Electric field lines emanating from a point positive
electric charge suspended over an infinite sheet of conducting material.
An electric field is generated by electric charge and timevarying magnetic fields. At each point in space, the electric field describes the electric force that would be experienced by a motionless test particle of unit positive charge. The concept of an electric field was introduced by Michael Faraday.
Contents

Qualitative description 1

Definition 2

Classical electrodynamics 2.1

Superposition 3

Array of discrete point charges 3.1

Continuum of charges 3.2

Electrostatic fields 4

Uniform fields 4.1

Parallels between electrostatic and gravitational fields 4.2

Electrodynamic fields 5

Energy in the electric field 6

Further extensions 7

Definitive equation of vector fields 7.1

Constitutive relation 7.2

See also 8

References 9

External links 10
Qualitative description
The electric field is a vector field. The field vector at a given point is defined as the force vector per unit charge that would be exerted on a stationary test charge at that point. An electric field is generated by electric charge (also called source charge), as well as by a timevarying magnetic field. The electric charge can be a single charge or a group of discrete charges or any continuous distribution of charge. Electric fields contain electrical energy with energy density proportional to the square of the field magnitude. The electric field is to charge as gravitational acceleration is to mass. The SI units of the field are newtons per coulomb (N⋅C^{−1}) or, equivalently, volts per metre (V⋅m^{−1}), which in terms of SI base units are kg⋅m⋅s^{−3}⋅A^{−1}.
An electric field that changes with time, such as due to the motion of charged particles producing the field, influences the local magnetic field. That is: the electric and magnetic fields are not separate phenomena; what one observer perceives as an electric field, another observer in a different frame of reference perceives as a mixture of electric and magnetic fields. For this reason, one speaks of "electromagnetism" or "electromagnetic fields". In quantum electrodynamics, disturbances in the electromagnetic fields are called photons.
Definition
Classical electrodynamics
The electric field is defined in classical electrodynamics as follows (it is not used in quantum electrodynamics, in which case electric potentials are more fundamental).
Consider a point charge q with position (x, y,z). Now suppose the charge is subject to a force F_{on q} due to a field generated by other charges. Since this force varies with the position of the charge and by Coulomb's Law it is defined at all points in space, F_{on q} is a continuous function of the charge's position. This suggests that there is some property of the space that causes the force that is exerted on the charge q. This property is called the electric field and it is defined by

\mathbf{E}(x,y,z)\equiv \frac{\mathbf{F}_{\text{on }q}(x,y,z)}{q}
Notice that the magnitude of the electric field has dimensions of force/charge. Mathematically, the E field can be thought of as a function that associates a vector with every point in space. Each such vector's magnitude is proportional to how much force a charge at that point would "feel" if it were present and this force would have the same direction as the electric field vector at that point. The electric field defined above is caused by a configuration of other electric charges. This means that the charge q in the equation above is not the charge that is generating the electric field, but rather, being acted upon by it.
The definition is part of the Lorentz force law, which provides a general definition of the classical electric and magnetic fields as well as the equation of motion for the charge q.
This definition does not give a means of computing the electric field caused by a group of charges  one has to solve Maxwell's equations.
Superposition
Array of discrete point charges
Electric fields satisfy the superposition principle. If more than one charge is present, the total electric field at any point is equal to the vector sum of the separate electric fields that each point charge would create in the absence of the others. That is,

\mathbf{E} = \sum_i \mathbf{E}_i = \mathbf{E}_1 + \mathbf{E}_2 + \mathbf{E}_3 + \cdots \,\!
where E_{i} is the electric field created by the ith point charge.
At any point of interest, the total Efield due to N point charges is simply the superposition of the Efields due to each point charge, given by

\mathbf{E} = \sum_{i=1}^N \mathbf{E}_i = \frac{1}{4\pi\varepsilon_0} \sum_{i=1}^N \frac{Q_i}{r_i^2} \mathbf{\hat{r}}_i.
where Q_{i} is the electric charge of the ith point charge, \mathbf{\hat{r}}_i the corresponding unit vector of r_{i}, which is the position of charge Q_{i} with respect to the point of interest.
Continuum of charges
It holds for an infinite number of infinitesimally small elements of charges – i.e. a continuous distribution of charge. By taking the limit as N approaches infinity in the previous equation, the electric field for a continuum of charges can be given by the integral:

\mathbf{E} = \int_V d\mathbf{E} = \frac{1}{4\pi\varepsilon_0} \int_V\frac{\rho}{r^2} \mathbf{\hat{r}}\,\mathrm{d}V = \frac{1}{4\pi\varepsilon_0} \int_V\frac{\rho}{r^3} \mathbf{r}\,\mathrm{d}V \,\!
where ρ is the charge density (the amount of charge per unit volume), ε_{0} the permittivity of free space, and dV is the differential volume element. This integral is a volume integral over the region of the charge distribution.
The equations above express the electric field of point charges as derived from Coulomb's law, which is a special case of Gauss's Law. While Coulomb's law is only true for stationary point charges, Gauss's law is true for all charges either in static form or in motion. Gauss's Law establishes a more fundamental relationship between the distribution of electric charge in space and the resulting electric field. It is one of Maxwell's equations governing electromagnetism.
Gauss's law allows the Efield to be calculated in terms of a continuous distribution of charge density. In differential form, it can be stated as

\nabla \cdot \mathbf{E} = \frac{\rho}{\varepsilon _0}
where ∇⋅ is the divergence operator, ρ is the total charge density, including free and bound charge, in other words all the charge present in the system.
Electrostatic fields
Electrostatic fields are Efields which do not change with time, which happens when the charges are stationary.
Illustration of the electric field surrounding a positive (red) and a negative (blue) charge.
Electric field between two conductors
The electric field E at a point r, that is, E(r), is equal to the negative gradient of the electric potential \scriptstyle \mathbf{\Phi}(\mathbf{r}) , a scalar field at the same point:

