Partitioning experiments between a basaltic melt from Mt. Etna and a low-density hydrous fluid or vapor containing H(2)O or H(2)O-CO(2) were performed at 1200-1260 degrees C, at pressures between 1 and 200 MPa, either near the nickel-nickel oxide (NNO) buffer or at two log units above it (NNO + 2), and with different chloride concentrations. Most of the experiments were done at chloride-brine-undersaturated conditions, although at the highest Cl concentrations explored brine saturation might have been reached. The average partition coefficients (D(Cl)(fluid/melt)) over the range of Cl concentrations were derived on a weight basis by plotting the calculated concentrations of Cl in the fluid phase versus the measured ones in the melt. For H(2)O-Cl experiments in which the Cl concentration in the melt was <= 0.4 wt.%, a negative dependence between D(Cl)(f/m) and pressure is observed. D(Cl)(fluid/melt) in H(2)O + Cl-bearing experiments ranges between 11-14 at 1 and 25 MPa to 6 at 200 MPa at NNO: and between 4 at 50 MPa and 13 at 100 MPa at Delta NNO >= 2. Addition of CO(2) at NNO yields lower partition coefficients than in CO(2)-free conditions over the pressure range investigated. The negative pressure dependence observed for H(2)O-Cl experiments disappears when CO(2) is present in the system. Overall, once CO(2) is introduced in the system, Cl fugacity in the silicate melt tends to increase, thus resulting in a decrease of D(Cl)(f/m). Application to Mt. Etna shows that the composition of the volcanic plume in terms of Cl records very shallow pressures of magma equilibration with its exsolved fluid.
Chlorine partitioning between a basaltic melt and H2O-CO2 fluids at Mount Etna.
Ottolini L
2009
Abstract
Partitioning experiments between a basaltic melt from Mt. Etna and a low-density hydrous fluid or vapor containing H(2)O or H(2)O-CO(2) were performed at 1200-1260 degrees C, at pressures between 1 and 200 MPa, either near the nickel-nickel oxide (NNO) buffer or at two log units above it (NNO + 2), and with different chloride concentrations. Most of the experiments were done at chloride-brine-undersaturated conditions, although at the highest Cl concentrations explored brine saturation might have been reached. The average partition coefficients (D(Cl)(fluid/melt)) over the range of Cl concentrations were derived on a weight basis by plotting the calculated concentrations of Cl in the fluid phase versus the measured ones in the melt. For H(2)O-Cl experiments in which the Cl concentration in the melt was <= 0.4 wt.%, a negative dependence between D(Cl)(f/m) and pressure is observed. D(Cl)(fluid/melt) in H(2)O + Cl-bearing experiments ranges between 11-14 at 1 and 25 MPa to 6 at 200 MPa at NNO: and between 4 at 50 MPa and 13 at 100 MPa at Delta NNO >= 2. Addition of CO(2) at NNO yields lower partition coefficients than in CO(2)-free conditions over the pressure range investigated. The negative pressure dependence observed for H(2)O-Cl experiments disappears when CO(2) is present in the system. Overall, once CO(2) is introduced in the system, Cl fugacity in the silicate melt tends to increase, thus resulting in a decrease of D(Cl)(f/m). Application to Mt. Etna shows that the composition of the volcanic plume in terms of Cl records very shallow pressures of magma equilibration with its exsolved fluid.I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.