A small bob of mass 100 mg and charge +10 µC is connected to an insulating string of length 1 m. It is brought near to an infinitely long non-conducting sheet of charge density \( \sigma \) as shown in figure. If the string subtends an angle of 45° with the sheet at equilibrium, the charge density of sheet will be :
From the diagram in the solution, we have the force acting on the charge due to the electric field of the sheet:
The force is given by: \[ F_e = qE = mg \] where \( q \) is the charge and \( E \) is the electric field due to the sheet. The electric field is related to the charge density \( \sigma \) as: \[ E = \frac{\sigma}{2 \epsilon_0} \] Thus, the equation becomes: \[ q \left( \frac{\sigma}{2 \epsilon_0} \right) = mg \] Rearranging to solve for \( \sigma \): \[ \sigma = \frac{2g m}{q} \] Substitute the known values: \[ \sigma = \frac{2 \times 8.85 \times 10^{-12} \times 100 \times 10^{-6} \times 10}{10 \times 10^{-6}} \] \[ \sigma = 17.7 \times 10^{-10} \text{ C/m}^2 \] \[ \sigma = 1.77 \text{ nC/cm}^2 \] Thus, the charge density of the sheet is \( 1.77 \) nC/cm\(^2\).
The largest $ n \in \mathbb{N} $ such that $ 3^n $ divides 50! is:
The term independent of $ x $ in the expansion of $$ \left( \frac{x + 1}{x^{3/2} + 1 - \sqrt{x}} \cdot \frac{x + 1}{x - \sqrt{x}} \right)^{10} $$ for $ x>1 $ is: