The given data:
Length of rod, \(\ell = 60 \, \text{cm} = 0.6 \, \text{m}\), Angular velocity, \(\omega = 20 \, \text{rad/s}\), Magnetic field, \(B = 0.5 \, \text{T}\).
The potential difference \(V_O - V_A\) between the ends of a rod rotating in a magnetic field is given by:
\[ V_O - V_A = \frac{B \omega \ell^2}{2}. \]
Substitute the values:
\[ V_O - V_A = \frac{0.5 \times 20 \times (0.6)^2}{2} = \frac{0.5 \times 20 \times 0.36}{2}. \]
\[ V_O - V_A = \frac{3.6}{2} = 1.8 \, \text{V}. \]
However, since the magnetic field is parallel to the axis of rotation, no emf is induced across the rod. Therefore,
\[ V_A = V_B \implies V_A - V_B = 0. \]
Answer: \(0 \, \text{V}\)
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:
For the thermal decomposition of \( N_2O_5(g) \) at constant volume, the following table can be formed, for the reaction mentioned below: \[ 2 N_2O_5(g) \rightarrow 2 N_2O_4(g) + O_2(g) \] Given: Rate constant for the reaction is \( 4.606 \times 10^{-2} \text{ s}^{-1} \).