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Published byReynard Mills Modified over 8 years ago
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Spin of a Batted Baseball Alan M. Nathan a, Jonas Contakos a, Russ Kesman a, Biju Mathew b, Wes Lukash b a University of Illinois at Urbana-Champaign b Rawlings Sporting Goods
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FMFM mg FdFd Spin Affects Batted Ball Trajectories Familiar Effects: Backspin keeps fly ball in air longer –greater distance Topspin makes line drives nosedive – and leads to grounders with tricky bounces Sidespin makes ball slice or hook toward foul pole Backspin sometimes leads to “paradoxical popups”
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2000 fps
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friction normal force v Mechanism for Batted Ball Spin Rolling: e x =0 Sliding: e x <0 Gripping: e x >0 Superball: e x ~ 0.8 “usual” assumption e x =0 Low speed: e x ~0.16
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Scattering Geometry Measure v 1, v 2, 1, 2, Infer v 1 : 85-120 mph 1 : 0, 1000-3000 rpm
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Normalized Final Spin vs. Incident Angle to Normal ( ) Final spins depend on , ~independent of initial spin Incident topspin Incident backspin Incident topspin Incident backspin Zero incident spin Incident topspin Incident backspin
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Final vs. Initial Tangential Speed Zero incident spin Incident topspin Incident backspin Data consistent with e x =0.3 (gripping) Data inconsistent with e x =0 (rolling) For >40 0, “gross slip” ensues Slope = -e x
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Angular Momentum Conservation about Contact Point
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CoF and Ratio of Tangential to Normal Impulse Data consistent with very low CoF, ~0.15
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Summary of Conclusions Final spin for given v Ti nearly independent of initial spin Data consistent with e x =0.30, implying considerable “overspin” Data consistent with angular momentum conservation Data consistent with very low CoF –puzzling!
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…and finally v 0 = 96.6 mph, = 30.5 o, R = 374 ft b = 3300 rpm s = 425 rpm The Grip Doesn’t Matter!
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