When a hot solid particle is submerged into an ambient fluid near a fr
ee liquid-gas interface, a non-uniform temperature field around the pa
rticle produces surface tension gradients at the interface and generat
es thermocapillary how in the surrounding fluid. This flow sets the pa
rticle itself in motion towards or away from the interface. In the fir
st part of the paper, the interaction between a hot spherical solid pa
rticle and a plane undeformable liquid-gas interface is studied. The v
elocity of the thermocapillary induced motion of the solid particle is
proportional to the surface tension gradient at the liquid-gas interf
ace, and is calculated in the approximation of the Stokes how and a ze
ro Peclet number as a function of the separation distance between the
particle and the interface. The asymptotic cases of both small and lar
ge separation distances are studied. In the second part of the paper,
the interaction between a hot solid sphere and a gas bubble submerged
into an ambient fluid is studied in the limiting case when the separat
ion distance between them tends to zero. The velocity of a pairwise mi
gration of a particle and a bubble in contact is calculated as a funct
ion of their radius ratio. The asymptotic values of the individual vel
ocities of a solid particle and a gas bubble in near contact are also
computed. The relative velocity of their motion towards each Ether is
found to be proportional to the separation distance between them. In t
he third part of the paper, we investigate the effect of gravity on th
e thermocapillary driven motion of a solid particle for the two cases.
It is shown that due to the thermocapillary interaction, a particle c
an move against the buoyancy forces. (C) 1997 American Institute of Ph
ysics.