2010
DOI: 10.1016/j.icarus.2010.01.024
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Mercury’s magnetospheric magnetic field after the first two MESSENGER flybys

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Cited by 112 publications
(138 citation statements)
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“…The recent magnetic field measurements of the NASA MErcury Surface, Space ENvironment, GEochemistry, and Ranging (MESSENGER) mission, operated around Mercury from 2008 to April 2015 (Solomon et al 2007), indicate that Mercury's magnetic dipole moment is offset northward from the planet's centre by 0.2 R M (where R M is Mercury's radius, equal to 2440 km) (Alexeev et al 2010;Anderson et al 2011a). The relative dimension of Mercury with respect to the dimension of its own magnetosphere is much larger than in the Earth's case (see also Fig.…”
Section: Space Weather At Mercurymentioning
confidence: 99%
“…The recent magnetic field measurements of the NASA MErcury Surface, Space ENvironment, GEochemistry, and Ranging (MESSENGER) mission, operated around Mercury from 2008 to April 2015 (Solomon et al 2007), indicate that Mercury's magnetic dipole moment is offset northward from the planet's centre by 0.2 R M (where R M is Mercury's radius, equal to 2440 km) (Alexeev et al 2010;Anderson et al 2011a). The relative dimension of Mercury with respect to the dimension of its own magnetosphere is much larger than in the Earth's case (see also Fig.…”
Section: Space Weather At Mercurymentioning
confidence: 99%
“…Anderson et al (2008Anderson et al ( , 2010 and Uno et al (2009) found a number of dipole representations with moments ranging from 240 to 270 nT-R m 3 and dipole tilts of 5 -12 from the rotation axis, as well as (northward) offset dipole models that fit equally well with reduced dipole moment and negligible tilt. Alexeev et al (2010) modeled the Mariner 10 and MESSENGER flybys, fitting an elaborate external field model to each, individually, concluding that Mercury's internal field is best represented by an axial dipole, with a moment of 196 nT-R m 3 , offset from the planet's center by 405 km (0.17R m )…”
Section: Modelsmentioning
confidence: 99%
“…Alexeev et al (2010) To a rough approximation, the heliopause can also be described as a paraboloid of revolution. Following Alexeev (1986) and Alexeev and Kalegaev (1995), we can consider the heliopause to be a thin dissipative boundary with R 1 ≈ 121.7 AU where the magneticfield value changes abruptly.…”
Section: Necessary Conditions For Dynamo Actionmentioning
confidence: 99%