1 Solution notation, formulae and model sources. Unless otherwise noted, the compositional variables v, w, x, y, and z may vary between zero and unity and are determined in Perple_X as a function of the computational variables by free-energy minimization. Symbol AbFsp(C1) Solution feldspar Aki(fab) akimotoite Aki(stx7) akimotoite Aki(stx8) akimotoite Amph(DHP) Amph(DPW) Anth clinoamphibole clinoamphibole anthophyllite A-phase Atg B Bio(HP) phase A antigorite brucite biotite Bio(TCC) biotite Formula KyNaxCa1–x–yAl2–x–ySi2+x+yO8, x+y≤1 Notes Source C1 structural state. x>2/3, 1–x– [28] y<~1/10. Dubious, see warnings in solution model file. MgxFe1–x–yAl2ySi1–yO3, x+y≤1 Estimated regular parameter from [17] source. Ilmenite structure. Use with sfo05ver.dat [33,44]. MgxFe1–x–yAl2ySi1–yO3, x+y≤1 Ilmenite structure. Use with [45] stx07ver.dat [45]. MgxFe1–x–yAl2ySi1–yO3, x+y≤1 Ilmenite structure. Use with [55] stx08ver.dat [55]. Superceded by Amph(DPW) [11] Superceded by cAmph(DP). [12] Mg7xFe7(1–x)Si8O22(OH)2 Ideal, does not extrapolate well to high pressure (P>3GPa). Mg7xFe7(1–x)Si2O8(OH)6 Ideal. Mg48xFe48(1–x)Si34O85(OH)62 Ideal. MgxFe1–x(OH)2 Ideal. K[MgxFeyMn1–x–y]3–wAl1+2wSi3– Speciation model, new parameters [42] from THERMOCALC, extended to wO10(OH)2, x+y≤1 cover Mn-solution. K[MgxFeyMn1–x–y]3–u–v– Ti-oxy and Fe3+-Tschermaks [46] 3+ wFe wTiuAl1+vSi3–vO10(OH)2-2u, exchanges. x+y≤1, u+v+w≤1 2 C2/c(stx) C2/c pyroxene [MgxFe1–x]4Si4O12 Use with sfo05ver.dat [33,44] and stx07ver.dat [45]. Use with stx08ver.dat [55]. Costly speciation model, see commentary in solut_09.dat. [44] C2/c(stx8) cAmph(DP) C2/c pyroxene clinoamphibole casmelt Cc(AE) melt calcite CF(stx8) calcium ferrite Chl(HP) chlorite chum clinohumite Chum Clint Cpx(h) clinohumite clintonite clinopyroxene Cpx(HP) clinopyroxene [MgxFe1–x]4Si4O12 [55] Ca2(y+u+v)Nau+2(w+z)[MgxFe1–x]7– [14] 3u–2v–4(w+z)Fe3+2zAl4y+3v+2wSi8– (y+v)O22(OH)2, u+v+w+y+z≤1 CaO-Al2O3-SiO2 melt Dubious. [6] Ca1–xMgxCO3 Entropy model should be checked [2] against source. NaxMgyFe1–x–yAl2-xSixO4, Use with stx08ver.dat [55]. [55] x+y≤1 [MgxFewMn1–x–w]5–y+zAl2(1+y– Speciation model. Under most [29] circumstances afchl endmember z)Si3–y+zO10(OH)8, x+w≤1 can be excluded to save computational resources. Ti-F-OH-Mg-clinohumite. Model should be checked against [15] source. Mg9xFe9(1–x)Si4O16(OH)2 Ideal. CaMg3–xAl2+2xSi2–xO10(OH)2 Ideal. Na1–yCay+z[MgxFe1–x]y–zAl1High structural state, entropy [21,22] model should be verified against y+zSi2+zO6, y+z≤1 sources. Stability seems excessive. Na1–yCayMgxyFe(1–x)yAlySi2O6 Disordered, new parameters from [26] THERMOCALC, extended to cover Acmite, CaTs, and Cr-solution 3 Cpx(l) clinopyroxene Cpx(stx) Cpx(stx7) Cpx(stx8) clinopyroxene clinopyroxene clinopyroxene Ctd(HP) chloritoid Cumm