The specific heat and related thermophysical properties of liquid Fe 77.5 Cu 13 Mo 9.5 monotectic alloy were investigated by an electromagnetic levitation drop calorimeter over a wide temperature range from 1482 to 1818 K. A maximum undercooling of 221 K (0.13 T m ) was achieved and the specific heat was determined as 44.71 J·mol −1 ·K −1 . The excess specific heat, enthalpy change, entropy change and Gibbs free energy difference of this alloy were calculated on the basis of experimental results. It was found that the calculated results by traditional estimating methods can only describe the solidification process under low undercooling conditions. Only the experimental results can reflect the reality under high undercooling conditions. Meanwhile, the thermal diffusivity, thermal conductivity, and sound speed were derived from the present experimental results. Furthermore, the solidified microstructural morphology was examined, which consists of (Fe) and (Cu) phases. The calculated interface energy was applied to exploring the correlation between competitive nucleation and solidification microstructure within monotectic alloy.high undercooling, specific heat, monotectic alloy, thermophysical property, rapid solidificationThe thermophysical properties of undercooled liquid metals and alloys have aroused great research interest in the field of materials physics in recent years [1][2][3][4][5][6] . Specific heat, one of the most important thermophysical properties, has a significant influence on developing the current solidification theory [3][4][5][6] . Due to the metastable state of undercooled alloy melts, the conventional experimental methods cannot be applied to determining their thermophysical properties. This results in great difficulty to obtain these important data. Therefore, the thermodynamic research of highly undercooled metals and alloys has been in the qualitative or semi-quantitative state.Up to now, the experimental data for undercooled metals and alloys are still very scarce, although there have been some reports. In the recent literature, only the measurements of some pure metals and simple binary alloys are available. For monotectic alloys, the second liquid phase L 2