The capacitance of a parallel plate capacitor with a dielectric inserted is given by: \[ C = \frac{\epsilon_0 A}{d} \] where:
- \( \epsilon_0 \) is the permittivity of free space,
- \( A \) is the area of the plates,
- \( d \) is the distance between the plates. When a dielectric material of dielectric constant \( K \) is inserted into a portion of the capacitor, the capacitance increases.
If half of the area is occupied by the dielectric, the effective capacitance can be calculated by considering the contribution of the dielectric. Let the original capacitance without the dielectric be \( C_0 = \frac{\epsilon_0 A}{d} \).
After inserting the dielectric, the capacitance becomes: \[ C_{\text{new}} = C_0 \left( 1 + K \right) \] where \( K \) is the dielectric constant.
Since half of the area is occupied by the dielectric, the total effective capacitance will be: \[ C_{\text{new}} = (1 + K)C \]
Thus, the new capacitance is \( (1 + K)C \).
Therefore, the correct answer is: \( \text{(3) } (1 + K)C \)
Four capacitors each of capacitance $16\,\mu F$ are connected as shown in the figure. The capacitance between points A and B is __ (in $\mu F$)
Two point charges M and N having charges +q and -q respectively are placed at a distance apart. Force acting between them is F. If 30% of charge of N is transferred to M, then the force between the charges becomes:
If the ratio of lengths, radii and Young's Moduli of steel and brass wires in the figure are $ a $, $ b $, and $ c $ respectively, then the corresponding ratio of increase in their lengths would be: