Hamiltonian systems describing particle motion in a wave with time-dep
endent (chirped) frequency are studied. The wave is found to form a si
ngle-node separatrix (bucket) moving in the phase space at a rate prop
ortional to that of the frequency change. Particles trapped inside the
bucket undergo convection, while untrapped particles colliding with t
he bucket get a resonant kick, in phase space. In toroidal systems, th
ese effects can result in a large radial convective flux roughly propo
rtional to the size of the bucket and the frequency chirping. Possible
applications of this novel mechanism to tokamak plasmas are discussed
.