1 2 Online resource 1 for: 3 4 5 The ~AD 1250 effusive eruption of El Metate shield volcano 6 (Michoacán, Mexico): Magma source, crustal storage, eruptive 7 dynamics, and lava rheology 8 9 Magdalena Oryaëlle Chevrel*, Marie-Noëlle Guilbaud and Claus Siebe 10 Departamento de Vulcanología, Instituto de Geofísica, Universidad Nacional Autónoma de 11 México, Coyoacán, México D.F., México 12 *e-mail:[email protected] 1 METHODS FOR THERMO-BAROMETRY AND HYGROMETRY CALCULATIONS 13 14 15 16 1. Olivine-liquid thermometer: 17 18 19 20 21 22 23 In order to constrain the temperature of olivine crystallisation we chose the olivineliquid thermometer based on the Fe–Mg exchange between olivine and the liquid from which olivine crystallized. We used the equation 22 from Putirka (2008), which is a modification of the Beattie (1993) thermometer, in order to correct the systematic temperature overestimation: 𝑇 = {15294.6 + 1318.8𝑃(𝐺𝑃𝑎) + 2.4834[𝑃(𝐺𝑃𝑎)]2 } 𝑜𝑙⁄𝑙𝑖𝑞 𝑙𝑖𝑞 𝐿 )] ÷ {8.048 + 2.8352 ln 𝐷𝑀𝑔 + 2.097 ln[1.5(𝐶𝑀𝑁 + 2.575 ln[3(𝑋𝑆𝑖𝑂 )] 2 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 − 1.41𝑁𝐹 + 0.222𝐻2 𝑂𝑙𝑖𝑞 + 0.5𝑃(𝐺𝑃𝑎)} Where: ⁄ 𝑜𝑙 𝑙𝑖𝑞 𝑙𝑖𝑞 𝑂𝑙 𝐷𝑀𝑔 = 𝑋𝑀𝑔 ⁄𝑋𝑀𝑔 𝑙𝑖𝑞 𝑙𝑖𝑞 𝑙𝑖𝑞 𝑙𝑖𝑞 𝑙𝑖𝑞 𝑙𝑖𝑞 𝐿 𝐶𝑀𝑁 = 𝑋𝐹𝑒𝑂 + 𝑋𝑀𝑛𝑂 + 𝑋𝑀𝑔𝑂 + 𝑋𝐶𝑎𝑂 + 𝑋𝐶𝑜𝑂 + 𝑋𝑁𝑖𝑂 𝐿 𝐿 𝑁𝐹 = 7⁄2 ln(1 − 𝑋𝐴𝑙𝑂 ) + 7 ln(1 − 𝑋𝑇𝑖𝑂 ) 1.5 2 When using the olivine-liquid thermometer we took the pressure values suggested by Hasenaka and Carmichael (1987) and Hasenaka et al. (1994) who showeded that most shield lavas from the MGVF plot between the 8-kbar dry liquidus boundary defined by Baker and Eggler (1987) and the 1-bar plagioclase-saturated liquidus boundaries of Grove et al. (1982) on the olivine-augite-quartz diagram. Based on this we took 8 kbar as a maximum pressure limit for olivine crystallization. Considering that olivine is the first mineral to crystallize, we assumed that the composition of the olivine core is in equilibrium with a liquid having the composition of the bulk rock. Equilibrium was tested considering the constant Fe-Mg exchange coefficient between olivine and the liquid: KD(Fe-Mg)ol-liq = 0.3 ±0.03 that is independent of T and composition. We used a graphical method by plotting the olivine Mg# versus liquid Mg# on the Rhodes’ diagram (Dungan et al. 1978; Rhodes et al. 1979a; Fig A1). The olivine-liquid pairs falling outside of this interval were disregarded. We noted that the migration of the points toward an iron-rich olivine composition indicates differentiation processes of the melt as olivine crystallizes. Olivine rims are found in equilibrium with a recalculated melt composition (equals to the bulk rock composition minus the composition of olivine core according to their proportion is the samples). We then took a lower pressure (5 kbar) to estimate the lower temperature of olivine crystallisation. The error associated with this thermometer is estimated to be ± 43 ºC. 2 55 56 57 58 59 60 61 62 63 64 65 66 67 68 69 70 71 72 73 74 75 76 77 78 Fig. A1: Rhodes’ diagram: test for olivine–liquid equilibrium. Continuous line represents the constant KD(FeMg)ol-liq = 0.3 and the dashed lines represent the interval: ± 0.03. 