# Electromagnetic wave equation

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Electromagnetic wave equation

The electromagnetic wave equation is a second-order partial differential equation that describes the propagation of electromagnetic waves through a medium or in a vacuum. The homogeneous form of the equation, written in terms of either the electric field E or the magnetic field B, takes the form:

:$left\left( abla^2 - \left\{ 1 over \left\{c\right\}^2 \right\} \left\{partial^2 over partial t^2\right\} ight\right) mathbf\left\{E\right\} = 0$

:$left\left( abla^2 - \left\{ 1 over \left\{c\right\}^2 \right\} \left\{partial^2 over partial t^2\right\} ight\right) mathbf\left\{B\right\} = 0$

where "c" is the speed of light in the medium. In a vacuum, "c" = "c"0 = 299,792,458 meters per second, which is the speed of light in free space. [ Current practice is to use "c"0 to denote the speed of light in vacuum according to ISO 31. In the original Recommendation of 1983, the symbol "c" was used for this purpose. See [http://physics.nist.gov/Pubs/SP330/sp330.pdf NIST "Special Publication 330", Appendix 2, p. 45 ] ]

The electromagnetic wave equation derives from Maxwell's equations.

It should also be noted that in most older literature, B is called the "magnetic flux density" or "magnetic induction".

peed of propagation

In vacuum

If the wave propagation is in vacuum, then

:$c = c_o = \left\{ 1 over sqrt\left\{ mu_o varepsilon_o \right\} \right\} = 2.99792458 imes 10^8$ meters per second

is the speed of light in vacuum, a "defined" value that sets the standard of length, the meter (unit). The magnetic constant $mu_0$ and the vacuum permittivity $varepsilon_0$ are important physical constants that play a key role in electromagnetic theory. Their values (also a matter of definition) in SI units taken from [http://physics.nist.gov/cuu/Constants/index.html NIST] are tabulated below:

In a material medium

The speed of light in a linear, isotropic, and non-dispersive material medium is

:$c = \left\{ c_0 over n \right\} = \left\{ 1 over sqrt\left\{ mu varepsilon \right\} \right\}$

where

:$n = sqrt\left\{ mu varepsilon over mu_0 varepsilon_0 \right\}$

is the refractive index of the medium, $mu$ is the magnetic permeability of the medium, and $varepsilon$ is the electric permittivity of the medium.

The origin of the electromagnetic wave equation

Conservation of charge

Conservation of charge requires that the time rate of change of the total charge enclosed within a volume "V" must equal the net current flowing into the surface "S" enclosing the volume:

:$oint limits_S mathbf\left\{j\right\} cdot d mathbf\left\{A\right\} = - \left\{d over d t\right\} int limits_V ho cdot dV$

where j is the current density (in Amperes per square meter) flowing through the surface and ρ is the charge density (in coulombs per cubic meter) at each point in the volume.

From the divergence theorem, this relationship can be converted from integral form to differential form:

:$abla cdot mathbf\left\{j\right\} = - \left\{ partial ho over partial t\right\}$

Ampère's circuital law prior to Maxwell's correction

In its original form, Ampère's circuital law relates the magnetic field B to the current density j:

:$oint limits_C mathbf\left\{B\right\} cdot d mathbf\left\{l\right\} = iint limits_S mu mathbf\left\{j\right\} cdot d mathbf\left\{A\right\}$

where "S" is an open surface terminated in the curve "C". This integral form can be converted to differential form, using Stokes' theorem:

:$abla imes mathbf\left\{B\right\} = mu_0 mathbf\left\{j\right\}$

Inconsistency between Ampère's circuital law and the law of conservation of charge

Taking the divergence of both sides of Ampère's circuital law gives:

:$abla cdot \left( abla imes mathbf\left\{B\right\} \right) = abla cdot mu_0 mathbf\left\{j\right\}$

The divergence of the curl of any vector field, including the magnetic field B, is always equal to zero:

:$abla cdot \left( abla imes mathbf\left\{B\right\}\right) = 0$

Combining these two equations implies that

:$abla cdot mu_0 mathbf\left\{j\right\} = 0$

Because $mu_0$ is nonzero constant, it follows that

:$abla cdot mathbf\left\{j\right\} = 0$

However, the law of conservation of charge tells that

:$abla cdot mathbf\left\{j\right\} = - \left\{ partial ho over partial t \right\}$

Hence, as in the case of Kirchhoff's circuit laws, Ampère's circuital law would appear only to hold in situations involving constant charge density. This would rule out the situation that occurs in the plates of a charging or a discharging capacitor.

