Replenishment rates of crustal magma and their bearing on potential sources of thermal energy

Abstract A general model of magma intrusion into the crust is developed which is based on a viscous-dissipation, forced-convection flow process driven by gravitational-buoyancy forces. Although some of the points in this general model have been studied before, it is possible with the present model to go further and calculate magma volumetric intrusion rates from fundamental properties and parameters. Equations for forced convection in a conduit with viscous dissipation are combined with results for the temperature dependence of magma viscosity. The volumetric intrusion rate is shown to be not a function of viscosity as might be expected, but rather a function primarily of the rate of change of viscosity with temperature. The model predictions for intrusion rate correlate well with field results for several sites where data exist for both intrusion or extrusion rate and for the temperature-dependent behavior of magma viscosity. The model predicts magma chamber replenishment rates equivalent to thermal energy rates on the order 10 GW (gigawatts) for a single active magma site. Assuming active magma sites on a 50-km spacing along volcanic lineaments leads to an estimate of a renewable magma intrusion rate into the crust of the western U.S. on the order of 2 TW (terawatts).

[1]  B. Marsh On the cooling of ascending andesitic magma , 1978, Philosophical Transactions of the Royal Society of London. Series A, Mathematical and Physical Sciences.

[2]  J. Nicholls,et al.  High-temperature properties of silicate liquids: applications to the equilibration and ascent of basic magma , 1977, Philosophical Transactions of the Royal Society of London. Series A, Mathematical and Physical Sciences.

[3]  D. Swanson Magma Supply Rate at Kilauea Volcano, 1952-1971 , 1972, Science.

[4]  J. Ritchey The dykes of Scotland , 1939, Transactions of the Edinburgh Geological Society.

[5]  D. L. Peck,et al.  The viscosity of basaltic magma; an analysis of field measurements in Makaopuhi lava lake, Hawaii , 1968 .

[6]  D. Dzurisin,et al.  Magma supply and storage at Kilauea volcano, Hawaii, 1956 1983 , 1984 .

[7]  H. Hardee,et al.  A new method of predicting the critical temperature of explosives for various geometries , 1972 .

[8]  H. R. Shaw Links between magma‐tectonic rate balances, plutonism, and volcanism , 1985 .

[9]  S. Solomon Mare volcanism and lunar crustal structure , 1975 .

[10]  F. Gauthier Mount Etna and the 1971 eruption - Field and laboratory studies of the rheology of Mount Etna lava , 1973, Philosophical Transactions of the Royal Society of London. Series A, Mathematical and Physical Sciences.

[11]  H. Weed,et al.  Dynamic viscosity of some silicate melts to 1688°C under atmospheric pressure , 1980 .

[12]  A. D. Young,et al.  An Introduction to Fluid Mechanics , 1968 .

[13]  H. C. Hardee,et al.  Permeable convection above magma bodies , 1982 .

[14]  H. Hardee,et al.  The extraction of heat from magmas based on heat transfer mechanisms , 1977 .

[15]  J. Crisp Rates of magma emplacement and volcanic output , 1984 .

[16]  D. Turcotte,et al.  A porous flow model for magma migration in the asthenosphere , 1978 .

[17]  H. S. Yoder,et al.  Viscosities of basalt and andesite melts at high pressures , 1976 .

[18]  H. Yoder Experimental methods for determination of transport properties of magma , 1981 .

[19]  H. Hardee,et al.  Viscous dissipation effects in magma conduits , 1977 .

[20]  S. Fedotov Mechanism of magma ascent and deep feeding channels of island arc volcanoes , 1975 .

[21]  G. Wadge,et al.  The output of the Etna volcano , 1975, Nature.

[22]  H. Hardee Incipient magma chamber formation as a result of repetitive intrusions , 1982 .

[23]  H. Hardee,et al.  PREDICTING THE CRITICAL BOUNDARY TEMPERATURE OF MULTIDIMENSIONAL EXPLOSIVES. , 1972 .

[24]  J. Pearson The Lubrication Approximation Applied to Non-Newtonian Flow Problems: A Perturbation Approach , 1967 .

[25]  I. Gruntfest,et al.  Thermal Feedback in Liquid Flow; Plane Shear at Constant Stress , 1963 .

[26]  Herbert R. Shaw,et al.  Rheology of Basalt in the Melting Range , 1969 .

[27]  Robert L. Smith Ash-flow magmatism , 1979 .

[28]  A. Acrivos,et al.  The effective thermal conductivity of sheared suspensions , 1976, Journal of Fluid Mechanics.

[29]  Lionel Wilson,et al.  Ascent and eruption of basaltic magma on the earth and moon , 1981 .

[30]  A. McBirney,et al.  Properties of some common igneous rocks and their melts at high temperatures , 1973 .

[31]  S. Fedotov Temperatures of entering magma, formation and dimensions of magma chambers of volcanoes , 1982 .

[32]  S. Uyeda,et al.  Thermal instabilities during flow of magma in volcanic conduits , 1974 .

[33]  N. L. Johnson,et al.  Temperatures Generated by the Flow of Liquids in Pipes , 1964 .

[34]  H. Schouten,et al.  A mechanism for magmatic accretion under spreading centres , 1984, Nature.

[35]  H. Schouten,et al.  The memory of the accreting plate boundary and the continuity of fracture zones , 1982 .

[36]  J. Pearson Variable-viscosity flows in channels with high heat generation , 1977, Journal of Fluid Mechanics.

[37]  H. Ockendon Channel flow with temperature-dependent viscosity and internal viscous dissipation , 1979 .

[38]  John King Vennard,et al.  Elementary Fluid Mechanics , 1940 .

[39]  Louis A. Pipes,et al.  Applied Mathematics for Engineers and Physicists , 1959 .

[40]  H. R. Shaw Obsidian‐H2O viscosities at 1000 and 2000 bars in the temperature range 700° to 900°C , 1963 .

[41]  J. Whitehead,et al.  Dynamics of laboratory diapir and plume models , 1975 .