View source for Near and far field

{{Short description|Regions of an electromagnetic field}}
{{About|the electromagnetic concept|the mathematical|Near-field (mathematics)}}
{{Redirect|Far field}}
[[File:FarNearFields-USP-4998112-1.svg|thumb|265px|Order of the [[Fraunhofer diffraction]] (inner, ''reactive near field'') and [[Fresnel diffraction]] (outer, ''radiative near field'') regions, relative to the ''far field''.]]
{{Antennas|sources/regions}}

The '''near field''' and '''far field''' are regions of the [[electromagnetic field|electromagnetic (EM) field]] around an object, such as a transmitting [[antenna (radio)|antenna]], or the result of radiation scattering off an object. Non-radiative ''near-field'' behaviors dominate close to the antenna or scatterer, while [[electromagnetic radiation]] ''far-field'' behaviors predominate at greater distances.

'''Far-field''' {{math|'''E'''}} (electric) and {{math|'''B'''}} (magnetic) radiation field strengths decrease as the distance from the source increases, resulting in an [[inverse-square law]] for the ''[[power (physics)|power]]'' intensity of [[electromagnetic radiation]] in the transmitted signal. By contrast, the '''near-field'''{{'}}s {{math|'''E'''}} and {{math|'''B'''}} strengths decrease more rapidly with distance: The radiative field decreases by the [[inverse-square law|inverse-distance squared]], the reactive field by an inverse-''cube'' law, resulting in a diminished power in the parts of the electric field by an inverse fourth-power and sixth-power, respectively. The rapid drop in power contained in the near-field ensures that effects due to the near-field essentially vanish a few wavelengths away from the radiating part of the antenna, and conversely ensure that at distances a small fraction of a wavelength from the antenna, the near-field effects overwhelm the radiating far-field.

==Summary of regions and their interactions==
[[File:Felder um Dipol.svg|thumb|200px|'''Near field''': This dipole pattern shows a magnetic field {{math|'''B'''}} in red. The potential energy momentarily stored in this magnetic field is indicative of the reactive near field.]]
[[File:Sidelobes en.svg|thumb|200px|'''Far field:''' The radiation pattern can extend into the far field, where the reactive stored energy has no significant presence.]]

In a normally-operating antenna, positive and negative charges have no way of leaving the metal surface, and are separated from each other by the excitation "signal" voltage (a transmitter or other EM exciting potential). This generates an oscillating (or reversing) electrical dipole, which affects both the near field and the far field.

The boundary between the ''near field'' and ''far field'' regions is only vaguely defined, and it depends on the dominant [[wavelength]] ({{mvar|λ}}) emitted by the source and the size of the radiating element.

===Near field===
The ''near field'' refers to places nearby the antenna conductors, or inside any polarizable media surrounding it, where the generation and emission of electromagnetic waves can be interfered with while the field lines remain electrically attached to the antenna, hence absorption of radiation in the near field by adjacent conducting objects detectably affects the loading on the signal generator (the transmitter). The electric and magnetic fields can exist independently of each other in the near field, and one type of field can be disproportionately larger than the other, in different subregions.

:An easy-to-observe example of a near-field effect is the change of noise levels picked up by a set of [[dipole antenna#"Rabbit ears" TV antenna|rabbit ear TV antennas]] when a human body part is moved in close to the "ears". Likewise the change in sound quality of an FM radio tuned to a distant station when a person walks about in the area within an arm's length of its antenna.

The near field is governed by [[multipole radiation |multipole type fields]], which can be considered as collections of dipoles with a fixed [[phase (waves)|phase relationship]].
The general purpose of [[antenna (radio)|conventional antennas]] is to communicate wirelessly over long distances, well into their far fields, and for calculations of radiation and reception for many simple antennas, most of the complicated effects in the near field can be conveniently ignored.

====Reactive near field====
The interaction with the medium (e.g. body capacitance) can cause energy to deflect back to the source feeding the antenna, as occurs in the ''reactive'' near field. This zone is roughly within {{sfrac|1|6}} of a wavelength of the nearest antenna surface.

