"Electric fields" redirects here. For the Australian band, see
Electric Fields.
Electric field
Effects of an electric field. The girl is touching an
electrostatic generator, which charges her body with a high voltage. Her hair, which is charged with the same polarity, is repelled by the electric field of her head and stands out from her head.
An electric field (sometimes called E-field[1]) is the
physical field that surrounds electrically
charged particles. Charged particles exert attractive forces on each other when their charges are opposite, and repulse each other when their charges are the same. Because these forces are exerted mutually, two charges must be present for the forces to take place. The electric field of a single charge (or group of charges) describes their capacity to exert such forces on another charged object. These forces are described by
Coulomb's law, which says that the greater the magnitude of the charges, the greater the force, and the greater the distance between them, the weaker the force. Thus, we may informally say that the greater the charge of an object, the stronger its electric field. Similarly, an electric field is stronger nearer charged objects and weaker further away. Electric fields originate from electric charges and time-varying
electric currents. Electric fields and
magnetic fields are both manifestations of the
electromagnetic field, Electromagnetism is one of the four
fundamental interactions of nature.
Electric fields are important in many areas of
physics, and are exploited in electrical technology. For example, in
atomic physics and
chemistry, the interaction in the electric field between the
atomic nucleus and
electrons is the force that holds these particles together in atoms. Similarly, the interaction in the electric field between atoms is the force responsible for
chemical bonding that result in
molecules.
The electric field is defined as a
vector field that associates to each point in space the force per unit of
charge exerted on an infinitesimal
test charge at rest at that point.[2][3][4] The
SI unit for the electric field is the
volt per
meter (V/m), which is equal to the
newton per
coulomb (N/C).[5]
Description
The electric field is defined at each point in space as the force that would be experienced by a
infinitesimally small stationary
test charge at that point divided by the charge.[6]: 469–70 The electric field is defined in terms of
force, and force is a
vector (i.e. having both
magnitude and
direction), so it follows that an electric field may be described by a
vector field.[6]: 469–70 The electric field acts between two charges similarly to the way that the
gravitational field acts between two
masses, as they both obey an
inverse-square law with distance.[7] This is the basis for
Coulomb's law, which states that, for stationary charges, the electric field varies with the source charge and varies inversely with the square of the distance from the source. This means that if the source charge were doubled, the electric field would double, and if you move twice as far away from the source, the field at that point would be only one-quarter its original strength.
The electric field can be visualized with a set of
lines whose direction at each point is the same as those of the field, a concept introduced by
Michael Faraday,[8] whose term '
lines of force' is still sometimes used. This illustration has the useful property that the
strength of the field is proportional to the density of the lines.[9] Field lines due to stationary charges have several important properties, including always originating from positive charges and terminating at negative charges, they enter all good conductors at right angles, and they never cross or close in on themselves.[6]: 479 The field lines are a representative concept; the field actually permeates all the intervening space between the lines. More or fewer lines may be drawn depending on the precision to which it is desired to represent the field.[8] The study of electric fields created by stationary charges is called
electrostatics.
Faraday's law describes the relationship between a time-varying magnetic field and the electric field. One way of stating Faraday's law is that the
curl of the electric field is equal to the negative
time derivative of the magnetic field.[10]: 327 In the absence of time-varying magnetic field, the electric field is therefore called
conservative (i.e. curl-free).[10]: 24, 90–91 This implies there are two kinds of electric fields: electrostatic fields and fields arising from time-varying magnetic fields.[10]: 305–307 While the curl-free nature of the static electric field allows for a simpler treatment using electrostatics, time-varying magnetic fields are generally treated as a component of a unified
electromagnetic field. The study of magnetic and electric fields that change over time is called
electrodynamics.
Electric fields are caused by
electric charges, described by
Gauss's law,[11] and time varying
magnetic fields, described by
Faraday's law of induction.[12] Together, these laws are enough to define the behavior of the electric field. However, since the magnetic field is described as a function of electric field, the equations of both fields are coupled and together form
Maxwell's equations that describe both fields as a function of charges and
currents.
