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Capacity Susceptance

Steinmetz identifies C as electrostatic capacity and gives capacity susceptance as:

b=2πfCb = 2\pi f C BC=ωCB_C = \omega C BC=2πfCB_C = 2\pi f C

For a pure capacitance:

XC=1ωCX_C = \frac{1}{\omega C}

while capacitive susceptance is:

BC=ωCB_C = \omega C

They are reciprocal in the pure case, but in a general complex circuit one must take the reciprocal of the whole impedance, not just one component.

If:

f=60 Hz,C=10 μFf = 60\ \mathrm{Hz},\quad C = 10\ \mu\mathrm{F}

then:

BC=2π(60)(10×106)0.00377 SB_C = 2\pi(60)(10 \times 10^{-6}) \approx 0.00377\ \mathrm{S}

and the corresponding pure-capacitive reactance magnitude is:

XC=1BC265 ΩX_C = \frac{1}{B_C} \approx 265\ \Omega
Physical Meaning

Susceptance tells how much quadrature current a dielectric or condenser draws per volt. It is field storage seen from the admittance side of the calculation.