Step 1: Set up:
Let the cells have emf \( E_1, E_2 \) and internal resistances \( r_1, r_2 \). Join their positive terminals at A and their negative terminals at B.
Let the cells send currents \( I_1 \) and \( I_2 \) into the external circuit, so the total current is \( I = I_1 + I_2 \).
Step 2: Terminal voltage of each cell:
Both cells are across the same two points, so the voltage \( V = V_A - V_B \) is the same.
\( V = E_1 - I_1 r_1 \) and \( V = E_2 - I_2 r_2 \).
So \( I_1 = \dfrac{E_1 - V}{r_1} \) and \( I_2 = \dfrac{E_2 - V}{r_2} \).
Step 3: Add the currents:
\[ I = I_1 + I_2 = \left(\frac{E_1}{r_1} + \frac{E_2}{r_2}\right) - V\left(\frac{1}{r_1} + \frac{1}{r_2}\right) \]
Solve for V:
\[ V = \frac{E_1 r_2 + E_2 r_1}{r_1 + r_2} - I\,\frac{r_1 r_2}{r_1 + r_2} \]
Step 4: Compare with one cell:
A single cell gives \( V = E_{eq} - I r_{eq} \). So
\[ E_{eq} = \frac{E_1 r_2 + E_2 r_1}{r_1 + r_2}, \qquad r_{eq} = \frac{r_1 r_2}{r_1 + r_2} \]
Final Answer:
\( E_{eq} = \dfrac{E_1 r_2 + E_2 r_1}{r_1 + r_2} \) and \( r_{eq} = \dfrac{r_1 r_2}{r_1 + r_2} \).
\[ \boxed{E_{eq} = \frac{E_1 r_2 + E_2 r_1}{r_1 + r_2},\ r_{eq} = \frac{r_1 r_2}{r_1 + r_2}} \]