Editing Dipole

{{short description|Electromagnetic phenomenon}}
{{about|the electromagnetic phenomenon||dipole (disambiguation)}}
[[File:VFPt Dipole field.svg|thumb|right|250px|The magnetic field of a sphere with a north magnetic pole at the top and a  south magnetic pole at the bottom. By comparison, [[Earth's magnetic field|Earth]] has a ''south'' magnetic pole near its north geographic pole and a ''north'' magnetic pole near its South Pole.]]

In [[physics]], a '''dipole''' ({{etymology|grc|''{{Wikt-lang|grc|δίς}}'' ({{grc-transl|δίς}})|twice||''{{Wikt-lang|grc|πόλος}}'' ({{grc-transl|πόλος}})|axis}})<ref>[https://www.perseus.tufts.edu/hopper/text?doc=Perseus%3Atext%3A1999.04.0057%3Aentry%3Ddi%2Fs δίς], Henry George Liddell, Robert Scott, ''A Greek-English Lexicon'', on Perseus</ref><ref>[https://www.perseus.tufts.edu/hopper/text?doc=Perseus%3Atext%3A1999.04.0057%3Aentry%3Dpo%2Flos πόλος], Henry George Liddell, Robert Scott, ''A Greek-English Lexicon'', on Perseus</ref><ref>{{cite encyclopedia |title=dipole, n. |encyclopedia=[[Oxford English Dictionary]] |edition=2nd |publisher=[[Oxford University Press]] |year=1989}}</ref> is an [[electromagnetic]] phenomenon which occurs in two ways:
* An [[electric dipole moment|electric dipole]] deals with the separation of the positive and negative [[electric charge]]s found in any electromagnetic system. A simple example of this system is a pair of charges of equal magnitude but opposite sign separated by some typically small distance. (A permanent electric dipole is called an [[electret]].)
* A [[magnetic dipole]] is the closed circulation of an [[electric current]] system. A simple example is a single loop of wire with constant current through it. A [[bar magnet]] is an example of a magnet with a permanent [[magnetic dipole moment]].<ref>
{{cite book
 | last = Brau | first = Charles A.
 | title=Modern Problems in Classical Electrodynamics
 | publisher=Oxford University Press
 | year=2004
 | isbn=0-19-514665-4
}}</ref><ref name=":0">
{{cite book | last = Griffiths | first = David J. | title = Introduction to Electrodynamics | edition = 3rd | publisher = Prentice Hall | year = 1999 | isbn = 0-13-805326-X | url-access = registration | url = https://archive.org/details/introductiontoel00grif_0 }}
</ref>

Dipoles, whether electric or magnetic, can be characterized by their dipole moment, a vector quantity. For the simple electric dipole, the [[electric dipole moment]] points from the negative charge towards the positive charge, and has a magnitude equal to the strength of each charge times the separation between the charges. (To be precise: for the definition of the dipole moment, one should always consider the "dipole limit", where, for example, the distance of the generating charges should ''converge'' to 0 while simultaneously, the charge strength should ''diverge'' to infinity in such a way that the product remains a positive constant.)

For the magnetic (dipole) current loop, the [[magnetic dipole moment]] points through the loop (according to the [[right hand grip rule]]), with a magnitude equal to the current in the loop times the area of the loop.

Similar to magnetic current loops, the [[electron]] particle and some other [[fundamental particle]]s have magnetic dipole moments, as an electron generates a [[magnetic field]] identical to that generated by a very small current loop. However, an electron's magnetic dipole moment is not due to a current loop, but to an [[Intrinsic and extrinsic properties|intrinsic]] property of the electron.<ref>{{cite book|title=Introduction to Quantum Mechanics|last=Griffiths|first=David J.|publisher=Prentice Hall|year=1994|isbn=978-0-13-124405-4}}</ref> The electron may also have an ''electric'' dipole moment though such has yet to be observed (see [[electron electric dipole moment]]).
[[File:DipoleContourPoint.svg|thumb|right|250px|Contour plot of the [[Electrostatics#Electrostatic potential|electrostatic potential]] of a horizontally oriented electrical dipole of infinitesimal size. Strong colors indicate highest and lowest potential (where the opposing charges of the dipole are located).]]

