




|
A condition in space in the vicinity of an electrically
charged body such that the forces due to the charge are detectable. An
electric field (or electrostatic field) exists in a region if an electric
charge at rest in the region experiences a force of electrical origin.
Since an electric charge experiences a force if it is in the vicinity
of a charged body, there is an electric field surrounding any charged
body.
The electric field intensity (or field strength) E at
a point in an electric field has a magnitude given by the quotient obtained
when the force acting on a test charge q' placed at that point is divided
by the magnitude of the test charge q'. Thus, it is force per unit charge.
A test charge q' is one whose magnitude is small enough so it does not
alter the field in which it is placed. The direction of E at
the point is the direction of the force F on a positive
test charge placed at the point. Thus, E is a vector point
function, since it has a definite magnitude and direction at every point
in the field, and its defining equation is Eq. (1).
E = F/q' (1)
Electric flux density or electric displacement D in a dielectric (insulating)
material is related to E by either of the equivalent equations shown as Eqns.
(2), where P is the polarization of the
D =ε0 E+PD = ε E (2)
medium, and ε is the permittivity of the dielectric which is related to ε0,
by the equation ε = kε0, k being the
relative dielectric constant of the dielectric. In empty space, D = ε0E.
In addition to electrostatic fields produced by separations of electric charges,
an electric field is also produced by a changing magnetic field. |
|