Electric displacement field
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In physics, the electric displacement field or electric flux density is a vector-valued field <math>\mathbf{D}</math> that appears in Maxwell's equations. It accounts for the effects of bound charges within materials. "D" stands for "displacement," as in the related concept of displacement current in dielectrics.
[edit] Definition
In general, D is defined by the relation
- <math>\mathbf{D} = \varepsilon_{0} \ \mathbf{E} \ + \ \mathbf{P}</math>
where E is the electric field, <math>\varepsilon_{0}</math> is the vacuum permittivity, and P is the polarization density of the material.
In most ordinary materials, however, D may be calculated with the simpler formula
- <math>\mathbf{D} = \varepsilon \mathbf{E}</math>
where <math>\varepsilon</math> is the permittivity of the material; in linear isotropic media this will be a constant, and in linear anisotropic media it will be a rank 2 tensor (a matrix)
[edit] Displacement field in a capacitor
Consider an infinite parallel plate capacitor placed in space (or in a medium) with no free charges present except on the capacitor. In SI units, the charge density on the plates is equal to the value of the D field between the plates. This follows directly from Gauss's law, by integrating over a small rectangular box straddling the plate of the capacitor:
- <math>\oint_A \mathbf{D} \cdot d\mathbf{A} = Q</math>
The part of the box inside the capacitor plate has no field, so that part of the integral is zero. On the sides of the box, <math>d\mathbf{A}</math> is perpendicular to the field, so that part of the integral is also zero, leaving:
- <math>|\mathbf{D}| = \frac{Q}{A}</math>
which is the charge density on the plate.
[edit] Units
In the standard SI system of units D is measured in coulombs per square meter (C/m2).
This choice of units results in one of the simplest forms of the Ampère-Maxwell equation:
<math>\nabla \times \mathbf{H} = \mathbf{J} + \frac{\partial \mathbf{D}}{\partial t} </math>
If one chooses both B and H to be measured in teslas, and E and D to be measured in newtons per coulomb, then the formula is modified to be:
<math>\nabla \times \mathbf{H} = \mu_0 \mathbf{J} + \frac{1}{c^2} \frac{\partial \mathbf{D}}{\partial t} </math>
Therefore it is seen as being preferential to express B & H, and D & E in different sets of units.
Choice of units has differed in history, for instance in the electromagnetic system of scientific units, in which the unit of charge is defined such that <math>1 / 4\pi\varepsilon_0 = 1</math> (dimensionless), D and E are expressed in the same units.it:Campo di spostamento elettrico nl:Elektrische verplaatsing ja:電束密度 pl:Indukcja elektryczna sr:Електрична индукција

