透过凸起的镜子:赫尔姆霍尔特的教训,以了解时空理论中的动力学和时间几何学之间的联系
1Philosophy Institute, Pontifical Catholic University of Chile, Chile.
Studies in history and philosophy of science
|December 25, 2024
概括
时方几何学和时空中的动力学理论不是单向的,而是双向的. 这挑战了传统的观点,即一个元素从根本上解释了另一个元素,而是提出了一个相互关联的关系.
科学领域:
- 物理学哲学 物理学的哲学
- 空间时间理论 空间时间理论
- 几何学的基础 几何学的基础
背景情况:
- 时空理论的哲学在过去的二十年中看到了动态主义观点的兴起.
- 在几何学家和动力学家之间存在一场关于时间几何学和动力学之间的解释优先级的辩论.
- 这两种观点都假设一个单向的解释箭头,这意味着一个组件的基本性和优先权超过另一个.
研究的目的:
- 挑战时空理论中单向解释的假设.
- 提出一种替代的框架来理解时间地质与动态之间的联系.
- 在这种情况下,重新评估基本性和优先权的概念.
主要方法:
- 在时空理论中的动态主义和几何主义观点的分析.
- 借鉴赫尔曼··赫尔姆霍尔茨和大卫·希尔伯特对几何学的基本观点.
- 概念上重新评估时间地质与动力学之间的关系.
主要成果:
- 假设一个单向的解释箭头 (无论是时间地质学解释动力学还是相反) 是一个误解.
- 时方几何学和时空理论中的动力学最好被理解为密不可分的相互联系的对应物.
- 这两个元素之间的基本优先权要求是毫无根据的.
结论:
- 时刻几何与时空理论中的动态之间的关系以双向,而不是单向的箭头为特征.
- 这种双向的理解更准确地描述了它们之间的相互联系.
- 关于解释优先级的辩论需要根据这种相互联系重新构建.
相关概念视频
Space-Time Curvature and the General Theory of Relativity
2.6K
In 1905, Albert Einstein published his special theory of relativity. According to this theory, no matter in the universe can attain a speed greater than the speed of light in a vacuum, which thus serves as the speed limit of the universe.
This has been verified in many experiments. However, space and time are no longer absolute. Two observers moving relative to one another do not agree on the length of objects or the passage of time. The mechanics of objects based on Newton's laws of...
This has been verified in many experiments. However, space and time are no longer absolute. Two observers moving relative to one another do not agree on the length of objects or the passage of time. The mechanics of objects based on Newton's laws of...
2.6K
Kinematic Equations - III
7.5K
The first two kinematic equations have time as a variable, but the third kinematic equation is independent of time. This equation expresses final velocity as a function of the acceleration and distance over which it acts. The fourth kinematic equation does not have an acceleration term and provides the final position of the object at time t in terms of the initial and final velocities. This equation is useful when the value of the constant acceleration is unknown.
Using the kinematic equations,...
Using the kinematic equations,...
7.5K
Dynamics of Circular Motion
13.4K
An object undergoing circular motion, like a race car, is accelerating because it is changing the direction of its velocity. This centrally directed acceleration is called centripetal acceleration. This acceleration acts along the radius of the curved path (thus is also referred to as radial acceleration).
Any acceleration must be produced by some force. Therefore, any force or combination of forces can cause centripetal acceleration. A few examples include the tension in the rope on a...
Any acceleration must be produced by some force. Therefore, any force or combination of forces can cause centripetal acceleration. A few examples include the tension in the rope on a...
13.4K
Kinematic Equations - I
10.3K
When an object moves with constant acceleration, the velocity of the object changes at a constant rate throughout the motion. The kinematic equations of motions are derived for such cases where the acceleration of the object is constant. The first kinematic equation gives an insight into the relationship between velocity, acceleration, and time. We can see, for example:
10.3K
Rotation with Constant Angular Acceleration - II
5.9K
Kinematics is the description of motion. The kinematics of rotational motion discusses the relationships between rotation angle, angular velocity, angular acceleration, and time. One can describe many things with great precision using kinematics, but kinematics does not consider causes. For example, a large angular acceleration describes a very rapid change in angular velocity without any consideration of its cause. Thus, rotational kinematics does not represent the laws of nature.
The first...
The first...
5.9K
Measuring Acceleration Due to Gravity
529
Consider a coffee mug hanging on a hook in a pantry. If the mug gets knocked, it oscillates back and forth like a pendulum until the oscillations die out.
A simple pendulum can be described as a point mass and a string. Meanwhile, a physical pendulum is any object whose oscillations are similar to a simple pendulum, but cannot be modeled as a point mass on a string because its mass is distributed over a larger area. The behavior of a physical pendulum can be modeled using the principles of...
A simple pendulum can be described as a point mass and a string. Meanwhile, a physical pendulum is any object whose oscillations are similar to a simple pendulum, but cannot be modeled as a point mass on a string because its mass is distributed over a larger area. The behavior of a physical pendulum can be modeled using the principles of...
529


