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Team 9159: Higher in the Air: Design of Snowboard Course

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<strong>Team</strong> # <strong>9159</strong> page5 <strong>of</strong> 22<br />

At last, to optimize <strong>the</strong> shape <strong>of</strong> <strong>the</strong> halfpipe, we take various requirements<br />

<strong>in</strong>to consideration, <strong>in</strong>clud<strong>in</strong>g construction difficulty, players’ safety and <strong>the</strong>ir performance.<br />

2 Symbols, Hypo<strong>the</strong>sis and Explanations<br />

2.1 Symbols Used <strong>in</strong> this Paper<br />

We list <strong>the</strong> quantities we use as follows. Some are geometric parameters <strong>of</strong><br />

<strong>the</strong> halfpipe, some are physical quantities <strong>in</strong> <strong>the</strong> slid<strong>in</strong>g process. Symbols and<br />

correspond<strong>in</strong>g parameters are shown <strong>in</strong> Tab. 1 and Fig. 2.<br />

Fig 2: Cross section <strong>of</strong> <strong>the</strong> halfpipe, perpendicular to <strong>the</strong> ground<br />

2.2 Hypo<strong>the</strong>sis<br />

• We treat <strong>the</strong> snowboarder as a mass po<strong>in</strong>t with mass m, ignor<strong>in</strong>g body twists<br />

<strong>of</strong> snowboarder and o<strong>the</strong>r geometrical properties.<br />

• The mass po<strong>in</strong>t moves right on <strong>the</strong> snowboard course ra<strong>the</strong>r than travel<strong>in</strong>g<br />

along <strong>the</strong> trajectory <strong>of</strong> <strong>the</strong> orig<strong>in</strong>al gravity center <strong>of</strong> a snowboarder above <strong>the</strong><br />

snow surface.<br />

5

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