![]() |
![]() |
![]() |
KINK AXES
Since kink-bands are formed by interlayer slip, they are of subclass 1B
style i.e. the orthogonal thickness within the kink-band and in the
un-deflected layering remains the same. Such kink-bands are called REVERSE
OR CONTRACTIONAL KINK-BANDS. Conversely, if the orthogonal thickness
within the kink-band is systematically reduced than that in the
un-deflected layering the kink-bands are called NORMAL OR EXTENSIONAL
KINK-BANDS. The difference between the normal and reverse kink bands is
shown in figure accompanying this text. If the compressive stress acts
parallel to the layering, conjugate kink-bands or box folds are produced
but if it acts at an angle to the layering, a single set of kink-bands are
developed more or less at the exclusion of the other. Patterson and Weiss
(1966) produced conjugate and single kink-bands experimentally and one of
their significant conclusions has been that under large shortening,
kink-bands are converted into chevron folds. Dewey (1966) made significant
contribution towards our understanding of the nature and origin of
kink-bards and Arvid Johnson and his coworkers have presented through a
series of papers (see 1976 numbers of Tectonophysics) the origin of
kink-bands by extensive theoretical treatment of the problem of their
origin and geometry.
|