The near field has been of increasing interest, particularly in the development of [[capacitive sensing]] technologies such as those used in the touchscreens of smart phones and tablet computers. Although the far field is the usual region of antenna function, certain devices that are called ''antennas'' but are specialized for [[near-field communication]] do exist. [[Electromagnetic induction|Magnetic induction]] as seen in a [[transformer]] can be seen as a very simple example of this type of near-field electromagnetic interaction.
For example send / receive coils for [[Radio-frequency identification|RFID]], and emission coils for [[inductive charging|wireless charging]] and [[induction heating|inductive heating]]; however their technical classification as "antennas" is contentious.

====Radiative near field====
The interaction with the medium can fail to return energy back to the source, but cause a distortion in the electromagnetic wave that deviates significantly from that found in free space, and this indicates the ''radiative'' near-field region, which is somewhat further away. Passive reflecting elements can be placed in this zone for the purpose of beam forming, such as the case with the [[Yagi–Uda antenna]]. Alternatively, multiple active elements can also be combined to form an antenna array, with lobe shape becoming a factor of element distances and excitation phasing.

===Transition zone===
Another intermediate region, called the ''transition zone'', is defined on a somewhat different basis, namely antenna geometry and excitation wavelength. It is approximately one wavelength from the antenna, and is where the electric and magnetic parts of the radiated waves first balance out: The electric field of a [[dipole antenna|linear antenna]] gains its corresponding magnetic field, and the magnetic field of a [[loop antenna]] gains its electric field. It can either be considered the furthest part of the near field, or the nearest part of the far field. It is from beyond this point that the electromagnetic wave becomes self-propagating. The electric and magnetic field portions of the wave are proportional to each other at a ratio defined by the characteristic impedance of the medium through which the wave is propagating.

===Far field===
In contrast, the ''far field'' is the region in which the field has settled into "normal" [[electromagnetic radiation]]. In this region, it is dominated by transverse [[electric field|electric]] or [[magnetic field]]s with [[dipole|electric dipole]] characteristics.
In the far-field region of an antenna, radiated power decreases as the [[inverse-square law|square of distance]], and [[absorption (electromagnetic radiation)|absorption of the radiation]] does not feed back to the transmitter.

In the far-field region, each of the electric and magnetic parts of the EM field is "produced by" (or associated with) a change in the other part, and the ratio of electric and magnetic field intensities is simply the [[wave impedance]] in the medium.

Also known as the ''radiation-zone'', the far field carries a relatively uniform wave pattern. The radiation zone is important because far fields in general fall off in amplitude by <math>\ \tfrac{1}{r}\ .</math> This means that the total energy per unit area at a distance {{mvar|r}} is proportional to <math>\ \tfrac{1}{r^2}\ .</math> The area of the sphere is proportional to <math>r^2</math>, so the total energy passing through the sphere is constant. This means that the far-field energy actually escapes to infinite distance (it ''radiates'').

==Definitions==
The separation of the electric and magnetic fields into components is mathematical, rather than clearly physical, and is based on the relative rates at which the amplitude of different terms of the electric and magnetic field equations diminish as distance from the radiating element increases. The amplitudes of the far-field components fall off as <math>1/r</math>, the ''radiative'' near-field amplitudes fall off as <math>1/r^2</math>, and the ''reactive'' near-field amplitudes fall off as <math>1/r^3</math>.{{efn|name=power_vs_amplitude|Amplitude fall-off is not to be confused with the ''power'' fall-off; power falls off as the amplitude squared.}} Definitions of the ''regions'' attempt to characterize locations where the activity of the associated field ''components'' are the strongest. Mathematically, the distinction between ''field components'' is very clear, but the demarcation of the spatial ''field regions'' is subjective. All of the field components overlap everywhere, so for example, there are always substantial far-field and radiative near-field components in the closest-in near-field reactive region.

The regions defined below categorize field behaviors that are variable, even within the region of interest. Thus, the boundaries for these regions are approximate [[rules of thumb]], as there are no precise cutoffs between them: All behavioral changes with distance are smooth changes. Even when precise boundaries can be defined in some cases, based primarily on antenna type and antenna size, experts may differ in their use of nomenclature to describe the regions. Because of these nuances, special care must be taken when interpreting technical literature that discusses far-field and near-field regions.

