Concept:
The deflecting torque acting on a current carrying coil placed in a magnetic field is
\[
\tau = NBAI\sin\theta
\]
where
• \(N\) = number of turns,
• \(B\) = magnetic field,
• \(A\) = area of coil,
• \(I\) = current through coil,
• \(\theta\) = angle between magnetic field and normal to the coil.
In an ordinary magnetic field, the torque depends on \(\theta\). Hence the torque changes as the coil rotates.
Step 1: Understand the purpose of radial magnetic field.
In a moving coil galvanometer, the pole pieces are specially shaped so that the magnetic field becomes radial.
In a radial magnetic field, the plane of the coil always remains parallel to the magnetic field lines.
Therefore,
\[
\theta = 90^\circ
\]
for all positions of the coil.
Step 2: Substitute into torque equation.
Since
\[
\sin 90^\circ =1,
\]
the torque becomes
\[
\tau = NBAI.
\]
This expression is independent of the angular position of the coil.
Hence the torque remains constant during rotation.
Step 3: Analyse other options.
• Soft iron core increases magnetic field strength but does not make torque independent of orientation.
• Hair spring provides restoring torque only.
• Eddy currents provide damping and do not affect constant torque.
Therefore,
\[
\boxed{\text{Correct Option (B)}}
\]