14285/14286 (F1): Ten olivine core analyses (Fo83) in equilibrium with the bulk rock composition (KD = 0.290 ±0.017) yield 1176 ºC (3ºC of stdev) at 8 kbar. Five olivine rims (Fo75) are found to be in equilibrium with a residual liquid after 6 % of olivine and 0.5 % of Fe-Ti oxide crystallization at KD = 0.288±0.008 yield T= 1065ºC at 5 kbar. 1205 (F4b) Ten olivine core analyses (Fo82) are found in equilibrium with the bulk rock composition (KD = 0.283 ±0.023) and yield 1135 ºC (3ºC of stdev) at 8 kbar. Eight olivine rim analyses (Fo78) in equilibrium with a residual liquid after 2 % of olivine crystallization (KD = 0.292±0.020) yield T= 1084ºC at 5 kbar. 2. Two pyroxenes thermo-barometer: Since Opx and Cpx are both present in all rocks, we used the two-pyroxene thermobarometer proposed by Brey and Köhler (1990) and recalibrated by Putirka (2008) that is based on the partitioning of enstatite + ferrosilite (= Fm2Si2O6 = EnFs; FmO = FeO + MgO + MnO) between clinopyroxene and orthopyroxene. We used Eq. 37 from Putirka (2008) that is restricted to Cpx with Mg#>0.75 to estimate the temperature: 3 104 𝑋 𝑐𝑝𝑥 𝑐𝑝𝑥 𝑜𝑝𝑥 𝑐𝑝𝑥 ) = 13.4 − 3.4 ln ( 𝐸𝑛𝐹𝑠 + 23.85(𝑋𝑀𝑛 ) 𝑜𝑝𝑥 ) + 5.59 ln(𝑋𝑀𝑔 ) − 8.8(𝑀𝑔# 𝑇(°𝐶) 𝑋𝐸𝑛𝐹𝑠 79 80 81 82 83 84 85 86 87 88 89 90 91 92 93 94 95 96 97 98 99 100 101 102 103 104 105 106 107 108 𝑜𝑝𝑥 𝑐𝑝𝑥 + 6.48(𝑋𝐹𝑚𝐴𝑙 ) − 2.38(𝑋𝐷𝑖 ) − 0.044𝑃(𝑘𝑏𝑎𝑟) 2 𝑆𝑖𝑂6 The output of this equation is then used as input into Eq. 39 to calculate the pressure: 𝑜𝑝𝑥 𝑜𝑝𝑥 𝑜𝑝𝑥 𝑃(𝑘𝑏𝑎𝑟) = −94.25 + 0.045𝑇(°𝐶) + 187.7(𝑋𝐴𝑙(𝑉𝐼) ) + 246.8(𝑋𝐹𝑚𝐴𝑙 ) − 212.5(𝑋𝐸𝑛 ) 2 𝑆𝑖𝑂6 1.66 𝑜𝑝𝑥 𝑐𝑝𝑥 𝑐𝑝𝑥 + 127.5(𝑎𝐸𝑛 )− − 69.4(𝑋𝐸𝑛𝐹𝑠 ) − 133.9(𝑎𝐷𝑖 ) 𝐾𝑓 where: 𝑜𝑝𝑥 𝑎𝐸𝑛 = 𝑜𝑝𝑥 0.5𝑋𝑀𝑔 𝑜𝑝𝑥 0.5𝑋𝑀𝑔 ( 𝑜𝑝𝑥 𝑜𝑝𝑥 𝑜𝑝𝑥 𝑜𝑝𝑥 𝑜𝑝𝑥 ) ( 𝑜𝑝𝑥 𝑜𝑝𝑥 𝑜𝑝𝑥 𝑜𝑝𝑥 𝑜𝑝𝑥 𝑜𝑝𝑥 ) 𝑋𝐶𝑎 + 0.5𝑋𝑀𝑔 + 0.5𝑋𝐹𝑒 0.5𝑋𝐹𝑒 + 𝑋𝐶𝑟 + 0.5𝑋𝑀𝑔 2+ + 𝑋𝑀𝑛 + 𝑋𝑁𝑎 2+ + 𝑋𝐹𝑒 3+ + 𝑋𝐴𝑙(𝑉𝐼) + 𝑋𝑇𝑖 and 𝑐𝑝𝑥 𝑐𝑝𝑥 𝑐𝑝𝑥 𝑐𝑝𝑥 𝑐𝑝𝑥 𝑐𝑝𝑥 𝑐𝑝𝑥 𝑎𝐷𝑖 = (𝑋𝐶𝑎 )⁄(𝑋𝐶𝑎 + 0.5𝑋𝑀𝑔 + 0.5𝑋𝐹𝑒 2+ + 𝑋𝑀𝑛 + 𝑋𝑁𝑎 ) We performed several iterations by solving simultaneously the two equations, which is accomplished by using the output of one equation as an input for the other, to find the best solutions for both equations. As with the other systems, we tested for equilibrium using the Mg-Fe exchange partition coefficient: KD (Fe-Mg)cpx-opx =(XFecpx / XMgcpx)/( XFeopx / XMgopx) =1.090 ± 0.14. We excluded the clinopyroxene–orthopyroxene pairs that lie beyond the area delimited by the dashed lines (Fig. A3). The precision is estimated to be ± 38 ºC and ±2.8 kbar. 4 109 110 111 Fig. A3: Test for equilibrium of cpx-opx pairs. 112 113 14285 (F1): In this sample we did not find pyroxene phenocrysts. Five pairs of opx-cpx microlites where encountered in equilibrium and yielded 1074ºC and 3.5 kbar. 114 115 Six pairs of opx-cpx microlites forming olivine reaction rims indicate 1100ºC and a pressure near surface (negative value of P). 116 117 1205 (F4b): Nine cpx-opx pairs (both phenocrysts and microphenocrysts) were found to be in equilibrium and indicate 987 ºC and 4.2 kbar. 118 119 14282 (F4): Sixteen cpx-opx pairs (both phenocrysts and microphenocrysts) were found to be in equilibrium and indicate an average T=989 ºC and P=4.1 kbar. 120 121 14268 (F5): Sixteen cpx-opx pairs (both phenocrysts and microphenocrysts) were found to be in equilibrium and indicate an average T=971 ºC and P= 2.1 kbar. 122 14298 (F6): Six cpx-opx microphenocryst pairs indicate 946 °C and 0.63 kbar. 123 124 14309 (F7): Only one microlite cpx-opx pair was found in equilibrium and resulted in 894 °C and 0 kbar. 125 126 1210 (F11): The average value of 7 combinations of microlite cpx-opx pairs found at the rim of the hornblende crystal indicates T=979 ºC and P= 0.9 kbar. 127 128 129 14308 (F12): Only one pair of pyroxene phenocrysts was in equilibrium and yielded T=938 ºC and P= 0 kbar. Four pairs of microlites forming the hornblende reaction rim indicate T=966 ºC and P= 1.16 kbar. 130 131 3. Amphibole thermo-barometer and hygrometer: 132 133 134 135 We used the thermo-barometer of Ridolfi et al. (2010). This model was chosen because it is applicable to amphibole-bearing calc-alkaline products of subduction-related settings. It is based on empirical formulations which work independently with different compositional components (i.e. Si*, AlT, Mg*, [6]Al*) of a single amphibole crystal. 136 The thermometer is related to the silica index (Si*) defined as: 137 𝑇 = −151.487𝑆𝑖 ∗ + 2041 5 138 where [4] 139 140 [6] [6] 𝐴𝑙 𝐴𝑙 𝑇𝑖 𝐹𝑒 3+ 𝐹𝑒 2+ 𝑀𝑔 𝐵𝐶𝑎 𝐵𝑁𝑎 𝐴𝑁𝑎 [4] 𝑆𝑖 = 𝑆𝑖 + − 2 𝑇𝑖 − − + + + + + − 15 2 1.8 9 3.3 26 5 1.3 15 𝐴 [ ] + 2.3 ∗ 141 The accuracy of the thermometer is estimated to be of ±22°C. 142 143 The water content of the melt in equilibrium with the amphibole when it crystallizes can be retrieved using the octahedral aluminum index [6]Al* via: 144 𝐻2 𝑂𝑚𝑒𝑙𝑡 = 5.215 𝐴𝑙 ∗ + 12.28 145 [6] where [4] 146 [6] ∗ 𝐴𝑙 = [6] [6] 𝐴𝑙 𝑆𝑖 + 𝑇𝑖 𝐶𝐹𝑒 2+ 𝑀𝑔 𝐵𝐶𝑎 + 𝐴[ ] 𝐴𝑁𝑎 𝐹𝑒# 𝐴𝑙 + − − − + + − 1.56𝐾 − 13.9 5 3 1.7 1.2 2.7 1.6 147 148 Uncertainty of H2O wt. % is between 0.8 and 1 wt. %. 