A permanent magnet, such as a bar magnet, owes its magnetism to the intrinsic magnetic dipole moment of the electron. The two ends of a bar magnet are referred to as poles (not to be confused with [[magnetic monopole|monopoles]], see [[#Classification|Classification]] below) and may be labeled "north" and "south". In terms of the Earth's magnetic field, they are respectively "north-seeking" and "south-seeking" poles: if the magnet were freely suspended in the Earth's magnetic field, the north-seeking pole would point towards the north and the south-seeking pole would point towards the south. The dipole moment of the bar magnet points from its magnetic [[south pole|south]] to its magnetic [[north pole]]. In a magnetic [[compass]], the north pole of a bar magnet points north. However, that means that Earth's geomagnetic north pole is the ''south'' pole (south-seeking pole) of its dipole moment and vice versa.

The only known mechanisms for the creation of magnetic dipoles are by current loops or quantum-mechanical [[Spin (physics)|spin]] since the existence of [[magnetic monopole]]s has never been experimentally demonstrated.

== Classification ==
[[File:VFPt dipole electric.svg|thumb|250px|Electric field lines of two opposing charges separated by a finite distance.]]
[[File:VFPt dipole magnetic2.svg|250px|right|thumb|Magnetic field lines of a ring current of finite diameter.]]
[[File:VFPt dipole point.svg|thumb|250px|Field lines of a point dipole of any type, electric, magnetic, acoustic, etc.]]

A ''physical dipole'' consists of two equal and opposite point charges: in the literal sense, two poles. Its field at large distances (i.e., distances large in comparison to the separation of the poles) depends almost entirely on the dipole moment as defined above. A ''point (electric) dipole'' is the limit obtained by letting the separation tend to 0 while keeping the dipole moment fixed. The field of a point dipole has a particularly simple form, and the order-1 term in the [[multipole expansion]] is precisely the point dipole field.

Although there are no known [[magnetic monopole]]s in nature, there are magnetic dipoles in the form of the quantum-mechanical [[Spin (physics)|spin]] associated with particles such as [[electron]]s (although the accurate description of such effects falls outside of classical electromagnetism). A theoretical magnetic ''point dipole'' has a magnetic field of exactly the same form as the electric field of an electric point dipole. A very small current-carrying loop is approximately a magnetic point dipole; the magnetic dipole moment of such a loop is the product of the current flowing in the loop and the (vector) area of the loop.

Any configuration of charges or currents has a 'dipole moment', which describes the dipole whose field is the best approximation, at large distances, to that of the given configuration.  This is simply one term in the multipole expansion when the total charge ("monopole moment") is 0—as it ''always'' is for the magnetic case, since there are no magnetic monopoles.  The dipole term is the dominant one at large distances:  Its field falls off in proportion to {{sfrac|1|''r''<sup>3</sup>}}, as compared to {{sfrac|1|''r''<sup>4</sup>}} for the next ([[quadrupole]]) term and higher powers of {{sfrac|1|''r''}} for higher terms, or {{sfrac|1|''r''<sup>2</sup>}} for the monopole term.

== Molecular dipoles ==
<!-- This section is linked from [[Ammonia]] and redirects from [[Molecular dipole]] -->
{{See also|Chemical polarity|Dipole moments of molecules}}

Many [[molecule]]s have such dipole moments due to non-uniform distributions of positive and negative charges on the various atoms.  Such is the case with polar compounds like [[hydrogen fluoride]] (HF), where [[electron density]] is shared unequally between atoms. Therefore, a molecule's dipole is an [[electric dipole]] with an inherent electric field that should not be confused with a [[magnetic dipole]], which generates a magnetic field.

The physical chemist [[Peter Debye|Peter J. W. Debye]] was the first scientist to study molecular dipoles extensively, and, as a consequence, dipole moments are measured in the non-[[SI]] unit named ''[[debye]]'' in his honor.

For molecules there are three types of dipoles:
; Permanent dipoles: These occur when two atoms in a molecule have substantially different [[electronegativity]] : One atom attracts electrons more than another, becoming more negative, while the other atom becomes more positive. A molecule with a permanent dipole moment is called a ''polar'' molecule. See [[Intermolecular force#Dipole–dipole interactions|dipole–dipole attractions]].
; Instantaneous dipoles : These occur due to chance when [[electron]]s happen to be more concentrated in one place than another in a [[molecule]], creating a temporary dipole. These dipoles are smaller in magnitude than permanent dipoles, but still play a large role in chemistry and biochemistry due to their prevalence. See [[London dispersion force|instantaneous dipole]].
; Induced dipoles : These can occur when one molecule with a permanent dipole repels another molecule's electrons, ''inducing'' a dipole moment in that molecule. A molecule is ''polarized'' when it carries an induced dipole. See [[Intermolecular force#Debye (permanent–induced dipoles) force|induced-dipole attraction]].

