Difference between revisions of "Sample data table"
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! Date || Start Time || End Time || Singles Counts Top (N_1) || Singles Counts Bottom (N_2)|| <math>\frac{N_1-N_2}{N_1+N_2}</math> || Coincidence Counts || Coinc/Hour || Coinc/min || <math>\sqrt{N}</math> || <math>\sqrt{(x_i-\bar{x})^2}</math> | ! Date || Start Time || End Time || Singles Counts Top (N_1) || Singles Counts Bottom (N_2)|| <math>\frac{N_1-N_2}{N_1+N_2}</math> || Coincidence Counts || Coinc/Hour || Coinc/min || <math>\sqrt{N}</math> || <math>\sqrt{(x_i-\bar{x})^2}</math> | ||
+ | |- | ||
|1: pm || 2: pm || 1 || || || || || | |1: pm || 2: pm || 1 || || || || || | ||
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|3:pm || 4: pm || 1 || || || || || | |3:pm || 4: pm || 1 || || || || || | ||
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| || || || || || || || <math>\sigma = \sqrt{\frac{\sum (x_i - \bar{x})^2}{N-1}}</math> | | || || || || || || || <math>\sigma = \sqrt{\frac{\sum (x_i - \bar{x})^2}{N-1}}</math> |
Revision as of 22:27, 21 November 2007
Cosmic rates measured each hour when the telecope accepts cosmics which intersect the earth's surface at 330 degrees to the perpendicular.
Time Start | Time Stop | Time elapsed (hour) | Singles Counts (on top) | Singles Counts (on bottom) | Coinc. Counts | Coinc. per hour | ||
4: pm of 11/ | 1: pm of 11/ | 21 |
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) | Singles Counts (on bottom) | Coinc. Counts | Coinc. per hour | ||
1: pm | 2: pm | 1 | ||||||
2: pm | 3: pm | 1 | ||||||
3:pm | 4: pm | 1 | ||||||
1: pm | 4: pm | 3 |
Date | Start Time | End Time | Singles Counts Top (N_1) | Singles Counts Bottom (N_2) | Coincidence Counts | Coinc/Hour | Coinc/min | |||
---|---|---|---|---|---|---|---|---|---|---|
1: pm | 2: pm | 1 | ||||||||
2: pm | 3: pm | 1 | ||||||||
3:pm | 4: pm | 1 | ||||||||
1: pm | 4: pm | 3 |