As the second most abundant rock-forming mineral in the continental crust, quartz has been considerably studied by the geophysics and mechanics communities (for instance, deformation features in quartz have long been recognized as the most reliable indicators of major shock events on Earth [French & Koeberl, 2010; Grieve et al., 1996; Stöffler, 1972; Stöffler & Langenhorst, 1994]). Understanding of the mechanical response of quartz to extreme conditions is essential to understanding planetary impacts, underground explosions and other geological and seismic events. A great deal is known about the mechanical behavior of quartz, but comprehensive constitutive models that can describe the material behavior under a variety of loading conditions are lacking. In particular, comprehensive modeling of impact events requires sophisticated constitutive models which can describe the response of quartz under dynamic loading conditions and for arbitrary loading paths. Note that the spatial distributions and evolution of stress states (i.e., the loading path) are always complex within natural impact events. Under large confinements or high loading rates, many different deformation mechanisms (e.g., dislocations, twinning, phase transformation, and amorphization) may be activated in geomaterials, as can failure mechanisms such as fracture. Most constitutive models for minerals are phenomenological rather than physics-based (or mechanism-based). Phenomenological models are generally computationally efficient and have their parameters calibrated through impact experiments. As an example, several models for the equation of state (EOS) of quartz have been developed by Swegle (1990); Boettger (1992); and Luo et al. (2003), generally focused on phase transitions and incorporating simple elastic-plastic strength models. Similarly, various models implemented in commercial softwares can be applied to geomaterials once the full set of model parameters is calibrated (