To solve this problem, we will use the transformer equations and Ohm's Law. We know that the ratio of turns in the primary coil (\(N_p\)) to the secondary coil (\(N_s\)) is 20:1, and an ideal transformer maintains the ratios of voltage and current according to these turns. Therefore, the voltage across the secondary coil (\(V_s\)) can be obtained using the formula:
\[ \frac{V_p}{V_s} = \frac{N_p}{N_s} \]
Given \(V_p = 240 \text{V}\), \(N_p:N_s = 20:1\), we find:
\[ V_s = \frac{V_p \times N_s}{N_p} = \frac{240 \times 1}{20} = 12 \text{V} \]
Now, using Ohm's Law (\(V = IR\)), where \( R \) is the resistance connected to the secondary coil (\(R = 6.0 \, \Omega\)), the current through the secondary coil (\(I_s\)) is:
\[ I_s = \frac{V_s}{R} = \frac{12}{6} = 2 \text{A} \]
An ideal transformer conserves power, so power in the primary coil (\(P_p\)) equals power in the secondary coil (\(P_s\)). Therefore:
\[ P_p = V_p \times I_p = P_s = V_s \times I_s \]
Solving for the primary current (\(I_p\)):
\[ I_p = \frac{V_s \times I_s}{V_p} = \frac{12 \times 2}{240} = 0.10 \text{A} \]
Thus, the current drawn by the transformer from the source is \(0.10 \, \text{A}\).
Correct Answer: 0.10 A
A coil of area A and N turns is rotating with angular velocity \( \omega\) in a uniform magnetic field \(\vec{B}\) about an axis perpendicular to \( \vec{B}\) Magnetic flux \(\varphi \text{ and induced emf } \varepsilon \text{ across it, at an instant when } \vec{B} \text{ is parallel to the plane of the coil, are:}\)


The graph shows the variation of current with voltage for a p-n junction diode. Estimate the dynamic resistance of the diode at \( V = -0.6 \) V.
