Question 11 Mark
A rod of length l rotates with a small but uniform angular velocity $\omega$ about its perpendicular bisector. A uniform magnetic field B exists parallel to the axis of rotation. The potential difference between the centre of the rod and an end is:
- $\text{zero}$
- $\frac{1}{8}\omega\text{Bl}^2$
- $\frac{1}{2}\omega\text{Bl}^2$
- $\text{B}\omega\text{l}^2$
Answer

Take a small element dx at a distance of 'x' centre
$\text{Þ}\text{d}\in\int_{0}^{\frac{1}{2}}\text{B}\omega\text{x}\text{dx}=\frac{\text{B}\omega\text{x}^2}{2}\Big|_{0}^{\frac{1}{2}}$
$\in=\frac{1}{8}\omega\text{Bl}^2$
View full question & answer→- $\frac{1}{8}\omega\text{Bl}^2$

Take a small element dx at a distance of 'x' centre
$\text{Þ}\text{d}\in\int_{0}^{\frac{1}{2}}\text{B}\omega\text{x}\text{dx}=\frac{\text{B}\omega\text{x}^2}{2}\Big|_{0}^{\frac{1}{2}}$$\in=\frac{1}{8}\omega\text{Bl}^2$













