Notes for AKT-140115/0:30:33: Difference between revisions

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2. For a rigid body in <math>\mathbb{R}^3</math>, the configuration space is <math>\mathbb{R}^3 \times SO(3)</math>. Generally, it is <math>\mathbb{R}^n \times SO(n)</math>, where <math>SO(n)</math> is the special orthogonal group.
2. For a rigid body in <math>\mathbb{R}^3</math>, the configuration space is <math>\mathbb{R}^3 \times SO(3)</math>. Generally, it is <math>\mathbb{R}^n \times SO(n)</math>, where <math>SO(n)</math> is the special orthogonal group.
3. The torus with its diagonal removed, <math>S^1 \times \mathbb{R}</math>, is the configuration space of two points on <math>S^1</math>. This is <math>C_2(S^1)</math>


'''Reference:''' [https://en.wikipedia.org/wiki/Configuration_space_(mathematics)]
'''Reference:''' [https://en.wikipedia.org/wiki/Configuration_space_(mathematics)]

Latest revision as of 01:22, 20 June 2018

Configuration space Given a topological space , the th ordered configuration space of denoted by is the set of -tuples of pairwise distinct points in , that is .


In physics, parameters are used to define the configuration of a system and the vector space defined by these parameters is the configuration space of the system. It is used to describe the state of a whole system as a single point in a higher-dimensional space.

Examples of Configuration space

1. The configuration space of a particle in is . For particles in , it is

2. For a rigid body in , the configuration space is . Generally, it is , where is the special orthogonal group.

3. The torus with its diagonal removed, , is the configuration space of two points on . This is

Reference: [1]