Jökull


Jökull - 01.01.2019, Page 97

Jökull - 01.01.2019, Page 97
Nikkola et al. 0 20 40 60 80 100 0 20 40 60 80 100 0 50 100 150 80 81 82 83 84 85 86 0 50 100 150 0 20 40 60 80 100 0 20 40 60 80 100 80 81 82 83 84 85 86 80 81 82 83 84 85 86 80 81 82 83 84 85 86 80 81 82 83 84 85 86 80 81 82 83 84 85 86 Ol81_1 t = 22.3 days Fo-core = 82.9 Ol82_1 t = 9.2 days Fo-core = 82.45 Ol45_1 t = 36.7 days Fo-core = 80.8 Ol76_1 t = 17.9 days Fo-core = 84.4 Ol83_2 t = 33.4 days Fo-core = 81.65 Ol89_1 t = 23.1 days Fo-core = 82.9 Ol91_1 t = 10.3 days Fo-core = 84.0 Fo Fo Fo Fo Fo Fo Distance ( m)μ Distance ( m)μ Distance ( m)μ Distance ( m)μ Distance ( m)μ Distance ( m)μ Distance ( m)μ a b c d f g 80 81 82 83 84 85 86 Fo 0 20 40 60 80 100 e ’mixing plateau’ ’core plateau’ Figure 6. a-g)Fe-Mg zonation in the seven complex reverse zoned olivine macrocrysts used for dif- fusion modelling. The blue dots show the measured forsterite (Fo) content near the olivine rims, the orange stippled line is the assumed initial olivine compo- sition, and the orange curve is the calculated end result of dif- fusive re-equilibration after time (t). – a-g) Fe-Mg-beltun í sjö ólivíndílum með flókna öfuga beltun og notaðir voru við líkan- reikninga efnasveimis. Bláu punktarnir sýna mælt forsterít- gildi (Fo) nærri rimum ólivíns. Gula brotalínan á hverri mynd er áætluð samsetning ólivíns í upp- hafi líkanreiknings og heila gula línan er reiknuð samsetning af völdum efnasveimis eftir tíma t. Kahl et al., 2015); however, the timescales are sen- sitive to the selected model temperature. Consider- ing the primitive nature of the Brattaskjól ankaramite, we surmise that 1170◦C is fair, although conservative (potentially low) estimate of the diffusion T (see Fig- ure 5). We prefer a lower model temperature to avoid underestimating the diffusion time scales, because, ir- respective of the model conditions, the resulting diffu- sion timescales are the maximum time scales of sub- surface storage and ascent (after magmatic recharge) as the crystals are hosted by a lava flow. Lava flow fields insulate themselves effectively (e.g., Hon et al., 1994; Self et al., 1998; Harris and Rowland, 2009) and hence lava-hosted olivine crystals may remain at high but gradually decreasing temperature for weeks to months after eruption. We cannot separate diffu- sion in a lava flow/lava lake and diffusion occurring at depth during subsurface ascent; this is the caveat of working with crystalline lava samples instead of tephra. 96 JÖKULL No. 69, 2019
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