, Arnold (1949). "Chapter 16".
*Partial Differential Equations in Physics*. New York: Academic Press. ISBN 978-0126546569.

- Howe, M. S. (1998).
*Acoustics of fluid-structure interactions*. New York: Cambridge University Press. ISBN 978-0-521-63320-8.

- Helmholtz Equation at EqWorld: The World of Mathematical Equations.
- "Helmholtz equation",
*Encyclopedia of Mathematics*, EMS Press, 2001 [1994] - Vibrating Circular Membrane by Sam Blake, The Wolfram Demonstrations Project.
- Green's functions for the wave, Helmholtz and Poisson equations in a two-dimensional boundless domain