Difference between revisions of "Sample data table"

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|<math>\sqrt{(x_i-\bar{x})^2}</math>
 
|<math>\sqrt{(x_i-\bar{x})^2}</math>
 
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| || || || || || || || <math>\sigma = \sqrt{\frac{\sum (x_i - \bar{x})^2}{N-1}}</math>
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Cosmic rates measured when the telecope accepts cosmics which intersect the earth's surface at 30 degrees to the perpendicular.
 
{| border="5"
 
{| border="5"
! 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>
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! Run Number || Date || Start Time || End Time || Run 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>  
|1: pm || 2: pm || 1 ||  ||  ||  ||  ||
 
 
|-
 
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|2: pm || 3: pm || 1 ||  ||  ||  ||  ||  
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| || 11/ to 11/ || 4: pm || 1: pm || 21 ||  ||  ||  || || || ||
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|}<br>
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Cosmic rates measured each hour when the telecope accepts cosmics which intersect the earth's surface perpendicularly (defined as zero degrees).
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{| border="5"
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! Run Number || Date || Start Time || End Time || Run 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>
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|-
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| || 11/ || 1: pm || 2: pm || 1 ||  ||  ||  ||  ||  ||  ||  ||
 
|-
 
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|3:pm || 4: pm || 1 ||  ||  ||  ||  ||  
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| || 11/ || 2: pm || 3: pm || 1 ||  ||  ||  ||  ||  ||  ||  ||
 
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|-
|
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| || 11/ || 3: pm || 4: pm || 1 ||  ||  ||  ||  ||  ||  ||  ||
 
|-
 
|-
| || || || || || || || <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>
 
|-
 
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|1: pm || 4: pm || 3 ||  ||  ||  ||  ||  
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| || 11/ || 1: pm || 4: pm || 3 ||  ||  ||  ||  ||  ||  ||  ||  
 
|}<br>
 
|}<br>

Latest revision as of 21:00, 3 December 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 [math]\sqrt{N}[/math] [math]\sqrt{(x_i-\bar{x})^2}[/math]
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 [math]\sqrt{N}[/math] [math]\sqrt{(x_i-\bar{x})^2}[/math]
1: pm 2: pm 1
2: pm 3: pm 1
3:pm 4: pm 1
[math]\sigma = \sqrt{\frac{\sum (x_i - \bar{x})^2}{N-1}}[/math]
1: pm 4: pm 3



Cosmic rates measured when the telecope accepts cosmics which intersect the earth's surface at 30 degrees to the perpendicular.

Run Number Date Start Time End Time Run 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]
11/ to 11/ 4: pm 1: pm 21



Cosmic rates measured each hour when the telecope accepts cosmics which intersect the earth's surface perpendicularly (defined as zero degrees).

Run Number Date Start Time End Time Run 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]
11/ 1: pm 2: pm 1
11/ 2: pm 3: pm 1
11/ 3: pm 4: pm 1
[math]\sigma = \sqrt{\frac{\sum (x_i - \bar{x})^2}{N-1}}[/math]
11/ 1: pm 4: pm 3