Do(AE) cummingtonite dolomite Do(HP) Ep(HP) dolomite epidote F fluid F(salt) fluid feldspar feldspar Fphl Fsp(C1) phlogopite feldspar Na1–yCay+z[MgxFe1–x]y–zAl1y+zSi2+zO6, y+z≤1 Low structural state, entropy [21,22] model should be verified against sources. Stability seems reasonable. Ca2yMg4–2x–2yFe2xSi4O12 Use with sfo05ver.dat [33,44]. [44] Ca2yMg4–2x–2yFe2xSi4O12 Use with stx07ver.dat [45]. [45] [Ca1–x–yNaxMgy]2[FewMgy+zAl1–w– Use with stx08ver.dat [55]. [55] x–y–z]2Si4O12, w+x+y+z≤1 MgxFeyMn1–x–yAl2SiO5(OH)2, [53] x+y≤1 Mg7xFe7(1–x)Si8O22(OH)2 Ideal. CaMgxFe1–x(CO3)2 Entropy model should be checked [2] against source. CaMgxFe1–x(CO3)2 [30] Ca2Al3–2xFe2xSi3O12OH Speciation model, parameters from THERMOCALC. Can be used with any Perple_X (H2O)x(CO2)1–x [10] internal fluid EoS that allows XCO2 as an independent variable. (H2O)x(CO2)y(NaCl)1–x–y Choose fluid EoS #5 (CORK) to [3] use this model! VERTEX will automatically computer activities from the Hafner et al. H2O-CO2-NaCl EoS. KyNaxCa1–x–yAl2–x–ySi2+x+yO8, High structural state. [19] x+y≤1 KMg3AlSi3O10(OH)2(1–x)Fx Ideal. KyNaxCa1–x–yAl2–x–ySi2+x+yO8, C1 structural state. See [28] x+y≤1 warnings in solution model file. 4 GaHcSp spinel MgxFeyZn1–x–yAl2O3, x+y≤1 GCOHF fluid H2xO1–x Gl glaucophane Na2Mg3xFe3(1–x)Al2Si8O22(OH)2 GlTrTs clinoamphibole Ca2–2wNa2w[MgxFe1–x]3+2yAl3–3y– wSi7+w+yO22(OH)2, w+y≤1 GlTrTsPg clinoamphibole Ca2–2wNaz+2w[MgxFe1–x]3+2y+zAl3– 3y–wSi7+w+yO22(OH)2, w+y+z≤1 GrAd GrAd(EWHP) garnet garnet Ca3Fe3+2(1–x)Al2xSi3O12 [FexCayMg1–x–y]3[Fe1– wAlw]2Si3O12 x+y ≤1 Fe3xCa3yMg3zMn3(1–x–y– z)Al2Si3O12, x+y+z≤1 Fe3xCa3yMg3zMn3(1–x–y– z)Al2Si3O12, x+y+z≤1 Fe3xCa3yMg3zMn3(1–x–y– z)Al2Si3O12, x+y+z≤1 [FexCayMg(1-x+y+z/3)]3Al2– 2zSi3+zO12, x+y≤1 GrPyAlSp(B) garnet GrPyAlSp(G) garnet Gt(HP) garnet Gt(stx) garnet Gt(stx8) garnet [(Na1/3Al2/3)wFexCayMg1-w-xy]3[MgzAl1-z-wSiw+z]2Si2O12, w+x+y+z≤1 Normal spinel, data from Jiri [37] Konopasek. Can be used with any Perple_X [9] internal fluid EoS that allows XO as an independent variable. Ideal. GlTrTsPg model should be preferable. Can be used in preference to [49,51] GlTrTsPg to save computational resources for non-pargasitic (high P) clinoamphibole. Preferable for calculations over [49,51] a large pressure range. See also GlTrTs and TrTsPg(HP). Ideal. Verify in original reference [16] that W’s are for ionic model. [5] Check against published version. [20] [30] Limited majoritic substitution. [44] Use with sfo05ver.dat [33,44] and stx07ver.dat [45]. Use with stx08ver.dat [55]. [55] 5 Gt(WPH) garnet hCrd cordierite IlGkPy IlHm(A) ilmenite ilmenite [FexCayMgzMn1–x–y–z]3[Fe1– wAlw]2Si3O12 x+y+z≤1 Mg2xFe2yMn2(1–x– y)Al4Si5O18•(H2O)z, x+y≤1 MgxMnyFe1–x–yTiO3, x+y≤1 Fe2–xTixO3 Kf alkali feldspar NaxK1–xAlSi3O8 KN-Phen mica lcENDI clinopyroxne KxNa1–xMgyFezAl3– 2(y+z)Si3+y+zO10(OH)2, z+y≤1 Ca1–yMg1+ySi2O6 lcFSHD clinopyroxne Ca1–yFe1+ySi2O6 M(HP) MaPa magnesite margarite MgxFe1–xCO3 CaxNa1–xAl3+xSi3-xO10(OH)2 melt(HP) melt Na-Mg-Al-Si-K-Ca-Fe hydrous silicate melt Parameters change with the wind. [53] Ideal Ideal. ilmenite coexisiting with [1] magnetite, its performance at T~1473 K criticized by Ghiorso, but this probably the best model for T<1073 K. Gives solvus critical T~973 K, x~1/2. Waldbaum & Thompson mixing model [48] for sanidine combined with low structural state endmembers. Extension of MuPa solution model for phengite. C2/c structure. Model should be [13] checked against source. C2/c structure. Model should be [13] checked against source. [30] Unpublished fit to field observations, gives solvus with Tcrit=972 K, Xma=1/3. Model does not behave well at [27,50] high pressure (P>1GPa), see other warnings in solution model file. For granitic compositions. 6 MELTS(GS) melt MF Mn-Opx magnesioferrite orthopyroxene Mica(CHA) mica Mica(CHA1) mica Mont Mt(W) MtUl(A) monticellite magnetite magnetite MuPa mica Neph(FB) O(HP) O(SG) nepheline olivine olivine O(stx) O(stx7) O(stx8) oCcM(HP) olivine olivine olivine dolomite Na-Mg-Al-Si-K-Ca-Fe hydrous silicate melt Model for P<1GPa, see warnings [23] in solution model file. For mafic-ultramafic compositions. MgxFe3–xO4 Ideal. [MnwMgxFe1–x–w]2–yAl2ySi2–yO6, Should be merged with Opx(HP). x+w≤1 KyCaxNa1–x–y(Mg1-vFev)zMgw Less costly than Mica(CHA1) [4,8] TiwAl3+x-w-zSi3-x+zO10(OH)2, because it does not allow Ti and x+y≤1, w+z≤y, Tschermaks substitutions in Caand Na- subsystems. KyCaxNa1–x–y(Mg1-vFev)w+z See Mica(CHA); allows Ti and [4,8] TiwAl3+x-w-zSi3-x+zO10(OH)2, Tschermaks substitutions in Cax+y≤1, w+z≤1 and Na- subsystems. CaxMg2–xSiO4 Ideal. TixFe3–xO4 Valid from 800 to 1300 C. [54] TixFe3–xO4 Akimoto model. Gives solvus [1] critical T~763K, x~1/3. KxNa1–xAl3Si3O10(OH)2 Basis for most white mica [7] models. NaxK1–xAlSiO4 [18] Mg2xFe2yMn2(1–x–y)SiO4, x+y≤1 [30] Mg2xFe2–2xSiO4 Original model refit with one- [43] parameter speciation model. [MgxFe1–x]2SiO4 Use with sfo05ver.dat [33,44] [44] [MgxFe1–x]2SiO4 Use with stx07ver.dat [45]. [45] [MgxFe1–x]2SiO4 Use with stx08ver.dat [55]. [55] Ca1–xMgxCO3 Speciation model. [28] 7 Omph(HP) clinopyroxene Nay[CaMgxFe1–x]1–yAlySi2O6 Omph(GHP) clinopyroxene Opx(HP) Opx(stx) orthopyroxene orthopyroxene Nay+w[CaMgxFe2+(1–x)]1–y– wAlyFe3+wSi2O6 [MgxFe1–x]2–yAl2ySi2–yO6 [MgxFe1–x]4–2yAl4(1–y)Si4O12 Opx(stx8) orthopyroxene OrFsp(C1) feldspar oAmph(DP) orthoamphibole Osm(HP) P Pheng(HP) osumilite periclase mica Pl(h) Pl(I1,HP) plagioclase feldspar Pl(stx8) pMELTS(G) plagioclase melt Pmp pumpellyite Speciation model, new parameters [26] from THERMOCALC, extended to Fesolution. Costly speciation model. [25] Speciation