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Combined Rotational and Translational Motion
We can dynamically describe the process of rolling without slipping by
first drawing a figure and showing the relative velocities of various
points on a wheel:
Given that we define the axis of rotation in this way, we can relate the velocity of the center of mass to the angular velocity of the ball. We know that the center of mass is a distance r away from the axis of rotation (the ground). Thus, by our equation for relating v and σ, we see that:
vcm = σr |
K | = | ![]() ![]() ![]() | |
K | = | ![]() ![]() |
In combining our study of combined motion with our study of rotational dynamics, we gain the ability to predict the motion of an object in a variety of situations. The next step in the development of our understanding of rotational motion is the introduction of the concept of angular momentum. (Note: the next section in this SparkNote is actually a calculus-based section describing the derivation of inertial momentum. This is not a topic covered in courses such as AP Physics. If you would like to skip the topic and go on to Angular Momentum, it's fairly obvious where you should click.)
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