An alternating current source is connected in the following figure (a series combination of an inductor \(L\), a capacitor \(C\) and a resistor \(R\) across an AC source of rms voltage \(V\)). Determine the value of current flowing in the resistance \(R\) in the condition of resonance.
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At resonance \(X_L=X_C\), so the impedance drops to just \(R\). Apply \(I=V/Z\).
Step 1: Identify the circuit and the resonance condition. The circuit is a series \(L\)-\(C\)-\(R\) combination fed by an AC source of rms voltage \(V\). The impedance of a series LCR circuit is \[ Z=\sqrt{R^{2}+\left(X_{L}-X_{C}\right)^{2}} \] where \(X_{L}=\omega L\) is the inductive reactance and \(X_{C}=\dfrac{1}{\omega C}\) is the capacitive reactance.
Step 2: Apply the resonance condition. At resonance the inductive and capacitive reactances become equal, so \[ X_{L}=X_{C}\ \Rightarrow\ X_{L}-X_{C}=0 \]
Step 3: Find the impedance at resonance. Substituting \(X_{L}-X_{C}=0\): \[ Z=\sqrt{R^{2}+0}=R \] So at resonance the circuit behaves as a pure resistance \(R\); the impedance is minimum.
Step 4: Apply Ohm's law for AC to get the current. The same current flows through every element of a series circuit, so the current through \(R\) equals the source current: \[ I=\frac{V}{Z}=\frac{V}{R} \]
Result: The current in resistance \(R\) at resonance is maximum and equals \[\boxed{I=\dfrac{V}{R}}\]