model. Use with sfo05ver.dat [33,44] and stx07ver.dat [45]. Use with stx08ver.dat [55]. [26] [44] [CawFexMg1–x–w]2[FexAlyMg1–x– [55] y]2Si4O12, x+w≤1, x+y≤1 KyNaxCa1–x–yAl2–x–ySi2+x+yO8, C1 structural state. y>1/3, 1–x– [28] x+y≤1 y<~1/10. Dubious, see warnings in solution model file. Ca2uNau+2(w+z)[MgxFe1–x]7–3u–2v– Two parameter speciation model [14] (costly), see comments in 4(w+z)Fe3+2zAl4y+3v+2wSi8– solut_09.dat. (y+v)O22(OH)2, u+v+w+y+z≤1 KFe2–2xMg2x+yAl5–ySi7+yO30 Ideal. [31] MgxFe1–xO Ideal. KxNa1–xMgyFezAl3– Only for potassic phengite. Parameters from THERMOCALC. 2(y+z)Si3+y+zO10(OH)2 NaxCa1–xAl2–xSi2+xO8 High structural state. [36] KyNaxCa1–x–yAl2–x–ySi2+x+yO8, I1 structural state. y<0.04, 1– [28] x+y≤1 x–y<~1/10. See warnings in solution model file. NaxCa1–xAl2–xSi2+xO8 Use with stx08ver.dat [55]. [55] Na-Mg-Al-Si-K-Ca-Fe Model for P>1 GPa? See warnings [24] hydrous silicate melt in solution model file. For mafic-ultramafic compositions. pmp-fpmp-mpmp Model from Claudio Mazzoli. 8 Ppv(og) post-perovskite MgxFe1–x–yAl2ySi1–yO3, x+y≤1 Ppv(stx8) Pu(MW) Pv(fab) post-perovskite pumpellyite perovskite MgxFe1–x–yAl2ySi1–yO3, x+y≤1 pmp-fpmp-mpmp MgxFe1–x–yAl2ySi1–yO3, x+y≤1 Pv(stx7) perovskite Qpx clinopyroxene Ring(stx) Ring(stx7) Ring(stx8) San San(TH) Sapp ringwoodite ringwoodite ringwoodite sanidine sanidine sapphirine Scap Scp scapolite scapolite Sp(GS) spinel Sp(HP) Sp(JR) spinel spinel Ideal (Henry’s law limit). Use with sfo05ver.dat [33,44] and stx07ver.dat [45]. Use with stx08ver.dat [55]. [38],[39] [55] [35] Estimated regular parameter from [17] source. Use with sfo05ver.dat [33,44]. MgxFe1–x–yAl2ySi1–yO3, x+y≤1 Use with stx07ver.dat [45] and [45] stx08ver.dat [55]. Ca1–yMgx(1+y)Fe(1–x)(1+y)Si2O6 C2/c structure. Model should be [40] checked against source. [MgxFe1–x]2SiO4 Use with sfo05ver.dat [33,44]. [44] [MgxFe1–x]2SiO4 Use with stx07ver.dat [45]. [45] [MgxFe1–x]2SiO4 Use with stx08ver.dat [55]. [55] NaxK1–xAlSi3O8 [48] NaxK1–xAlSi3O8 [47] [MgxFe1–x]4–y/2Al9–ySi2–y/2O20 Ideal, site occupancies as in THERMOCALC but extended for Fesolution, see model comments. Na3–3xCa1+3xAl3(1+x)Si6–3xO24CO3 Presumably from B.K. Kuhn’s Phd. mizzonite-meionite Site occupancies as in R. Abart’s Ph.D. thesis, ETH, 1995. MgxFe1–xAl2O3 From Ganguly & Saxena,'87. Ghiorso ’91 is similar. MgxFe1–xAl2O3 MgxFe1–xAl2O3 [32] 9 Sp(stx) spinel MgxFe1–xAl2O3 Sp(stx7) Sp(stx8) St(HP) spinel spinel staurolite Sud sudoite MgxFe1–xAl2O3 MgxFe1–xAl2O3 Mg4xFe4yMn4(1–x– y)Al18Si7.5O48H4, x+y≤1 Mg2xFe2–2xAl4Si3O10(OH)4 Sud(Livi) sudoite T talc TiBio(HP) biotite TiBio(WPH) biotite Toop-melt melt Tr tremolite TrTsPg(HP) clinoamphibole Ca2Naz[MgxFe1–x]3+2y+zAl3– 3ySi7+yO22(OH)2, y+z≤1 Wad(stx) Wad(stx7) Wad(stx8) waddsleyite waddsleyite waddsleyite [MgxFe1–x]2SiO4 [MgxFe1–x]2SiO4 [MgxFe1–x]2SiO4 1/8 inverse spinel. Use with sfo05ver.dat [33,44] Use with stx07ver.dat [45]. Use with stx08ver.dat [55]. Parameters from THERMOCALC. Ideal, mixing on 2 octahedral sites. Mg2xFe2–2xAl4Si3O10(OH)4 Ideal, mixing on 4 octahedral sites. [MgxFe1–x]3–yAl2ySi4–yO10(OH)2 Ideal. K[MgxFeyMn1–x–y]3–w– z/2TizAl1+2wSi3–wO10(OH)2, x+y≤1 K[MgxFe1–x]3–u–v– wFe3+wTiuAl1+vSi3–vO10(OH)2-2u, u+v+w≤1 Toop-Samis model for anhydrous silicate melts Ca2Mg5xFe5(1–x)Si8O22(OH)2 [44] [45] [55] [34] Bio(HP) extended to cover a, dubious, Ti substitution. [42,53] Superior to TiBio(HP), but dubious Ti site population, cf Bio(TCC). [52] [41] Ideal. GlTrTsPg model should be preferable. Use in preference to GlTrTsPg to [49,51] reduce costs for glaucophanepoor (low P) clinoamphibole. Use with sfo05ver.dat [33,44] [44] Use with stx07ver.dat [45]. [45] Use with stx08ver.dat [55]. [55] 10 Wus(fab) magnesiowuestite MgxFe1–xO Wus(stx7) magnesiowuestite MgxFe1–xO Estimated regular parameter from [17] source. Use with sfo05ver.dat [33,44] Use with stx07ver.dat [45] and [45] stx08ver.dat [55]. [1] Andersen DJ,Lindsley DH (1988) Internally Consistent Solution Models for Fe-Mg-Mn-Ti Oxides - Fe-Ti Oxides. American Mineralogist 73:714-26. [2] Anovitz L,Essene EJ (1987) Phase equilibria in the system CaCO -MgCO3-FeCO3. Journal of Petrology 28:389-414. [3] Aranovich LY, Haefner A, Connolly JAD, Gerya TV,Ulmer P (2005) Experimental determination of H2O and CO2 activity-composition relations in the H2O-CO2-NaCl fluids by reversed dehydration and decarbonation reaction. Manuscript 822-8. [4] Auzanneau E, Schmidt MW, Vielzeuf D,Connolly JAD (2010) Titanium in phengite: a geobarometer for high temperature eclogites. Contributions To Mineralogy And Petrology 159:1-24. [5] Berman RG (1990) Mixing Properties of Ca-Mg-Fe-Mn Garnets. American Mineralogist 75:328-44. [6] Berman RG,Brown TH (1984) A thermodynamic model for multicomponent melts, with application to the system CaO-Al2O3-SiO2. Geochimica Et Cosmochimica Acta 48:661-78. [7] Chatterjee ND,Froese E (1975) A thermodynamic study of the pseudo-binary join muscoviteparagonite in the system KAlSi3O8-NaAlSi3O8-Al2O3-SiO2-H2O. American Mineralogist 60:985-93. [8] Coggon R,Holland TJB (2002) Mixing properties of phengitic micas and revised garnet-phengite thermobarometers. Journal of Metamorphic Geology 20:683-96. [9] Connolly JAD (1995) Phase-diagram methods for graphitic rocks and application to the system C-O-H-FeO-TiO2-SiO2. Contributions to Mineralogy and Petrology 119:94-116. [10] Connolly JAD,Trommsdorff V (1991) Petrogenetic grids for metacarbonate rocks - pressuretemperature phase-diagram projection for mixed-volatile systems. Contributions to Mineralogy and Petrology 108:93-105. 