The term ''near-field region'' (also known as the ''near field'' or ''near zone'') has the following meanings with respect to different [[telecommunications]] technologies:
* The close-in region of an [[antenna (radio)|antenna]] where the angular [[field (physics)|field]] distribution is dependent upon the distance from the antenna.
* In the study of diffraction and antenna design, the near field is that part of the radiated field that is below distances shorter than the [[Fraunhofer distance]],<ref>{{cite book |title=Antenna Theory: Analysis and Design |first=Constantine A. |last=Balanis |edition=3rd |year=2005 |at=Chapter&nbsp;2, page&nbsp;34}}</ref> which is given by <math>d_\text{F} = \frac{2 D^2}{\lambda}</math> from the source of the diffracting edge or antenna of longitude or diameter {{mvar|D}}.
* In [[fiber-optic communication]], the region near a source or [[aperture]] that is closer than the [[Rayleigh length]]. (Presuming a Gaussian beam, which is appropriate for fiber optics.)

===Regions according to electromagnetic length===
The most convenient practice is to define the size of the regions or zones in terms of fixed numbers (fractions) of wavelengths distant from the center of the radiating part of the antenna, with the clear understanding that the values chosen are only approximate and will be somewhat inappropriate for different antennas in different surroundings. The choice of the cut-off numbers is based on the relative strengths of the field component amplitudes typically seen in ordinary practice.

====Electromagnetically short antennas====
[[File:Field regions for typical antennas vector.svg|thumb|left|500px|alt=Antenna field regions for antennas that are equal to, or shorter than, one-half wavelength of the radiation they emit, such as the whip antenna of a citizen's band radio, or the antenna in an AM radio broadcast tower.|Field regions for antennas equal to, or shorter than, one-half wavelength of the radiation they emit, such as the whip antenna of a citizen's band radio, or an AM radio broadcast tower.]]
{{Clear}}

For antennas shorter than half of the wavelength of the radiation they emit (i.e., electromagnetically "short" antennas), the far and near regional boundaries are measured in terms of a simple ratio of the distance {{mvar|r}} from the [[radio frequency|radiating source]] to the [[wavelength]] {{mvar|λ}} of the radiation. For such an antenna, the near field is the region within a radius {{math|''r'' ≪ ''λ''}}, while the far-field is the region for which {{math|''r'' ≫ 2 ''λ''}}. The transition zone is the region between {{math|''r'' {{=}} ''λ''}} and {{math|''r'' {{=}} 2 ''λ'' }}.

The length of the antenna, {{mvar|''D''}}, is not important, and the approximation is the same for all shorter antennas (sometimes idealized as so-called ''point antennas''). In all such antennas, the short length means that charges and currents in each sub-section of the antenna are the same at any given time, since the antenna is too short for the RF transmitter voltage to reverse before its effects on charges and currents are felt over the entire antenna length.

====Electromagnetically long antennas====
For antennas physically larger than a half-wavelength of the radiation they emit, the near and far fields are defined in terms of the '''[[Fraunhofer distance]]'''. Named after [[Joseph von Fraunhofer]], the following formula gives the [[Fraunhofer distance]]:
:<math display=block>d_\text{F} \; = \; \frac{2 D^2}{\lambda} \, ,</math>

where {{mvar|D}} is the largest dimension of the radiator (or the [[diameter]] of the [[Antenna (radio)|antenna]]) and {{mvar|λ}} is the [[wavelength]] of the radio [[wave]]. Either of the following two relations are equivalent, emphasizing the size of the region in terms of wavelengths {{math|λ}} or diameters {{math|D}}:
:<math display=block>d_\text{F} \; = \; 2 { \left( { D \over \lambda } \right) }^2 \lambda \; = \; 2 { \left( { D \over \lambda } \right) } D</math>

This distance provides the limit between the near and far field. The parameter {{mvar|D}} corresponds to the physical length of an antenna, or the diameter of a reflector ("dish") antenna.

