Integral quantities in electrostatics
Generally the integral quantities of interest in electrostatic analysis are: electric charge, potential difference, mechanical force and torque, field energy.
The following notations are used in formulas:
E - electric field strength;
D - vector of electric flux density (electric displacement);
U - electric potential.
Name, |
Formula and Description |
Electric charge qfInt_KGrad_n_ds |
q = s∮ (D·n)ds According to the Gauss theorem, total electric charge in a particular volume can be calculated as a flux of electric displacement over its closed boundary. |
Mechanical force qfInt_MaxwellForce |
F = 1/2·s∮( E·(n·D) + D·(n·E) - n·(E·D) )ds Total electric force acting on bodies contained in a particular volume. The integral is evaluated over the volume's boundary. |
Mechanical torque qfInt_MaxwellTorque |
T = 1/2·s∮( [r×E]·(n·D) + [r×D]·(n·E) - [r×n]·(E·D) )ds Total torque of electric forces acting on bodies contained in a particular volume.
|
Stored energy qfInt_ElectrostaticEnergy |
W = 1/2·v∫ (E·D)dv Electric field energy in a particular volume. |
Surface energy qfInt_GradKGrad_n_ds |
WS = 1/2·s∫ (E·D)ds |
Potential difference qfInt_Grad_t_dl |
ΔU = L∫ (E·t)dl 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 |
Average volume potential qfInt_Potential_dv |
Uv = 1/V·v∫ U·dv |
Average volume strength qfInt_Grad_dv |
Ea = 1/V·v∫ E·dv Average electric filed strength in a particular volume. |
Average volume displacement qfInt_KGrad_dv |
Da = 1/V·v∫ D·dv Average electric displacement vector in a particular volume. |
Mean square strength qfInt_Grad2_dv |
Ea2 = 1/V·v∫ E2·dv |
Mean square displacement qfInt_KGrad2_dv |
Da2 = 1/V·v∫ D2·dv |
Line integral of displacement qfInt_KGrad_t_dl |
x = L∫ (D·t)dl |
Surface integral of strength qfInt_Grad_n_ds |
x = s∫ (E·n)ds |