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Tangential Velocity as a Cross Product
Referring again to Fig.B.4, we can write the
tangential velocity vector
as a vector cross product of
the angular-velocity vector
(§B.4.11) and the position
vector
:
 |
(B.17) |
To see this, let's first check its direction and then its magnitude.
By the right-hand rule,

points up out of the page in
Fig.
B.4. Crossing that with

, again by the right-hand
rule, produces a tangential velocity vector

pointing as shown
in the figure. So, the direction is correct. Now, the magnitude:
Since

and

are mutually
orthogonal, the angle between them
is

, so that, by Eq.

(
B.16),
as desired.
Previous: Mass Moment of Inertia as a Cross ProductNext: Angular Momentum
About the Author: Julius Orion Smith III
Julius Smith's background is in electrical engineering (BS Rice 1975, PhD Stanford 1983). He is presently Professor of Music and Associate Professor (by courtesy) of Electrical Engineering at
Stanford's Center for Computer Research in Music and Acoustics (CCRMA), teaching courses and pursuing research related to signal processing applied to music and audio systems. See
http://ccrma.stanford.edu/~jos/ for details.