地球の渦巻磁気層におけるイオン結合なしの電子磁気再接続
T D Phan1, J P Eastwood2, M A Shay3
1Space Sciences Laboratory, University of California, Berkeley, CA, USA. phan@ssl.berkeley.edu.
Nature
|May 11, 2018
まとめ
科学者は地球の磁気殻に 電子ジェットを観測し 新しい磁気再接続の形を明らかにしました このプロセスは,イオンカップリングなしで小規模な電流シートで渦巻のエネルギー転送を駆動します.
科学分野:
- プラズマ物理学
- 宇宙物理学
- 天体物理学
背景:
- 磁気再接続は磁気エネルギーを 粒子エネルギーに変換します これは宇宙や実験室の プラズマに不可欠です
- 標準モデルは電子スケールの拡散領域での再接続を記述し,その後にイオンジェットが続きます.
- 運動スケールでの渦巻性プラズマエネルギー分散における再接続の役割は理論化されているが,観測証拠は欠けている.
研究 の 目的:
- 磁気再接続とプラズマジェットを小規模な渦巻プラズマで調査する.
- 地球の磁殻との再接続の 観測証拠を提供するためです
- 標準的なイオン結合噴射を超えた代替再接続モデルを探求する.
主な方法:
- 地球の渦巻磁気層の電子スケールの電流シートの現地観測.
- 磁場,電場,粒子エネルギー化に関する分析
- 標準および代替再接続モデルとの観測の比較
主要な成果:
- 電子スケールの電流シートの中で 二方向の超イオンアルフェニック電子ジェットが検出されました
- 観測された平行電場と 磁気から粒子へのエネルギー変換の強化
- イオンジェットや 広範囲の電流層は 見つかりませんでした 標準モデルと矛盾しています
結論:
- この研究は,小規模な渦巻性プラズマにおける再接続プラズマジェットの最初の観測証拠を示しています.
- イオン結合のない電子ジェットによって駆動される新しい再接続形態が特定されました.
- この電子スケール再接続メカニズムは,宇宙プラズマの渦巻エネルギー転送と分散に寄与します.
さらに関連する動画
09:06Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope
Published on: March 24, 2019
6.6K
07:42Optimizing Magnetic Force Microscopy Resolution and Sensitivity to Visualize Nanoscale Magnetic Domains
Published on: July 20, 2022
2.5K
関連する概念動画
Magnetic Fields
6.0K
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...
6.0K
Magnetic Field Lines
5.5K
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:
5.5K
Magnetic Field due to Moving Charges
11.3K
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...
11.3K
Ferromagnetism
2.8K
Materials like iron, nickel, and cobalt consist of magnetic domains, within which the magnetic dipoles are arranged parallel to each other. The magnetic dipoles are rigidly aligned in the same direction within a domain by quantum mechanical coupling among the atoms. This coupling is so strong that even thermal agitation at room temperature cannot break it. The result is that each domain has a net dipole moment. However, some materials have weaker coupling, and are ferromagnetic at lower...
2.8K
Magnetostatic Boundary Conditions
1.9K
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...
1.9K
Magnetic Susceptibility and Permeability
2.9K
In linear magnetic materials, like paramagnets and diamagnets, magnetization is proportional to the magnetic field intensity. The constant of proportionality, a dimensionless number, is called magnetic susceptibility. The value of the susceptibility depends on the type of material.
When diamagnetic materials are placed under an external magnetic field, the moments opposite to the field are induced. Hence, the susceptibility for diamagnets has a minimal negative value of 10-5–10-6. Since...
When diamagnetic materials are placed under an external magnetic field, the moments opposite to the field are induced. Hence, the susceptibility for diamagnets has a minimal negative value of 10-5–10-6. Since...
2.9K
