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相关概念视频

Kepler's First Law of Planetary Motion01:10

Kepler's First Law of Planetary Motion

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In the early 17th century, German astronomer and mathematician Johannes Kepler postulated three laws for the motion of planets in the solar system. He formulated his first two laws based on the observations of his forebears, Nikolaus Copernicus and Tycho Brahe.
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Gravitation Between Spherically Symmetric Masses01:14

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The gravitational potential energy between two spherically symmetric bodies can be calculated from the masses and the distance between the bodies, assuming that the center of mass is concentrated at the respective centers of the bodies.
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Kepler's Second Law of Planetary Motion01:29

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In the early 17th century, German astronomer and mathematician Johannes Kepler postulated three laws for the motion of planets in the solar system. His first law states that all planets orbit the Sun in an elliptical orbit, with the Sun at one of the ellipse's foci. Therefore, the distance of a planet from the Sun varies throughout its revolution around the Sun.
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Kepler's Third Law of Planetary Motion01:18

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In the early 17th century, German astronomer and mathematician Johannes Kepler postulated three laws for the motion of planets in the solar system. In 1909, he formulated his first two laws based on the observations of his forebears, Nikolaus Copernicus and Tycho Brahe. However, in 1918, he published his third law of planetary motion, which gives a precise mathematical relationship between a planet's average distance from the Sun and the amount of time it takes to revolve around the Sun. It...
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Electric Field of a Charged Disk01:23

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The simplest case of a surface charge distribution is the uniformly charged disk. Calculating its electric field also helps us calculate the electric field of a large plane of charge.
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In uniform circular motion, the particle executing circular motion has a constant speed, and the circle is at a fixed radius. However, not all circular motion occurs at a constant speed. A particle can travel in a circle and speed up or slow down, showing an acceleration in the direction of motion. In that case, the motion is called non-uniform circular motion, and an additional acceleration is introduced, which is in the direction tangential to the circle. 
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Laboratory Drop Towers for the Experimental Simulation of Dust-aggregate Collisions in the Early Solar System
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一个年轻的原行星盘中的螺旋密度波

Laura M Pérez1, John M Carpenter2, Sean M Andrews3

  • 1Max-Planck-Institut für Radioastronomie, Auf dem Hügel 69, 53121 Bonn, Germany. lperez@mpifr-bonn.mpg.de.

Science (New York, N.Y.)
|October 7, 2016
PubMed
概括
此摘要是机器生成的。

天文学家使用阿塔卡马大毫米/亚毫米阵列探测到一颗年轻恒星原行星盘的中平面. 这些结构可能表明盘子中最密集区域的行星形成活动.

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科学领域:

  • 天文学
  • 天体物理学
  • 星球科学

背景情况:

  • 理论上,螺旋密度波是由于引力而形成的.
  • 之前对原行星盘中的螺旋结构的观测无法探测中间平面,其中大部分磁盘质量存在,行星形成发生.

研究的目的:

  • 在原行星盘的中平面研究螺旋密度波.
  • 确定是否可以观察到螺旋结构到达磁盘中平面.

主要方法:

  • 使用阿塔卡马大毫米/亚毫米阵列 (ALMA) 进行高分辨率观测.
  • 分析了来自年轻恒星Elias 2-27的原行星盘的毫米波辐射.

主要成果:

  • 在伊利亚斯2-27原行星盘中检测到一对相对应的螺旋臂.
  • 证实这些螺旋臂延伸到磁盘的外部区域, 并可追溯到中间平面.
  • 观察到螺旋臂内部的发射间隙,靠近中心恒星.

结论:

  • 探测到的螺旋臂可能代表密度波在磁盘中平面传播的冲击.
  • 这些发现为原行星盘的行星形成区域中发生的现象提供了观察证据.