Solveeit Logo

Question

Question: ...

A

(E1+E2C1+C2)C2\left(\frac{E_1+E_2}{C_1+C_2}\right)C_2

B

(E1E2C1+C2)C2\left(\frac{E_1-E_2}{C_1+C_2}\right)C_2

C

(E1+E2C1+C2)C1\left(\frac{E_1+E_2}{C_1+C_2}\right)C_1

D

(E1E2C1+C2)C1\left(\frac{E_1-E_2}{C_1+C_2}\right)C_1

Answer

(E1E2C1+C2)C1\left(\frac{E_1-E_2}{C_1+C_2}\right)C_1

Explanation

Solution

The problem asks for the potential difference between points 'a' and 'b' in the given circuit. The circuit consists of two capacitors C1C_1 and C2C_2, and two batteries E1E_1 and E2E_2, arranged in a closed loop.

To solve this, we apply the superposition principle, a valid method for linear circuits like those with capacitors and batteries. We consider the effect of each battery acting alone and then combine the results.

  1. Effect of E1E_1 alone (short E2E_2):

    The circuit becomes a series combination of C1C_1 and C2C_2 connected across E1E_1. The equivalent capacitance is Ceq=C1C2C1+C2C_{eq} = \frac{C_1 C_2}{C_1+C_2}. The charge on each capacitor is Q=E1Ceq=E1C1C2C1+C2Q = E_1 C_{eq} = E_1 \frac{C_1 C_2}{C_1+C_2}. The potential difference across C2C_2 (which is VaVbV_a - V_b due to E1E_1) is VC2,E1=Q/C2=E1C1C2(C1+C2)C2=E1C1C1+C2V_{C2, E1} = Q/C_2 = \frac{E_1 C_1 C_2}{(C_1+C_2)C_2} = \frac{E_1 C_1}{C_1+C_2}.

  2. Effect of E2E_2 alone (short E1E_1):

    The circuit becomes a series combination of C1C_1 and C2C_2 connected across E2E_2. The equivalent capacitance is Ceq=C1C2C1+C2C_{eq} = \frac{C_1 C_2}{C_1+C_2}. The charge on each capacitor is Q=E2Ceq=E2C1C2C1+C2Q' = E_2 C_{eq} = E_2 \frac{C_1 C_2}{C_1+C_2}. Now, consider the direction. E2E_2 drives charge in the opposite direction compared to E1E_1 for VaVbV_a-V_b. The positive terminal of E2E_2 is at 'b'. So, VbV_b is higher than VYV_Y. The potential difference across C2C_2 is VaVbV_a - V_b. If E2E_2 is the only source, it will charge C2C_2 such that Vb>VaV_b > V_a (positive charge on lower plate of C2C_2). So, VbVa=Q/C2=E2C1C2(C1+C2)C2=E2C1C1+C2V_b - V_a = Q'/C_2 = \frac{E_2 C_1 C_2}{(C_1+C_2)C_2} = \frac{E_2 C_1}{C_1+C_2}. Therefore, VaVbV_{a} - V_{b} due to E2E_2 alone is VC2,E2=E2C1C1+C2V_{C2, E2} = -\frac{E_2 C_1}{C_1+C_2}.

  3. Total potential difference:

    VaVb=VC2,E1+VC2,E2=E1C1C1+C2E2C1C1+C2V_a - V_b = V_{C2, E1} + V_{C2, E2} = \frac{E_1 C_1}{C_1+C_2} - \frac{E_2 C_1}{C_1+C_2}. VaVb=(E1E2)C1C1+C2V_a - V_b = \frac{(E_1 - E_2) C_1}{C_1+C_2}.

Therefore, the final answer is (E1E2C1+C2)C1\left(\frac{E_1-E_2}{C_1+C_2}\right)C_1.