Following a scheme developed for a subduction zone by Savage in 1983, which
was successfully applied to a transform plate boundary by Matsu'ura and ot
hers in 1986, a dislocation model for a plate collision zone is formulated.
The solution consists of a rigid plate motion and a tensile dislocation. I
n addition to this, a strike-slip dislocation is needed when the collision
boundary is not perpendicular to the plate converging direction. Theoretica
lly predicted gradual change in horizontal displacements over the collision
zone well explains the results of GPS continuous observation in central Ja
pan where the Eurasian and Okhotsk plates are thought to be colliding. The
maximum uplift rate is predicted as 1/pi times that of converging velocity,
however the observed uplift rate is much smaller than that, although verti
cal movements observed by GPS network is much less accurate than horizontal
movements. A comparison of the theoretical results with the observation su
ggests relatively thin elastic plates, whose thickness is about 30 km,The o
btained dislocation model has a close connection with a horizontal detachme
nt fault. The displacement fields above the advancing and retreating edges
of a horizontal rectangular detachment fault are mathematically equivalent
to those of collision and rift zones, respectively, and lateral edges to a
transform fault boundary. The displacement fields at a colliding and a rift
ing boundaries are the same except for their signs.