Lecture 2 - Rigid Body Motion

Rigid Motions

Rigid motions is all about describing things with respect to each other.
It is about describing things (points and vectors) in a frame (e.g. $x_{1}, y_{1}, z_{1}$ ) with respect to a reference frame (e.g. $x_{0}, y_{0}, z_{0}$ ).
The first step is representing the target frame with respect to the reference frame (devising a relationship between the two frames)
- If we have this relationship, we can represent any point in the target frame with respect to the reference frame
- These types of relationships are called Coordinate Transformations (as in transforming the coordinates of one frame to the coordinates of another frame, seeing how something in the target frame can be described with respect to the reference frame)
- There are a lot of transformations
  - Rotation
  - Translation
  - Reflection
  - Scaling
  - Shear
- For robotics, rotation and translation are the most important transformations

Rotation

Describing the rotation of a point to another frame with respect to an original frame is just projecting this point on the axes of the original frame (unit vector of the original frame)

$p^{0} = p^{1} \cdot \vec{u} = [\begin{matrix} p \cdot x_{0} \\ p \cdot y_{0} \\ p \cdot z_{0} \end{matrix}]$

Questions

Parameterization

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vs.
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Homogenous Transformation

Transformation is Easier Than Solving Quadratic Equation - YouTube

General Remarks

Coordinate vector vs. Free vector in space
Rotation of frames (frames that are not parallel) makes the difference between coordinate vector and free vector. This demands the description of rotation between the frames
Sequence of rotation, axis of rotation
Current frame -> post multiply | base frame -> pre multiply
Parameterization
- Euler angles (ZYZ)
- yaw, pitch, roll
Homogenous transformation matrix