Impulse propagation in small-diameter (1-3-mu-m) axons with inhomogene
ous geometry was simulated. The fibres were represented by a series of
3-mu-m-long compartments. The cable equation was solved for each comp
artment by a finite-difference approximation (Cooley and Dodge 1966).
First-order differential equations governing temporal changes in membr
ane potential or Hodgkin-Huxley (1952) conductance parameters were sol
ved by numerical integration. It was assumed that varicosity and inter
varicosity segments had the same specific cable constants and excitabi
lity properties, and differed only in length and diameter. A single lo
ng varicosity or a 'clump' of 3-mu-m-long varicosities changed the poi
nt-to-point (axial) conduction velocity within as well as to either si
de of the geometrically inhomogeneous regions. When 2-mu-m-diameter, 3
-mu-m-long varicosities were distributed over the 1-mu-m-diameter fibe
r length as observed in serotonergic axons, mean axial conduction velo
city was between that of uniform-diameter 1 and 2-mu-m fibers, and cha
nged predictably with different cable parameters. Fibers with inexcita
ble varicosity membranes also supported impulse propagation. These sim
ulations provided a general theoretical basis for the slow (< 1 M/s) c
onduction velocity attributed to small-diameter unmyelinated varicose
axons.