Abstract Viscosity of silicate melts governs magma transport and influences mantle dynamics, yet effects of pressure and water on melt viscosity remain poorly understood. Here, we report in situ falling‐sphere viscosity measurements on diopside (Di) melts with 0–3 wt.% H 2 O along the liquidus up to 7 GPa and 2103 K using synchrotron X‐ray radiography. By incorporating our hydrous melt data into a previously validated model for the dry system, the effects of pressure, temperature, and H 2 O contents on Di melt viscosity can be satisfactorily captured by the function: where T* is the homologous temperature, x H2O is the molar % H 2 O, η 0 = 8.90 (1.50) × 10 −8 Pa s, b 0 = 3.02 (0.10), and H* ( P ) = 15.72 (0.03)−0.35 (0.01)· P + 1.07 (0.07) × 10 −2 · P 2 −1.19 (0.14) × 10 −4 P 3 , ×10 −3 GPa −1 . Adding 3 wt.% H 2 O systematically reduces viscosity by ∼0.7 log units. For both dry and hydrous melts, viscosity along the liquidus decreases monotonically with increasing pressure, suggesting that moderate hydration may not significantly alter the compressional behavior of Di melts. Combining the Di viscosity model with models for feldspar and olivine, we simulated the viscosity of analog basaltic magmas under mantle conditions. Increasing H 2 O content from 0 to 3wt.% raises mobility of basaltic magma increases by >1 order of magnitude. In hot plume settings, the mobility further increases by a factor of 30 relative to typical ambient mantle. Assuming a simple percolation model, the increased mobility corresponds to faster melt ascent in mantle plumes that could, in part, explain the voluminous magmatism of large igneous provinces.
Chen et al. (Mon,) studied this question.