Step 1: Understanding the Concept:
When a charged capacitor is connected to an uncharged one, the total charge is conserved but distributed across both.
Due to this redistribution, some energy is lost (mainly as heat and radiation), and the final energy is less than the initial energy.
Key Formula or Approach:
1. Initial Energy: \(U_i = \frac{1}{2}CV^2\)
2. Common Potential: \(V_c = \frac{C_1V_1 + C_2V_2}{C_1 + C_2}\)
3. Final Energy: \(U_f = \frac{1}{2}(C_1 + C_2)V_c^2\)
Step 2: Detailed Explanation:
1. Initial Energy calculation:
\(C = 900 \text{ pF} = 900 \times 10^{-12} \text{ F}\), \(V = 100 \text{ V}\).
\[ U_i = \frac{1}{2} \times 900 \times 10^{-12} \times (100)^2 = 450 \times 10^{-12} \times 10^4 = 4.5 \times 10^{-6} \text{ J} \]
2. Common Potential calculation:
Since \(C_1 = C_2 = 900 \text{ pF}\) and the second is uncharged:
\[ V_c = \frac{C \times 100 + C \times 0}{C + C} = \frac{100C}{2C} = 50 \text{ V} \]
3. Final Energy of system (b):
The total capacitance is \(C_{total} = C + C = 1800 \text{ pF}\).
\[ U_f = \frac{1}{2} \times (1800 \times 10^{-12}) \times (50)^2 \]
\[ U_f = 900 \times 10^{-12} \times 2500 = 225 \times 10^4 \times 10^{-12} = 2.25 \times 10^{-6} \text{ J} \]
Step 3: Final Answer:
The energy stored by the system is \(2.25 \times 10^{-6}\) J.