The response of the toroidal flow velocity to being abruptly locked in
the vicinity of a magnetohydrodynamic (MHD) tearing-mode-induced magn
etic island is examined analytically and numerically using a diffusive
transport model in a cylindrical plasma. The resultant toroidal momen
tum confinement is shown to degrade significantly after mode locking,
as is often observed on many tokamaks and reversed field pinches (RFPs
). The degraded toroidal momentum confinement time in the core and edg
e regions of the plasma are evaluated and compared with experimental o
bservations. The mode Locking time-scale itself is also investigated b
y using a model toroidal torque balance equation. The decrease of mode
frequency during mode locking seems to be governed mainly by the elec
tromagnetic torque exerted on the resistive layer. For tokamak plasmas
, the mode locking time-scale is found to be much shorter than the dif
fusion time-scale, which is in general agreement with experimental obs
ervations.