Q-factor in an LRC series circuit

Last weekend BINSIC drove me mad in a desperate rush to finish. This weekend I have been obsessed by this problem, but have finally worked it out.

The Q factor measures the width of a signal at half the resonant power (it is a dimensionless quantity and measures lots of things, but we’ll stick with this for now).

For an AC LRC series circuit, at half power the impedance equals \sqrt{2}R and so the reactances equal R or minus R, i.e.,

X_L - X_C = R at the high frequency end and (1)

X_L - X_C = -R at the low frequency end. (2)

Looking at the angular frequencies, this gives for (1)

\omega_hL - \frac{1}{\omega_hC} = R

and for (2)

\omega_lL - \frac{1}{\omega_lC} = -R

Subtract (2) from (1) and we get

2R = L(\omega_h - \omega_l) + \frac{1}{C}(\frac{1}{\omega_l} - \frac{1}{\omega_h})

Now \omega_h - \omega_l is the bandwidth and we will label this \Delta for ease of exposition.

And we can see that \frac{1}{\omega_l}-\frac{1}{\omega_h} can be expanded to:

\frac{\omega_h-\omega_l}{\omega_h\omega_l} = \frac{\Delta}{\omega_h\omega_l}

And (here’s one of the parts I stumbled on), \omega_h\omega_l is the square of the resonant frequency \omega_0 (as this is a geometric and not arithmetic mean).

So now we have:

2R = L\Delta + \frac{\Delta}{C{\omega_0}^2}

and so 2R = \Delta(L + \frac{1}{C{\omega_0}^2}) and \Delta = \frac{2RC{\omega_0}^2}{LC{\omega_0}^2 + 1}

Now, Q = \frac{\omega_0}{\Delta}, so…

Q = \omega_0\frac{LC{\omega_0}^2 + 1}{2C{\omega_0}^2R}

Now, {\omega_0}^2 = \frac{1}{LC} (from the resonant frequency definition, see the previous blog)

And so we get Q = \frac{1}{\sqrt{LC}}\frac{2}{\frac{2CR}{LC}} = \frac{1}{R}\sqrt{\frac{L}{C}}, the definition you’ll see in a textbook.

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