MHT CET · Physics · Capacitance
Two identical capacitors have the same capacitance ' \(\mathrm{C}\) '. One of them is charged to a potential \(V_1\) and the other to \(V_2\). The negative ends of the capacitors are connected together. When the positive ends are also connected, the decrease in energy of the combined system is
- A \(\frac{1}{4} \mathrm{C}\left(\mathrm{V}_1^2-\mathrm{V}_2^2\right)\)
- B \(\frac{1}{4} C\left(V_1^2+V_2^2\right)\)
- C \(\frac{1}{4} C\left(V_1-V_2\right)^2\)
- D \(\frac{1}{4} \mathrm{C}\left(\mathrm{V}_1+\mathrm{V}_2\right)^2\)
Answer & Solution
Correct Answer
(C) \(\frac{1}{4} C\left(V_1-V_2\right)^2\)
Step-by-step Solution
Detailed explanation
Initial energy of the combined system
\(
\mathrm{U}_1=\frac{1}{2} \mathrm{CV}_1^2+\frac{1}{2} \mathrm{CV}_2^2=\frac{\mathrm{C}}{2}\left(\mathrm{~V}_1^2+\mathrm{V}_2^2\right)
\)
On joining the two condensers in parallel, common potential,
\(
\mathrm{V}=\frac{\mathrm{V}_1+\mathrm{V}_2}{2}
\)
\(\therefore \quad\) Final energy of the combined system:
\(
\mathrm{U}_2 \equiv \frac{1}{2}(\mathrm{C}+\mathrm{C})\left(\frac{\mathrm{V}_1+\mathrm{V}_2}{2}\right)^2 \text {. }
\)
\(\therefore \quad\) - Decrease in energy will be:
\(
\begin{aligned}
\Delta \mathrm{U} & =\mathrm{U}_{\mathrm{L}}-\mathrm{U}_2 \\
& =\frac{\mathrm{C}}{2}\left(\mathrm{~V}_1^2+\mathrm{V}_2^2\right)-\frac{1}{2}(\mathrm{C}+\mathrm{C})\left(\frac{\mathrm{V}_1+\mathrm{V}_2}{2}\right)^2 \\
& =\frac{1}{4} \mathrm{C}\left(\mathrm{V}_1-\mathrm{V}_2\right)^2
\end{aligned}
\)
\(
\mathrm{U}_1=\frac{1}{2} \mathrm{CV}_1^2+\frac{1}{2} \mathrm{CV}_2^2=\frac{\mathrm{C}}{2}\left(\mathrm{~V}_1^2+\mathrm{V}_2^2\right)
\)
On joining the two condensers in parallel, common potential,
\(
\mathrm{V}=\frac{\mathrm{V}_1+\mathrm{V}_2}{2}
\)
\(\therefore \quad\) Final energy of the combined system:
\(
\mathrm{U}_2 \equiv \frac{1}{2}(\mathrm{C}+\mathrm{C})\left(\frac{\mathrm{V}_1+\mathrm{V}_2}{2}\right)^2 \text {. }
\)
\(\therefore \quad\) - Decrease in energy will be:
\(
\begin{aligned}
\Delta \mathrm{U} & =\mathrm{U}_{\mathrm{L}}-\mathrm{U}_2 \\
& =\frac{\mathrm{C}}{2}\left(\mathrm{~V}_1^2+\mathrm{V}_2^2\right)-\frac{1}{2}(\mathrm{C}+\mathrm{C})\left(\frac{\mathrm{V}_1+\mathrm{V}_2}{2}\right)^2 \\
& =\frac{1}{4} \mathrm{C}\left(\mathrm{V}_1-\mathrm{V}_2\right)^2
\end{aligned}
\)
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