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Integral quantities in AC conduction

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For the AC conduction analysis, the most interesting integral values are: active, reactive and apparent current through particular surface, Joule heat, mechanical force and torque, field energy.
The following notations are used in formulas:

Since AC conduction problems' formulations use complex values that represent the real world quantities sinusoidally changing with time, the integral values might appear in the following different ways:

Name,
ActiveField constant

Formula and Description

Active current through a given surface

qfInt_Jactive

IA = s (jA·n)ds

Complex value. Active electric current through a particular surface.

Reactive current through a given surface

qfInt_Jreactive

IRE = s (jRE·n)ds

Complex value. Reactive electric current through a particular surface.

Apparent current through a given surface

qfInt_Japparent

IAPP = s (jAPP·n)ds

Complex value. Apparent electric current through a particular surface.

Active power produced in a volume

qfInt_PowerActive

PA = v (E·jA)dv

Oscillated value. Joule heat power produced in a particular volume.

Reactive power produced in a volume

qfInt_PowerReactive

PRE = v (E·jRE)dv

Oscillated value. Reactive power produced in a particular volume.

Apparent power produced in a volume

qfInt_PowerApparent

PAPP = v (E·jAPP)dv

Oscillated value. Apparent power produced in a particular volume.

Mechanical force

qfInt_MaxwellForce

F = 1/2·s(E·(n·D) + D·(n·E) - n·(E·D))ds

Oscillated vector. Electric force acting on bodies contained in a particular volume. Evaluated by calculating of Maxwell stress tensor over volume’s bounding surface.

Mechanical torque

qfInt_MaxwellTorque

T = 1/2·s([r×E]·(n·D) + [r×D]·(n·E) - [r×n]·(E·D))ds

Oscillated value. Electric force torque acting on bodies contained in a particular volume, where r is a radius vector of the point of integration.
The torque vector is parallel to z-axis in the planar case, and is identically equal to zero in the axisymmetric one. The torque is considered relative to the origin of the coordinate system. The torque relative to any other arbitrary point can be obtained by adding extra term of [F×r0], where F is the total force and r0 is the radius vector of the point.

Electric field energy

qfInt_ElectrostaticEnergy

W = 1/2·v (E·D)dv

Oscillated value. Electric field energy in a particular volume.

Surface energy

qfInt_GradKGrad_n_ds

WS = 1/2·s (E·D)ds

Oscillated value.

Potential difference

qfInt_Grad_t_dl

ΔU = L (E·t)dl

Complex value. The potential difference between the ending and started points of a contour can be calculated as a line integral over the contour of electric field strength.

Average surface potential

qfInt_Potential_ds

Us = 1/S·s U·ds

Complex value.

Average volume potential

qfInt_Potential_dv

Uv = 1/V·v U·dv

Complex value.

Average volume strength

qfInt_Grad_dv

Ea = 1/V·v E·dv

Complex vector. Average electric field strength vector in a particular volume.

Average volume displacement

qfInt_KGrad_dv

Da = 1/V·v D·dv

Complex vector. Average electric displacement vector in a particular volume.

Mean square strength

qfInt_Grad2_dv

Ea2 = 1/V·v E2·dv

Oscillated value.

Mean square displacement

qfInt_KGrad2_dv

Da2 = 1/V·v D2·dv

Oscillated value.

Electric charge

qfInt_Grad_n_ds

Qs = s (E·n)ds

Complex value. The total electric charge in a particular volume can be calculated as a flux of electric displacement over the volume’s closed boundary.

Line integral of displacement

qfInt_KGrad_t_dl

x = L (D·t)dl

Complex value.