- Timestamp:
- 08/13/10 16:49:31 (14 years ago)
- File:
-
- 1 edited
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trunk/Mars/NEWS
r9851 r9861 66 66 This is the time spread (rms) around the mean of the arrival times. 67 67 It is calulated as 68 <math>\sqrt{\sum{ t_i}/n}</math>68 <math>\sqrt{\sum{(t_i-<t>)^2}/n}</math> 69 69 ** MHillasExt.fTimeSpreadWeighted: 70 70 This is the weighted time spread (rms) around the weighted mean of the arrival times. 71 71 It is calulated as 72 <math>\frac{1}{\sum{n_i}}\sqrt{\sum{n_i^2(t_i-<wt>)^2}}}</math> 73 or 74 <math>\frac{1}{\sum{n_i}}\sqrt{\sum{n_i^2t_i^2}+<wt>^2\sum{n_i^2}-2<wt>\sum{t_in_i^2}}</math> 72 <math>\frac{1}{\sum{w_i}}\sqrt{\sum{w_i(t_i-<wt>)^2}}}</math> 73 ** MHillasExt.fSlopeSpread: 74 This is the time spread (rms) around the slope of the arrival times. 75 It is calulated as 76 <math>\sqrt{\sum{(t_i-slope*(\cos\delta*x_i+\sin\delta*y_i)-<dt>)^2}/n}</math> 77 ** MHillasExt.fSlopeSpreadWeighted: 78 This is the weighted time spread (rms) around the slope of the arrival times. 79 It is calulated as 80 <math>\frac{1}{\sum{w_i}}\sqrt{\sum{w_i*(t_i-slope*(\cos\delta*x_i+\sin\delta*y_i)-<dt>)^2}</math> 75 81 76 82 ;trainenergy.C:
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