More generally, an induced dipole of ''any'' polarizable charge distribution ''ρ'' (remember that a molecule has a charge distribution) is caused by an electric field external to ''ρ''. This field may, for instance, originate from an ion or polar molecule in the vicinity of ''ρ'' or may be macroscopic (e.g., a molecule between the plates of a charged [[capacitor]]). The size of the induced dipole moment is equal to the product of the strength of the external field and the dipole [[polarizability]] of ''ρ''.

Dipole moment values can be obtained from measurement of the [[dielectric constant]]. Some typical gas phase values given with the unit [[debye]] are:<ref>
{{cite book
 | last = Weast | first = Robert C.
 | title=CRC Handbook of Chemistry and Physics
 | edition = 65th
 | publisher=CRC Press
 | year=1984
 | isbn=0-8493-0465-2
}}</ref>
* [[carbon dioxide]]: 0
* [[carbon monoxide]]: 0.112&nbsp;D
* [[ozone]]: 0.53&nbsp;D
* [[phosgene]]: 1.17&nbsp;D
* [[ammonia]]: 1.42&nbsp;D
* [[water vapor]]: 1.85&nbsp;D
* [[hydrogen cyanide]]: 2.98&nbsp;D
* [[cyanamide]]: 4.27&nbsp;D
* [[potassium bromide]]: 10.41&nbsp;D

[[File:Carbon-dioxide-2D-dimensions.svg|thumb|160 px|The linear molecule CO<sub>2</sub> has a zero dipole as the two bond dipoles cancel.]]
Potassium bromide (KBr) has one of the highest dipole moments because it is an [[ionic compound]] that exists as a molecule in the gas phase.

[[File:H2O 2D labelled.svg|thumb|160 px|The bent molecule H<sub>2</sub>O has a net dipole. The two bond dipoles do not cancel.]]
The overall dipole moment of a molecule may be approximated as a [[Euclidean vector#Addition and subtraction|vector sum]] of [[bond dipole moment]]s. As a vector sum it depends on the relative orientation of the bonds, so that from the dipole moment information can be deduced about the [[molecular geometry]].

For example, the zero dipole of CO<sub>2</sub> implies that the two C=O bond dipole moments cancel so that the molecule must be linear. For H<sub>2</sub>O the O−H bond moments do not cancel because the molecule is bent. For ozone (O<sub>3</sub>) which is also a bent molecule, the bond dipole moments are not zero even though the O−O bonds are between similar atoms. This agrees with the Lewis structures for the resonance forms of ozone which show a positive charge on the central oxygen atom.

[[File:Ozone-resonance-Lewis-2D.svg|center|400px|Resonance Lewis structures of the ozone molecule]]
{{multiple image
 | align=right
 | image1=Cis-1,2-dichloroethene.png
 | width1=150
 | caption1=''Cis'' isomer, dipole moment 1.90&nbsp;D
 | image2=Trans-1,2-dichloroethene.png
 | width2=150
 | caption2=''Trans'' isomer, dipole moment zero
}}
An example in organic chemistry of the role of geometry in determining dipole moment is the [[cis–trans isomerism|''cis'' and ''trans'' isomers]] of [[1,2-dichloroethene]]. In the ''cis'' isomer the two polar C−Cl bonds are on the same side of the C=C double bond and the molecular dipole moment is 1.90&nbsp;D. In the ''trans'' isomer, the dipole moment is zero because the two C−Cl bonds are on opposite sides of the C=C and cancel (and the two bond moments for the much less polar C−H bonds also cancel).

Another example of the role of molecular geometry is [[boron trifluoride]], which has three polar bonds with a difference in [[electronegativity]] greater than the traditionally cited threshold of 1.7 for [[ionic bonding]]. However, due to the equilateral triangular distribution of the fluoride ions centered on and in the same plane as the boron cation, the symmetry of the molecule results in its dipole moment being zero.

