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Space Grant Consortium - University of Wisconsin - Green Bay

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agrees with the accepted model for sound transmission. Tests were also done in a bell jar to<br />

analyze the effects <strong>of</strong> air pressure on<br />

sound. Figure 8 shows the tests being<br />

done:<br />

The program output a speed <strong>of</strong> 454.38<br />

meters per second. Again, note the<br />

attenuation from the control case, shown<br />

below in Figure 9:<br />

0.5<br />

0.4<br />

0.3<br />

0.2<br />

0.1<br />

0<br />

-0.1<br />

-0.2<br />

-0.3<br />

-0.4<br />

-0.5<br />

5 5.0001 5.0002 5.0003 5.0004 5.0005 5.0006 5.0007 5.0008 5.0009 5.001<br />

Figure 9: Low Pressure Conditions<br />

This time, the low peaks are shifted to the left. The calculated increase in speed also agrees with<br />

the accepted system for analyzing sound transmission.<br />

A second experimental apparatus <strong>of</strong> identical dimensions that returns the same numbers as the<br />

flight apparatus was constructed. This setup will run under normal, dry air conditions during the<br />

flight. This will serve as the control and basis for comparison <strong>of</strong> the flight data.<br />

Table 2 shows additional results from the cold tests:<br />

17<br />

Figure 8: Bell Jar Testing

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