Lasers nd application in modifying the characteristics of metallic surfaces in industry. In the present study, a laser non-conduction heating situation is investigated and the recession velocity of the surface is computed after considering: (a) constant temperature evaporation at the surface and (b) the steady evaporation condition. It is found that, in the initial phase of evaporation, the velocity of the liquid-vapour interface (recession velocity) predicted from constant temperature evaporation at the surface condition is more realistic than that corresponding to the steady evaporation situation. M oreover, as evaporation progresses, the magnitude of the surface temperature increases because of recoil pressure developed at the vapour-liquid interface. Consequently, the surface temperature rises and the recession velocity is determined from a steady heating situation in place of that predicted from constant temperature evaporation at the surface condition. NOTATION C p speci c heat (J/kg K ) I surf laser power intensity available at the surface (W/m 2 ) I 0 laser power intensity (W/m 2 ) k thermal conductivity (W/m K ) L ev latent heat of evaporation (J/kg) T …x , t † temperature (K ) T b evaporation temperature (K ) T s surface temperature (K ) V recession velocity (m/s) a thermal diffusivity (m 2 /s) d absorption coef cient (m ¡1 ) r density of the workpiece material (kg/m 3 )