HR: 0800h
AN: T41A-1161 [Abstracts]
TI: Plate Kinematic Model and Resulting Evolution of Oceanic Transform Fault Tectonics Adjacent to the
Macquarie Triple Junction, SW Pacific
AU: Symons, C M
EM: csymons@ucsd.edu
AF: Geological Data Center, Scripps Institution of Oceanography, University of California San Diego, 9500
Gilman Drive Dept 0220
, La Jolla, CA 92093-0220
United States
AU: * Meckel, T A
EM: tmeckel@usgs.gov
AF: Institute for Geophysics, Jackson School of Geosciences, The University of Texas at Austin, 4412
Spicewood Springs Rd. #600, Austin, TX 78759-8500
United States
AU: * Meckel, T A
EM: tmeckel@usgs.gov
AF: Department of Geological Sciences, Jackson School of Geosciences, The University of Texas at Austin, 1
University Station C1100, Austin, TX 78712-0254
United States
AU: Mosher, S
EM: mosher@mail.utexas.edu
AF: Department of Geological Sciences, Jackson School of Geosciences, The University of Texas at Austin, 1
University Station C1100, Austin, TX 78712-0254
United States
AU: Coffin, M F
EM: mcoffin@ori.u-tokyo.ac.jp
AF: Ocean Research Institute, University of Tokyo, 1-15-1 Minamidai, Nakano-ku, Tokyo, 164-8639
Japan
AB:
This research presents reconstructions illustrating the configuration of the Australian-Pacific-Antarctic plate system and
the Macquarie Triple Junction (MTJ) at 7 times from 33.3 Ma to the present (A13o, A8o, A6o, A5o, A3Ay, A2Ay, and 0). Plate
kinematic models are used to characterize the style of plate interaction between the three plates as the dominantly
Ridge-Transform-Transform triple junction evolved. Models of MTJ evolution presented here focus on the complex crustal
interactions that occurred at the southern Australian-Pacific plate boundary during this time, and constrain the tectonic
evolution of the obliquely-convergent transform boundary that actively constructs the southern Macquarie Ridge Complex.
Surprising results include the apparent shortening of the easternmost Southeast Indian Ridge (SEIR) by ~200 km during the
lengthening of the transform due to southern migration of the MTJ. Such behavior explains the curved shape of the transform
that evolved into the Hjort Trench and may be one process by which the Hjort region has accommodated convergence during its
transition from transform fault to obliquely convergent incipient subduction zone. Differences between the amount of
observed subduction at the Puysegur and Hjort Trenches may be a result of the partial accommodation of convergence by
shortening of the easternmost SEIR spreading segment adjacent to the Hjort Trench during transform fault evolution.
Reconstructions indicate that the Antarctic-Pacific boundary was a transform fault connecting the Antarctic-Pacific spreading
ridge system with the SEIR for times between 33.3 and 5.9 Ma. Between 26.6 and 10.9 Ma the Antarctic-Pacific boundary was
likely a leaky transform, accommodating some divergence between the two plates. At 5.9 Ma, a change in Antarctic-Pacific
relative plate motion caused the transform fault to evolve into a spreading ridge. The spreading since 5.9 Ma served to more
efficiently link the SEIR and Antarctic-Pacific spreading ridge systems, as the relative motion of the Antarctic-Pacific and
Antarctic-Macquarie plates became similar in direction and magnitude.
DE: 8150 Plate boundary--general (3040)
DE: 8155 Plate motions--general
DE: 8157 Plate motions--past (3040)
DE: 8158 Plate motions--present and recent (3040)
DE: 3040 Plate tectonics (8150, 8155, 8157, 8158)
SC: Tectonophysics [T]
MN: 2004 AGU Fall Meeting