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Unformatted text preview: 3 1 v v Cf Ci Cf Of Cf Ci Of Ci Oyf Cyi yf yi Cf Ci Cxf Cxi xf xi Cf Ci Of Cf = θ = = θ = = θ = θ = θ + = + = = θ + = + = = θ Summary of analogy between translational and rotational kinematic equations: x a 2 v v t a 2 1 t v x x at v v 2 v v v x 2 i 2 f 2 x x f i AV =+ + = + = + = Translational Rotational αθ = ϖϖ α + ϖ + θ = θ α + ϖ = ϖ ϖ + ϖ = ϖ 2 t 2 1 t t 2 2 i 2 f 2 f i AV...
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This note was uploaded on 04/09/2008 for the course PHYS 131 taught by Professor Reay during the Fall '08 term at Ohio State.
 Fall '08
 Reay
 Energy, Momentum

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