To resolve this, we apply transformer equations and Ohm's Law. Given a primary to secondary turns ratio (\(N_p:N_s\)) of 20:1, an ideal transformer maintains voltage and current ratios proportional to these turns. Consequently, the secondary coil voltage (\(V_s\)) is calculated as:
\[ \frac{V_p}{V_s} = \frac{N_p}{N_s} \]
With \(V_p = 240 \text{V}\) and \(N_p:N_s = 20:1\), we determine:
\[ V_s = \frac{V_p \times N_s}{N_p} = \frac{240 \times 1}{20} = 12 \text{V} \]
Next, utilizing Ohm's Law (\(V = IR\)) and the secondary coil resistance (\(R = 6.0 \, \Omega\)), we find the secondary coil current (\(I_s\)):
\[ I_s = \frac{V_s}{R} = \frac{12}{6} = 2 \text{A} \]
An ideal transformer conserves power, meaning primary coil power (\(P_p\)) equals secondary coil power (\(P_s\)). Therefore:
\[ P_p = V_p \times I_p = P_s = V_s \times I_s \]
Solving for the primary current (\(I_p\)):
\[ I_p = \frac{V_s \times I_s}{V_p} = \frac{12 \times 2}{240} = 0.10 \text{A} \]
The current drawn by the transformer from the source is therefore \(0.10 \, \text{A}\).
Correct Answer: 0.10 A