Maxwell's correction to Ampère's circuital law

Gauss's law in integral form states:

:$oint limits_S mathbf\left\{E\right\} cdot d mathbf\left\{A\right\} = frac\left\{1\right\}\left\{varepsilon_0\right\} int limits_V ho cdot dV ,$

where "S" is a closed surface enclosing the volume "V". This integral form can be converted to differential form using the divergence theorem:

:$abla cdot varepsilon_0 mathbf\left\{E\right\} = ho$

Taking the time derivative of both sides and reversing the order of differentiation on the left-hand side gives:

:$abla cdot varepsilon_0 \left\{partial mathbf\left\{E\right\} over partial t \right\} = \left\{ partial ho over partial t\right\}$

This last result, along with Ampère's circuital law and the conservation of charge equation, suggests that there are actually "two" origins of the magnetic field: the current density j, as Ampère had already established, and the so-called displacement current:

:$\left\{partial mathbf\left\{D\right\} over partial t \right\} = varepsilon_0 \left\{partial mathbf\left\{E\right\} over partial t \right\}$

So the corrected form of Ampère's circuital law becomes:

:$abla imes mathbf\left\{B\right\} = mu_0 mathbf\left\{j\right\} + mu_0 varepsilon_0 \left\{partial mathbf\left\{E\right\} over partial t \right\}$

Maxwell's hypothesis that light is an electromagnetic wave

In his 1864 paper entitled A Dynamical Theory of the Electromagnetic Field, Maxwell utilized the correction to Ampère's circuital law that he had made in part III of his 1861 paper [http://vacuum-physics.com/Maxwell/maxwell_oplf.pdf On Physical Lines of Force] . In PART VI of his 1864 paper which is entitled 'ELECTROMAGNETIC THEORY OF LIGHT' [ [http://www.zpenergy.com/downloads/Maxwell_1864_4.pdf Maxwell 1864 4] (page 497 of the article and page 9 of the pdf link)] , Maxwell combined displacement current with some of the other equations of electromagnetism and he obtained a wave equation with a speed equal to the speed of light. He commented:

:"The agreement of the results seems to show that light and magnetism are affections of the same substance, and that light is an electromagnetic disturbance propagated through the field according to electromagnetic laws." [ See [http://www.zpenergy.com/downloads/Maxwell_1864_5.pdf Maxwell 1864 5] , page 499 of the article and page 1 of the pdf link]

Maxwell's derivation of the electromagnetic wave equation has been replaced in modern physics by a much less cumbersome method involving combining the corrected version of Ampère's circuital law with Faraday's law of induction.

To obtain the electromagnetic wave equation in a vacuum using the modern method, we begin with the modern 'Heaviside' form of Maxwell's equations. In a vacuum, these equations are:

:$abla cdot mathbf\left\{E\right\} = frac \left\{ ho\right\} \left\{epsilon_0\right\}$

:$abla imes mathbf\left\{E\right\} = -frac\left\{partial mathbf\left\{B \left\{partial t\right\}$

:$abla cdot mathbf\left\{B\right\} = 0$

:$abla imes mathbf\left\{B\right\} =mu_0 varepsilon_0 frac\left\{ partial mathbf\left\{E \left\{partial t\right\}$

