Consider two infinitely large plane parallel conducting plates as shown below. The plates are uniformly charged with a surface charge density \( +\sigma \) and \( -\sigma \). The force experienced by a point charge \( +q \) placed at the mid point between the plates will be:
Let the charge distribution on the two plates be \( \sigma \) and \( -\sigma \), with the point charge \( q \) placed at the midpoint between the plates.
The electric field due to each plate at the midpoint is as follows:
For Plate 1, the electric field is \( \frac{\sigma}{2 \epsilon_0} \) directed away from the plate, and for Plate 2, the electric field is \( \frac{\sigma}{2 \epsilon_0} \) directed towards the plate.
Thus, the net electric field experienced by the charge \( q \) is: \[ E_{\text{net}} = \frac{3\sigma}{2 \epsilon_0} \] Now, the force on the charge \( q \) is given by: \[ F = qE = q \times \frac{3\sigma}{2 \epsilon_0} = \frac{3q\sigma}{2 \epsilon_0} \]
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: