A星や白矮星における磁場の化石の起源
Jonathan Braithwaite1, Hendrik C Spruit
1Max-Planck-Institute for Astrophysics, Postfach 1317, 85741 Garching, Germany.
Nature
|October 16, 2004
まとめ
Ap星,磁気白矮星,マグネタールの強い恒星磁場は,化石の磁場である可能性が高い. 数値シミュレーションは,これらの安定したフィールドが不安定な初期状態から進化し,それらの説明を統一することを示しています.
科学分野:
- 天文学と天体物理学について
- 星の磁気は,星の磁気である
- 計算物理学の物理
背景:
- いくつかのメインシーケンスの星 (Ap星) は,強い,静的な,大規模な二極磁場を示します.
- 2つの仮説が存在する:化石フィールド (形成の残骸) またはダイナモプロセス.
- ダイナモ仮説は,力場強度と回転相関の欠如を説明するために苦労します.
研究 の 目的:
- 恒星の磁場の安定性と進化を調査する.
- 化石フィールドが,観測された恒星の磁場特性を説明できるかどうかを判断する.
- 異なる種類の恒星における恒星磁気に関する統一的な説明を提供するため.
主な方法:
- 磁場進化の数値シミュレーション.
- 任意の初期フィールドから安定した磁気構成の発展をモデリングする.
- シミュレーション結果をAp星,磁性白矮星,磁星に関する観測データと比較する.
主要な成果:
- シミュレーションにより,不安定な初期フィールドから,安定した磁場構成が発達することが示されています.
- シミュレートされた安定フィールドは,観測された恒星の磁場の性質と一致します.
- この発見は,これらの恒星のダイナモ生成に対する化石フィールド理論を支持する.
結論:
- 化石フィールドは,Ap星,磁性白矮星,磁星で観測される強力な磁場に対する実行可能で統一的な説明である.
- 安定した磁気構成は,進化の過程から自然に生じる可能性があります.
- この研究は,恒星の磁力の起源に関する長年の疑問を解決します.
さらに関連する動画
05:17Enhancement of the Initial Growth Rate of Agricultural Plants by Using Static Magnetic Fields
Published on: July 8, 2016
13.5K
11:04Geomagnetic Field Gmf and Plant Evolution: Investigating the Effects of Gmf Reversal on Arabidopsis thaliana Development and Gene Expression
Published on: November 30, 2015
13.7K
関連する概念動画
Magnetic Fields
6.6K
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...
6.6K
Magnetic Field Lines
4.8K
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:
4.8K
Magnetic Field due to Moving Charges
10.7K
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...
10.7K
Atomic Nuclei: Nuclear Magnetic Moment
2.4K
All atomic nuclei are positively charged. When they have a nonzero spin, they behave like rotating charges. As a consequence of their charge and spin, these nuclei generate a magnetic field (B). This, in turn, gives rise to a magnetic moment (μ), which is randomly oriented in the absence of an external magnetic field. When an external magnetic field (B0) is applied, the magnetic moment vectors can align with the field or against it in 2 + 1 orientations. A hydrogen nucleus, which is just a...
2.4K
Energy In A Magnetic Field
2.4K
If a magnetic field is sustained, there must be a current in a closed circuit or loop, implying some energy has been spent in creating the field. If this energy is not dissipated via the circuit's resistance, it is stored in the field.
Take an ideal inductor with zero resistance. Although it's practically impossible, assume that the coil's resistance is so small that it is practically negligible. The loss of the field's energy to dissipate thermal energy (or heat) is thus...
Take an ideal inductor with zero resistance. Although it's practically impossible, assume that the coil's resistance is so small that it is practically negligible. The loss of the field's energy to dissipate thermal energy (or heat) is thus...
2.4K
Magnetic Field Due To A Thin Straight Wire
5.6K
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.
5.6K
