For 'n' identical cells, each with emf $\epsilon$ and internal resistance $r$, connected in parallel, the equivalent emf $\epsilon_{eq}$ is:
Using the extended formula for parallel combination (Eq. 3.59): $\epsilon_{eq}/r_{eq} = \epsilon_1/r_1 + ... + \epsilon_n/r_n$. If all cells are identical ($\epsilon_1 = ... = \epsilon = \epsilon$) and ($r_1 = ... = r_n = r$), then $1/r_{eq} = n/r$, so $r_{eq} = r/n$. Substituting back: $\epsilon_{eq}/(r/n) = n(\epsilon/r) \Rightarrow \epsilon_{eq} = (r/n) \times n(\epsilon/r) = \epsilon$. Thus, for identical cells in parallel, the equivalent emf is equal to the emf of a single cell.