“…In this paper the effects of fo2 and melt H20 content on <1 <1 <1 <1 <1 <1 <1 <1 <1 <1 <1 <1 <1 <1 <1 <1 <1 <1 +1 <1 <1 <1 <1 <1 <1 -1 <1 <1 <1 +1 -1 <1 <1 <1 -1 <1 <1 <1 <1 <1 <1 <1 <1 <1 <1 <1 <1 <1 <1 <1 <1 <1 <1 <1 <1 <1 <1 3.96 + 1 g1(75), pl(16), opx(6), mt(3), ame 0.21 < 1 g1(66), p1(24), opx(7), mt(3), ame 0.63 < 1 gl(60), pl(30), opx(7), mt(3), ame 0.12 < 1 g1(95), pl(1), mt(4), ame 2.75 < 1 g1(63), p1(29), opx(6), mt(2), ame 0.15 < 1 g1(62), p1(28), opx(7), mt(3), ame 1.03 < 1 g1(59), pl(31), opx(5), cpx(3), mt(2), ame 0.57 < 1 all20 calculated from H20 in glass using the model of Burnham [1979] (see also text); log fo2 calculated from experimental fH2 (see text) and calculated fH20 (obtained from aH20); ANNO = log fo2 -log fo2 of the NNO buffer calculated at P and T [Chou, 1987] (Table 2), infrared spectroscopy could not be used as a routine method for H20 analysis. The glass H20 contents were thus measured using the "by-difference" method [Devine et al, 1995]. The difference from 100% of electron microprobe analyses (after correction of the alkalies) was calibrated against the dissolved glass H20 content by using the three hydrous glasses described above as standards, analyzed together with the experimental glasses during each microprobe session.…”