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Question: A ring of radius $r$ carries a charge of uniform linear charge density $\lambda$. A uniform magnetic...

A ring of radius rr carries a charge of uniform linear charge density λ\lambda. A uniform magnetic field B0B_0 exists in the space as shown. Find the angular impulse acting on the wheel when the field is switched off.

Answer

πλr3B0\pi \lambda r^3 B_0

Explanation

Solution

When the magnetic field changes, an induced electric field is generated. According to Faraday's Law of Induction, Edl=dΦBdt\oint \vec{E} \cdot d\vec{l} = -\frac{d\Phi_B}{dt}. For a uniform magnetic field BB changing with time, the induced electric field at the radius rr of the ring is E=r2dBdtE = -\frac{r}{2} \frac{dB}{dt}. The force on an infinitesimal charge element dq=λdldq = \lambda dl is dF=dqEdF = dq E. The torque dτd\tau on this element is dτ=rdF=r(dq)Ed\tau = r dF = r (dq) E. Substituting dq=λrdθdq = \lambda r d\theta and E=r2dBdtE = -\frac{r}{2} \frac{dB}{dt}, we get dτ=λr32dBdtdθd\tau = -\frac{\lambda r^3}{2} \frac{dB}{dt} d\theta. Integrating over the ring gives the total torque τ=πλr3dBdt\tau = -\pi \lambda r^3 \frac{dB}{dt}. The angular impulse is Jθ=τdt=(πλr3dBdt)dt=πλr3dBJ_\theta = \int \tau dt = \int \left(-\pi \lambda r^3 \frac{dB}{dt}\right) dt = -\pi \lambda r^3 \int dB. Since the field is switched off, the change in magnetic field is ΔB=BfinalBinitial=0B0=B0\Delta B = B_{final} - B_{initial} = 0 - B_0 = -B_0. Thus, Jθ=πλr3(B0)=πλr3B0J_\theta = -\pi \lambda r^3 (-B_0) = \pi \lambda r^3 B_0.