== Quantum-mechanical dipole operator ==
Consider a collection of ''N'' particles with charges ''q<sub>i</sub>'' and position vectors '''r'''<sub>''i''</sub>. For instance, this collection may be a molecule consisting of electrons, all with [[electron charge|charge]] −''e'', and nuclei with charge ''eZ<sub>i</sub>'', where ''Z<sub>i</sub>'' is the [[atomic number]] of the ''i''&thinsp;th nucleus.
The dipole observable (physical quantity) has the quantum mechanical '''dipole operator''':{{citation needed|date=April 2015}}
: <math>\mathfrak{p} = \sum_{i=1}^N \, q_i \, \mathbf{r}_i \, .</math>

Notice that this definition is valid only for neutral atoms or molecules, i.e. total charge equal to zero. In the ionized case, we have
: <math>\mathfrak{p} = \sum_{i=1}^N \, q_i \, (\mathbf{r}_i - \mathbf{r}_c) ,</math>
where <math> \mathbf{r}_c</math> is the center of mass of the molecule/group of particles.<ref>{{Cite web|url=http://www.av8n.com/physics/electric-dipole.htm#eq-dipole-ref|title = The Electric Dipole Moment Vector -- Direction, Magnitude, Meaning, et cetera}}</ref>

== Atomic dipoles ==
<!-- This section is linked from [[Intermolecular force]] -->
A non-degenerate (''S''-state) atom can have only a zero permanent dipole. This fact follows quantum mechanically from the inversion symmetry of atoms. All 3 components of the dipole operator are antisymmetric under [[Inversion in a point|inversion]] with respect to the nucleus,
: <math> \mathfrak{I} \;\mathfrak{p}\;  \mathfrak{I}^{-1} = -\mathfrak{p}, </math>
where <math>\mathfrak{p}</math> is the dipole operator  and <math>\mathfrak{I}</math> is the inversion operator.

The permanent dipole moment  of an atom in a non-degenerate state (see [[degenerate energy level]]) is given as the expectation (average) value of the dipole operator,
: <math>\left\langle \mathfrak{p} \right\rangle = \left\langle\, S\, | \mathfrak{p} |\, S \,\right\rangle,</math>
where <math> |\, S\, \rangle </math> is an ''S''-state, non-degenerate, wavefunction, which is symmetric or antisymmetric under inversion: <math> \mathfrak{I}\, |\, S\, \rangle = \pm|\, S\, \rangle</math>. Since the product of the wavefunction (in the ket) and its complex conjugate (in the bra) is always symmetric under inversion and its inverse,
: <math>
   \left\langle \mathfrak{p} \right\rangle =
   \left\langle\, \mathfrak{I}^{-1}\, S\, | \mathfrak{p} |\, \mathfrak{I}^{-1}\, S\, \right\rangle =
   \left\langle\, S\, | \mathfrak{I}\, \mathfrak{p}\, \mathfrak{I}^{-1} |\, S\, \right\rangle =
  -\left\langle \mathfrak{p} \right\rangle
</math>
it follows that the expectation value changes sign under inversion.  We used here the fact that <math> \mathfrak{I}</math>, being a symmetry operator, is [[unitary operator|unitary]]: <math> \mathfrak{I}^{-1} =  \mathfrak{I}^{*}\,</math> and [[Hermitian adjoint#Definition for bounded operators between Hilbert spaces|by definition]] the Hermitian adjoint <math> \mathfrak{I}^*\,</math> may be moved from bra to ket and then becomes <math> \mathfrak{I}^{**} = \mathfrak{I}\,</math>. Since the only quantity that is equal to minus itself is the zero, the expectation  value vanishes,
: <math>\left\langle \mathfrak{p} \right\rangle = 0.</math>

In the case of open-shell atoms with degenerate  energy levels, one could define a dipole moment by the aid of the first-order [[Stark effect]]. This gives a non-vanishing dipole (by definition proportional to a non-vanishing first-order Stark shift) only if some of the wavefunctions belonging to the degenerate energies have opposite [[parity (physics)|parity]]; i.e., have different behavior under inversion. This is a rare occurrence, but happens for the excited H-atom, where 2s and 2p states are "accidentally" degenerate (see article [[Laplace–Runge–Lenz vector#Quantum mechanics of the hydrogen atom|Laplace–Runge–Lenz vector]] for the origin of this degeneracy) and have opposite parity (2s is even and 2p is odd).

