The bootstrap current in a non-Maxwellian tokamak plasma with electron
cyclotron heating is calculated. The calculation is exact in the limi
t of highly charged ions, where pitch-angle scattering dominates over
quasilinear diffusion, and shows that the current is entirely determin
ed by the pressure of the trapped electrons. If the ion charge is fini
te, the current is shown to consist of two terms: one driven by collis
ions, and one driven by the heating and losses. The former is calculat
ed approximately by using a model collision operator, and is found to
be determined by the distribution of trapped electrons alone; the latt
er is discussed qualitatively.