Step 1: Use charge conservation.
The total charge before and after connection must remain constant because the battery is removed.
Initial charge on first capacitor: \[ Q_i = C_1 V_1 = 10 \times 50 = 500 \, \text{pC} \]
Step 2: After connection, voltage becomes common.
Let \(C_2\) be the capacitance of the second capacitor and \(V_f = 20 \, \text{V}\). Final charge on both capacitors combined: \[ Q_f = (C_1 + C_2)V_f \] By conservation of charge: \[ Q_i = Q_f \Rightarrow 500 = (10 + C_2) \times 20 \] \[ 10 + C_2 = 25 \Rightarrow C_2 = 15 \, \text{pF} \]
Step 3: Conclusion.
Hence, the capacitance of the second capacitor = 15 pF.
In a coaxial cable, the radius of the inner conductor is 2 mm and that of the outer one is 5 mm. The inner conductor is at a potential of 10 V, while the outer conductor is grounded. The value of the potential at a distance of 3.5 mm from the axis is: 
A sphere of radius \( R \) has a uniform charge density \( \rho \). A sphere of smaller radius \( \frac{R}{2} \) is cut out from the original sphere, as shown in the figure. The center of the cut-out sphere lies at \( z = \frac{R}{2} \). After the smaller sphere has been cut out, the magnitude of the electric field at \( z = -\frac{R}{2} \) is \( \frac{\rho R}{n \epsilon_0} \). The value of the integer \( n \) is: 