In the special case of a
steady state (stationary charges and currents), the Maxwell-Faraday inductive effect disappears. The resulting two equations (Gauss's law and Faraday's law with no induction term ), taken together, are equivalent to
Coulomb's law, which states that a particle with electric charge at position exerts a force on a particle with charge at position of:[13]
where
is the force on charged particle caused by charged particle .
Note that must be replaced with ,
permittivity, when charges are in non-empty media.
When the charges and have the same sign this force is positive, directed away from the other charge, indicating the particles repel each other. When the charges have unlike signs the force is negative, indicating the particles attract.
To make it easy to calculate the
Coulomb force on any charge at position this expression can be divided by leaving an expression that only depends on the other charge (the source charge)[14][4]
where
is the component of the electric field at due to .
This is the electric field at point due to the point charge ; it is a
vector-valued function equal to the Coulomb force per unit charge that a positive point charge would experience at the position .
Since this formula gives the electric field magnitude and direction at any point in space (except at the location of the charge itself, , where it becomes infinite) it defines a
vector field.
From the above formula it can be seen that the electric field due to a point charge is everywhere directed away from the charge if it is positive, and toward the charge if it is negative, and its magnitude decreases with the
inverse square of the distance from the charge.
The Coulomb force on a charge of magnitude at any point in space is equal to the product of the charge and the electric field at that point
Due to the
linearity of
Maxwell's equations, electric fields satisfy the
superposition principle, which states that the total electric field, at a point, due to a collection of charges is equal to the vector sum of the electric fields at that point due to the individual charges.[4] This principle is useful in calculating the field created by multiple point charges. If charges are stationary in space at points , in the absence of currents, the superposition principle says that the resulting field is the sum of fields generated by each particle as described by Coulomb's law:
where
is the unit vector in the direction from point to point
is the displacement vector from point to point .
Continuous charge distributions
The superposition principle allows for the calculation of the electric field due to a distribution of
charge density. By considering the charge in each small volume of space at point as a point charge, the resulting electric field, , at point can be calculated as
where
is the unit vector pointing from to .
is the displacement vector from to .
The total field is found by summing the contributions from all the increments of volume by
integrating the charge density over the volume :
If a system is static, such that magnetic fields are not time-varying, then by Faraday's law, the electric field is
curl-free. In this case, one can define an
electric potential, that is, a function such that .[15] This is analogous to the
gravitational potential. The difference between the electric potential at two points in space is called the
potential difference (or voltage) between the two points.
In general, however, the electric field cannot be described independently of the magnetic field. Given the
magnetic vector potential, A, defined so that , one can still define an electric potential such that:
where is the
gradient of the electric potential and is the
partial derivative of A with respect to time.
The equations of electromagnetism are best described in a continuous description. However, charges are sometimes best described as discrete points; for example, some models may describe
electrons as point sources where charge density is infinite on an infinitesimal section of space.
A charge located at can be described mathematically as a charge density , where the
Dirac delta function (in three dimensions) is used. Conversely, a charge distribution can be approximated by many small point charges.
Electrostatic fields are electric fields that do not change with time. Such fields are present when systems of charged matter are stationary, or when
electric currents are unchanging. In that case,
Coulomb's law fully describes the field.[17]
Parallels between electrostatic and gravitational fields
This suggests similarities between the electric field E and the gravitational field g, or their associated potentials. Mass is sometimes called "gravitational charge".[18]
A uniform field is one in which the electric field is constant at every point. It can be approximated by placing two conducting
plates parallel to each other and maintaining a
voltage (potential difference) between them; it is only an approximation because of boundary effects (near the edge of the planes, electric field is distorted because the plane does not continue). Assuming infinite planes, the magnitude of the electric field E is:
where ΔV is the
potential difference between the plates and d is the distance separating the plates. The negative sign arises as positive charges repel, so a positive charge will experience a force away from the positively charged plate, in the opposite direction to that in which the voltage increases. In micro- and nano-applications, for instance in relation to semiconductors, a typical magnitude of an electric field is in the order of 106 V⋅m−1, achieved by applying a voltage of the order of 1 volt between conductors spaced 1 μm apart.