Having an antenna electromagnetically longer than one-half the dominated wavelength emitted considerably extends the near-field effects, especially that of focused antennas. Conversely, when a given antenna emits high frequency radiation, it will have a near-field region larger than what would be implied by a lower frequency (i.e. longer wavelength).

Additionally, a far-field region distance {{math|''d''<sub>F</sub>}} must satisfy these two conditions.<ref>{{cite book |author=Rappaport, Theodore S. |title=Wireless Communications Principles and Practice |edition=19th printing, 2nd |publisher=Prentice-Hall |year=2010 |page=108}}</ref>{{Clarify|reason=These are imprecise, dumbed-down versions of what has been said more clearly above.|date=May 2015}}
:<math display=block>d_\text{F} \gg D\,</math>
:<math display=block>d_\text{F} \gg \lambda\,</math>

where {{mvar|D}} is the largest physical linear dimension of the antenna and {{math|''d''<sub>F</sub>}} is the far-field distance. The far-field distance is the distance from the transmitting antenna to the beginning of the Fraunhofer region, or far field.

====Transition zone====
The ''transition zone'' between these near and far field regions, extending over the distance from one to two wavelengths from the antenna,{{citation needed|date=December 2011}} is the intermediate region in which both near-field and far-field effects are important. In this region, near-field behavior dies out and ceases to be important, leaving far-field effects as dominant interactions. (See the "Far Field" image above.)

===Regions according to diffraction behavior===
[[File:FarNearFields-USP-4998112.svg|thumb|left|500px |alt=Near- and far-field regions for an antenna larger (diameter or length {{mvar|D}}) than the wavelength of the radiation it emits, so that {{math|{{frac|''D''|λ}} ≫ 1}}. Examples are radar dishes and other highly directional antennas. |Near- and far-field regions for an antenna larger (diameter or length {{mvar|D}}) than the wavelength of the radiation it emits, so that {{math|{{frac|''D''|λ}} ≫ 1}}. Examples are radar dishes, satellite dish antennas, radio telescopes, and other highly directional antennas.]]
{{clear}}

====Far-field diffraction====
{{Main|Fraunhofer diffraction}}
As far as acoustic wave sources are concerned, if the source has a maximum overall dimension or aperture width ({{mvar|D}}) that is large compared to the wavelength {{mvar|λ}}, the far-field region is commonly taken to exist at distances, when the Fresnel parameter <math>S</math> is larger than 1:<ref>{{cite book |title=Acoustic Waves: Devices, imaging, and analog signal processing |editor=Kino, G. |publisher=Prentice Hall |year=2000 |at=Chapter&nbsp;3, page&nbsp;165}}</ref>
:<math display=block>S = {4\lambda \over D^2} r > 1, \text{ for } r > r_\text{F} = {D^2 \over 4\lambda}.</math>

For a [[light beam|beam]] focused at infinity, the far-field region is sometimes referred to as the ''Fraunhofer region''. Other synonyms are ''far field'', ''far zone'', and ''radiation field''. Any [[electromagnetic radiation]] consists of an [[electric field]] component {{math|'''E'''}} and a [[magnetic field]] component {{math|'''H'''}}. In the far field, the relationship between the electric field component {{math|'''E'''}} and the magnetic component {{math|'''H'''}} is that characteristic of any freely propagating wave, where {{math|'''E'''}} and {{math|'''H'''}} have equal [[Euclidean vector#Length|magnitudes]] at any point in space (where measured in units where [[speed of light|{{math|''c'']] {{=}} 1}}).

====Near-field diffraction====
{{Main|Fresnel diffraction}}
In contrast to the far field, the [[diffraction]] pattern in the near field typically differs significantly from that observed at infinity and varies with distance from the source. In the near field, the relationship between {{math|'''E'''}} and {{math|'''H'''}} becomes very complex. Also, unlike the far field where [[electromagnetic wave]]s are usually characterized by a single [[polarization (waves)|polarization]] type (horizontal, vertical, circular, or elliptical), all four polarization types can be present in the near field.<ref name=OSHA-EM-rad/>

The near field is a region in which there are strong inductive and capacitive effects from the currents and charges in the antenna that cause electromagnetic components that do not behave like far-field radiation. These effects decrease in power far more quickly with distance than do the far-field radiation effects. Non-propagating (or evanescent) fields extinguish very rapidly with distance, which makes their effects almost exclusively felt in the near-field region.

