Based on analyses for the electromagnetic pressure on the melt and the heat induced in the melt, the ratio of heat to pressure Q 0 /P m is de®ned, to give the relationship between Q 0 /P m and the thickness a, the electromagnetic parameter (mg) of the melt and the electric current frequency f under the electromagnetic con®nement and shaping process. If Q 0 /P m is large, any adjustment to the melt shape will easily cause a variation of the temperature in the melt. In this situation, there appears to be a more sensitive interaction between the shape and the temperature ®eld and a more narrow adjustment range for the process. Experiments on thin plate samples with a cross-section of 6 mm £ 18 mm are done with two kinds of induction coils. The results show that when a coil with a trumpet inside wall is used and the positions of the melt top and the S/L interface are properly selected, the melt periphery is nearly vertical and the temperature gradient ahead of the S/L interface is high. Under these conditions, a more stable and wider coupling between the shape and the temperature ®eld is continuously maintained and samples with a smooth surface and unidirectional crystals are successfully obtained. q