Electromagnetic fields are electric and magnetic fields, which may change with time, for instance when charges are in motion. Moving charges produce a magnetic field in accordance with
Ampère's circuital law (
with Maxwell's addition), which, along with Maxwell's other equations, defines the magnetic field, , in terms of its curl:
That is, both
electric currents (i.e. charges in uniform motion) and the (partial) time derivative of the electric field directly contributes to the magnetic field. In addition, the
Maxwell–Faraday equation states
These represent two of
Maxwell's four equations and they intricately link the electric and magnetic fields together, resulting in the
electromagnetic field. The equations represent a set of four coupled multi-dimensional partial differential equations which, when solved for a system, describe the combined behavior of the electromagnetic fields. In general, the force experienced by a test charge in an electromagnetic field is given by the
Lorentz force law:
where ε is the
permittivity of the medium in which the field exists, its
magnetic permeability, and E and B are the electric and magnetic field vectors.
As E and B fields are coupled, it would be misleading to split this expression into "electric" and "magnetic" contributions. In particular, an electrostatic field in any given frame of reference in general transforms into a field with a magnetic component in a relatively moving frame. Accordingly, decomposing the electromagnetic field into an electric and magnetic component is frame-specific, and similarly for the associated energy.
The total energy UEM stored in the electromagnetic field in a given volume V is
In the presence of matter, it is helpful to extend the notion of the electric field into three vector fields:[20]
where P is the
electric polarization – the volume density of
electric dipole moments, and D is the
electric displacement field. Since E and P are defined separately, this equation can be used to define D. The physical interpretation of D is not as clear as E (effectively the field applied to the material) or P (induced field due to the dipoles in the material), but still serves as a convenient mathematical simplification, since Maxwell's equations can be simplified in terms of
free charges and currents.
For linear,
homogeneous,
isotropic materials E and D are proportional and constant throughout the region, there is no position dependence:
For inhomogeneous materials, there is a position dependence throughout the material:[22]
For anisotropic materials the E and D fields are not parallel, and so E and D are related by the
permittivity tensor (a 2nd order
tensor field), in component form:
For non-linear media, E and D are not proportional. Materials can have varying extents of linearity, homogeneity and isotropy.
Relativistic effects on electric field
Point charge in uniform motion
The invariance of the form of
Maxwell's equations under
Lorentz transformation can be used to derive the electric field of a uniformly moving point charge. The charge of a particle is considered frame invariant, as supported by experimental evidence.[23] Alternatively the electric field of uniformly moving point charges can be derived from the
Lorentz transformation of
four-force experienced by test charges in the source's rest frame given by
Coulomb's law and assigning electric field and magnetic field by their definition given by the form of
Lorentz force.[24] However the following equation is only applicable when no acceleration is involved in the particle's history where
Coulomb's law can be considered or symmetry arguments can be used for solving
Maxwell's equations in a simple manner. The electric field of such a uniformly moving point charge is hence given by:[25]
where is the charge of the point source, is the position vector from the point source to the point in space, is the ratio of observed speed of the charge particle to the speed of light and is the angle between and the observed velocity of the charged particle.
The above equation reduces to that given by Coulomb's law for non-relativistic speeds of the point charge. Spherically symmetry is not satisfied due to breaking of symmetry in the problem by specification of direction of velocity for calculation of field. To illustrate this, field lines of moving charges are sometimes represented as unequally spaced radial lines which would appear equally spaced in a co-moving reference frame.[23]
For the motion of a
charged particle, considering for example the case of a moving particle with the above described electric field coming to an abrupt stop, the electric fields at points far from it do not immediately revert to that classically given for a stationary charge. On stopping, the field around the stationary points begin to revert to the expected state and this effect propagates outwards at the
speed of light while the electric field lines far away from this will continue to point radially towards an assumed moving charge. This virtual particle will never be outside the range of propagation of the disturbance in
electromagnetic field, since charged particles are restricted to have speeds slower than that of light, which makes it impossible to construct a
Gaussian surface in this region that violates
Gauss' law. Another technical difficulty that supports this is that charged particles travelling faster than or equal to speed of light no longer have a unique retarded time. Since electric field lines are continuous, an
electromagnetic pulse of radiation is generated that connects at the boundary of this disturbance travelling outwards at the
speed of light.[27] In general, any accelerating point charge radiates
electromagnetic waves however,
non-radiating acceleration is possible in a systems of charges.
