Two identical capacitors have same capacitance $C$. One of them is charged to the potential $V$ and other to the potential $2 \mathrm{~V}$. The negative ends of both are connected together. When the positive ends are also joined together, the decrease in energy of the combined system is :
Solution
<p>To solve the problem, let's start by considering the energy stored in each capacitor before they are connected together.
<p>The energy stored in a capacitor is given by the formula:</p></p>
<p>$E = \frac{1}{2} C V^2$</p>
<p>Where $E$ is the energy, $C$ is the capacitance, and $V$ is the potential.
<p>For the first capacitor charged to the potential $V$, the energy stored is:</p></p>
<p>$E_1 = \frac{1}{2} C V^2$</p>
<p>For the second capacitor charged to the potential $2V$, the energy stored is:</p>
<p>$E_2 = \frac{1}{2} C (2V)^2 = \frac{1}{2} C \cdot 4V^2 = 2 CV^2$</p>
<p>The total initial energy stored in the system is the sum of $E_1$ and $E_2$:</p>
<p>$E_{\text{initial}} = E_1 + E_2 = \frac{1}{2} CV^2 + 2 CV^2 = \frac{5}{2} CV^2$</p>
<p>When the two capacitors are connected together, their potentials will become equal because they are identical capacitors. Let's denote this final potential as $V_f$. The total charge before and after the connection remains constant because charge is conserved. Therefore, we can write:</p>
<p>$C \cdot V + C \cdot 2V = 2C \cdot V_f$</p>
<p>Simplifying this equation gives us the final potential:</p>
<p>$V + 2V = 2 V_f$</p>
<p>$3V = 2 V_f$</p>
<p>$V_f = \frac{3}{2} V$</p>
<p>The final energy stored in the system when the capacitors are connected is now the total energy stored across both capacitors at the final potential $V_f$:</p>
<p>$$E_{\text{final}} = 2 \cdot \frac{1}{2} C V_f^2 = 2 \cdot \frac{1}{2} C \left(\frac{3}{2} V\right)^2 = C \cdot \frac{9}{4} V^2$$</p>
<p>The decrease in energy $ \Delta E $ of the combined system is the initial energy minus the final energy:</p>
<p>$\Delta E = E_{\text{initial}} - E_{\text{final}}$</p>
<p>$\Delta E = \frac{5}{2} CV^2 - \frac{9}{4} CV^2$</p>
<p>$\Delta E = \frac{10}{4} CV^2 - \frac{9}{4} CV^2$</p>
<p>$\Delta E = \frac{1}{4} CV^2$</p>
<p>The correct answer is:</p>
<p>Option A: $\frac{1}{4} CV^2$</p>
About this question
Subject: Physics · Chapter: Electrostatics · Topic: Electric Potential and Capacitance
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