Contains lumped impedance models and can also be regarded as a collection of basic formulas. Shunts are part of a separate package.
General relations.
r = R / R_base resistance x = 2*pi*f_nom*L/R_base reactance g = G / G_base conductance b = (2*pi*f_nom*C) / G_base susceptance G_base = 1/R_base
The reactance-matrix is
x = [x_s, x_m x_m, x_s]
with the relations
x1 = x_s - x_m, stray reactance x0 = x_s + x_m, zero reactance x_s = (x1 + x0)/2, self reactance single conductor x_m = (x0 - x1)/2, mutual reactance
Coupling.
-x_s < x_m < x_s uncoupled limit: x_m = 0, x0 = x_s fully positive coupled: x_m = x_s, x0 = 2*x_s fully negative coupled: x_m = -x_s, x0 = 0
The resistance matrix is
r = [r1, 0 0, r2]
The susceptance matrix is
b = [ b_pg + b_pp, -b_pp -b_pp, b_pg + b_pp]
where _pg denotes 'phase-to-ground' and _pp 'phase-to-phase' in analogy to the three-phase notation. More precisely (for a one-phase system) _pp means 'conductor-to-conductor'.
The corresponding conduction matrix is (in analogy to susceptance)
g = [g_pg + g_pp, -g_pp -g_pp, g_pg + g_pp]
Name | Description |
---|---|
Resistor | Resistor, 1-phase |
Conductor | Conductor, 1-phase |
Inductor | Inductor with series resistor, 1-phase |
Capacitor | Capacitor with parallel conductor, 1-phase |
Impedance | Impedance (inductive) with series resistor, 1-phase |
Admittance | Admittance (capacitive) with parallel conductor, 1-phase |
Varistor | Varistor, 1-phase |
ResistorSym | Symmetrical capacitor with neutral access |
CapacitorSym | Symmetrical capacitor with neutral access |
DClink | DC-link with filter circuit |
DClinkSym | Symmetrical DC-link with filter circuit and neutral access |
Partials | Partial models |