A. Yin et G. Oertel, KINEMATICS AND STRAIN DISTRIBUTION OF A THRUST-RELATED FOLD SYSTEM INTHE LEWIS THRUST PLATE, NORTHWESTERN MONTANA (USA), Journal of structural geology, 15(6), 1993, pp. 707-719
In order to understand interactions between motion along thrusts and t
he associated style of deformation and strain distribution in their ha
ngingwalls, geologic mapping and strain measurements were conducted in
an excellently exposed thrUSt-related fold system in the Lewis thrust
plate, northwestern Montana. This system consists of: (1) an E-direct
ed basal thrust (the Gunsight thrust) that has a flat-ramp geometry an
d a slip of about 3.6 km; (2) an E-verging asymmetric anticline with i
ts nearly vertical forelimb truncated by the basal thrust from below;
(3) a 4-km wide fold belt, the frontal fold complex, that lies directl
y in front of the E-verging anticline; (4) a W-directed bedding-parall
el fault (the Mount Thompson fault) that bounds the top of the frontal
fold belt and separates it from the undeformed to broadly folded stra
ta above; and (5) regionally developed, W-dipping spaced cleavage. Alt
hough the overall geometry of the thrust-related fold system differs f
rom any previously documented fault-related folds, the E-verging antic
line itself resembles geometrically a Rich-type fault-bend fold. The o
bserved initial cut-off and fold interlimb angles of this anticline, h
owever, cannot be explained by cross-section balancing models for the
development of either a fault-bend fold or a fault-propagation fold. P
ossible origins for the E-verging anticline include (1) the fold initi
ated as an open fault-bend fold and tightened only later during its em
placement along the basal thrust and (2) the fold started as either a
fault-bend or a fault-propagation fold, but simultaneous or subsequent
volume change incompatible with any balanced cross-section models alt
ered its shape. Strain in the thrust-related fold system was determine
d by the preferred orientation of mica and chlorite grains. The direct
ion and magnitude of the post-compaction strain varies from place to p
lace. Strains in the forelimb of the hangingwall anticline imply beddi
ng-parallel thinning at some localities and thickening at others. This
inhomogeneity may be caused by the development of thrusts and folds.
Strain in the backlimb of the hangingwall anticline implies bedding-pa
rallel stretching in the thrust transport direction. This could be the
effect of bending as the E-verging anticline was tightened and transp
orted across the basal thrust ramp. Strain measured next to the Gunsig
ht thrust again indicates locally varying shortening and extension in
the transport direction, perhaps in response to inhomogeneous friction
on the fault or else to a history of alternating strain hardening and
softening in the basal thrust zone.