終止ショックをヘリオシートに横切る:磁場
L F Burlaga1, N F Ness, M H Acuña
1NASA-Goddard Space Flight Center, Greenbelt, MD 20771, USA. Leonard.F.Burlaga@nasa.gov
まとめ
ヴォイジャー1号のデータは,94AUのターミネーションショックの横断を明らかにしています. 磁場強度は著しく増加し,予測から逸脱し,ヘリオシートにおけるガウス分布を示した.
科学分野:
- 宇宙物理学 宇宙物理学
- ヘリオフィジックス ヘリオフィジックス
- 惑星科学は惑星科学である.
背景:
- ヘリオスフィアは,太陽の磁場と太陽風が支配する広大な宇宙領域です.
- 終止ショックは,太陽風が急に減速する境界をマークします.
- ヴォイジャー1号のミッションは,ヘリオスフィアの外部の領域のインシット測定を行っています.
研究 の 目的:
- 磁場データを分析するために,ボイジャー1号がヘリオスフィアの終結ショックを横断した.
- ヘリオシートにおける磁場特性を特徴付けるために.
- パーカーのモデルのような理論的モデルと観測を比較する.
主な方法:
- ボーイジャー1号の搭載機器による磁場測定.
- 終結ショックにおける磁場強度の圧縮比の分析.
- ヘリオシェイダーの磁場データの統計分析,分布と方向を含む.
主要な成果:
- ヴォイジャー1号は,2004年12月16日ごろ,94AUで終結ショックを横断しました.
- 観測された磁場圧縮比は,ショック全体で3.05 ± 0.04でした.
- 平均ヘリオシート磁場強度は0.136 ± 0.035 nTで,パーカーのモデル予測の約4.2倍でした.
- ヘリオシート磁場は,一般的にパーカー螺旋に沿って太陽から遠ざかっています.
- 宇宙線の強度は,ヘリオシートにおける磁場強度の増加と相関する.
結論:
- ヘリオスフィアの終端衝撃は,惑星間磁場を著しく圧縮する.
- ヴォイジャー1号のデータは,パーカーのモデルによって予測されたより強いヘリオシート磁場を示しています.
- ヘリオシェアの磁場構造と宇宙線への影響は複雑で,さらなる研究が必要である.
関連する概念動画
Magnetic Fields
A moving charge or a current creates a magnetic field in the surrounding space, in addition to its electric field. The magnetic field exerts a force on any other moving charge or current that is present in the field. Like an electric field, the magnetic field is also a vector field. At any position, the direction of the magnetic field is defined as the direction in which the north pole of a compass needle points.
A magnetic field is defined by the force that a charged particle experiences...
A magnetic field is defined by the force that a charged particle experiences...
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 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...
Potential Due to a Magnetized Object
Magnetic dipoles in magnetic materials are aligned when placed under an external magnetic field. For paramagnets and ferromagnets, dipole alignment occurs in the direction of the magnetic field. However, the dipoles align opposite to the field in the case of diamagnets. This state of magnetic polarization due to the external field is called magnetization. Magnetization is defined as the dipole moment per unit volume. It plays a similar role to polarization in electrostatics.
The vector...
The vector...
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...