Taking the curl of the curl equations gives::$abla imes abla imes mathbf\left\{E\right\} = -frac\left\{partial \right\} \left\{partial t\right\} abla imes mathbf\left\{B\right\} = -mu_0 varepsilon_0 frac\left\{partial^2 mathbf\left\{E\right\} \right\} \left\{partial t^2\right\}$

:$abla imes abla imes mathbf\left\{B\right\} = mu_0 varepsilon_0 frac\left\{partial \right\} \left\{partial t\right\} abla imes mathbf\left\{E\right\} = -mu_o varepsilon_o frac\left\{partial^2 mathbf\left\{B\left\{partial t^2\right\}$

By using the vector identity

:$abla imes left\left( abla imes mathbf\left\{V\right\} ight\right) = abla left\left( abla cdot mathbf\left\{V\right\} ight\right) - abla^2 mathbf\left\{V\right\}$

where $mathbf\left\{V\right\}$ is any vector function of space, it turns into the wave equations:

:$\left\{partial^2 mathbf\left\{E\right\} over partial t^2\right\} - \left\{c_0\right\}^2 cdot abla^2 mathbf\left\{E\right\} = 0$

:$\left\{partial^2 mathbf\left\{B\right\} over partial t^2\right\} - \left\{c_0\right\}^2 cdot abla^2 mathbf\left\{B\right\} = 0$

where

:$c_0 = \left\{ 1 over sqrt\left\{ mu_0 varepsilon_0 \right\} \right\} = 2.99792458 imes 10^8$ meters per second

is the speed of light in free space.

Covariant form of the homogeneous wave equation

inertial reference frame leads to the theory of Special Relativity
These relativistic equations can be written in covariant form as

:$Box A^\left\{mu\right\} = 0$

where the electromagnetic four-potential is

:$A^\left\{mu\right\}=\left(varphi, mathbf\left\{A\right\} c\right)$

with the Lorenz gauge condition:

:$partial_\left\{mu\right\} A^\left\{mu\right\} = 0,$.

Here

:$Box = abla^2 - \left\{ 1 over c^2\right\} frac\left\{ partial^2\right\} \left\{ partial t^2\right\}$ is the d'Alembertian operator. The square box is not a typographical error; it is the correct symbol for this operator.

Homogeneous wave equation in curved spacetime

The electromagnetic wave equation is modified in two ways, the derivative is replaced with the covariant derivative and a new term that depends on the curvature appears.

:

where

:

is the Ricci curvature tensor and the semicolon indicates covariant differentiation.

The generalization of the Lorenz gauge condition in curved spacetime is assumed:

:$\left\{A^\left\{mu_\left\{ ; mu\right\} =0$.

Inhomogeneous electromagnetic wave equation

Localized time-varying charge and current densities can act as sources of electromagnetic waves in a vacuum. Maxwell's equations can be written in the form of a wave equation with sources. The addition of sources to the wave equations makes the partial differential equations inhomogeneous.

Solutions to the homogeneous electromagnetic wave equation

The general solution to the electromagnetic wave equation is a linear superposition of waves of the form

:$mathbf\left\{E\right\}\left( mathbf\left\{r\right\}, t \right) = g\left(phi\left( mathbf\left\{r\right\}, t \right)\right) = g\left( omega t - mathbf\left\{k\right\} cdot mathbf\left\{r\right\} \right)$

and

:$mathbf\left\{B\right\}\left( mathbf\left\{r\right\}, t \right) = g\left(phi\left( mathbf\left\{r\right\}, t \right)\right) = g\left( omega t - mathbf\left\{k\right\} cdot mathbf\left\{r\right\} \right)$

for virtually "any" well-behaved function "g" of dimensionless argument φ, where:$omega$ is the angular frequency (in radians per second), and :$mathbf\left\{k\right\} = \left( k_x, k_y, k_z\right)$ is the wave vector (in radians per meter).

Although the function "g" can be and often is a monochromatic sine wave, it does not have to be sinusoidal, or even periodic. In practice, "g" cannot have infinite periodicity because any real electromagnetic wave must always have a finite extent in time and space. As a result, and based on the theory of Fourier decomposition, a real wave must consist of the superposition of an infinite set of sinusoidal frequencies.

