In the circuit shown, the \(n:1\) step-down transformer and the diodes are ideal. The diodes have no voltage drop in forward-biased condition. If the input voltage (in Volts) is \(V_s(t) = 10\sin\omega t\) and the average value of load voltage \(V_L(t)\) (in Volts) is \(2.5/\pi\), the value of \(n\) is \(\_\_\_\_\).
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Show Hint
For rectifier circuits involving transformers, calculate the turns ratio by analyzing the relationship between the input and rectified output voltages, and remember the average voltage formula for rectified signals.
Step 1: Analyze the circuit functionality.
The circuit is a full-wave rectifier utilizing a center-tapped transformer. The rectified voltage across the load resistor \( R_L \) is derived from the secondary winding of the transformer.
Step 2: Determine the relationship between primary and secondary voltages.
The primary voltage is given as:
\[
V_s(t) = 10 \sin\omega t.
\]
The secondary voltage \( V_{sec}(t) \) is scaled by the transformer turns ratio \( n:1 \), such that:
\[
V_{sec}(t) = \frac{10}{n} \sin\omega t.
\]
Step 3: Rectified output voltage.
In a full-wave rectifier, the output is the absolute value of the secondary voltage:
\[
V_L(t) = \left| \frac{10}{n} \sin\omega t \right|.
\]
Step 4: Compute the average output voltage.
For a full-wave rectified sine wave, the average voltage is:
\[
V_{{avg}} = \frac{2V_{{peak}}}{\pi}.
\]
Substituting \( V_{{peak}} = \frac{10}{n} \), we get:
\[
V_{{avg}} = \frac{2}{\pi} \cdot \frac{10}{n}.
\]
Step 5: Solve for \(n\).
Given that \( V_{{avg}} = \frac{2.5}{\pi} \), equate and solve for \(n\):
\[
\frac{2}{\pi} \cdot \frac{10}{n} = \frac{2.5}{\pi}.
\]
Simplify:
\[
\frac{10}{n} = 2.5.
\]
\[n = \frac{10}{2.5} = 4.\]
The transformer turns ratio \(n\) is therefore 4, which matches option (1).
Final Answer:
\[\boxed{4}\]