The thermomechanical force acting on an asymmetrically heated body in
HE II is discussed The force is produced by the normal component flow
caused by the thermal inhomogeneity. The effect is calculated in terms
of linearized dissipative two-liquid hydrodynamics for the case of a
spherical body. For the 3-d geometry the force is essentially determin
ed by the viscous contribution (while that for a plane body would be c
aused by the hydrostatical fountain pressure). This fact results in th
e sensitivity of the effect to the boundary conditions for v(nperpendi
cular-to). Thus the experimental observation of the thermomechanical f
orce can give an opportunity for measurement of the unknown kinetic co
efficient.