 
  
  
   
  V. N. Biktashev[*],
  A. V. Holden,
  M. A. Tsyganov[ ]
] 
 
  (Department of Physiology, University of Leeds, Leeds LS2 9JT, UK) 
 
  J. Brindley, 
  N. A. Hill 
 
  (Department of Applied Mathematics,University of Leeds, Leeds LS2 9JT, UK) 
 
Submitted 1998/03/30, Accepted 1998/08/12
If an excitable medium is moving with relative shear, the waves of excitation may be broken by the motion. We consider such breaks for the case of a constant linear shear flow. The mechanisms and conditions for the breaking of solitary waves and wavetrains are essentially different: the solitary waves require the velocity gradient to exceed a certain threshold, whilst the breaking of repetitive wavetrains happens for arbitrarily small velocity gradients.
PACS:  
47.70.Fw, 82.40.Bj, 82.40.Ck, 87.10.+e, 87.22.As, 92.20.Jt, 92.20.Rb