大きな衝突クレーターにおけるピークリングの形成
Joanna V Morgan1, Sean P S Gulick2, Timothy Bralower3
1Department of Earth Science and Engineering, Imperial College London, SW7 2AZ, UK. j.morgan@imperial.ac.uk.
まとめ
巨大な衝突により 惑星のピークリングが形成され 深い岩石が上昇します シクスルブピークリングは 地下岩の断層から形成され 衝撃のメカニズムと地殻の変化を明らかにしています
科学分野:
- 惑星地質学
- 衝突クレーター
- 地理学
背景:
- 大規模な衝突で 惑星の表面が再現され 地殻の物質が混ざり合います
- 衝突クレーターの中央のピークは 大きさを増してピークリングに変化します
- ピークリングの形成と起源の深さは,限られた直接サンプリングのために議論されている.
研究 の 目的:
- チクスリブ峰の形成の仕組みと起源を調査する
- 惑星の地殻の進化における 大きな衝撃の役割を理解するためです
主な方法:
- エクスペディション364の掘削で得たチクスルブピークリングの岩石サンプル分析.
- 岩石の裂け方,衝撃効果,そして石質学の調査.
- 密度や地震速度などの物理的性質の測定
主要な成果:
- チクスルブピークリングの岩は 浮き上がり 破裂し 衝撃を受けた フェルシックの地下層物質です
- これらの岩は堤防と切断地帯によって切断されています.
- ピークリングの岩は異常な低密度と地震速度を示しています.
結論:
- 大きな衝突は惑星の地殻の中で 重要な垂直物質の流れを生成します
- シクスルーブのような 衝撃過程で 地殻の多孔性が増加します
- この研究はピークリング形成のメカニズムと 惑星の地殻への影響の直接的な証拠を提供します
さらに関連する動画
09:44Laboratory Drop Towers for the Experimental Simulation of Dust-aggregate Collisions in the Early Solar System
Published on: June 5, 2014
13.5K
08:00Directed Cellular Self-Assembly to Fabricate Cell-Derived Tissue Rings for Biomechanical Analysis and Tissue Engineering
Published on: November 25, 2011
19.6K
関連する概念動画
The Contractile Ring
7.4K
Contractile rings are composed of microfilaments and are responsible for separating the daughter cells during cytokinesis. Contractile ring assembly proceeds along with other cell cycle events; however, very few mechanistic details are known about the timing and coordination of the contractile rings with the cell cycle.
A small GTPase, RhoA, controls the function and assembly of the contractile ring. RhoA belongs to the Ras superfamily of proteins. The activation of formins by RhoA promotes...
A small GTPase, RhoA, controls the function and assembly of the contractile ring. RhoA belongs to the Ras superfamily of proteins. The activation of formins by RhoA promotes...
7.4K
The Contractile Ring
2.9K
2.9K
Ionic Crystal Structures
19.7K
Ionic crystals consist of two or more different kinds of ions that usually have different sizes. The packing of these ions into a crystal structure is more complex than the packing of metal atoms that are the same size.
Most monatomic ions behave as charged spheres, and their attraction for ions of opposite charge is the same in every direction. Consequently, stable structures for ionic compounds result (1) when ions of one charge are surrounded by as many ions as possible of the opposite...
Most monatomic ions behave as charged spheres, and their attraction for ions of opposite charge is the same in every direction. Consequently, stable structures for ionic compounds result (1) when ions of one charge are surrounded by as many ions as possible of the opposite...
19.7K
Impact
558
Impact occurs when two bodies collide, leading to the application of impulsive forces between them. Analyzing impact mechanics involves considering two colliding particles moving along a line known as the line of impact, which passes through their centers and is perpendicular to the contact plane.
When particles with different initial velocities collide, they induce deformation by applying equal and opposite impulses. At the point of maximum deformation, the particles move together with...
When particles with different initial velocities collide, they induce deformation by applying equal and opposite impulses. At the point of maximum deformation, the particles move together with...
558
Olefin Metathesis Polymerization: Ring-Opening Metathesis Polymerization (ROMP)
3.3K
Ring-opening metathesis polymerization or ROMP involves strained cycloalkenes as starting materials. The mechanism of ROMP proceeds by reacting cycloalkene with Grubbs catalyst to give metallacyclobutane intermediate which undergoes a ring-opening reaction to form new carbene. The new carbene reacts with another molecule of cycloalkene. Repetition of these steps leads to the formation of an unsaturated open-chain polymer product. All these steps are reversible, however, relieving the ring...
3.3K
Deformation in a Circular Shaft
1.0K
One of the distinctive characteristics of circular shafts is their ability to maintain their cross-sectional integrity under torsion. In other words, each cross-section continues to exist as a flat, unaltered entity, simply rotating like a solid, rigid slab. To understand the distribution of shearing stress within such a shaft, consider a cylindrical section inside this circular shaft. This section has a length of L and a radius of R, with one end fixed. The radius of the cylindrical section is...
1.0K
