近くにある木星の磁気尾部で局所的な再接続が確認されました
1C. T. Russell and M. G. Kivelson, Institute of Geophysics and Planetary Physics, and Department of Earth and Space Sciences, University of California, Los Angeles, CA 90095-1567, USA. K. K. Khurana and D. E. Huddleston, Institute of Geo.
まとめ
木星の磁気尾の局所的な磁場は,エピソード的な再接続を示唆し,プラズマの脱出を可能にします. ガリレオ宇宙船からのこれらの発見は,木星の磁気圏に強い垂直フィールドのポケットを明らかにしています.
科学分野:
- 惑星科学 惑星科学
- 宇宙物理学 宇宙物理学
- マグネトヒドロダイナミクス
背景:
- 木星は強力な磁気圏を持ち,磁気尾を含んでいる.
- プラズマは磁気圏内,特にイオの軌道付近から発生します.
- 磁気再接続は,惑星磁気尾のプラズマ脱出のための重要なプロセスです.
研究 の 目的:
- 木星の磁気尾の構造を調査する.
- 木星の磁気圏からプラズマが脱出するメカニズムを特定する.
- ガリレオ宇宙船によって観測された局所的な磁場異常を分析する.
主な方法:
- ガリレオ宇宙船によるインシトゥ測定.
- 木星の磁気尾の磁場データを分析した.
- 磁場構成要素の空間マッピング.
主要な成果:
- 強い北向きと南向きの磁場成分を持つ局部化された領域を観測した.
- これらの領域は,真夜中後の夜明け前のセクターで,木星の半径50を超えて発見されました.
- 観測された垂直磁場は,時には周囲の磁気尾や磁気ディスクの磁場よりも強いものであった.
結論:
- 局所的な磁場ポケットは,エピソード的な再接続イベントの結果である可能性があります.
- これらの出来事は,おそらく木星の磁気尾の近くのパッチを伴う.
- エピソード的再接続は,プラズマの脱出を磁気尾から容易にします.
関連する概念動画
Magnetism
Magnets are commonly found in everyday objects, such as toys, hangers, elevators, doorbells, and computer devices. Experimentation on these magnets shows that all magnets have two poles: one is labeled north (N) and the other south (S). Magnetic poles repel if they are alike and attract if unlike. Moreover, both poles of a magnet attract unmagnetized pieces of iron.
An individual magnetic pole cannot be isolated. No matter how small, every piece of a magnet contains a north pole and a south...
An individual magnetic pole cannot be isolated. No matter how small, every piece of a magnet contains a north pole and a south...
Magnetic Field Lines
The representation of magnetic fields by magnetic field lines is very useful in visualizing the strength and direction of the magnetic field. Each of the magnetic field lines forms a closed loop. The field lines emerge from the north pole (N), loop around to the south pole (S), and continue through the bar magnet back to the north pole.
Magnetic field lines follow several hard-and-fast rules:
Magnetic field lines follow several hard-and-fast rules:
Magnetic Field Of A Current Loop
Consider a circular loop with a radius a, that carries a current I. The magnetic field due to the current at an arbitrary point P along the axis of the loop can be calculated using the Biot-Savart law.
Magnetic Field due to Moving Charges
A stationary charge creates and interacts with the electric field, while a moving charge creates a magnetic field.
Consider a point charge moving with a constant velocity. Like the electric field, the magnetic field at any point is directly proportional to the magnitude of the charge and inversely proportional to the square of the distance between the source point and the field point. However, unlike the electric field, the magnetic field is always perpendicular to the plane containing the line...
Consider a point charge moving with a constant velocity. Like the electric field, the magnetic field at any point is directly proportional to the magnitude of the charge and inversely proportional to the square of the distance between the source point and the field point. However, unlike the electric field, the magnetic field is always perpendicular to the plane containing the line...
Magnetic Flux
The magnetic flux measures the number of magnetic field lines passing through a given surface area. The SI unit for magnetic flux is the weber (Wb). Magnetic flux is a scalar quantity. It depends on three factors: the strength of the magnetic field B, the area through which the field lines pass, and the relative orientation of the field with the surface area.
Suppose a surface is divided into elements of area dA. For each element, the component of the magnetic field that is normal to the...
Suppose a surface is divided into elements of area dA. For each element, the component of the magnetic field that is normal to the...
Magnetostatic Boundary Conditions
An electric field suffers a discontinuity at a surface charge. Similarly, a magnetic field is discontinuous at a surface current. The perpendicular component of a magnetic field is continuous across the interface of two magnetic mediums. In contrast, its parallel component, perpendicular to the current, is discontinuous by the amount equal to the product of the vacuum permeability and the surface current. Like the scalar potential in electrostatics, the vector potential is also continuous...


