STEM 隨筆︰古典力學︰運動學【三】

讀者切莫以為

pydy-tutorial-human-standing

筆記之第二章

n02_problem_introduction.ipynb

 

不過是簡單圖文介紹待求解的問題也?

姑且不論此系統之四個參考系以及六個重要點;單只就那三個『自由度』之『廣義座標』定奪,已經步入『位形空間』裡矣!

Configuration space (physics)

In classical mechanics, the parameters that define the configuration of a system are called generalized coordinates, and the vector space defined by these coordinates is called the configuration space of the physical system. It is often the case that these parameters satisfy mathematical constraints, such that the set of actual configurations of the system is a manifold in the space of generalized coordinates. This manifold is called the configuration manifold of the system.

Particle

The position of a single particle moving in ordinary Euclidean 3-space is defined by the vector r=(x, y, z), and therefore its configuration space is R3. If the particle is constrained to lie on a sphere, then its configuration space is the subset of coordinates in R3 that define points on the sphere S2.

For n particles the configuration space is R3n, or possibly the subspace where no two positions are equal.

An important problem in physics considers the set of all trajectories of a particle between two points, which is a configuration space that is also known as a function space M. In quantum mechanics one formulation uses histories, or trajectories, as configurations.

Rigid body

The set of coordinates that define the position of a reference point and the orientation of a coordinate frame attached to a rigid body in three-dimensional space form its configuration space, often denoted \displaystyle \mathbb {R} ^{3}\times \mathrm {SO} (3) where \displaystyle \mathbb {R} ^{3} represents the coordinates of the origin of the frame attached to the body, and \displaystyle \mathrm {SO} (3) represents the rotation matrices that define the orientation of this frame relative to a ground frame. A configuration of the rigid body is defined by six parameters, three from \displaystyle \mathbb {R} ^{3} and three from \displaystyle \mathrm {SO} (3) , and is said to have six degrees of freedom.

In robotics, configuration space refers to the set of reachable positions by a robot’s end-effector, considered as a rigid body in three-dimensional space.[1] Thus positions of the end-effector of a robot can be identified with the group of spatial rigid transformations, often denoted SE(3).

The joint parameters of the robot are used as generalized coordinates to define configurations. The set of joint parameter values is called the joint space. A robot’s forward and inverse kinematics equations define maps between configurations and end-effector positions, or between joint space and configuration space. Robot motion planning uses this mapping to find a path in joint space that provides an achievable route in the configuration space of the end-effector.

Phase space

In mechanics, the configuration of a system consists of the positions had by all components subject to kinematical constraints.[2] The set of velocities available to a system defines a plane tangent to the configuration manifold of the system. Momentum vectors are linear functionals of the tangent plane, known as cotangent vectors. Thus, the set of positions and momenta of a mechanical system forms the cotangent bundle of the configuration manifold.

This larger manifold is called the phase space of the system. The joint space and configuration space can be viewed as a bijection on the phase space of a mechanical system.

 

運動描述、分析之難易往往依賴『廣義座標』的選擇呦!?

更別講,還得用 SymPy mechanics 能將之表達出來呀?!

The Physics Vector Module

Abstract

In this documentation the components of the sympy.physics.vector module have been discussed. vector has been written to facilitate the operations pertaining to 3-dimensional vectors, as functions of time or otherwise, in sympy.physics.

……

Vector: Kinematics

This document will give some mathematical background to describing a system’s kinematics as well as how to represent the kinematics in physics.vector.

Introduction to Kinematics

The first topic is rigid motion kinematics. A rigid body is an idealized representation of a physical object which has mass and rotational inertia. Rigid bodies are obviously not flexible. We can break down rigid body motion into translational motion, and rotational motion (when dealing with particles, we only have translational motion). Rotational motion can further be broken down into simple rotations and general rotations.

Translation of a rigid body is defined as a motion where the orientation of the body does not change during the motion; or during the motion any line segment would be parallel to itself at the start of the motion.

Simple rotations are rotations in which the orientation of the body may change, but there is always one line which remains parallel to itself at the start of the motion.

General rotations are rotations which there is not always one line parallel to itself at the start of the motion.