Also, in the part of the near field closest to the antenna (called the ''reactive near field'', [[#Reactive near field, or the nearest part of the near field|see below]]), absorption of electromagnetic power in the region by a second device has effects that feed back to the transmitter, increasing the load on the transmitter that feeds the antenna by decreasing the antenna impedance that the transmitter "sees". Thus, the transmitter can sense when power is being absorbed in the closest near-field zone (by a second antenna or some other object) and is forced to supply extra power to its antenna, and to draw extra power from its own power supply, whereas if no power is being absorbed there, the transmitter does not have to supply extra power.

==Near-field characteristics==

The near field itself is further divided into the ''reactive'' near field and the ''radiative'' near field. The ''reactive'' and ''radiative'' near-field designations are also a function of wavelength (or distance). However, these boundary regions are a fraction of one wavelength within the near field. The outer boundary of the reactive near-field region is commonly considered to be a distance of <math display="inline">\frac{1}{2\pi}</math> times the wavelength (i.e., <math display="inline">\frac{\lambda}{2\pi}</math> or approximately {{math|0.159λ}}) from the antenna surface. The reactive near-field is also called the ''inductive'' near-field. The radiative near field (also called the ''Fresnel region'') covers the remainder of the near-field region, from <math display="inline">\frac{\lambda}{2\pi}</math> out to the Fraunhofer distance.<ref name=OSHA-EM-rad/>

===Reactive near field, or the nearest part of the near field===
In the reactive near field (very close to the antenna), the relationship between the strengths of the {{math|'''E'''}} and {{math|'''H'''}} fields is often too complicated to easily predict, and difficult to measure. Either field component ({{math|'''E'''}} or {{math|'''H'''}}) may dominate at one point, and the opposite relationship dominate at a point only a short distance away. This makes finding the true [[power density]] in this region problematic. This is because to calculate power, not only {{math|'''E'''}} and {{math|'''H'''}} both have to be measured but the [[phase (waves)|phase relationship]] between {{math|'''E'''}} and {{math|'''H'''}} as well as the angle between the two vectors must also be known in every point of space.<ref name=OSHA-EM-rad/>

In this reactive region, not only is an electromagnetic wave being radiated outward into far space but there is a reactive component to the electromagnetic field, meaning that the strength, direction, and phase of the electric and magnetic fields around the antenna are sensitive to EM absorption and re-emission in this region, and respond to it. In contrast, absorption far from the antenna has negligible effect on the fields near the antenna, and causes no back-reaction in the transmitter.

Very close to the antenna, in the reactive region, [[energy]] of a certain amount, if not absorbed by a receiver, is held back and is stored very near the antenna surface. This energy is carried back and forth from the antenna to the reactive near field by electromagnetic radiation of the type that slowly changes [[electrostatic]] and magnetostatic effects. For example, current flowing in the antenna creates a purely magnetic component in the near field, which then collapses as the antenna current begins to reverse, causing transfer of the field's magnetic energy back to electrons in the antenna as the changing magnetic field causes a self-inductive effect on the antenna that generated it. This returns energy to the antenna in a regenerative way, so that it is not lost. A similar process happens as electric charge builds up in one section of the antenna under the pressure of the signal voltage, and causes a local electric field around that section of antenna, due to the antenna's [[self-capacitance]]. When the signal reverses so that charge is allowed to flow away from this region again, the built-up electric field assists in pushing electrons back in the new direction of their flow, as with the discharge of any unipolar capacitor. This again transfers energy back to the antenna current.

Because of this energy storage and return effect, if either of the inductive or electrostatic effects in the reactive near field transfer any field energy to electrons in a different (nearby) conductor, then this energy is lost to the primary antenna. When this happens, an extra drain is seen on the transmitter, resulting from the reactive near-field energy that is not returned. This effect shows up as a different impedance in the antenna, as seen by the transmitter.

