A Performance Analysis System for the Sport of Bowling
A Performance Analysis System for the Sport of Bowling
A Performance Analysis System for the Sport of Bowling
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2.3 SENSING REQUIREMENTS<br />
The module must be able to sense when <strong>the</strong> ball is released, when it hits <strong>the</strong> lane, when it<br />
hits <strong>the</strong> pins, and <strong>the</strong> ball's angular velocity as it rolls down <strong>the</strong> lane. The module must<br />
be able to accurately sense <strong>the</strong> passage <strong>of</strong> time, and to record time-stamped samples <strong>of</strong><br />
<strong>the</strong> light wave<strong>for</strong>m and <strong>of</strong> <strong>the</strong> impacts <strong>the</strong> ball experiences. It also must be able to sense<br />
<strong>the</strong> presence <strong>of</strong> <strong>the</strong> communication device and contain a transceiver <strong>of</strong> some type so that<br />
<strong>the</strong> module can transfer in<strong>for</strong>mation to/from <strong>the</strong> MASTER application.<br />
The ease-<strong>of</strong>-use, size, cost, and power consumption criteria, combined with locating <strong>the</strong><br />
module underneath a finger insert, limit <strong>the</strong> types <strong>of</strong> sensors that <strong>the</strong> module can employ.<br />
2.3.1 Sensing Rotation <strong>of</strong> <strong>the</strong> Ball (Angular Velocity)<br />
Several methods have been considered to directly sense <strong>the</strong> rotation (angular velocity) <strong>of</strong><br />
<strong>the</strong> ball using passive techniques (measuring some response to ambient conditions):<br />
• Sensing <strong>the</strong> changing orientation <strong>of</strong> <strong>the</strong> ball in <strong>the</strong> earth's magnetic field.<br />
• Sensing <strong>the</strong> changing orientation <strong>of</strong> <strong>the</strong> ball in <strong>the</strong> earth's gravitational field.<br />
• Measuring <strong>the</strong> angular acceleration directly with an accelerometer.<br />
• Measuring <strong>the</strong> ambient light falling on a fixed point on <strong>the</strong> ball.<br />
Honeywell makes an integrated two-axis magnetometer (HMC1052) that physically fits<br />
<strong>the</strong> application, but <strong>the</strong> cost ($18) and peak current draw (~400 mAmps) are both<br />
prohibitive [17]. Analog Devices makes a dual-axis tilt sensor/accelerometer<br />
(ADXL202E) that also fits <strong>the</strong> application, both in size and power requirement, but its<br />
cost (~$15 in 1000 piece quantities) makes it too expensive <strong>for</strong> this application, although<br />
it could be used <strong>for</strong> a later upscale version <strong>of</strong> <strong>the</strong> module [15].<br />
The main thrust <strong>of</strong> <strong>the</strong> research <strong>for</strong> this project centers on <strong>the</strong> fourth, albeit less obvious,<br />
alternative. Besides presenting <strong>the</strong> feasibility <strong>of</strong> <strong>the</strong> in-situ sensor module, this paper<br />
demonstrates that a photometric sensor placed at <strong>the</strong> bottom <strong>of</strong> a finger hole, underneath<br />
a finger insert, can be used to accurately sense <strong>the</strong> angular velocity <strong>of</strong> <strong>the</strong> ball.<br />
TAOS (Texas Advanced Optical <strong>System</strong>s) makes a series <strong>of</strong> small, inexpensive, lowpower,<br />
integrated visible light detectors (TSL25x) that suit <strong>the</strong> application [23]. In<br />
addition, <strong>the</strong> same light sensor can also be used to detect <strong>the</strong> moment <strong>of</strong> release (indicated<br />
by a sudden transition from dark-to-light), and serve as <strong>the</strong> receiver <strong>for</strong> an IR-based<br />
wireless communications scheme. Refer to Figure 2-1 <strong>for</strong> <strong>the</strong> orientation <strong>of</strong> <strong>the</strong> light<br />
sensor in relation to <strong>the</strong> finger insert.<br />
An increasing light level is seen as <strong>the</strong> finger hole revolves up to face <strong>the</strong> ceiling, while a<br />
decreasing light level is sensed as <strong>the</strong> finger hole revolves toward <strong>the</strong> lane. Peaks in <strong>the</strong><br />
light wave<strong>for</strong>m occur at <strong>the</strong> top <strong>of</strong> each revolution (defined as <strong>the</strong> orientation <strong>of</strong> <strong>the</strong> ball<br />
when <strong>the</strong> finger holes are facing toward <strong>the</strong> ceiling), and valleys occur at <strong>the</strong> bottom <strong>of</strong><br />
each revolution (defined as <strong>the</strong> orientation <strong>of</strong> <strong>the</strong> ball when <strong>the</strong> finger holes are closest to<br />
<strong>the</strong> lane). In developing <strong>the</strong> light-sensor based module, it was <strong>the</strong> author's belief that <strong>the</strong><br />
ambient light level <strong>the</strong> sensor "sees" as <strong>the</strong> ball rotates would roughly transcribe a<br />
sinusoidal shape, and that <strong>the</strong> sampled and digitized light wave<strong>for</strong>m could be stored,<br />
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