\mathbf{E} = \nabla \Phi
where ∇ is the gradient operator. This is equivalent to the force definition above, since electric potential Φ is defined by the electric potential energy U per unit (test) positive charge:

\Phi = \frac{U}{q}
and force is the negative of potential energy gradient:

\mathbf{F} =  \nabla U
If several spatially distributed charges generate such an electric potential, e.g. in a solid, an electric field gradient may also be defined.
Uniform fields
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 edge effects. Ignoring such effects, the equation for the magnitude of the electric field E is:

E =  \frac{\Delta\phi}{d}
where Δϕ 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 nanoapplications, for instance in relation to semiconductors, a typical magnitude of an electric field is in the order of 1 volt/µm achieved by applying a voltage of the order of 1 volt between conductors spaced 1 µm apart.
Parallels between electrostatic and gravitational fields
Coulomb's law, which describes the interaction of electric charges:

\mathbf{F}=q\left(\frac{Q}{4\pi\varepsilon_0}\frac{\mathbf{\hat{r}}}{\mathbf{r}^2}\right)=q\mathbf{E}
is similar to Newton's law of universal gravitation:

\mathbf{F}=m\left(GM\frac{\mathbf{\hat{r}}}{\mathbf{r}^2}\right)=m\mathbf{g} .
This suggests similarities between the electric field E and the gravitational field g, so sometimes mass is called "gravitational charge".
Similarities between electrostatic and gravitational forces:

Both act in a vacuum.

Both are central and conservative.

Both obey an inversesquare law (both are inversely proportional to square of r).
Differences between electrostatic and gravitational forces:

Electrostatic forces are much greater than gravitational forces for natural values of charge and mass. For instance, the ratio of the electrostatic force to the gravitational force between two electrons is about 10^{42}.

Gravitational forces are attractive for like charges, whereas electrostatic forces are repulsive for like charges.

There are not negative gravitational charges (no negative mass) while there are both positive and negative electric charges. This difference, combined with the previous two, implies that gravitational forces are always attractive, while electrostatic forces may be either attractive or repulsive.
Electrodynamic fields
Electrodynamic fields are Efields which do change with time, when charges are in motion.
An electric field can be produced not only by a static charge, but also by a changing magnetic field (in which case it is a nonconservative field). Let B denote the magnetic flux density, and let A denote the magnetic vector potential. φ denotes the electric potential. Then the electric field E is given by

\mathbf{E} =  \nabla \varphi  \frac { \partial \mathbf{A} } { \partial t }
in which ∇φ denotes the gradient of φ, and B is given by

\mathbf{B} = \nabla \times \mathbf{A}
in which ∇× denotes the curl. By taking the curl of the electric field, we obtain

\nabla \times \mathbf{E} = \frac{\partial \mathbf{B}} {\partial t}
which is Faraday's law of induction, another one of Maxwell's equations.^{[1]}
Energy in the electric field
The electrostatic field stores energy. The energy density u (energy per unit volume) is given by^{[2]}

u = \frac{1}{2} \varepsilon \mathbf{E}^2 \, ,
where ε is the permittivity of the medium in which the field exists, and E is the electric field vector (in newtons per coulomb).
The total energy U stored in the electric field in a given volume V is therefore

U = \frac{1}{2} \varepsilon \int_{V} \mathbf{E}^2 \, \mathrm{d}V \, ,
Further extensions
Definitive equation of vector fields
In the presence of matter, it is helpful in electromagnetism to extend the notion of the electric field into three vector fields, rather than just one:^{[3]}

\mathbf{D}=\varepsilon_0\mathbf{E}+\mathbf{P}\!
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.
Constitutive relation
The E and D fields are related by the permittivity of the material, ε.^{[4]}^{[5]}
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:

\mathbf{D(r)}=\varepsilon\mathbf{E(r)}
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:

D_i=\varepsilon_{ij}E_j
For nonlinear media, E and D are not proportional. Materials can have varying extents of linearity, homogeneity and isotropy.
See also
References

^ Huray, Paul G. (2009), Maxwell's Equations, WileyIEEE, p. 205, , Chapter 7, p 205

^ Introduction to Electrodynamics (3rd Edition), D.J. Griffiths, Pearson Education, Dorling Kindersley, 2007, ISBN 8177582933

^ Electromagnetism (2nd Edition), I.S. Grant, W.R. Phillips, Manchester Physics, John Wiley & Sons, 2008, ISBN 9780471927129

^ Electricity and Modern Physics (2nd Edition), G.A.G. Bennet, Edward Arnold (UK), 1974, ISBN 0713124598

^ Electromagnetism (2nd Edition), I.S. Grant, W.R. Phillips, Manchester Physics, John Wiley & Sons, 2008, ISBN 9780471927129
External links

Electric field in "Electricity and Magnetism", R Nave – Georgia State University

'Gauss's Law' – Chapter 24 of Frank Wolfs's lectures at University of Rochester

'The Electric Field' – Chapter 23 of Frank Wolfs's lectures at University of Rochester

[1] – An applet that shows the electric field of a moving point charge.

Fields – a chapter from an online textbook

Learning by Simulations Interactive simulation of an electric field of up to four point charges

Java simulations of electrostatics in 2D and 3D

Interactive Flash simulation picturing the electric field of userdefined or preselected sets of point charges by field vectors, field lines, or equipotential lines. Author: David Chappell
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