@user079622
This is just a mathematical fact of rigid body motion, purely kinematically. It is just the way that rigid body motion behaves mathematically.
Suppose I have a rigid disk which is spinning about its center of mass. At a given instant I can plot the velocity of each point on the disk as follows:
View attachment 319993
The formula for the velocity field is ##\vec v=(y,-x)##. This is rotation around the center, as expected.
However, suppose instead of a disk rotating, we have a wheel rolling. Kinematically these are the same motion in different reference frames. Then at any given instant I can plot the velocity of each point on the wheel as follows:
View attachment 319994
The formula for the velocity field is ##\vec v=(y,-x)+(1,0)##. Notice that this motion is also a pure rotation, but about the bottom of the wheel, the point that it contacts the ground. Again, this is kinematically identical to the disk rotating about the center in a different reference frame.
These two points are not special. In fact, for any point on the wheel you can pick a reference frame where that point is momentarily at rest. When you do so the motion is as follows:
View attachment 319996
The formula for this velocity field is ##\vec v=(y,-x)+(0,0.7)##. Notice again that this motion is momentarily a pure rotation about the chosen point which happens to be ##(0.7,0)##.
This is a general feature of rigid body motion. You can always decompose the velocity of the material points in a rigid body into a pure rotation about any point and a rigid translation.