When \( n \) identical cells are connected in series, the total effective e.m.f. is given by: \[ E_{\text{total}} = nE \]. If two cells are connected with reverse polarity, their individual e.m.f.s subtract from the total e.m.f., resulting in: \[ E'_{\text{total}} = (n-2)E \]. Consequently, the potential difference across a single reversed cell 'X' equals the sum of the e.m.f.s of the two reversed cells: \[ V_X = 2E \]. Therefore, the potential difference across cell 'X' is \( 2E \).