The time-dependent total spin correlation functions of the two- and the thr
ee-dimensional classical XY models seem to have a very narrow first dynamic
scaling interval and, after this interval, a much broader anomalous second
dynamic scaling interval appears. In this paper, this intriguing feature f
ound in our previous work is re-examined. By introducing a phenomenological
characteristic time for this intermediate time interval, the second dynami
c scaling behavior can be explained. Moreover, the dynamic critical exponen
t found from this novel characteristic time is found to be identical to tha
t found from the usual dynamic scaling theory developed in the wave vector
and frequency domain. For continuous spin models, in which the spin variabl
e related to a long-range order parameter is not a constant of motion, our
method yielded the dynamic critical exponent with less computational effort
s.