For a point inside the wire (\(r<a\)), the magnetic field is given by:
\[B_1 \times 2\pi \frac{a}{2} = \mu_0 \frac{I}{4} \implies B_1 = \frac{\mu_0 I}{4\pi a}.\]
For a point outside the wire (\(r>a\)), the magnetic field is:
\[B_2 \times 2\pi \times 2a = \mu_0 I \implies B_2 = \frac{\mu_0 I}{4\pi a}.\]
The ratio of magnetic fields:
\[\frac{B_1}{B_2} = \frac{\frac{\mu_0 I}{4\pi a}}{\frac{\mu_0 I}{4\pi a}} = 1 : 1.\]
A current-carrying coil is placed in an external uniform magnetic field. The coil is free to turn in the magnetic field. What is the net force acting on the coil? Obtain the orientation of the coil in stable equilibrium. Show that in this orientation the flux of the total field (field produced by the loop + external field) through the coil is maximum.
The largest $ n \in \mathbb{N} $ such that $ 3^n $ divides 50! is:
Let \[ I(x) = \int \frac{dx}{(x-11)^{\frac{11}{13}} (x+15)^{\frac{15}{13}}} \] If \[ I(37) - I(24) = \frac{1}{4} \left( b^{\frac{1}{13}} - c^{\frac{1}{13}} \right) \] where \( b, c \in \mathbb{N} \), then \[ 3(b + c) \] is equal to: