Recently, the reactor mixing angle theta(13) has been measured precisely by Daya Bay, RENO, and T2K experiments with a moderately large value. However, the standard form of neutrino mixing patterns such as bimaximal, tri-bimaximal, golden ratio of types A and B, hexagonal, etc., which are based on certain flavor symmetries, predict vanishing theta(13). Using the fact that the neutrino mixing matrix can be represented as V-PMNS = U-l(dagger) UvPv, where U-l and U-v result from the diagonalization of the charged lepton and neutrino mass matrices and P-v is a diagonal matrix containing Majorana phases, we explore the possibility of accounting for the large reactor mixing angle by considering deviations both in the charged lepton and neutrino sector. In the charged lepton sector we consider the deviation as an additional rotation in the (12) and (13) planes, whereas in the neutrino sector we consider deviations to various neutrino mixing patterns through (13) and (23) rotations. We find that with the inclusion of these deviations it is possible to accommodate the observed large reactor mixing angle theta(13), and one can also obtain limits on the charge-conjugation parity-violating Dirac phased delta(CP) and Jarlskog invariant J(CP) for most of the cases. We then explore whether our findings can be tested in the currently running NuMI Off-axis v(e) Appearance experiment with three years of data taking in neutrino mode followed by three years with the anti-neutrino mode.