The magnetic force per unit length \( F/L \) on a current-carrying wire in a magnetic field is given by: \[ \frac{F}{L} = B I \sin \theta \] where - \( B = 200 \, {mT} = 200 \times 10^{-3} \, {T} = 0.2 \, {T} \), - \( I = 4\sqrt{3} \, {A} \), - \( \theta = 60^\circ \).
Calculate the force per unit length: \[ \frac{F}{L} = 0.2 \times 4\sqrt{3} \times \sin 60^\circ \] We know \[ \sin 60^\circ = \frac{\sqrt{3}}{2} \] So, \[ \frac{F}{L} = 0.2 \times 4\sqrt{3} \times \frac{\sqrt{3}}{2} = 0.2 \times 4 \times \frac{3}{2} = 0.2 \times 6 = 1.2 \, {N/m} \]
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.