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| | For each beam pulse:<br> | | For each beam pulse:<br> |
| − | <math>ADC_{aver}^{pulse}=\frac{\sum_{i=1}^{16}{ADC_{i}*i}}{\sum_{i=1}^{16}{ADC_{i}}};</math> | + | <math>ADC_{ave}^{pulse}=\frac{\sum_{i=1}^{16}{ADC_{i}*i}}{\sum_{i=1}^{16}{ADC_{i}}};</math> |
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| − | For distribution over all beam pilses:
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| | + | For distribution over all beam pulses:<br> |
| | + | <math>ADC_{ave}=\frac{\sum_{i=1}^{pulses}{ADC_{ave}^{pulse} - ADC_{ave}}}{\sum_{i=1}^{16}{ADC_{i}}};</math> |
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Revision as of 07:07, 27 March 2010
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For each beam pulse:
[math]ADC_{ave}^{pulse}=\frac{\sum_{i=1}^{16}{ADC_{i}*i}}{\sum_{i=1}^{16}{ADC_{i}}};[/math]
For distribution over all beam pulses:
[math]ADC_{ave}=\frac{\sum_{i=1}^{pulses}{ADC_{ave}^{pulse} - ADC_{ave}}}{\sum_{i=1}^{16}{ADC_{i}}};[/math]
Below is the plot of the charge in Faraday cup (pC) as a function of magnet current (vertical axis, A) (basically magnetic field) and ADC (horizontal axis).
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