It is demonstrated that a surface energy anisotropy (anchoring) defines the growth pattern of the fieldinduced transition in a smectic-A liquid crystal (Sm-A). The stable domain phase nucleates as rounded domains but expands as stripes. The change in growth pattern is accounted for a large anchoring strength W, -10 2 -10 ' J/m which is connected with the layer breaking in the vicinity of the cell plates. The temperature dependence of W, for Sm-A (substance CCN-47) is measured for the first time: