A deep dynamo generating Mercury’s magnetic field

Mercury has a global magnetic field of internal origin and it is thought that a dynamo operating in the fluid part of Mercury’s large iron core is the most probable cause. However, the low intensity of Mercury’s magnetic field—about 1% the strength of the Earth’s field—cannot be reconciled with an Earth-like dynamo. With the common assumption that Coriolis and Lorentz forces balance in planetary dynamos, a field thirty times stronger is expected. Here I present a numerical model of a dynamo driven by thermo-compositional convection associated with inner core solidification. The thermal gradient at the core–mantle boundary is subadiabatic, and hence the outer region of the liquid core is stably stratified with the dynamo operating only at depth, where a strong field is generated. Because of the planet’s slow rotation the resulting magnetic field is dominated by small-scale components that fluctuate rapidly with time. The dynamo field diffuses through the stable conducting region, where rapidly varying parts are strongly attenuated by the skin effect, while the slowly varying dipole and quadrupole components pass to some degree. The model explains the observed structure and strength of Mercury’s surface magnetic field and makes predictions that are testable with space missions both presently flying and planned.

[1]  Ulrich R. Christensen,et al.  Power requirement of the geodynamo from ohmic losses in numerical and laboratory dynamos , 2004, Nature.

[2]  D. Stevenson Reducing the non-axisymmetry of a planetary dynamo and an application to saturn , 1982 .

[3]  M. Matsushima,et al.  Dipolar and non‐dipolar dynamos in a thin shell geometry with implications for the magnetic field of Mercury , 2006 .

[4]  D. Stevenson Planetary magnetic fields , 2003 .

[5]  B. Buffett,et al.  The strength and efficiency of thermal and compositional convection in the geodynamo , 1995 .

[6]  N. Ness,et al.  Mercury's magnetic field , 1976, Nature.

[7]  U. Christensen,et al.  Dipole moment scaling for convection-driven planetary dynamos , 2005 .

[8]  David E. Smith,et al.  A procedure for determining the nature of Mercury's core , 2002 .

[9]  Jonathan M. Aurnou,et al.  A numerical study of dynamo action as a function of spherical shell geometry , 2005 .

[10]  J. Turner,et al.  Buoyancy Effects in Fluids , 1973 .

[11]  R. Phillips,et al.  Internal and tectonic evolution of Mercury , 2003 .

[12]  U. Christensen,et al.  Scaling properties of convection-driven dynamos in rotating spherical shells and application to planetary magnetic fields , 2006 .

[13]  M. Ross,et al.  Mercury's thermal history and the generation of its magnetic field , 1988 .

[14]  C. Jones,et al.  Influence of the Earth's inner core on geomagnetic fluctuations and reversals , 1993, Nature.

[15]  T. Hoolst,et al.  Mercury's tides and interior structure , 2003 .

[16]  Mioara Mandea,et al.  CHAOS—a model of the Earth's magnetic field derived from CHAMP, Ørsted, and SAC‐C magnetic satellite data , 2006 .

[17]  Carsten Kutzner,et al.  Simulated geomagnetic reversals and preferred virtual geomagnetic pole paths , 2004 .

[18]  M. Zuber,et al.  Thin shell dynamo models consistent with Mercury's weak observed magnetic field [rapid communication] , 2005 .

[19]  M. Zuber,et al.  Crustal remanence in an internally magnetized non-uniform shell: a possible source for Mercury’s magnetic field? , 2004 .

[20]  G. Schubert,et al.  Teleconvection: remotely driven thermal convection in rotating stratified spherical layers. , 2000, Science.

[21]  Paul H. Roberts,et al.  Equations governing convection in earth's core and the geodynamo , 1995 .