**Angular Displacement and Velocity**

When that ball you throw is spinning, it spins with a certain velocity (independent of the velocity of the ball itself as it flies through the air) that is called angular velocity. Like our usual translational velocity, angular velocity is basically the change in angular displacement over the change in time. In the illustration on the right we can see that linear displacement (across the circumference of the circle labeled s) is related to the radius of the circle and angular displacement q. In fact, the linear displacement is merely qr. Please note that q is in units of radians, not degrees (1 radian = 180/p degrees).

Angular velocity is the change in angular displacement over a change in time. Thus angular velocity is defined as follows:

You may notice we use the greek letter w instead of plain old v. This is to distinguish between velocity and angular velocity.

**Angular Acceleration**

Similar to translational kinematics, angular acceleration (a) is merely the change in angular velocity over the change in time:

Please note that the linear acceleration used here is the acceleration of a point on the circle parallel, or tangent, to its surface (thus, it is sometimes called tangental acceleration). This is not to be confused with centripetal acceleration, which is the acceleration towards the center of the circle.

To recap:

The equation for centripetal equation in terms of angular quantities is the last line written above.

**Kinematics Equations, Angular Style**

You know what? You can do the exact same derivations we did with translational kinematics to find rotational kinematics equations if we are considering a case with constant angular acceleration. Basically, what comes out is essentially the same equations but with different variables:

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