149 150 151 Finally, the confining pressure can be calculated from the following barometric equation: 𝑃 = 19.209𝑒 (1.438𝐴𝑙𝑇 ) 152 153 Maximum error of the pressure is estimated to be 0.4 kbar. 154 155 156 157 158 159 14268 (F5): Six hornblendes were analyzed for a total of 23 points, no obvious correlation was found between the core and the rim of the grains. The PT conditions range from 983 °C, and 4.7 kbars to 933 °C and 2.7 kbar for a water content between 5.1 and 6.4 wt. % H2O. Average values are: T=946 ºC (stdev 11ºC); P=3.1 kbar (stdev 0.4 kabr) and 5.5 wt. % H2O (0.3 stdev). 160 161 162 163 164 14298 (F6): Five hornblendes were analyzed for a total of 12 points. No obvious variation in P-T was found between the core and the rim of the grains. The P-T conditions range from 980 °C and 4.1 kbar to 950 °C and 2.6 kbar for a water content between 4.9 and 6.4 wt. % H2O. Average values are: T=972 ºC (stdev 11ºC); P=3.2 kbar (stdev 0.4 kabr) and 5.5 wt. % H2O (0.5 stdev). 165 166 167 168 169 14309 (F7): Five hornblendes were analyzed for a total of 14 points. No obvious variation in P-T was found between the core and the rim of the grains. The P-T conditions range from 981 °C and 3.6 kbar to 946 °C and 2.6 kbar for a water content between 5.1 and 6.1 wt. % H2O. Average values are: T=967 ºC (stdev 11ºC); P=3.2 kbar (stdev 0.3 kabr) and 5.6 wt. % H2O (0.3 stdev). 170 171 172 173 1210 (F11): Six hornblendes were analyzed for a total of 17 points. The PT conditions range from 940 °C and 4 kbar to 910 °C and 2.4 kbar for a water content between 5.3 and 7.3 wt. % H2O. Analyses of the rims seem to indicate lower P and T conditions. Average values are: T=921 ºC (stdev 9ºC); P=2.7 kbar (stdev 0.4 kbar) and 5.7 wt. % H2O (0.5 stdev). 174 175 176 14308 (F12): Three hornblendes were analyzed for a total of 23 points including one transect through an amphibole grain. The PT conditions range from 985 °C and 3.2 kbar to 930 °C and 6 177 178 2.4 kbar for a water content between 5 and 7 wt. % H2O. Average values are: T=953 ºC (stdev 10ºC); P=3.1 kbar (stdev 0.3 kbar) and 6.1 wt. % H2O (0.5 stdev). 179 Small variations are observed through the grain and a slight pressure drop at the rim: 180 181 182 Fig. A4: Estimated PT conditions through an amphibole grain from samples 14308 (F12). 183 184 185 186 The average and standard deviation of all the analyzed grains point toward 949 ± 20°C, 3 ± 0.4 kbar, and 6 ± 0.5 %H2Omelt. 187 188 189 190 191 192 193 194 195 196 197 198 199 200 201 202 203 204 205 206 207 208 209 210 211 212 213 214 215 216 217 218 219 4. Plagioclase-liquid hygrometer: We used the recent calibration from Waters and Lange (2015) that is based on the crystal-liquid exchange reaction between the anorthite (CaAl2Si2O8) and albite (NaAlSi3O8) components and uses thermodynamic data. Calculatations were performed using the spreadsheet given in the data repository of “American Mineralogist”. The standard error estimate on the hygrometer model is 0.35 wt% H2O. In the case of the samples containing olivine (14285 and 