Step 1: Understand induced current and phase shift.
In electromagnetic induction methods, the primary coil generates a time-varying magnetic field, which induces an electromotive force (EMF) in the secondary coil (coil B). The current induced in coil B gives rise to the secondary field. The phase shift between the primary and secondary fields is influenced by how coil B responds to this induced EMF, which depends on its electrical impedance.
Step 2: Impedance and phase shift.
The impedance \( Z \) of coil B has both resistive and inductive components, and the phase angle \( \phi \) between the voltage and current is given by:
\[
\tan \phi = \frac{\omega L}{R}
\]
where:
\( \omega \) = angular frequency
\( L \) = inductance of the coil
\( R \) = resistance of the coil
This implies that the phase shift is controlled by all three parameters: \( \omega \), \( L \), and \( R \).
Step 3: Role of total current \( I_P \).
While the magnitude of the primary field depends on the total current \( I_P \) flowing through the primary coil, the phase shift in the secondary field is determined by the impedance of coil B and the frequency. Hence, \( I_P \) does not directly control the phase shift. Option (D) is incorrect.
Final Answer:
Correct options: (A), (B), and (C)