Integral quantities in AC conduction
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:
E – complex vector of electric field strength;
D – complex vector of electric displacement;
jA – complex vector of active current density;
jRE – complex vector of reactive current density;
jAPP – complex vector of reactive current density;
U – complex value of electric potential;
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:
As a complex value, with amplitude and phase (e.g. current, potential).
As a complex vector, with the endpoint sweeping an ellipse in any complete time period (e.g. current density, field strength). The characteristics of complex vectors are: the amplitude (per coordinate), the phase, and the polarization coefficient.
As a oscillated value (e.g. ohmic loss power, field energy, etc.) pulsing around its mean value with double frequency. The characteristics of oscillated values are: the mean value, the phase, and the pulsation amplitude.
As a oscillated vector (e.g. mechanical forces) with magnitude and direction varying around its mean value with double frequency. The characteristics of oscillated vectors are: the mean value (length, slant and coordinates), and the variation amplitude (used, for example, to estimate the mechanical force limit for a period).
Name, |
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.
|
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. |