In addition, for a valid solution, the wave vector and the angular frequency are not independent; they must adhere to the dispersion relation:

:$k = | mathbf\left\{k\right\} | = \left\{ omega over c \right\} = \left\{ 2 pi over lambda \right\}$

where "k" is the wavenumber and λ is the wavelength.

The simplest set of solutions to the wave equation result from assuming sinusoidal waveforms of a single frequency in separable form:

:$mathbf\left\{E\right\} \left( mathbf\left\{r\right\}, t \right) = mathrm \left\{Re\right\} \left\{ mathbf\left\{E\right\} \left(mathbf\left\{r\right\} \right) e^\left\{ j omega t \right\} \right\}$

where
* $j ,$ is the imaginary unit,
* $omega = 2 pi f ,$"' is the angular frequency in radians per second,
* $f ,$ is the"' frequency in hertz, and
* $e^\left\{j omega t\right\} = cos\left(omega t\right) + j sin\left(omega t\right) ,$ is Euler's formula.

Plane wave solutions

Consider a plane defined by a unit normal vector :$mathbf\left\{n\right\} = \left\{ mathbf\left\{k\right\} over k \right\}$.

Then planar traveling wave solutions of the wave equations are:$mathbf\left\{E\right\}\left(mathbf\left\{r\right\}\right) = E_0 e^\left\{-j mathbf\left\{k\right\} cdot mathbf\left\{r\right\} \right\}$and:$mathbf\left\{B\right\}\left(mathbf\left\{r\right\}\right) = B_0 e^\left\{-j mathbf\left\{k\right\} cdot mathbf\left\{r\right\} \right\}$

where:$mathbf\left\{r\right\} = \left(x, y, z\right)$ is the position vector (in meters).

These solutions represent planar waves traveling in the direction of the normal vector $mathbf\left\{n\right\}$. If we define the z direction as the direction of $mathbf\left\{n\right\}$ and the x direction as the direction of $mathbf\left\{E\right\}$, then by Faraday's Law the magnetic field lies in the y direction and is related to the electric field by the relation:$c \left\{partial B over partial z\right\} = \left\{partial E over partial t\right\}$.Because the divergence of the electric and magnetic fields are zero, there are no fields in the direction of propagation.

This solution is the linearly polarized solution of the wave equations. There are also circularly polarized solutions in which the fields rotate about the normal vector.

pectral decomposition

Because of the linearity of Maxwell's equations in a vacuum, solutions can be decomposed into a superposition of sinusoids. This is the basis for the Fourier transform method for the solution of differential equations.The sinusoidal solution to the electromagnetic wave equation takes the form

:$mathbf\left\{E\right\} \left( mathbf\left\{r\right\}, t \right) = mathbf\left\{E\right\}_0 cos\left( omega t - mathbf\left\{k\right\} cdot mathbf\left\{r\right\} + phi_0 \right)$and:$mathbf\left\{B\right\} \left( mathbf\left\{r\right\}, t \right) = mathbf\left\{B\right\}_0 cos\left( omega t - mathbf\left\{k\right\} cdot mathbf\left\{r\right\} + phi_0 \right)$

where:$t$ is time (in seconds),:$omega$ is the angular frequency (in radians per second),:$mathbf\left\{k\right\} = \left( k_x, k_y, k_z\right)$ is the wave vector (in radians per meter), and:$phi_0 ,$ is the phase angle (in radians).The wave vector is related to the angular frequency by

:$k = | mathbf\left\{k\right\} | = \left\{ omega over c \right\} = \left\{ 2 pi over lambda \right\}$

where "k" is the wavenumber and λ is the wavelength.

The electromagnetic spectrum is a plot of the field magnitudes (or energies) as a function of wavelength.

Other solutions

Spherically symmetric and cylindrically symmetric analytic solutions to the electromagnetic wave equations are also possible.

