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| | For distribution over all beam pulses:<br> | | For distribution over all beam pulses:<br> |
| − | <math> ADC_{ave}=\frac {\sqrt{ \sum_{i=1}^{pulses}{ADC_{ave}^{pulse} - ADC_{ave}} }} | + | <math> ADC_{ave}={\sqrt{ \sum_{i=1}^{pulses}{ADC_{ave}^{pulse} - ADC_{ave} }} |
| − | { \sum_{i=1}^{16}{ADC_{i}}}; </math>
| + | ; </math> |
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Revision as of 07:11, 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}={\sqrt{ \sum_{i=1}^{pulses}{ADC_{ave}^{pulse} - ADC_{ave} }}
; [/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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