In the present study, the morphological instability during an electrochemical deposition is considered with a linear stability analysis, and also the effect of buoyancy-driven convection on the evolution of surface unevenness is tested. In the absence of buoyant forces, the surface concentration gradient enhanced the surface roughness while the surface tension stabilized the growth of protuberances on the surface, which is in good agreement with the existing results. Near the onset of convective motion, the surface irregularity is damped by an increase in the buoyant force. As the buoyancy is further strengthened, the phase transition from a stationary behavior to an oscillating one is observed.Many studies on morphological instability have been done since the original works of Mullins and Sekerka. 1,2 In their pioneering studies, they showed that the morphological instability sets in when the destabilizing surface-concentration gradient overcomes the stabilizing surface tension. Since then, the Mullins-Sekerka-type criterion has played a standard role in the studies on the evolution of surface irregularity, such as directional solidification, 3 chemical vapor deposition, 4 and electrochemical deposition. 5 In practice, it is important to control the surface roughness in the manufacturing process. 6 The electrochemical deposition system is very popular due to its simple process and low cost, but there is still a serious problem that involves the unavoidable appearance of morphological irregularities.Aogaki et al. 5 analyzed the powder crystal formation on the electrode surface under pontentiostatic conditions, and also focused systematically on the mechanism of morphological instability under the galvanostatic condition. 7,8 After these studies, much critical research was conducted on the effective factors that influence the onset of morphological instability, for example, the absence of ohmic potential, the variation of boundary-layer thickness, the effect of supporting electrolyte, the capillary effect, and the effect of additives. On the basis of the Mullins-Serkerka criterion, 1,2 they are well summarized by Schwarzacher. 9 In the electrochemical deposition system, another physical phenomenon is the onset of buoyancy-driven convection. If the upward facing cathode is located below the downward facing anode in the electrolyte-saturated cell, the electrodissolution and deposition of metal ion will proceed on the upper and lower electrodes with an external potential supply. Gradually, the concentration of electrolyte near the upper electrode becomes higher than that near the lower electrode. This causes such a buoyancy-driven convection as the Rayleigh-Bénard convection. 10 In the presence of buoyancy, the convection can lead to unexpected redistribution of concentration field near the growth front. The convective motion can be readjusted by moving the diffusion boundary layer, and therefore, the coupling behavior between convection and morphological change is very complicated. In case of the coupled morphologic...