The reactive component of the near field can give ambiguous or undetermined results when attempting measurements in this region. In other regions, the power density is inversely proportional to the square of the distance from the antenna. In the vicinity very close to the antenna, however, the energy level can rise dramatically with only a small decrease in distance toward the antenna. This energy can adversely affect both humans and measurement equipment because of the high powers involved.<ref name=OSHA-EM-rad/>

===Radiative near field (Fresnel region), or farthest part of the near field===
The radiative near field (sometimes called the ''Fresnel region'') does not contain reactive field components from the source antenna, since it is far enough from the antenna that back-coupling of the fields becomes out of phase with the antenna signal, and thus cannot efficiently return inductive or capacitive energy from antenna currents or charges. The energy in the radiative near field is thus all [[radiant energy]], although its mixture of magnetic and electric components are still different from the far field. Further out into the radiative near field (one half wavelength to 1 wavelength from the source), the {{math|'''E'''}} and {{math|'''H'''}} field relationship is more predictable, but the {{math|'''E'''}} to {{math|'''H'''}} relationship is still complex. However, since the radiative near field is still part of the near field, there is potential for unanticipated (or adverse) conditions.

For example, metal objects such as steel beams can act as antennas by inductively receiving and then "re-radiating" some of the energy in the radiative near field, forming a new radiating surface to consider. Depending on antenna characteristics and frequencies, such coupling may be far more efficient than simple antenna reception in the yet-more-distant far field, so far more power may be transferred to the secondary "antenna" in this region than would be the case with a more distant antenna. When a secondary radiating antenna surface is thus activated, it then creates its own near-field regions, but the same conditions apply to them.<ref name="OSHA-EM-rad">
{{cite web |author=Occupational Safety and Health Administration, Cincinnati Technical Center |date=May 20, 1990 |title=Electromagnetic Radiation and How It Affects Your Instruments. Near field vs. Far field. |url=https://www.osha.gov/radiofrequency-and-microwave-radiation/electromagnetic-field-memo#section_6 |access-date=2025-04-25 |publisher=U.S. Dept of Labor}} Department of Labor – Public Domain content. Most of the content referenced by this work in this article is copied from a public domain document. In addition, this paper has provided [https://www.osha.gov/radiofrequency-and-microwave-radiation/electromagnetic-field-memo#section_10 references].</ref>

===Compared to the far field===
The near field is remarkable for reproducing classical [[electromagnetic induction]] and electric charge effects on the EM field, which effects "die-out" with increasing distance from the antenna: The magnetic field component that’s in phase quadrature to electric fields is proportional to the inverse-cube of the distance (<math>1/r^3</math>) and electric field strength proportional to inverse-square of distance (<math>1/r^2</math>). This fall-off is far more rapid than the classical radiated far-field ({{math|'''E'''}} and {{math|'''B'''}} fields, which are proportional to the simple inverse-distance (<math>1/r</math>). Typically near-field effects are not important farther away than a few wavelengths of the antenna.

More-distant near-field effects also involve energy transfer effects that couple directly to receivers near the antenna, affecting the power output of the transmitter if they do couple, but not otherwise. In a sense, the near field offers energy that is available to a receiver {{em|only}} if the energy is tapped, and this is sensed by the transmitter by means of responding to electromagnetic near fields emanating from the receiver. Again, this is the same principle that applies in [[electromagnetic induction|induction coupled]] devices, such as a [[transformer]], which draws more power at the primary circuit, if power is drawn from the secondary circuit. This is different with the far field, which constantly draws the same energy from the transmitter, whether it is immediately received, or not.

The amplitude of other components (non-radiative/non-dipole) of the electromagnetic field close to the antenna may be quite powerful, but, because of more rapid fall-off with distance than <math>1/r</math> behavior, they do not radiate energy to infinite distances. Instead, their energies remain trapped in the region near the antenna, not drawing power from the transmitter unless they excite a receiver in the area close to the antenna. Thus, the near fields only transfer energy to very nearby receivers, and, when they do, the result is felt as an extra power draw in the transmitter. As an example of such an effect, power is transferred across space in a common [[transformer]] or [[metal detector]] by means of near-field phenomena (in this case [[inductive coupling]]), in a strictly short-range effect (i.e., the range within one wavelength of the signal).