== Field of a static magnetic dipole ==
{{see also|Magnet#Two models for magnets: magnetic poles and atomic currents}}

=== Magnitude ===
The far-field strength, ''B'', of a dipole magnetic field is given by
: <math>B(m, r, \lambda) = \frac{\mu_0}{4\pi} \frac{m}{r^3} \sqrt{1 + 3\sin^2(\lambda)} \, ,</math>
where
: ''B'' is the strength of the field, measured in [[tesla (unit)|tesla]]s
: ''r'' is the distance from the center, measured in metres
: ''λ'' is the magnetic latitude (equal to 90°&nbsp;−&nbsp;''θ'') where ''θ'' is the magnetic colatitude, measured in [[radian]]s or [[degree (angle)|degree]]s from the dipole axis<ref group="note">Magnetic colatitude is 0 along the dipole's axis and 90° in the plane perpendicular to its axis.</ref>
: ''m'' is the dipole moment, measured in [[ampere]]-square metres or [[joule]]s per [[tesla (unit)|tesla]]
: ''μ''<sub>0</sub> is the [[permeability (electromagnetism)|permeability of free space]], measured in [[henry (unit)|henries]] per metre.

Conversion to cylindrical coordinates is achieved using {{nowrap|''r''<sup>2</sup> {{=}} ''z''<sup>2</sup> + ''ρ''<sup>2</sup>}} and
: <math>\lambda = \arcsin\left(\frac{z}{\sqrt{z^2 + \rho^2}}\right)</math>
where ''ρ'' is the perpendicular distance from the ''z''-axis. Then,
: <math>B(\rho, z) = \frac{\mu_0 m}{4 \pi \left(z^2 + \rho^2\right)^\frac32} \sqrt{1 + \frac{3 z^2}{z^2 + \rho^2}}</math>

=== Vector form ===
The field itself is a vector quantity:
: <math>\mathbf{B}(\mathbf{m}, \mathbf{r}) =
  \frac{\mu_0}{4\pi} \ \frac{3(\mathbf{m} \cdot \hat{\mathbf{r}}) \hat{\mathbf{r}} - \mathbf{m}}{r^3}
  </math>
where
: '''B''' is the field
: '''r''' is the vector from the position of the dipole to the position where the field is being measured
: ''r'' is the absolute value of '''r''': the distance from the dipole
: '''r̂''' = {{sfrac|'''r'''|''r''}} is the unit vector parallel to '''r''';
: '''m''' is the (vector) dipole moment
: ''μ''<sub>0</sub> is the permeability of free space

This is ''exactly'' the field of a point dipole, ''exactly'' the dipole term in the multipole expansion of an arbitrary field, and ''approximately'' the field of any dipole-like configuration at large distances.

=== Magnetic vector potential ===
The [[vector potential]] '''A''' of a magnetic dipole is
: <math>\mathbf{A}(\mathbf{r}) = \frac{\mu_0}{4\pi} \frac{\mathbf{m} \times \hat{\mathbf{r}}}{r^2}</math>
with the same definitions as above.

== Field from an electric dipole ==
<!-- This section is linked from [[Intermolecular force]] -->
The [[electrostatic potential]] at position '''r''' due to an electric dipole at the origin is given by:
: <math> \Phi(\mathbf{r}) = \frac{1}{4\pi\epsilon_0}\,\frac{\mathbf{p}\cdot\hat{\mathbf{r}}}{r^2}</math>
where '''p''' is the (vector) [[Electric dipole moment|dipole moment]], and ''є''<sub>0</sub> is the [[permittivity of free space]].

