Unformatted text preview: OneDimensional Kinematics . Thus we can simply state the equations, alongside their translational analogues: v f = v o + at σ f = σ o + αt x f = x o + v o t + at 2 μ f = μ o + σ o t + αt 2 v f 2 = v o 2 + 2 ax σ f 2 = σ o 2 +2 αμ x = ( v o + v f ) t μ = ( σ o + σ f ) t These equations for rotational motion are used identically as the corollary equations for translational motion. In addition, like translational motion, these equations are only valid when the acceleration, α , is constant. These equations are frequently used and form the basis for the study of rotational motion....
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This note was uploaded on 02/09/2012 for the course PHY PHY2053 taught by Professor Davidjudd during the Fall '10 term at Broward College.
 Fall '10
 DavidJudd
 Physics

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