The molecular weight and solvent dependences of the characteristic time of chain collapse were studied for poly͑methyl methacrylate͒ ͑PMMA͒ of the molecular weight M w = 6.4ϫ 10 6 and 1.14 ϫ 10 7 in pure acetonitrile ͑AcN͒ and in the mixed solvent of AcN + water ͑10 vol % ͒. The size of PMMA chains was measured as a function of the time after the quench by static light scattering and the chain collapse processes were expressed by the plot of the expansion factor ␣ 2 vs ln t. The chain collapse in the mixed solvent AcN + water ͑10 vol % ͒ was found to occur much faster than that in pure AcN, though the measurement of the former collapse process required several hours. In order to make a comparison between the rates of chain collapses, the fast chain collapse process was superposed on the slow one by scaling the time of the fast process as ␥t. The scale factor ␥ was determined by comparing the chain collapse processes of nearly the same equilibrium expansion factor with each other. Accordingly, the superposition of the collapse for M w = 6.4ϫ 10 6 on that for M w = 1.14ϫ 10 7 yielded ␥ m = 4.0± 0.6 for the process in AcN + water and 5.5± 0.6 in AcN. The superposition of the chain collapse process in AcN + water on that in AcN yielded ␥ s = 9.5± 1.4 for M w = 6.4ϫ 10 6 and 12.0± 1.8 for M w = 1.14ϫ 10 7 . This analysis suggests that ␥ m and ␥ s are constant independent of each other. Thus, by assuming the molecular weight dependence of ␥ m ϳ M z , the characteristic time exp of chain collapse was conjectured as exp ϳ M z , where reflects the nature of solvent species. The ratio of for PMMA in AcN to that in AcN + water is given by ␥ s . The exponent was estimated to be z = 2.4± 0.7 for AcN + water and 3.0± 0.7 for AcN. These values are compatible with the theoretical prediction z = 3 based on a phenomenological model, though the observed characteristic times are longer by several orders of magnitude than those of the theoretical prediction.