Step 1: For a series \(R\!-\!L\!-\!C\) circuit driven by \(V\), the current amplitude is
\(|I|=\dfrac{|V|}{|Z|}\) with
\(|Z|=\sqrt{R^{2}+(\omega L-1/\omega C)^{2}}\).
Step 2: The resistor voltage amplitude equals the source amplitude:
\(|V_R|=|I|R=|V|\Rightarrow |Z|=R\).
Thus
\[
\sqrt{R^{2}+(\omega L-1/\omega C)^{2}}=R
\Rightarrow \omega L- \frac{1}{\omega C}=0,
\]
which is the resonance condition \(\omega_0=\dfrac{1}{\sqrt{LC}}\).
Step 3: With \(L=10\,\text{mH}=0.01\,\text{H}\) and \(C=1\,\mu\text{F}=10^{-6}\,\text{F}\),
\[
\omega_0=\frac{1}{\sqrt{(0.01)(10^{-6})}}
=\frac{1}{10^{-4}}=10^{4}\ \text{rad/s}.
\]