This term appears as the second term in the [[Multipole expansion#Expansion in Cartesian coordinates|multipole expansion]] of an arbitrary electrostatic potential Φ('''r'''). If the source of Φ('''r''') is a dipole, as it is assumed here, this term is  the only non-vanishing term in the multipole expansion of Φ('''r'''). The [[electric field]] from a dipole can be found from the [[gradient]] of this potential:
: <math> \mathbf{E} = - \nabla \Phi =\frac {1} {4\pi\epsilon_0} \ \frac{3(\mathbf{p}\cdot\hat{\mathbf{r}})\hat{\mathbf{r}}-\mathbf{p}}{r^3} - \delta^3(\mathbf{r})\frac{\mathbf{p}}{3\epsilon_0}.</math>

This is of the same form of the expression for the magnetic field of a point magnetic dipole, ignoring the delta function. 
In a real electric dipole, however, the charges are physically separate and the electric field diverges or converges at the point charges. 
This is different to the magnetic field of a real magnetic dipole which is continuous everywhere. The delta function represents the strong field pointing in the opposite direction between the point charges, which is often omitted since one is rarely interested in the field at the dipole's position. 
For further discussions about the internal field of dipoles, see<ref name=":0" /><ref>{{Cite book|title=Classical Electrodynamics, 3rd Ed.|last=Jackson|first=John D.|publisher=Wiley|year=1999|isbn=978-0-471-30932-1|pages=148–150}}</ref> or ''{{slink|Magnetic moment#Internal magnetic field of a dipole}}''.

== Torque on a dipole ==
Since the direction of an [[electric field]] is defined as the direction of the force on a positive charge, electric field lines point away from a positive charge and toward a negative charge.

When placed in a homogeneous [[electric field|electric]] or [[magnetic field]], equal but opposite [[force]]s arise on each side of the dipole creating a [[torque]] {{math|'''&tau;'''}}}:
: <math> \boldsymbol{\tau} = \mathbf{p} \times \mathbf{E}</math>
for an [[electrical dipole moment|electric dipole moment]] '''p''' (in coulomb-meters), or
: <math> \boldsymbol{\tau} = \mathbf{m} \times \mathbf{B}</math>
for a [[magnetic dipole moment]] '''m''' (in ampere-square meters).

The resulting torque will tend to align the dipole with the applied field, which in the case of an electric dipole, yields a potential energy of
: <math> U = -\mathbf{p} \cdot \mathbf{E}</math>.

The energy of a magnetic dipole is similarly
: <math> U = -\mathbf{m} \cdot \mathbf{B}</math>.

== Dipole radiation ==
[[File:Electric dipole radiation.gif|thumb|Modulus of the Poynting vector for an oscillating electric dipole (exact solution). The two charges are shown as two small black dots.]]
<!-- use of the far-field approximation for the near field yielded incorrect results, see archived discussion
[[File:dipole.gif|thumb|right|250px|Evolution of the magnetic field of an oscillating electric dipole. The field lines, which are horizontal rings around the axis of the vertically oriented dipole, are perpendicularly crossing the ''xy''-plane of the image. Shown as a colored [[Contour line|contour plot]] is the ''z''-component of the field. Cyan is zero magnitude, green–yellow–red and blue–pink–red are increasing strengths in opposing directions.]] -->
{{see also|Dipole antenna}}
In addition to dipoles in electrostatics, it is also common to consider an electric or magnetic dipole that is oscillating in time. It is an extension, or a more physical next-step, to [[spherical wave]] radiation.

In particular, consider a harmonically oscillating electric dipole, with [[angular frequency]] ''ω'' and a dipole moment ''p''<sub>0</sub> along the '''ẑ''' direction of the form
: <math>\mathbf{p}(\mathbf{r}, t) = \mathbf{p}(\mathbf{r})e^{-i\omega t} = p_0\hat{\mathbf{z}}e^{-i\omega t} .</math>

In vacuum, the exact field produced by this oscillating dipole can be derived using the [[retarded potential]] formulation as:
: <math>\begin{align}
  \mathbf{E} &= \frac{1}{4\pi\varepsilon_0} \left\{
      \frac{\omega^2}{c^2 r} \left( \hat{\mathbf{r}} \times \mathbf{p} \right) \times \hat{\mathbf{r}} +
      \left( \frac{1}{r^3} - \frac{i\omega}{cr^2} \right)
        \left( 3\hat{\mathbf{r}} \left[\hat{\mathbf{r}} \cdot \mathbf{p}\right] - \mathbf{p} \right)
    \right\} e^\frac{i\omega r}{c} e^{-i\omega t} \\
  \mathbf{B} &= \frac{\omega^2}{4\pi\varepsilon_0 c^3} (\hat{\mathbf{r}} \times \mathbf{p}) \left( 1 - \frac{c}{i\omega r} \right) \frac{e^{i\omega r/c}}{r} e^{-i\omega t}.
\end{align}</math>

