Using a power-law relation between three-dimensional nucleation rate J and dimensionless supersaturation ratio S, and the theory of regular solutions to describe the temperature dependence of solubility, a novel Nývlt-like equation of metastable zone width of solution relating maximum supercooling ΔT max with cooling rate R is proposed in the form: ln(ΔT max /T 0 ) = Φ + βlnR, with intercept Φ = {(1−m)/m}ln(ΔH s /R G T lim ) + (1/m)ln(f/KT 0 ) and slope β = 1/m. Here T 0 is the initial saturation temperature of solution in a cooling experiment, ΔH s is the heat of dissolution, R G is the gas constant, T lim is the temperature of appearance of first nuclei, m is the nucleation order, and K is a new nucleation constant connected with the factor f defined as the number of particles per unit volume. It was found that the value of the term Φ for a system at saturation temperature T 0 is essentially determined by the constant m and the factor f. The value of the factor f for a solute−solvent system at initial saturation temperature T 0 is determined by solute concentration c 0 . Analysis of the experiment data for four different solute-water systems according to the above equation revealed that: (1) the values of Φ and m for a system at a given temperature depend on the method of detection of metstable zone width, and (2) the value of slope β = 1/m for a system is practically a temperature-independent constant characteristic of the system, but the value of Φ increases with an increase in saturation temperature T 0 , following an Arrhenius-type equation with an activation energy E sat . The results showed, among others, that solubility of a solute is an important factor that determines the value of the nucleation order m and the activation energy E sat for diffusion. In general, the lower the solubility of a solute in a given solvent, the higher is the value of m and lower is the value of E sat .