3 11 [11] Dale J, Holland T,Powell R (2000) Hornblende-garnet-plagioclase thermobarometry: a natural assemblage calibration of the thermodynamics of hornblende. Contributions to Mineralogy and Petrology 140:353-62. [12] Dale J, Powell R, White RW, Elmer FL,Holland TJB (2005) A thermodynamic model for Ca-Na clinoamphiboles in Na2O-CaO-FeO-MgO-Al2O3-SiO2-H2O-O for petrological calculations. Journal of Metamorphic Geology 23:771-91. [13] Davidson PM, Lindsley DH,Carlson WD (1988) Thermochemistry of pyroxenes on the join Mg2Si2O6CaMgSi2O6 - a revision of the model for pressures up to 30-Kbar. American Mineralogist 73:1264-6. [14] Diener JFA, Powell R, White RW,Holland TJB (2007) A new thermodynamic model for clino- and orthoamphiboles in the system Na2O-CaO-FeO-MgO-Al2O3-SiO2-H2O-O. Journal of Metamorphic Geology 25:631-56. [15] Duffy CJ,Greenwood HJ (1979) Phase-equilibria in the system MgO-MgF2-SiO2-H2O. American Mineralogist 64:1156-74. [16] Engi M,Wersin X (1987) Something to do with grandite garnet. SMPM. [17] Fabrichnaya O (1998) The assessment of thermodynamic parameters for solid phases in the FeMg-O and Fe-Mg-Si-O systems. Calphad-Computer Coupling Of Phase Diagrams And Thermochemistry 22:85-125. [18] Ferry JM,Blencoe JG (1978) Subsolidus Phase Relations in Nepheline-Kalsilite System at 0.5, 2.0, and 5.0 Kbar. American Mineralogist 63:1225-40. [19] Fuhrman ML,Lindsley DH (1988) Ternary-Feldspar Modeling and Thermometry. American Mineralogist 73:201-15. [20] Ganguly J, Cheng WJ,Tirone M (1996) Thermodynamics of aluminosilicate garnet solid solution: New experimental data, an optimized model, and thermometric applications. Contributions to Mineralogy and Petrology 126:137-51. [21] Gasparik T (1984) Experimental study of subsolidus phase relations and mixing properties of pyroxene in the system CaO-Al2O3-SiO2. Geochimica Et Cosmochimica Acta 48:2537-45. [22] Gasparik T (1985) Experimental study of subsolidus phase relations and mixing properties of pyroxene and plagioclase in the system Na2O-CaO-Al2O3-SiO2. Contributions to Mineralogy and Petrology 89:346-57. [23] Ghiorso MS,Sack RO (1995) Chemical Mass-Transfer in Magmatic Processes .4. A Revised and Internally Consistent Thermodynamic Model for the Interpolation and Extrapolation of Liquid- 12 [24] [25] [26] [27] [28] [29] [30] [31] [32] [33] [34] Solid Equilibria in Magmatic Systems at Elevated-Temperatures and Pressures. Contributions to Mineralogy and Petrology 119:197-212. Ghiorso MS, Hirschmann MM, Reiners PW,Kress VC (2002) The pMELTS: A revision of MELTS for improved calculation of phase relations and major element partitioning related to partial melting of the mantle to 3 GPa. Geochemistry Geophysics Geosystems 3:art. no.