In cylindrical coordinates the wave equation can be written as follows:

:$mathbf\left\{E\right\} \left( mathbf\left\{r\right\}, t \right) = \left\{mathbf\left\{E\right\}_0 cos\left( omega t - mathbf\left\{k\right\} cdot mathbf\left\{r\right\} + phi_0 \right)over s\right\}$and:$mathbf\left\{B\right\} \left( mathbf\left\{r\right\}, t \right) = \left\{mathbf\left\{B\right\}_0 cos\left( omega t - mathbf\left\{k\right\} cdot mathbf\left\{r\right\} + phi_0 \right)over s\right\}$

ee also

Theory and Experiment

* Maxwell's equations
* Wave equation
* Electromagnetic modeling
* Charge conservation
* Light
* Electromagnetic spectrum
* Optics
* Special relativity
* General relativity
* Photon dynamics in the double-slit experiment
* Photon polarization
* Larmor power formula
* Theoretical and experimental justification for the Schrödinger equation

Applications

* Rainbow
* Laser
* Laser fusion
* Photography
* X-ray
* X-ray crystallography
* Optical computing
* Microwave
* Holography
* Microscope
* Telescope
* Gravitational lens

Notes

References

Electromagnetism

Journal articles

* Maxwell, James Clerk, "", Philosophical Transactions of the Royal Society of London 155, 459-512 (1865). (This article accompanied a December 8, 1864 presentation by Maxwell to the Royal Society.)

*cite book | author=Griffiths, David J.|title=Introduction to Electrodynamics (3rd ed.)| publisher=Prentice Hall |year=1998 |id=ISBN 0-13-805326-X
*cite book | author=Tipler, Paul | title=Physics for Scientists and Engineers: Electricity, Magnetism, Light, and Elementary Modern Physics (5th ed.) | publisher=W. H. Freeman | year=2004 | id=ISBN 0-7167-0810-8
* Edward M. Purcell, "Electricity and Magnetism" (McGraw-Hill, New York, 1985). ISBN 0-07-004908-4.
* Hermann A. Haus and James R. Melcher, "Electromagnetic Fields and Energy" (Prentice-Hall, 1989) ISBN 0-13-249020-X.
* Banesh Hoffmann, "Relativity and Its Roots" (Freeman, New York, 1983). ISBN 0-7167-1478-7.
* David H. Staelin, Ann W. Morgenthaler, and Jin Au Kong, "Electromagnetic Waves" (Prentice-Hall, 1994) ISBN 0-13-225871-4.
* Charles F. Stevens, "The Six Core Theories of Modern Physics", (MIT Press, 1995) ISBN 0-262-69188-4.
* Markus Zahn, "Electromagnetic Field Theory: a problem solving approach", (John Wiley & Sons, 1979) ISBN 0-471-02198-9

*cite book |author=Jackson, John D.|title=Classical Electrodynamics (3rd ed.)|publisher=Wiley|year=1998|id=ISBN 0-471-30932-X
* Landau, L. D., "The Classical Theory of Fields" (Course of Theoretical Physics: Volume 2), (Butterworth-Heinemann: Oxford, 1987). ISBN 0-08-018176-7.
*cite book | author=Maxwell, James C. | title=A Treatise on Electricity and Magnetism | publisher=Dover | year=1954 | id=ISBN 0-486-60637-6
* Charles W. Misner, Kip S. Thorne, John Archibald Wheeler, "Gravitation", (1970) W.H. Freeman, New York; ISBN 0-7167-0344-0. "(Provides a treatment of Maxwell's equations in terms of differential forms.)"

Vector calculus

*P. C. Matthews "Vector Calculus", Springer 1998, ISBN 3-540-76180-2
*H. M. Schey, "Div Grad Curl and all that: An informal text on vector calculus", 4th edition (W. W. Norton & Company, 2005) ISBN 0-393-92516-1.

Biographies

* Andre Marie Ampere
* Albert Einstein
* Heinrich Hertz
* Oliver Heaviside
* James Clerk Maxwell

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