Resonant Frequency, $f_p$ (Unity Power Factor)
We have derived the equation for $f_p$, which is given as
$$ f_p = f_s \sqrt{1 - { R_l^2 C \over L}} \tag{1}$$
We can rewrite the factor ${ R_l^2 C \over L}$ of Eq. (1) as
$$\begin{split}
{ R_l^2 C \over L} &= { 1 \over {L \over R_l^2 C}}= { 1 \over {w L \over w R_l^2 C}}\\
&= { 1 \over {w L \over R_l^2 wC}}={ 1 \over {X_L X_C \over R_l^2}}
\end{split}$$
and substitute ($X_L \approx X_C$):
$${ 1 \over {X_L X_C \over R_l^2}} = { 1 \over {X_L^2 \over R_l^2}} = { 1 \over Q_l^2}$$
Equation (1) then becomes
$$ f_p = f_s \sqrt{1 - { 1 \over Q_l^2}} \tag{1}$$
clearly revealing that as $Q_l$ increases, $f_p$ becomes closer and closer to $fs$.
$$ 1 - {1 \over Q_l^2} \approx 1$$
and
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