-1030. Green E, Holland T,Powell R (2007) An order-disorder model for omphacitic pyroxenes in the system jadeite-diopside-hedenbergite-acmite, with applications to eclogitic rocks. American Mineralogist 92:1181-9. Holland T,Powell R (1996) Thermodynamics of order-disorder in minerals. 2. Symmetric formalism applied to solid solutions. American Mineralogist 81:1425-37. Holland T,Powell R (2001) Calculation of phase relations involving haplogranitic melts using an internally consistent thermodynamic dataset. Journal of Petrology 42:673-83. Holland T,Powell R (2003) Activity-composition relations for phases in petrological calculations: an asymmetric multicomponent formulation. Contributions to Mineralogy and Petrology 145:492-501. Holland T, Baker J,Powell R (1998) Mixing properties and activity-composition relationships of chlorites in the system MgO-FeO-Al2O3-SiO2-H2O. European Journal of Mineralogy 10:395-406. Holland TJB,Powell R (1998) An internally consistent thermodynamic data set for phases of petrological interest. Journal of Metamorphic Geology 16:309-43. Holland TJB, Babu E,Waters DJ (1996) Phase relations of osumilite and dehydration melting in pelitic rocks: A simple thermodynamic model for the KFMASH system. Contributions To Mineralogy And Petrology 124:383-94. Jamieson HE,Roeder PL (1984) The Distribution of Mg and Fe-2+ between Olivine and Spinel at 1300-Degrees-C. American Mineralogist 69:283-91. Khan A, Connolly JAD,Olsen N (2006) Constraining the composition and thermal state of the mantle beneath Europe from inversion of long-period electromagnetic sounding data. Journal of Geophysical Research-Solid Earth 111. Livi KJT, Ferry JM, Veblen DR, Frey M,Connolly JAD (2002) Reactions and physical conditions during metamorphism of Liassic aluminous black shales and marls in central Switzerland. European Journal of Mineralogy 14:647-72. 13 [35] Massonne HJ,Willner AP (2008) Phase relations and dehydration behaviour of psammopelite and mid-ocean ridge basalt at very-low-grade to low-grade metamorphic conditions. European Journal of Mineralogy 20:867-79. [36] Newton RC, Charlu TV,Kleppa OJ (1980) Thermochemistry of the high structural state plagioclases. Geochemica Cosmochimica Acta 44:933-41. [37] Nichols GT, Berry RF,Green DH (1992) Internally Consistent Gahnitic Spinel-Cordierite-Garnet Equilibria in the Fmashzn System - Geothermobarometry and Applications. Contributions to Mineralogy and Petrology 111:362-77. [38] Oganov AR,Ono S (2004) Theoretical and experimental evidence for a post-perovskite phase of MgSiO3 in Earth's D '' layer. Nature 430:445-8. [39] Ono S,Oganov AR (2005) In situ observations of phase transition between perovskite and CaIrO3-type phase in MgSiO3 and pyrolitic mantle composition. Earth And Planetary Science Letters 236:914-32. [40] Ottonello G (1992) Interactions and mixing properties in the (C2/c) clinopyroxene