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The change in angular position with time, the angular analogue of linear velocity. It is a vector, having both magnitude and direction. In introductory mechanics we will almost always deal with cases of angular velocity about a single axis of rotation, so that the angular velocity is confined to one dimension. |
Mathematical Definition
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{composition-setup}{composition-setup} {table:border=1|frame=void|rules=cols|cellpadding=8|cellspacing=0} {tr:valign=top} {td:width=350|bgcolor=#F2F2F2} {live-template:Left Column} {td} {td} h1. Angular Velocity {excerpt}The change in [angular position] with time, the angular analogue of linear [velocity]. It is a [vector], having both magnitude and direction. In introductory mechanics we will almost always deal with cases of angular velocity about a single [axis of rotation], so that the angular velocity is confined to one dimension.{excerpt} h3. Mathematical Definition {latex}\begin{large}\[\omega = \frac{d{\theta}}{dt}\]\end{large}{latex} {note}Because we will always deal with |
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Because we will always deal with one-dimensional angular velocity (more specifically, the angular velocity about one chosen [ ]in any given problem), we have dropped the vector arrows from the definition. {note} {td} {tr} {table} {live-template:RELATE license} |