September 4, 2007 - Cosmic Telescope: Difference between revisions
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| Line 4: | Line 4: | ||
|Time Start | |Time Start | ||
|Time Stop | |Time Stop | ||
|Time elapsed (min.) | |Time elapsed (min.; hour) | ||
|Thresholds on both Scintillators | |Thresholds on both Scintillators | ||
|Singles Count (on top) | |Singles Count (on top) | ||
|Coinc. Counts | |Coinc. Counts | ||
|Coinc. per minute | |Coinc. per minute | ||
|Coinc. per Hour | |||
|Angle measure | |Angle measure | ||
|- | |- | ||
|1:35 pm on 8/31 | |1:35 pm on 8/31 | ||
|1:10 pm on 9/04 | |1:10 pm on 9/04 | ||
|5725 min | |5725 min; 95.42 hr | ||
|225 | |225 | ||
|626816 | |626816 | ||
|1654 | |1654 | ||
|.2889 | |.2889 | ||
|17.33 | |||
|75 degrees | |75 degrees | ||
|}<br> | |}<br> | ||
Revision as of 20:21, 11 September 2007
| Plateau Zeroing | ||||||||
|---|---|---|---|---|---|---|---|---|
| Time Start | Time Stop | Time elapsed (min.; hour) | Thresholds on both Scintillators | Singles Count (on top) | Coinc. Counts | Coinc. per minute | Coinc. per Hour | Angle measure |
| 1:35 pm on 8/31 | 1:10 pm on 9/04 | 5725 min; 95.42 hr | 225 | 626816 | 1654 | .2889 | 17.33 | 75 degrees |
Cosmic rates measured each hour when the telecope accepts cosmics which intersect the earth's surface perpendicularly (defined as zero degrees).
| Time Start | Time Stop | Time elapsed (hour) | Singles Count (on top) | Coinc. Counts | Coinc. per hour | [math]\displaystyle{ \sqrt{N} }[/math] | [math]\displaystyle{ \sqrt{(x_i-\bar{x})^2} }[/math] |
| 1:20 pm | 2:20 pm | 1 | 5694 | 127 | 127 | 11.3 | 121 |
| 2:20 pm | 3:20 pm | 1 | 4896 | 136 | 136 | 11.6 | 4 |
| 3:20 pm | 4:20 pm | 1 | 4655 | 151 | 151 | 12.2 | 169 |
Mean [math]\displaystyle{ \mu }[/math] = 138 counts per hour
Instrumental Uncertainty =[math]\displaystyle{ \sigma = \sqrt{\frac{\sum (x_i - \bar{x})^2}{N-1}} = 12.12 }[/math] counts per hour
The instrumental uncertainty is approximately equal to the Poisson sigma ([math]\displaystyle{ \sqrt{138}= 11.7 }[/math]) counts per hour.
The cosmic ray telescope counting experiment appears to be following Poisson statistics. See Statistics for Experimentalists