The Kobe earthquake (M 7.2) of January 17, 1995, which was the most da
maging earthquake in recent Japanese history, made manifest the need f
or reconsidering the method of evaluating active faults. An earthquake
of this magnitude at this time was unexpected according to convention
al evaluation, in which the potential magnitude of earthquakes at a ce
rtain site is estimated by considering the greatest earthquake in the
past 400 years and the length of the active fault. The following chara
cteristics of this earthquake made it appear unlikely by conventional
understanding: (1) the Kobe earthquake involved several neighboring fa
ults, which had been previously been identified as separate fault syst
ems: (2) the surface rupture of about 10 km length was much shorter th
an the 50 km seismic faulting; (3) the interval of 400 years between t
he Kobe and penultimate Keicho earthquake of 1596 AD (M 7.5), which ha
s been revealed by historical documents and some excavations, is much
shorter than the 2000 years estimated by calculating the average slip
rate of displaced landforms. These shortcomings imply that active faul
t evaluation with the traditional characteristic earthquake model whic
h deals with each fault separately, is not adequate for an area like J
apan where active faults swarm. New concepts such as the block rotatio
n model (Kanaori, 1990; Late Mesozoic-Cenozoic strike-slip and block r
otation in the inner belt of Southwest Japan. Tectonophysics, 177: 381
-399) considering the macroscopic tectonic framework for fault interac
tions are needed. Furthermore, fault dynamics cannot be ignored; physi
cal and temporal parameters associated with faulting, such as moment r
elease rate, must be considered for realistic and precise evaluation.