==Classical EM modelling==
[[File:FarNearFields-USP-4998112-2.svg|thumb|300px|A "[[radiation pattern]]" for an antenna, by definition showing only the far field.]]
Solving [[Maxwell's equations]] for the [[electric field|electric]] and [[magnetic field]]s for a localized oscillating source, such as an antenna, surrounded by a homogeneous material (typically [[vacuum]] or [[air]]), yields fields that, far away, decay in proportion to <math>1/r</math> where {{mvar|r}} is the distance from the source. These are the radiating fields, and the region where {{mvar|r}} is large enough for these fields to dominate is the far field.

In general, the fields of a source in a [[homogeneity (physics)|homogeneous]] [[isotropic]] [[transmission medium|medium]] can be written as a [[multipole expansion]].<ref>John David Jackson, ''Classical Electrodynamics'', 3rd edition (Wiley: New York, 1998)</ref> The terms in this expansion are [[spherical harmonic]]s (which give the angular dependence) multiplied by [[spherical Bessel function]]s (which give the radial dependence). For large {{mvar|r}}, the spherical Bessel functions decay as <math>1/r</math>, giving the radiated field above. As one gets closer and closer to the source (smaller {{mvar|r}}), approaching the near field, other powers of {{mvar|r}} become significant.

The next term that becomes significant is proportional to <math>1/r^2</math> and is sometimes called the ''induction term''.<ref>{{cite web |last1=Johansson |first1=J. |last2=Lundgren |first2=U. |title=EMC of Telecommunication Lines |url=http://www.dannex.se/theory/3.html}}</ref> It can be thought of as the primarily magnetic energy stored in the field, and returned to the antenna in every half-cycle, through self-induction. For even smaller {{mvar|r}}, terms proportional to <math>1/r^3</math> become significant; this is sometimes called the ''electrostatic field term'' and can be thought of as stemming from the electrical charge in the antenna element.

Very close to the source, the multipole expansion is less useful (too many terms are required for an accurate description of the fields). Rather, in the near field, it is sometimes useful to express the contributions as a sum of radiating fields combined with [[evanescent field]]s, where the latter are exponentially decaying with {{mvar|r}}. And in the source itself, or as soon as one enters a region of inhomogeneous materials, the multipole expansion is no longer valid and the full solution of Maxwell's equations is generally required.

===Antennas===

If an oscillating electrical current is applied to a conductive structure of some type, electric and magnetic fields will appear in space about that structure. If those fields are lost to a propagating space wave the structure is often termed an antenna. Such an antenna can be an assemblage of [[electrical conductor|conductor]]s in space typical of [[radio]] devices or it can be an [[aperture]] with a given current distribution radiating into space as is typical of [[microwave]] or [[optical device]]s. The actual values of the fields in space about the antenna are usually quite complex and can vary with distance from the antenna in various ways.

However, in many practical applications, one is interested only in effects where the distance from the antenna to the observer is very much greater than the largest dimension of the transmitting antenna. The equations describing the fields created about the antenna can be simplified by assuming a large separation and dropping all terms that provide only minor contributions to the final field. These simplified distributions have been termed the "far field" and usually have the property that the angular distribution of energy does not change with distance, although the energy levels still vary with distance and time. Such an angular energy distribution is usually termed an [[antenna pattern]].

Note that, by the principle of [[reciprocity (electromagnetism)|reciprocity]], the pattern observed when a particular antenna is transmitting is identical to the pattern measured when the same antenna is used for reception. Typically one finds simple relations describing the antenna far-field patterns, often involving trigonometric functions or at worst [[Fourier transform|Fourier]] or [[Hankel transform]] relationships between the antenna current distributions and the observed far-field patterns. While far-field simplifications are very useful in engineering calculations, this does not mean the near-field functions cannot be calculated, especially using modern computer techniques. An examination of how the near fields form about an antenna structure can give great insight into the operations of such devices.