For arbitrarily moving point charges, propagation of potential fields such as Lorenz gauge fields at the speed of light needs to be accounted for by using
Liénard–Wiechert potential.[28] Since the potentials satisfy
Maxwell's equations, the fields derived for point charge also satisfy
Maxwell's equations. The electric field is expressed as:[29]
where is the charge of the point source, is
retarded time or the time at which the source's contribution of the electric field originated, is the position vector of the particle, is a unit vector pointing from charged particle to the point in space, is the velocity of the particle divided by the speed of light, and is the corresponding
Lorentz factor. The retarded time is given as solution of:
The uniqueness of solution for for given , and is valid for charged particles moving slower than speed of light.
Electromagnetic radiation of accelerating charges is known to be caused by the acceleration dependent term in the electric field from which relativistic correction for
Larmor formula is obtained.[29]
There exist yet another set of solutions for Maxwell's equation of the same form but for advanced time instead of retarded time given as a solution of:
Since the physical interpretation of this indicates that the electric field at a point is governed by the particle's state at a point of time in the future, it is considered as an unphysical solution and hence neglected. However, there have been theories exploring the advanced time solutions of
Maxwell's equations, such as
Feynman Wheeler absorber theory.
The above equation, although consistent with that of uniformly moving point charges as well as its non-relativistic limit, are not corrected for quantum-mechanical effects.
Some common electric field values
Charge configuration
Figure
Electric field
Infinite wire
,
where is uniform linear charge density.
Infinitely large surface
where is uniform surface charge density.
Infinitely long cylindrical volume
where is uniform linear charge density.
Spherical volume
outside the sphere, where is the total charge uniformly distributed in the volume.
inside the sphere, where is the total charge uniformly distributed in the volume.
Spherical surface
outside the sphere, where is the total charge uniformly distributed on the surface.
inside the sphere for uniform charge distribution.
Charged Ring
,
on the axis, where is the total charge uniformly distributed on the ring.
Charged Disc
,
on the axis, where is the uniform surface charge density.
Electric Dipole
,
on the equatorial plane, where is the electric dipole moment.
,
on the axis (given that ), where can also be negative to indicate position at the opposite direction on the axis, and is the electric dipole moment.
Electric field infinitely close to a conducting surface in electrostatic equilibrium having charge density at that point is since charges are only formed on the surface and the surface at the infinitesimal scale resembles an infinite 2D plane. In the absence of external fields, spherical conductors exhibit a uniform charge distribution on the surface and hence have the same electric field as that of uniform spherical surface distribution.
^Purcell, Edward M.; Morin, David J. (2013). Electricity and Magnetism (3rd ed.). New York: Cambridge University Press. pp. 15–16.
ISBN978-1-107-01402-2.
^
abcGriffiths, David J. (1999). Introduction to electrodynamics (3rd ed.). Upper Saddle River, NJ: Prentice Hall.
ISBN0-13-805326-X.
OCLC40251748.
^Purcell, p. 25: "Gauss's Law: the flux of the electric field E through any closed surface ... equals 1/e times the total charge enclosed by the surface."
^Purcell, p7: "... the interaction between electric charges at rest is described by Coulomb's Law: two stationary electric charges repel or attract each other with a force proportional to the product of the magnitude of the charges and inversely proportional to the square of the distance between them.
^Naber, Gregory L. (2012). The Geometry of Minkowski spacetime: an introduction to the mathematics of the special theory of relativity. Springer. pp. 4–5.
ISBN978-1-4419-7837-0.
OCLC804823303.
^Purcell, Edward M.; David J. Morin (2013). Electricity and Magnetism (Third ed.). Cambridge. pp. 251–255.
ISBN978-1-139-01297-3.
OCLC1105718330.{{
cite book}}: CS1 maint: location missing publisher (
link)