quadrilateral. Contributions to Mineralogy and Petrology 111:53-60. [41] Ottonello G (2001) Thermodynamic constraints arising from the polymeric approach to silicate slags: the system CaO-FeO-SiO2 as an example. Journal of Non-Crystalline Solids 282:72-85. [42] Powell R,Holland T (1999) Relating formulations of the thermodynamics of mineral solid solutions: Activity modeling of pyroxenes, amphiboles, and micas. American Mineralogist 84:1-14. [43] Sack RO,Ghiorso MS (1989) Importance of considerations of mixing properties in establishing an internally consistent thermodynamic database - thermochemistry of minerals in the system Mg2SiO4-Fe2SiO4-SiO2. Contributions to Mineralogy and Petrology 102:41-68. [44] Stixrude L,Lithgow-Bertelloni C (2005) Mineralogy and elasticity of the oceanic upper mantle: Origin of the low-velocity zone. Journal of Geophysical Research-Solid Earth 110. [45] Stixrude L,Lithgow-Bertelloni C (2007) Influence of phase transformations on lateral heterogeneity and dynamics in Earth's mantle. Earth And Planetary Science Letters 263:45-55. [46] Tajcmanová L, Connolly JAD,Cesare B (2009) A thermodynamic model for titanium and ferric iron solution in biotite. . Journal of Metamorphic Geology 27:153-64. [47] Thompson JB,Hovis GL (1979) Entropy of Mixing in Sanidine. American Mineralogist 64:57-65. [48] Waldbaum DR,Thompson JB (1968) Mixing Properties Of Sanidine Crystalline Solutions .2. Calculations Based On Volume Data. American Mineralogist 53:2000-? 14 [49] Wei CJ,Powell R (2003) Phase relations in high-pressure metapelites in the system KFMASH (K2O-FeO-MgO-Al2O3-SiO2-H2O) with application to natural rocks. Contributions to Mineralogy and Petrology 145:301-15. [50] White RW, Powell R,Holland TJB (2001) Calculation of partial melting equilibria in the system Na2O-CaO-K2O-FeO-MgO-Al2O3-SiO2-H2O (NCKFMASH). Journal of Metamorphic Geology 19:13953. [51] White RW, Powell R,Phillips GN (2003) A mineral equilibria study of the hydrothermal alteration in mafic greenschist facies rocks at Kalgoorlie, Western Australia. Journal of Metamorphic Geology 21:455-68. [52] White RW, Powell R,Holland TJB (2007) Progress relating to calculation of partial melting equilibria for metapelites. Journal Of Metamorphic Geology 25:511-27. [53] White RW, Powell R, Holland TJB,Worley BA (2000) The effect of TiO2 and Fe2O3 on metapelitic assemblages at greenschist and amphibolite facies conditions: mineral equilibria calculations in the system K2O-FeO-MgO-Al2O3-SiO2-H2O-TiO2-Fe2O3. Journal of Metamorphic Geology 18:497-511. [54] Wood BJ, et al., Chapter 7, in Reviews in Mineralogy. 1991. [55] Xu W, Lithgow-Bertelloni C, Stixrude L,Ritsema J (2008) The effect of bulk composition and temperature on mantle seismic structure. Earth and Planetary Science Letters 275:70-9.