===Impedance===
The electromagnetic field in the far-field region of an antenna is independent of the details of the near field and the nature of the antenna. The wave impedance is the ratio of the strength of the electric and magnetic fields, which in the far field are in phase with each other. Thus, the far field "[[impedance of free space]]" is resistive and is given by:
:<math display=block> Z_0 \mathrel\overset{\underset{\mathrm{def}}{}}{=} \sqrt{\frac{\mu_0}{\,\varepsilon_0\,} \;} = \mu_0 c_0 = \frac{1}{\,\varepsilon_0 c_0\,} ~.</math>

With the usual approximation for the [[speed of light]] in free space {{math|''c''<sub>0</sub> ≈ 2.9979 × {{10^|8}} }}m''/''s, this gives the frequently used expression:
:<math display=block> Z_0 \approx \pi\,119.92\ \mathsf{\Omega} \approx \pi\,120\ \mathsf{\Omega} \approx 377\ \mathsf{\Omega} ~</math>

The electromagnetic field in the near-field region of an electrically small coil antenna is predominantly magnetic. For small values of <big>{{mvar|{{sfrac|r| λ }} }}</big> the impedance of a magnetic loop is low and inductive, at short range being asymptotic to:
:<math display=block>|Z_\mathsf{W}| \approx \pi^2\,240\ \mathsf{\Omega}\,\frac{r}{\,\lambda\,} \approx 2\,370\ \mathsf{\Omega}\,\frac{r}{\,\lambda\,} ~.</math>

The electromagnetic field in the near-field region of an electrically short rod antenna is predominantly electric. For small values of <big>{{mvar|{{sfrac|r| λ }} }}</big> the impedance is high and capacitive, at short range being asymptotic to:
:<math display=block>|Z_\mathsf{W}| \approx 60\ \mathsf{\Omega} \, \frac{\,\lambda\,}{r} ~.</math>

In both cases, the wave impedance converges on that of [[free space]] as the range approaches the far field.

==See also==
'''Local effects'''
*[[Fraunhofer diffraction]] for more on the far field
*[[Fresnel diffraction]] for more on the near field
*[[Induction heating|Inductive heating]] of ferrous metals
*[[Near-field communication]] for more on near-field communication technology
*[[Near-field magnetic induction communication]]
*[[Physics of magnetic resonance imaging]]
*[[Resonant inductive coupling]] for magnetic device applications
*[[RFID]] often operates at near field, but newer types of tags transmit radio waves and thus operate using the far field
*[[Subwavelength imaging]]
*[[Wireless power transfer]] for some power transfer applications

'''Other'''
*[[Antenna measurement]] covers Far-Field Ranges (FF) and Near-Field Ranges (NF), separated by the [[Fraunhofer distance]].
*[[Ground wave]]s: a mode of propagation
*[[Inverse-square law]]
*[[Self-focusing transducers]], harnessing the effect with acoustic waves
*[[Sky wave]]s: a mode of propagation

==Notes==
{{Notelist|1}}

==References==

===Citations===
{{Reflist|25em}}

===Public domain===
{{FS1037C MS188}}

{{US government sources}} [[Occupational Safety and Health Administration]].

==Patents==
*George F. Leydorf, {{US patent|3278937}}, Antenna near field coupling system. 1966.
*Grossi et al., {{US patent|3445844}}, Trapped Electromagnetic Radiation Communication System. 1969.
*{{US patent|3461453}}, Reducing-Noise With Dual-Mode Antenna. 1969.
*Coffin et al., {{US patent|3662389}}, Determination of Far Field Antenna Patterns Using Fresnel Probe Measurements. 1972.
*Hansen et al., {{US patent|3879733}}, Method and Apparatus for Determining Near-Field Antenna Patterns. 1975
*Wolff et al.,{{US patent|5459405}}, Method and apparatus for sensing proximity of an object using near-field effects

[[Category:Antennas]]
[[Category:Scattering, absorption and radiative transfer (optics)]]