1205) we bracket the minimum water content by that plagioclase crystalized shortly after olivine and therefore use a reclaculated liquid composition equals to the bulk rock composition to which we have subsatrcted the olvine composition according to their percentage. We first assume the PT conditions previously obtained for olivine core crystallisation (1176 ºC for 14285 and 1144 ºC for 1205, both at 8 kbar). Then for olivine rim crystallisation at (1065 ºC for 14285 and 1081 ºC for 1205, both at 5 kbar). For the sample 14282 from F4, that lacks olivine, we used the PT conditions from the two-pyroxene theremo-barometer (989 ºC and 4.1 kbar). In the case of hornblende-bearing lavas (F5, F6, F7, F11, and F12), we assume that plagioclase phenocrysts crystallised first and hence are in equilibrium with a liquid having the bulk rock composition. We used here the average PT conditions obtained previously using the amphibole thermo-barometer. Note that the obtained water content represents therefore a minimum value. Also, note that the changes in pressure affect the water content by less than the errors associated with the method. 14285 (F1): Four core plagioclase crystals were analyzed (An73), and results indicate water contents ranging between 1.9 +/- 0.08 wt. % H2O at 1176 ºC and 8 kbar and 3.5 +/- 0.08 wt. % H2O at 1065 ºC and 5 kbar. 1205 (F4b): Five plagioclase cores were analysed (An71) and results indicate water contents between 1.9 +/- 0.02 wt. % H2O at 1135 ºC and 8 kbar and 2.6 +/- 0.02 wt. % H2O at 1081 ºC and 5 kbar. 14282 (F4): 7 220 221 222 223 One plagioclase phenocryst and 6 microlites were analysed (An60), and results indicate water contents of 3.6 +/- 0.07 wt. % H2O, at 989 ºC and 4.1 kbar. 224 225 Six plagioclase cores were analyzed (An64) and results indicate water contents of 5.1 +/-0.03 wt. % H2O at 946ºC and 3.1 kbar. 226 14298 (F6): 227 228 Four plagioclase cores were analyzed (An63) and results indicate water contents 4.7 +/-0.1 wt. % H2O at 972ºC and 3.2 kbar. 229 14309 (F7): 230 231 Three plagioclase cores were analyzed (An74) and results indicate water contents 4.45 +/-0.08 wt. % H2O at 967ºC and 3.2 kbar. 232 1210 (F11): 233 234 Six plagioclase cores were analyzed (An70) and results indicate water contents 5.5 +/-0.07 wt. % H2O at 922ºC and 2.7 kbar. 235 14308 (F12): 236 237 Three plagioclase cores were analyzed (An64) and results indicate water contents 4.8 +/-0.04 wt. % H2O at 953ºC and 3.1 kbar. 14268 (F5): 238 239 8 240 241 242 243 References: Baker RB, Eggler DH (1987) Compositions of anhydrous and hydrous melts coexisting with plagioclase, augite, and olivine or low-Ca pyroxene from 1 atm to 8 kbar: Application to the Aleutian volcanic center of Atka. 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