Two condensers \( C_1 \) & \( C_2 \) in a circuit are joined as shown in the figure. The potential of point A is \( V_1 \) and that of point B is \( V_2 \). The potential at point D will be:
To determine the potential at point D in the circuit with capacitors \(C_1\) and \(C_2\), we can use the principle of charge conservation on capacitors. Since these capacitors are connected in a combination involving points A and B, we consider the equivalent single capacitor between A and B and calculate its potential.
The charge \(Q\) on a capacitor is given by \(Q = CV\), where \(C\) is the capacitance and \(V\) is the potential across its plates. For this system in equilibrium, the sum of the charges on both capacitors should be equal:
\(Q_1 = C_1(V_1 - V_D)\)
\(Q_2 = C_2(V_D - V_2)\)
Since no charge is lost, \(Q_1 = Q_2\). Hence,
\(C_1(V_1 - V_D) = C_2(V_D - V_2)\)
Expanding and rearranging gives:
\(C_1V_1 - C_1V_D = C_2V_D - C_2V_2\)
Bringing terms involving \(V_D\) on one side:
\(C_1V_D + C_2V_D = C_1V_1 + C_2V_2\)
Factoring out \(V_D\):
\(V_D(C_1 + C_2) = C_1V_1 + C_2V_2\)
Solving for \(V_D\):
\(V_D = \frac{C_1V_1 + C_2V_2}{C_1 + C_2}\)
Thus, the potential at point D is \( \frac{C_1V_1 + C_2V_2}{C_1 + C_2} \).
Step 1: Understanding the Concept of Potential Division in a Capacitor Network In a series capacitor network, the charge on each capacitor remains the same. However, the voltage is divided across the capacitors in proportion to their capacitances. The potential at a point between two capacitors is given by the formula: \[ V_D = \frac{C_1 V_1 + C_2 V_2}{C_1 + C_2} \] where: - \( C_1 \) and \( C_2 \) are the capacitances of the two capacitors, - \( V_1 \) and \( V_2 \) are the potentials at points A and B respectively.
Step 2: Explanation of the Formula Since charge conservation applies, the potential at the junction \( D \) can be derived using the principle of charge distribution, which leads to the formula: \[ V_D = \frac{C_1 V_1 + C_2 V_2}{C_1 + C_2} \]
Step 3: Conclusion Thus, the potential at point D is given by: \[ V_D = \frac{C_1V_1 + C_2V_2}{C_1 + C_2} \] which matches option (3).
A 3 kg block is connected as shown in the figure. Spring constants of two springs \( K_1 \) and \( K_2 \) are 50 Nm\(^{-1}\) and 150 Nm\(^{-1}\) respectively. The block is released from rest with the springs unstretched. The acceleration of the block in its lowest position is ( \( g = 10 \) ms\(^{-2}\) )