ランニングカメの筋肉力:労働を最小限に抑える経済性
T J Roberts1, R L Marsh, P G Weyand
1Harvard University, Museum of Comparative Zoology, Concord Field Station, Bedford, MA 01730, USA.
まとめ
走る動物の筋肉とはエネルギーを吸収して放出します. 筋肉は,活発な支柱として機能し,広範な作業を行うのではなく,経済的に力を提供することにより,走行経済性を改善します.
科学分野:
- バイオメカニクス バイオメカニクス
- 動物の移動 動物の移動
- 筋肉の生理学について
背景:
- 筋肉とは,運動に不可欠であり,機械的な作業を吸収して放出します.
- 彼らの役割を理解することは,走行メカニズムと経済を理解する鍵です.
研究 の 目的:
- 走行中に筋肉とによって行われる機械的作業を調査する.
- 筋肉機能が走行経済にどのように影響するかを判断する.
主な方法:
- 走るカメの脇腹腹筋筋における力と繊維の長さの直接測定.
- 走行サイクル中の機械作業の吸収と放出の分析.
主要な成果:
- と筋肉のスプリングは,伸縮と後退を通じて重要な機械的作業を提供します.
- 主に活発な筋肉繊維は,体重を支えるために高い力を生み出します.
- レベルランニングでは,活発な筋肉は最小限に短縮され,ほとんど作業をしない.
結論:
- 筋肉は走行中にアクティブなストラットとして機能し,体重のサポートのために力の生産を最適化します.
- この"ストラット"メカニズムは,活発な筋肉の働きを最小限に抑えることで,走行経済性を高めます.
関連する概念動画
Work-energy Theorem
According to Newton’s second law of motion, the sum of all the forces acting on a particle (net force) determines the rate of change in the momentum of the particle (motion). Therefore, we should consider the work done by all forces acting on a particle, or the net work, to see its effect on the particle’s motion.
The work-energy theorem equates work done by all the forces on an object to the change in its kinetic energy. The theorem can be used to calculate work done by a force when...
The work-energy theorem equates work done by all the forces on an object to the change in its kinetic energy. The theorem can be used to calculate work done by a force when...
Power Expended by a Constant Force
The relationship between work done and the time taken to do it can be explained using the concept of power. For example, several sprinters in a race may have the same velocity when they reach the finish line, therefore doing the same amount of work, but the winner does it in the least amount of time. Thus, power is defined as the rate of doing work. Since work can vary as a function of time, the average power is defined as the work done during a time interval, divided by the time interval.
Conservative Forces
According to the law of conservation of energy, any transition between kinetic and potential energy conserves the total energy of the system. Hence, the work done by a conservative force is completely reversible. It is path independent, which means that we can start and stop at any two points in the transition, and the total energy of the system (kinetic plus potential energy at these points) will remain conserved. This is characteristic of a conservative force. Some important examples of...
Conservative Forces
Conservative forces are an essential concept in the field of mechanical engineering. Understanding the properties and characteristics of these forces is crucial to the design and analysis of mechanical systems.
Conservative forces are forces that are dependent only on the initial and final positions of an object and that are independent of the path that the object takes between these positions. These forces conserve energy, which means that the work done by the force is independent of the path...
Conservative forces are forces that are dependent only on the initial and final positions of an object and that are independent of the path that the object takes between these positions. These forces conserve energy, which means that the work done by the force is independent of the path...
Work and Energy for Variable Forces
When an object is acted upon by a variable force, the amount of work done and the change in energy of the object can be more complex to calculate compared to when a constant force is applied. Work is the product of force and displacement, while energy is the capacity of a system to do work. When a constant force is applied to an object, the work done can be calculated as the product of the force and the distance moved in the direction of the force. However, when a variable force is applied, the...
Work Done by Many Forces
The total work done on an object acted upon by multiple forces can be computed using two methods that give the same result. In one method, the work done by each force is first calculated. Then, those values are summed algebraically to calculate the total work done by all the forces. In the second method, the net force is first calculated by a vector sum of all the forces. Then, the work done by this force is obtained.
Since forces perpendicular to the displacement do no work, they do not...
Since forces perpendicular to the displacement do no work, they do not...


