Let the capacitance of the first capacitor be \( C_1 = 100 \, \text{pF} \) and its initial voltage be \( V_i = 60 \, \text{V} \).
The initial charge on the first capacitor is \( Q_i = C_1 V_i = (100 \, \text{pF})(60 \, \text{V}) = 6000 \, \text{pC} \).
A second uncharged capacitor with capacitance \( C_2 \) is connected in parallel to the first capacitor. When capacitors are connected in parallel, the voltage across them becomes equal.
The final voltage across the second capacitor is given as \( V_f = 20 \, \text{V} \).
Since they are in parallel, the final voltage across the first capacitor is also \( V_f = 20 \, \text{V} \).
The total charge in the system is conserved. The initial charge was only on the first capacitor, \( Q_i = 6000 \, \text{pC} \).
After connecting the second capacitor, this charge is distributed between the two capacitors.
The final charge on the first capacitor is \( Q_{f1} = C_1 V_f = (100 \, \text{pF})(20 \, \text{V}) = 2000 \, \text{pC} \).
The final charge on the second capacitor is \( Q_{f2} = C_2 V_f = C_2 (20 \, \text{V}) \).
By conservation of charge: \[ Q_i = Q_{f1} + Q_{f2} \] \[ 6000 \, \text{pC} = 2000 \, \text{pC} + C_2 (20 \, \text{V}) \] \[ 4000 \, \text{pC} = C_2 (20 \, \text{V}) \] \[ C_2 = \frac{4000 \, \text{pC}}{20 \, \text{V}} = 200 \, \text{pF} \] The capacitance of the second capacitor is 200 pF. Alternatively, using the formula for the final voltage when a charged capacitor \( C_1 \) with initial voltage \( V_i \) is connected in parallel to an uncharged capacitor \( C_2 \): \[ V_f = \frac{C_1 V_i}{C_1 + C_2} \] Given \( V_f = 20 \, \text{V} \), \( C_1 = 100 \, \text{pF} \), and \( V_i = 60 \, \text{V} \): \[ 20 = \frac{(100)(60)}{100 + C_2} \] \[ 20 (100 + C_2) = 6000 \] \[ 2000 + 20 C_2 = 6000 \] \[ 20 C_2 = 4000 \] \[ C_2 = \frac{4000}{20} = 200 \, \text{pF} \]
Four capacitors each of capacitance $16\,\mu F$ are connected as shown in the figure. The capacitance between points A and B is __ (in $\mu F$)
Match List-I with List-II: List-I
The dimension of $ \sqrt{\frac{\mu_0}{\epsilon_0}} $ is equal to that of: (Where $ \mu_0 $ is the vacuum permeability and $ \epsilon_0 $ is the vacuum permittivity)