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Conductance |
Admittance |
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In direct current circuits, conductance
is expressed by, ![]() where G = conductance in mhos, R = resistance in ohms, In d-c circuits involving resistances R1, R2, R3, etc. in parallel, the total conductance is expressed by Gtotal = G1 + G2 + G3 ...etc. and the total current by Itotal = E Gtotal and the amount of current in any single resistor, R2 for example, in a parallel group, by ![]() R, E and I in Ohm's law formulas for d-c circuits may be expressed in terms of conductance as follows: ![]() ![]() ![]() where G = conductance in mhos, R = resistance in ohms, E = potential in volts, I = current in amperes, |
In an alternating current circuit,
the admittance of a series circuit is expressed by, ![]() Admittance is also expressed as the reciprocal of impedance, or ![]() where Y = admittance in mhos, R = resistance in ohms, X = reactance in ohms, Z = impedance in ohms, |
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R and X in Terms of G and B | ||
Resistance and reactance may be expressed
in terms of conductance and susceptance as follows: ![]() ![]() |
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G, B, Y and Z in Parallel Circuits | ||
Susceptance |
In any given a-c
circuit containing a number of smaller
parallel circuits only, the effective conductance GT is expressed by GT = G1 + G2 + G3...etc. and the effective susceptance BT by BT = B1 + B2 + B3...etc. and the effective admittance YT by ![]() and the effective impedance ZT by ![]() where R = resistance in ohms, X = reactance (capacitive or induc- tive) in ohms, G = conductance in mhos, B = susceptance in mhos, Y = admittance in mhos, Z = impedance in ohms, |
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In an alternating current
circuit, the susceptance of a
series circuit is expressed by ![]() or, when the resistance is 0, susceptance becomes the reciprocal of reactance, or ![]() where B = susceptance in mhos, R = resistance in ohms, X = reactance in ohms, |
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