関連する実験動画
Updated: Jul 11, 2026

11:47
A 100 KW Class Applied-field Magnetoplasmadynamic Thruster
Published on: December 22, 2018
まとめ
パイオニア10号のデータによると,木星の磁場は地球の磁場と対極にあり,外側の磁気圏では著しく偏移し,伸びている. これらの発見は,木星の磁気圏を形作る複雑なプラズマ相互作用を強調しています.
科学分野:
- 惑星科学 惑星科学
- マグネトヒドロダイナミクス
- 宇宙物理学 宇宙物理学
背景:
- 木星には強力な磁場があり,太陽風とダイナミックに相互作用しています.
- 惑星の磁気圏を理解することは,宇宙探査と天体生物学にとって極めて重要です.
- 以前の観測は,木星の周りの複雑な磁場構造を暗示していた.
研究 の 目的:
- 磁気二極 Moment と木星の磁場の向きを特徴づけるために.
- 木星の磁気圏の構造と行動,太陽風との相互作用を調査する.
- 木星の磁気圏に影響を与えるプラズマ効果を特定するために.
主な方法:
- パイオニア10号のベクトルヘリウム磁気計のデータを活用した.
- 磁場測定を分析し,二極パラメータと空間的変動を決定しました.
- 磁気圏の磁場構成と,太陽風との相互作用をモデル化した.
主要な成果:
- 木星の磁気二極は,地球の磁気二極と比べて逆転しており,モメントは4.0ガウスR ((J) ((3) で,傾きは15度.
- 二極は北に0.1R(J) と北緯170度に向かって0.2R(J) の偏移がある.
- 外部磁気圏の赤道に平行するフィールドラインの激しい伸びが観察され,プラズマの影響が顕著であることを示しています.
結論:
- 木星の磁気圏は,内部プラズマダイナミクスによって引き起こされる複雑なフィールド構成を示しています.
- 外側の磁気圏は,熱圧,遠心力,微分回転の証拠を示しています.
- 木星の磁気圏は,薄い外界と分離した弓の衝撃があり,地球のそれと似ています.
関連する概念動画
Magnetic Field of a Solenoid
A solenoid is a conducting wire coated with an insulating material, wound tightly in the form of a helical coil. The magnetic field due to a solenoid is the vector sum of the magnetic fields due to its individual turns. Therefore, for an ideal solenoid, the magnetic field within the solenoid is directly proportional to the number of turns per unit length and the current. Conversely, the magnetic field outside the solenoid is zero.
Consider a solenoid with 100 turns wrapped around a cylinder of...
Consider a solenoid with 100 turns wrapped around a cylinder of...
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 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 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 A Thin Straight Wire
Consider an infinitely long straight wire carrying a current I. The magnetic field at point P at a distance a from the origin can be calculated using the Biot-Savart law.
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...

