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a : Black Hills quartzite, β - quartz
b : synthetic specimens (CaAl 2 Si 2 O 8 )
c : synthetic specimens (Ca(Mg 0.8 Fe 0.2 )Si 2 O 6 )
d : synthetic specimens (Ca 0.97 (Mg 0.8 Fe 0.2 )Si 1.99 O 6 )
e :Ca 0.98 Mg 0.79 Fe 0.256 Al 0.017 Na 0.012 Si 2 O 6
f :(Mg 0.89 Fe 0.8 Ca 0.3 )SiO 3
g : synthetic specimens ((Mg 0.94 Fe 0.04 Ca 0.02 ) 2 Si 2 O 6 ,(Mg 0.906 Fe 0.091 Ni 0.003 ) 2 Si 2 O 6 ). Water content was not measured.
h : synthetic specimens (Py, Py 70 Alm 16 Gr 14 )
i : A universal flow law based on the results on different garnets
j : synthetic specimens (Py 88 Alm 10 Gr 2 )
k : synthetic specimens
l : Maryland diabase
m : synthetic specimens ( 50% garnet, 40% omphasite, 10% quartz)
n : synthetic specimens San Carlos olivine + orthopyroxene mixture (60:40), no report on water content.
o : synthetic specimens forsterite and Mg-enstatite (97:03 to 80:20).
p : synthetic specimens forsterite + Mg-enstatite (60:40).
q : lherzolite (62% olivine, 26% orthopyroxene, 10% clinopyroxene, 2% spinel)
r : A , r , V are not determined separately. Assuming V = 20 cm 3 / mol, A and r were calculated.
s : r / n = 0.5 was constrained by the experiments. If n = 4then r = 2.
t : Influence of friction is reduced using a liquid pressure confining mediuO.
u : One type of high-pressure deformation apparatus operated to 10 GPa.
v : A room pressure deformation apparatus controlled by a servo system.
w : One type of high-pressure deformation apparatus operated to 23 GPa.
Data source:
Bystricky, M. and Mackwell, S.J., 2001. Creep of dry clinopyroxene aggregates. Journal of Geophysical Research, 106: 13443-13454.
Caristan, Y., 1982. The transition from high-temperature creep to fracture in Maryland diabase. Journal of Geophysical Research, 887: 6781-6790.
Chen, S., Hiraga, T. and Kohlstedt, D.L., 2006. Water weakening of clinopyroxene in the dislocation creep regime. Journal of Geophysical Research, 111: 10.1029/2005JB003885.
Gleason, G.C. and Tullis, J., 1995. A flow law for dislocation creep of quartz aggregates determined with the molten slat cell. Tectonophysics, 247: 1-23.
Hier-Majumder, S., Mei, S. and Kohlstedt, D.L., 2005. Water weakening of clinopyroxene in diffusion creep regime. Journal of Geophysical Research, 110: 10.1029/2004JB003414.
Hirth, G. and Kohlstedt, D.L., 1995. Experimental constraints on the dynamics of partially molten upper mantle: deformation in the diffusion creep regime. Journal of Geophysical
Research, 100: 1981-2001.
Ji, S., Wang, Z. and Wirth, R., 2001. Bulk flow strength of forsterite-enstatite composites as a function of forsterite content. Tectonophysics, 341: 69-93.
Jin, Z.M., Zhang, J., Green, H.W., II. and Jin, S., 2001. Eclogite rheology: implications for subducting lithosphere. Geology, 29: 667-670.
Karato, S. and Jung, H., 2003. Effects of pressure on high-temperature dislocation creep in olivine polycrystals. Philosophical Magazine, A., 83: 401-414.
Karato, S., Wang, Z., Liu, B. and Fujino, K., 1995. Plastic deformation of garnets: systematics and implications for the rheology of the mantle transition zone. Earth and Planetary
Science Letters, 130: 13-30.
Kawazoe, T., Karato, S., Otsuka, K., Jing, Z. and Mookherjee, M., 2009. Shear deformation of dry polycrystalline olivine under deep upper mantle conditions using a rotational
Drickamer apparatus (RDA). Physics of the Earth and Planetary Interiors, 174: 128-137.
Lawlis, J.D., 1998. High Temperature Creep of Synthetic Olivine-Enstatite Aggregates. Ph D Thesis, The Pennsylvania State University, 131 pp.
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