The torque \(\tau\) is given by: 
\[ \tau = pE \sin \theta \] This can be written as: \[ \tau = (2aq) E \sin \theta \] Substituting the known values: \[ \tau = \left(5 \times 10^{-3} \times 1 \times 10^{-12} \times 10^3\right) \times \frac{4}{5} \] Simplifying: \[ \tau = 4 \times 10^{-12} \, \text{Nm} \] The direction of the torque is along the negative \(Z\)-direction.
Predict the direction of induced current in the situations described by the following Figs. 6.18(a) to (f ).
A long solenoid with 15 turns per cm has a small loop of area 2.0 cm2 placed inside the solenoid normal to its axis. If the current carried by the solenoid changes steadily from 2.0 A to 4.0 A in 0.1 s, what is the induced emf in the loop while the current is changing?
A rectangular wire loop of sides 8 cm and 2 cm with a small cut is moving out of a region of uniform magnetic field of magnitude 0.3 T directed normal to the loop. What is the emf developed across the cut if the velocity of the loop is 1 cm s-1 in a direction normal to the (a) longer side, (b) shorter side of the loop? For how long does the induced voltage last in each case?
A 1.0 m long metallic rod is rotated with an angular frequency of 400 rad s-1 about an axis normal to the rod passing through its one end. The other end of the rod is in contact with a circular metallic ring. A constant and uniform magnetic field of 0.5 T parallel to the axis exists everywhere. Calculate the emf developed between the centre and the ring.
A horizontal straight wire 10 m long extending from east to west is falling with a speed of 5.0 m s-1, at right angles to the horizontal component of the earth’s magnetic field, 0.30 \(\times\)10-4 Wb m-2 .