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Admittance, Conductance, Susceptance

Steinmetz introduces admittance as the reciprocal of impedance:

Y=1ZY = \frac{1}{Z}

The OCR candidate gives the component form:

Y=gjbY = g - jb

where g is conductance and b is susceptance.

If:

Z=r+jxZ = r + jx

then:

Y=1r+jxY = \frac{1}{r + jx}

Multiply numerator and denominator by the conjugate:

Y=rjxr2+x2Y = \frac{r - jx}{r^2 + x^2}

So, under this sign convention:

g=rr2+x2g = \frac{r}{r^2 + x^2} b=xr2+x2b = \frac{x}{r^2 + x^2}

This page is essential because it prevents a common beginner error:

  • Conductance is not generally 1/r.
  • Susceptance is not generally 1/x.

They are components of the reciprocal of the full complex impedance.

If:

Z=6+j8 ΩZ = 6 + j8\ \Omega

then:

Y=6j862+82=0.06j0.08 SY = \frac{6 - j8}{6^2 + 8^2} = 0.06 - j0.08\ \text{S}

Thus:

g=0.06 S,b=0.08 Sg = 0.06\ \text{S},\quad b = 0.08\ \text{S}
Modern Translation

Modern notation often writes admittance as Y = G + jB. When translating Steinmetz, the sign convention should be named explicitly rather than silently rewritten.