Analyzing the Setup
Imagine you are tracing the path of a single closed loop circuit. We have two cells connected in this loop: E1 with an EMF of 6 V and an internal resistance of 2Ω, and E2 with an EMF of 4 V and an internal resistance of 8Ω.
The most critical step is to look closely at their polarities. The negative terminal of the 6 V cell faces the negative terminal of the 4 V cell, meeting at point X. Because they are pushing current in opposite directions, they are in direct opposition to each other.
The Master Equation
Since the cells are opposing, the net electromotive force (EMF) driving the circuit will be the difference between their individual EMFs. The total resistance of the circuit is simply the sum of their internal resistances, as they are connected in series within the loop.
We can use Ohm's law for the entire loop to find the current:
I=Reqεnet=r1+r2E1−E2
Calculating the Current
Let's substitute the given values into our master equation. The 6 V cell is stronger than the 4 V cell, so the net EMF is 6−4=2 V. The total resistance is 2+8=10Ω.
Now, which way does this current flow? The 6 V cell dominates the circuit, pushing current out of its positive terminal. Therefore, the current flows clockwise, meaning it travels from Y to X through the top branch.
The Charging Cell
We need to find the potential difference across points X and Y, which is exactly the terminal voltage across cell E2. Notice a fascinating detail: the current of 0.2 A is entering the positive terminal of the 4 V cell.
This means the cell is being charged, not discharged! When a cell is being charged by an external source, its terminal voltage is greater than its EMF. The formula we must use is:
Final Calculation
Let's plug in the numbers for our charging cell. The EMF is 4 V, the current is 0.2 A, and its internal resistance is 8Ω.
Multiplying 0.2 by 8 gives us 1.6 V. Adding this to the 4 V of EMF, we get:
The total potential difference across points X and Y is exactly 5.6 V.