If an excitable medium is moving with relative shear, the waves of exc
itation may be broken by the motion. We consider such breaks for the c
ase of a constant linear shear flow. The mechanisms and conditions for
the breaking of solitary waves and wave trains are essentially differ
ent: the solitary waves require the velocity gradient to exceed a cert
ain threshold, while the breaking of repetitive wave trains happens fo
r arbitrarily small velocity gradients.