若い中間質量星の非常に規則的な高周波パルスモード
Timothy R Bedding1,2, Simon J Murphy3,4, Daniel R Hey3,4
1Sydney Institute for Astronomy (SIfA), School of Physics, University of Sydney, Camperdown, New South Wales, Australia. tim.bedding@sydney.edu.au.
Nature
|May 15, 2020
まとめ
アステロシズモロジーは,新たに発見された定期的な高周波パルスシーケンスのおかげで,δ スクティの星におけるパルスモードを特定することができます. この画期的な発見は 中間質量星の内部構造を理解するのに役立ちます
科学分野:
- 天文学と天体物理学
- 恒星物理学
- アステロ地震学
背景:
- アステロシズモロジーは,恒星の内部構造を研究するために,恒星のパルス周波数を用いる.
- 以前の研究では 赤い巨星や白矮星のような様々な星の 脈動モードを成功裏に特定しました
- δ スクティ星は,中等質量パルス星のグループで,体系的なモード識別に抵抗した複雑なパルススペクトルを持っています.
研究 の 目的:
- 質量の中間のメインシーケンス星 (δ スクティ星) の決定的なモード識別を可能にします.
- ランダムな刺激と急速な回転によって引き起こされるパルスモードを特定する課題を克服する.
主な方法:
- 高周波パルスモードの検出 メインシーケンス60の中間質量星.
- 脈動スペクトルの分析により,非常に規則的なシーケンスが特定される.
- 宇宙運動と脈動モデリングを用いて,若い恒星連合の恒星メンバーの確認.
主要な成果:
- 60 δ スクティ星の高周波パルスモードの 驚くほど規則的なシーケンスの発見
- 恒星の決定的なモードの識別が成功しました
- 既知の若い星団のメンバーとしていくつかの星を識別する.
結論:
- この研究は δ スクティの星におけるモード識別のための新しい方法を確立している.
- この発見は 中間の質量の恒星の内部構造について 重要な洞察を与えてくれます
- この結果は,アステロシズモロジーを星動力学と人口研究と結びつけています.
関連する概念動画
Frequency of Spring-Mass System
7.1K
One interesting characteristic of the simple harmonic motion (SHM) of an object attached to a spring is that the angular frequency, and the period and frequency of the motion, depend only on the mass and the force constant of the spring, and not on other factors such as the amplitude of the motion or initial conditions. We can use the equations of motion and Newton's second law to find the angular frequency, frequency, and period.
Consider a block on a spring on a frictionless surface. There...
Consider a block on a spring on a frictionless surface. There...
7.1K
Forced Oscillations
7.5K
When an oscillator is forced with a periodic driving force, the motion may seem chaotic. The motions of such oscillators are known as transients. After the transients die out, the oscillator reaches a steady state, where the motion is periodic, and the displacement is determined.
7.5K
Pulse rhythm
1.2K
Pulse rhythm refers to the pattern of pulsations within specific intervals, offering valuable insights into the regularity or irregularity of the heart's beats as observed through the pattern of pulsation within specific intervals. A regular pulse exhibits a consistent heart rate with uniform waveforms and pulsation force, variations of which can be classified as normal, weak, or bounding.
Conversely, an irregular pulse pattern is termed dysrhythmia, stemming from disruptions in cardiac...
Conversely, an irregular pulse pattern is termed dysrhythmia, stemming from disruptions in cardiac...
1.2K
Modes of Standing Waves - I
3.8K
A close look at earthquakes provides evidence for the conditions appropriate for resonance, standing waves, and constructive and destructive interference. A building may vibrate for several seconds with a driving frequency matching the building's natural frequency of vibration; this produces a resonance that results in one building collapsing while the neighboring buildings do not. Often, buildings of a certain height are devastated, while other taller buildings remain intact. This...
3.8K
Atomic Nuclei: Larmor Precession Frequency
2.5K
The earth's gravitational field produces a 'twisting force' perpendicular to the angular momentum of a spinning mass (such as a spinning top) that causes the mass to 'wobble' around the gravitational field axis in a phenomenon called precession. Similarly, the magnetic moment (μ) of a spinning nucleus precesses due to an external magnetic field directed along the z-axis. The precession of the magnetic moment vector about the magnetic field is called Larmor precession,...
2.5K
Modes of Standing Waves: II
1.5K
The starting point for expressing the modes of standing waves is understanding the boundary conditions that the waves must follow. The boundary conditions are derived from the physical understanding of how the standing waves are sustained, that is, how the vibrating particles of the medium behave at the boundaries imposed on them.
For a tube open at one end and closed at the other filled with air, the modes are such that there is always an antinode at the open end and a node at the closed end....
For a tube open at one end and closed at the other filled with air, the modes are such that there is always an antinode at the open end and a node at the closed end....
1.5K


