The magnetic field at point \( A \), \( B_A \), is given by:
\[ B_A = \frac{\mu_0 I}{2 \pi r} + \frac{\mu_0 (2I)}{2 \pi (3r)} = \frac{5 \mu_0 I}{6 \pi r}. \]
The magnetic field at point \( C \), \( B_C \), is given by:
\[ B_C = \frac{\mu_0 (2I)}{2 \pi r} + \frac{\mu_0 I}{2 \pi (3r)} = \frac{7 \mu_0 I}{6 \pi r}. \]
The ratio of magnetic fields \( B_A \) to \( B_C \) is:
\[ \frac{B_A}{B_C} = \frac{5}{7}. \]
Thus, we find:
\[ x = 5. \]
Choose the correct set of reagents for the following conversion:
A bead of mass \( m \) slides without friction on the wall of a vertical circular hoop of radius \( R \) as shown in figure. The bead moves under the combined action of gravity and a massless spring \( k \) attached to the bottom of the hoop. The equilibrium length of the spring is \( R \). If the bead is released from the top of the hoop with (negligible) zero initial speed, the velocity of the bead, when the length of spring becomes \( R \), would be (spring constant is \( k \), \( g \) is acceleration due to gravity):