Variables for describing angular motion

At the start of this class, we defined a set of variables to describe the motion of objects: position, velocity, and acceleration. Although we didn't emphasize it at the time, these quantities pertain to LINEAR motion: bulk movement of an object from one location to another.


Video of marbles in slow motion from The Beauty of Slow Motion

For the next few weeks, we will investigate a different sort of motion: ROTATIONAL motion, in which the center of an object doesn't translate from one place to another, but during which its parts do move in circular paths around its center.


Video of windmill courtesy of Jonathan Cutrer

In order to describe this new sort of motion, we will need to use a new set of variables. Each of the LINEAR quantities has an ANGULAR counterpart. Note that both the symbol and the units are different.


Derivatives with respect to time

Physicists have defined the angular quantities so that they have exactly the same relative relationships with respect to time as their linear counterparts.

In the linear realm, velocity is the derivative of displacement (or position) with respect to time. Likewise, in the rotational realm, angular velocity is the derivative of angular position with respect to time.

In the same way, angular acceleration is the first derivative of angular velocity, and the second derivative of angular position.