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A Performance Analysis System for the Sport of Bowling

A Performance Analysis System for the Sport of Bowling

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The ball's angular velocity increases until <strong>the</strong> discrepancy between <strong>the</strong> angular and linear<br />

velocities is resolved (a condition called roll out). If <strong>the</strong> ball rolls out be<strong>for</strong>e reaching <strong>the</strong><br />

pins, it is no longer skidding, and <strong>the</strong> continuing decrease in its linear velocity due to<br />

rolling friction also directly impacts <strong>the</strong> angular velocity (it begins to monotonically<br />

decrease, as well). Under normal circumstances, <strong>the</strong> ball does not roll out be<strong>for</strong>e hitting<br />

<strong>the</strong> pins, and <strong>the</strong>re<strong>for</strong>e, <strong>the</strong> angular velocity generally increases until <strong>the</strong> ball hits <strong>the</strong> pins.<br />

Given a uni<strong>for</strong>m light distribution along <strong>the</strong> length <strong>of</strong> <strong>the</strong> lane, <strong>the</strong> light level seen by<br />

SMARTDOT will be at its highest (brightest) when <strong>the</strong> module faces directly towards <strong>the</strong><br />

ceiling, and at its lowest (darkest) when <strong>the</strong> module faces directly towards <strong>the</strong> floor, with<br />

a smooth transition occurring between those two points. Under <strong>the</strong>se circumstances, a<br />

graph <strong>of</strong> <strong>the</strong> light wave<strong>for</strong>m appears as an increasing frequency "chirp". The peaks and<br />

valleys <strong>of</strong> <strong>the</strong> sinusoid are spaced fur<strong>the</strong>r apart near <strong>the</strong> release point, and get closer<br />

toge<strong>the</strong>r as <strong>the</strong> ball approaches <strong>the</strong> pins. Figure 3-5, which is a capture <strong>of</strong> <strong>the</strong> filtered<br />

"Wave<strong>for</strong>m" screen from <strong>the</strong> MASTER program, depicts this wave<strong>for</strong>m.<br />

If <strong>the</strong> ball rolls out, its angular velocity reaches a maximum at <strong>the</strong> roll out point, and <strong>the</strong>n<br />

begins decreasing. It is possible to use this in<strong>for</strong>mation to detect whe<strong>the</strong>r or not roll out<br />

has occurred by looking <strong>for</strong> a decrease in <strong>the</strong> angular velocity.<br />

Recall also that friction-reducing lane oil is regularly applied to <strong>the</strong> first 30-40 feet <strong>of</strong> <strong>the</strong><br />

lane. There<strong>for</strong>e, <strong>the</strong> ball is more prone to sliding on <strong>the</strong> upper half <strong>of</strong> <strong>the</strong> lane (nearer <strong>the</strong><br />

foul line), with <strong>the</strong> majority <strong>of</strong> <strong>the</strong> increase in angular velocity occurring on <strong>the</strong> lower<br />

half <strong>of</strong> <strong>the</strong> lane (nearer <strong>the</strong> pins). There<strong>for</strong>e, a graph <strong>of</strong> <strong>the</strong> angular velocity <strong>of</strong> <strong>the</strong> ball<br />

versus time (or distance from <strong>the</strong> foul line) will have a hyperbolic or exponential shape,<br />

assuming roll out has not occurred. The graph <strong>of</strong> <strong>the</strong> linear velocity will mirror that <strong>of</strong><br />

<strong>the</strong> angular velocity, starting high and falling <strong>of</strong>f at <strong>the</strong> end. Figure 3-7, which is a<br />

capture <strong>of</strong> <strong>the</strong> "<strong>Analysis</strong>" screen from <strong>the</strong> MASTER program, depicts <strong>the</strong>se two graphs.<br />

If <strong>the</strong> ball had rolled out, <strong>the</strong> graph <strong>of</strong> its angular velocity in Figure 3-7 would display an<br />

inflection point at <strong>the</strong> point <strong>of</strong> roll out, decreasing after roll out, while <strong>the</strong> graph <strong>of</strong> its<br />

linear velocity would continue to decrease. Figure 3-9 depicts a wave<strong>for</strong>m that resulted<br />

from <strong>the</strong> ball rolling out be<strong>for</strong>e hitting <strong>the</strong> pins.<br />

3.1.2 The "Real" Wave<strong>for</strong>m<br />

The "jagged" appearance <strong>of</strong> <strong>the</strong> raw data wave<strong>for</strong>m, as shown in Figure 3-1, indicates<br />

that a good deal <strong>of</strong> high frequency "noise" has been captured along with <strong>the</strong> desired<br />

wave<strong>for</strong>m. Since <strong>the</strong> module filters out <strong>the</strong> 120 Hz flicker <strong>of</strong> <strong>the</strong> overhead fluorescent<br />

lights while capturing <strong>the</strong> wave<strong>for</strong>m, this noise must have ano<strong>the</strong>r cause. In fact, <strong>the</strong><br />

noise could be <strong>the</strong> result <strong>of</strong> three additional sources: <strong>the</strong> non-homogenous nature <strong>of</strong> <strong>the</strong><br />

overhead lighting; <strong>the</strong> directionality <strong>of</strong> <strong>the</strong> light sensor that was introduced by placing <strong>the</strong><br />

SMARTDOT module at <strong>the</strong> bottom <strong>of</strong> a finger hole, 1 3 / 8 inches below <strong>the</strong> surface <strong>of</strong> <strong>the</strong><br />

ball; and from "aliasing" <strong>of</strong> frequencies greater than one-half <strong>the</strong> sampling frequency.<br />

These higher frequencies might result from flash bulbs, reflections, etc. O<strong>the</strong>r than <strong>the</strong>se<br />

transient sources, aliasing should have minimal impact, since <strong>the</strong>re are no significant<br />

sources <strong>of</strong> flickering light greater than 120 Hz in a bowling center.<br />

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