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A Performance Analysis System for the Sport of Bowling

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known, <strong>the</strong> linear momentum (and thus <strong>the</strong> linear velocity) <strong>for</strong> that revolution can also be<br />

found. Once <strong>the</strong> linear velocity <strong>for</strong> each revolution is known, <strong>the</strong> location <strong>of</strong> each<br />

revolution <strong>of</strong> <strong>the</strong> ball and <strong>the</strong> ball l<strong>of</strong>t distance, relative to <strong>the</strong> foul line, can be found.<br />

Putting those assumptions and deductions into more <strong>for</strong>mal terms, <strong>the</strong> assumption that <strong>the</strong><br />

ball does not lose energy over time means that <strong>the</strong> ball possesses constant energy<br />

throughout its trip to <strong>the</strong> pins, and that its energy at any instant is equal to its energy at<br />

any o<strong>the</strong>r instant [8].<br />

The total energy <strong>of</strong> <strong>the</strong> ball (E) is <strong>the</strong> sum <strong>of</strong> its potential (P) and kinetic (K) energies:<br />

E = P + K.<br />

Since <strong>the</strong> ball rolls on a flat, level lane surface, <strong>the</strong>re is no potential energy (P = 0), and<br />

E = K.<br />

Since it is assumed that <strong>the</strong> ball has constant energy from its release at <strong>the</strong> foul line to its<br />

impact with <strong>the</strong> pins,<br />

K R = K i = K P ,<br />

where K i is <strong>the</strong> energy <strong>of</strong> <strong>the</strong> ball <strong>for</strong> each revolution i between release (K R ) and pin<br />

impact (K P ).<br />

The assumption <strong>of</strong> constant energy implies that energy losses due to vibration, heat, wind<br />

resistance, and noise generation are negligible. There<strong>for</strong>e <strong>the</strong> only components <strong>of</strong> <strong>the</strong><br />

energy <strong>of</strong> <strong>the</strong> ball are its angular momentum (K ω ) and its linear momentum (K v ), thus<br />

K = K ω + K v .<br />

The angular momentum <strong>of</strong> an object with angular velocity ω is given by<br />

K ω = ½Iω 2 ,<br />

where I is <strong>the</strong> moment <strong>of</strong> inertia <strong>of</strong> <strong>the</strong> rotating object.<br />

The moment <strong>of</strong> inertia I <strong>of</strong> a bowling ball with mass m and radius R falls somewhere<br />

between <strong>the</strong> moments <strong>of</strong> inertia <strong>of</strong> a solid sphere and a spherical shell, such that<br />

2 / 5 mR 2 < I < 2 / 3 mR 2 .<br />

The actual moment <strong>of</strong> inertia <strong>for</strong> a given ball will fall between <strong>the</strong>se two values, but<br />

closer to <strong>the</strong> first, since <strong>the</strong> density <strong>of</strong> a bowling ball in <strong>the</strong> 12-16 pound range is fairly<br />

constant across <strong>the</strong> radius <strong>of</strong> <strong>the</strong> ball [8].<br />

The 2 / 5 R 2 term is a constant, where R is <strong>the</strong> radius <strong>of</strong> <strong>the</strong> ball (nominally 4.3"), so if<br />

k = 2 / 5 R 2 = 0.4 · (0.3583 ft) 2 = 0.05136 ft 2 ,<br />

<strong>the</strong>n<br />

K ω = ½kmω 2 .<br />

The linear momentum <strong>of</strong> an object with mass m and linear velocity v is<br />

K v = ½mv 2 .<br />

There<strong>for</strong>e, <strong>the</strong> total kinetic energy K <strong>of</strong> <strong>the</strong> ball, under <strong>the</strong> assumptions, is given by<br />

K = ½mv 2 + ½kmω 2<br />

= ½m(v 2 + kω 2 ), where k = 0.05136 ft 2 .<br />

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