For {{sfrac|''rω''|''c''}}&nbsp;≫&nbsp;1, the far-field takes the simpler form of a radiating "spherical" wave, but with angular dependence embedded in the cross-product:<ref>[[David J. Griffiths]], Introduction to Electrodynamics, Prentice Hall, 1999, page 447</ref>
: <math>\begin{align}
  \mathbf{B}
    &=  \frac{\omega^2}{4\pi\varepsilon_0 c^3} (\hat{\mathbf{r}} \times \mathbf{p}) \frac{e^{i\omega (r/c - t)}}{r}
     =  \frac{\omega^2 \mu_0 p_0 }{4\pi c} (\hat{\mathbf{r}} \times \hat{\mathbf{z}}) \frac{e^{i\omega (r/c - t)}}{r}
     = -\frac{\omega^2 \mu_0 p_0 }{4\pi c} \sin(\theta) \frac{e^{i\omega (r/c - t)}}{r} \mathbf{\hat{\phi}} \\
  \mathbf{E}
    &=  c \mathbf{B} \times \hat{\mathbf{r}}
     = -\frac{\omega^2 \mu_0 p_0}{4\pi} \sin(\theta) \left(\hat{\phi} \times \mathbf{\hat{r}}\right) \frac{e^{i\omega (r/c - t)}}{r}
     = -\frac{\omega^2 \mu_0 p_0}{4\pi} \sin(\theta) \frac{e^{i\omega (r/c - t)}}{r} \hat{\theta}.
\end{align}</math>

The time-averaged [[Poynting vector]]
: <math>\langle \mathbf{S} \rangle = \left(\frac{\mu_0 p_0^2\omega^4}{32\pi^2 c}\right) \frac{\sin^2(\theta)}{r^2} \mathbf{\hat{r}}</math>
is not distributed isotropically, but concentrated around the directions lying perpendicular to the dipole moment, as a result of the non-spherical electric and magnetic waves. In fact, the [[spherical harmonic]] function (sin ''θ'') responsible for such [[torus|toroidal]] angular distribution is precisely the ''l''&nbsp;=&nbsp;1 "p" wave.

The total time-average power radiated by the field can then be derived from the Poynting vector as
: <math>P = \frac{\mu_0 \omega^4 p_0^2}{12\pi c}.</math>

Notice that the dependence of the power on the fourth power of the frequency of the radiation is in accordance with the [[Rayleigh scattering]], and the underlying effects why the sky consists of mainly blue colour.

A circular polarized dipole is described as a superposition of two linear dipoles.

== See also ==
* [[Polarization density]]
* [[Magnet#Two models for magnets: magnetic poles and atomic currents|Magnetic dipole models]]
* [[Dipole model of the Earth's magnetic field]]
* [[Electret]]
* [[Indian Ocean Dipole]] and [[Subtropical Indian Ocean Dipole]], two oceanographic phenomena
* [[Magnetic dipole–dipole interaction]]
* [[Spin magnetic moment]]
* [[Magnetic monopole|Monopole]]
* [[Solid harmonics]]
* [[Axial multipole moments]]
* [[Cylindrical multipole moments]]
* [[Spherical multipole moments]]
* [[Laplace expansion (potential)|Laplace expansion]]
* [[Molecular solid]]
* [[Magnetic moment#Internal magnetic field of a dipole]]

== Notes ==
{{reflist|group="note"}}

== References ==
{{reflist}}

== External links ==
* [https://geomag.usgs.gov USGS Geomagnetism Program]
* [https://lightandmatter.com/html_books/4em/ch05/ch05.html Fields of Force] {{Webarchive|url=https://web.archive.org/web/20101214091300/http://lightandmatter.com/html_books/4em/ch05/ch05.html |date=2010-12-14 }}: a chapter from an online textbook
* [https://demonstrations.wolfram.com/ElectricDipolePotential/ Electric Dipole Potential] by [[Stephen Wolfram]] and [http://demonstrations.wolfram.com/EnergyDensityOfAMagneticDipole/ Energy Density of a Magnetic Dipole] by Franz Krafft. [[Wolfram Demonstrations Project]].

[[Category:Electromagnetism]]
[[Category:Potential theory]]