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328   CHAPTER 10



                  presence of low viscosity, partially molten   penetrates into Eurasia. Surface denudation
                  crust beneath Tibet. Variations in crustal   also requires the suture (S) to advance, which
                                                                                          −1
                  thickness between the high plateau and the   is modeled at a rate of V s  = 25 mm a .
                  Ganga foreland, the rate of denudation and   Although S moves during the model, the
                  upper crustal strength also affect the style of   results in Fig. 10.27c–e are shown with a

                  the deformation. The models are relatively   fixed point “S” to keep the size of the
                  insensitive to channel heterogeneities and to   diagrams manageable. Advancing subduction
                  variations in the behavior of the mantle     requires the removal of Eurasian lithosphere,
                  lithosphere beneath the modeled plateau.     which also is modeled by subduction. Indian
                The thermomechanical models of Beaumont        lower crust is subducted along with its
                  et al. (2004) consist of a vertical plane divided   underlying mantle lithosphere. No
                  into crust and mantle layers (Fig. 10.27a). A   displacements occur out of the plane of the
                  passive marker grid and numbered vertical    model.
                  markers track the progressive deformation of      As Indian lithosphere is underthrust beneath

                  the model during convergence. The suture     southern Tibet, channel flow initiates by the
                  (S) marks the position where Indian          development of partially molten material in
                  lithosphere is subducted beneath Eurasia and   the mid-lower crust beneath the plateau (Fig.
                  descends into the mantle at a constant       10.27c,d). Coeval thrust- and normal-sense
                  velocity (V p ) and a constant dip angle (θ).   shear zones develop across the lower and
                  This point is allowed to migrate during      upper parts of the channel, respectively.
                  convergence. The basal velocity condition    These shear zones are interpreted to
                  drives fl ow in the upper plate. The crust    correspond to the Main Central Thrust and
                  consists of upper and middle quartzo-        the South Tibetan Detachment Fault. The
                  felspathic layers overlying a dry granulitic   channel propagates through the converging
                  lower crust that are modeled using a viscous-  crust. Efficient erosion at the southern edge

                  plastic power-law rheology. The initial      of the plateau leads to a coupling between
                  thermal structure (Fig. 10.27b) shows two    the channel flow and surface denudation.

                  radioactive layers (A 1 , A 2 ) that provide   Denudation causes the surface position of
                  internal heat to the crust. The lithosphere-  the suture (S) to migrate toward India

                  asthenosphere boundary is defined to be at    relative to the mantle (Fig. 10.27c–e) because
                  the 1350°C isotherm. Given a basal heat fl ux   it creates an imbalance in the flux of crustal

                               −2
                  of q m  = 20 mW m , a surface heat fl ux of q s    material through the model. The fi nal
                            −2
                  = 71.25 mW m , and a surface temperature     position of the suture after 51–54 Ma mimics
                  (T s ) of 0°C with no heat fl ux through the   the position of the Indus–Zangbo suture
                  sides of the model, the Moho temperature is   within the Tibetan Plateau.
                  704°C. Other important model properties      The coupling between channel fl ow and surface
                  include an extra increment of viscous        denudation eventually leads to the ductile
                  weakening in the crust, which simulates the   extrusion and exhumation of hot material in
                  presence of a small amount of partial melt,   the channel between the coeval thrust and
                  and surface denudation scaled to 1.0–        normal faults (Fig. 10.27d,e). The
                        −1
                  20 mm a .                                    exhumation exposes the high-grade
                Figure 10.27c–e show the results of a model    metamorphic rocks and migmatite
                  that provides an internally consistent       (i.e. a mixed rock consisting of both
                  explanation of the large-scale geometry and   metamorphic and igneous components) of
                  tectonic features of the Himalaya and        the Greater Himalaya. The provenance of
                  southern Tibet. This model incorporates      the channel material is derived from two
                                        −1
                  a convergence rate of 50 mm a  and           sources. Initially, melt weakening in the
                  advancing subduction, which mimics the       middle crust occurs just to the south of point
                  manner in which precollisional suture zones   “S” (Fig. 10.27c). Later, as the suture is
                  wrap around the rigid India indenter as it   advected southward, material is derived from
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