Step 1: Input waveform.
Supply:
\[
v_{in} = 100 \sin(100\pi t), V_m = 100
\]
Step 2: Controlled rectifier operation.
Average load voltage:
\[
V_{dc} = \frac{V_m}{2\pi} \int_{\alpha}^{\pi+\alpha} \sin\theta \, d\theta
\]
Step 3: Solve integral.
\[
V_{dc} = \frac{V_m}{2\pi} \left[ -\cos\theta \right]_{\alpha}^{\pi+\alpha}
= \frac{V_m}{2\pi} \left( -\cos(\pi+\alpha) + \cos(\alpha) \right)
\]
\[
= \frac{V_m}{2\pi} \left( -(-\cos\alpha) + \cos\alpha \right)
= \frac{V_m}{2\pi} (2\cos\alpha)
\]
\[
V_{dc} = \frac{V_m}{\pi} \cos\alpha
\]
Step 4: Substitute values.
\(V_m = 100, \; \alpha = 60^\circ\):
\[
V_{dc} = \frac{100}{\pi} \cdot \cos(60^\circ) = \frac{100}{\pi} \cdot 0.5 = \frac{50}{\pi}
\]
\[
V_{dc} \approx 15.92 \, V
\]
Correction (since conduction occurs over two intervals due to T2 firing at 240°):
Effective average doubled:
\[
V_{dc} \approx 31.83 \, V
\]
Final Answer:
\[
\boxed{31.83 \, V}
\]
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