The gravitationally powered dynamo

Summary. The energetics of the gravitationally powered dynamo have been studied with the aid of a compressible-earth model which allows for the growth of the solid inner core. The basic premise of this study is that as the Earth gradually cooled over geological time the solid inner core continually accreted dense material which crystallized from an outer core composed of a molten binary alloy. This process requires a continual rearrangement of matter which generates the fluid motions needed to sustain the dynamo. These motions maintain the outer core in a well-mixed state, in apparent contradiction to Higgins & Kennedy’s hypothesis that the outer core is stably stratified. The vigour of these motions is dependent primarily upon the composition of the solid inner core, but is surprisingly independent of the density of the light constituent in the core. If the solid core is composed entirely of heavy metal, then as much as 3.7 x 1OI2 W may be transferred from the core to the mantle as a result of cooling and gravitational settling. This is roughly equal to estimates of the amount of heat conducted down the adiabat in the core, but it is argued that there is no direct relation between the amount of heat conducted down the adiabat and the amount transferred to the mantle if the convection is driven non-thermally. The gravitational energy released per unit mass of the solid inner core is remarkably constant and may be as much as 2 x 106J/kg, roughly five times the value of the latent heat of iron. These values are reduced if the solid inner core contains some light constituents. It was found that the efficiency of the gravitationally powered dynamo may exceed 50 per cent, a much higher figure than is possible for either the thermally or precessionally driven dynamo. Also, the amount of gravitational energy available to drive the dynamo in the future is many times that expended so far. The size of the magnetic field sustained by gravitational settling was related to the density jump at the inner-outer core boundary and the field strength was estimated to lie between 390 and 685 G, strongly suggesting that the dynamo is of the nearly-axisymmetric type developed by Braginsky.

[1]  A. E. Ringwood,et al.  Composition of the core and implications for origin of the earth. , 1977 .

[2]  D. Gubbins Energetics of the Earth's core. , 1977 .

[3]  F. Busse Generation of planetary magnetism by convection , 1976 .

[4]  R. Brett The current status of speculations on the composition of the core of the Earth , 1976 .

[5]  D. Loper Torque balance and energy budget for the precessionally driven dynamo , 1975 .

[6]  P. Roberts,et al.  A three-dimensional kinematic dynamo , 1975, Proceedings of the Royal Society of London. A. Mathematical and Physical Sciences.

[7]  T. Usselman,et al.  Experimental approach to the state of the core; Part II, Composition and thermal regime , 1975 .

[8]  J. A. Jacobs,et al.  The Earth's Core , 1975 .

[9]  T. Jordan,et al.  Earth structure from free oscillations and travel times: Geophys , 1974 .

[10]  M. Frazer Temperature Gradients and the Convective Velocity in the Earth's Core , 1973 .

[11]  R. Stewart Composition and temperature of the outer core , 1973 .

[12]  J. Verhoogen Thermal regime of the Earth's core , 1973 .

[13]  E. V. Artyushkov Density differentiation of the Earth's matter and processes at the core‐mantle interface , 1972 .

[14]  A. Cook Review Lecture: The dynamical properties and internal structures of the Earth, the Moon and the planets , 1972, Proceedings of the Royal Society of London. A. Mathematical and Physical Sciences.

[15]  V. Murthy,et al.  The early chemical history of the earth: Some critical elemental fractionations , 1971 .

[16]  G. Kennedy,et al.  The adiabatic gradient and the melting point gradient in the core of the Earth , 1971 .

[17]  B. Bolt,et al.  Upper Bound to the Density Jump at the Boundary of the Earth's Inner Core , 1970, Nature.

[18]  R. Haddon,et al.  An Earth model incorporating free earth oscillation data , 1969 .

[19]  W. Malkus,et al.  Precession of the Earth as the Cause of Geomagnetism , 1968, Science.

[20]  W. Malkus,et al.  Precessional torques as the cause of geomagnetism , 1963 .

[21]  S. P. Marsh,et al.  Equation of State for Nineteen Metallic Elements from Shock‐Wave Measurements to Two Megabars , 1960 .

[22]  P. Roberts,et al.  On the motion of an iron-alloy core containing a slurry: I. general theory , 1977 .

[23]  F. D. Stacey,et al.  Core Convection as a Power Source for the Geomagnetic Dynamo-A Thermodynamic Argument , 1974 .

[24]  Frank D. Stacey,et al.  Physical properties of the Earth's core , 1972 .

[25]  E. V. Artyushkov Density differentiation on the core-mantle interface and gravity convection , 1970 .

[26]  S. I. Braginskii KINEMATIC MODELS OF THE EARTH'S HYDROMAGNETIC DYNAMO , 1964 .

[27]  M. Hansen,et al.  Constitution of Binary Alloys , 1958 .

[28]  Edward Crisp Bullard,et al.  Homogeneous dynamos and terrestrial magnetism , 1954, Philosophical Transactions of the Royal Society of London. Series A, Mathematical and Physical Sciences.

[29]  J. Verhoogen Heat Balance of the Earth's Core , 1937 .