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GP-B Post-Flight Analysis—Final Report - Gravity Probe B - Stanford ...

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Figure 11-14. Y axis, B side RMS pointing noise equivalent due to detector noiseThe average, maximum, and minimum noise for the four channels are given in Table 11-5. The noise variationswith time are clearly correlated with the summed weighted currents (the denominator of the normalizedpointing signal), which vary with the intensity of the guide star. Requirement 7.5.2 of T003 requires that theRMS noise, as defined in the equation above, be less than 75 marcsec. This is met only for the X-axis for the A-side electronics and the X-axis for the B-side electronics. The average noise for the Y-axis for the A-sideelectronics is 83.8 marcsec, just 12% above the requirement.Table 11-5. On-orbit detector pair characteristicsChannel(Rotation Axis/Electronic Side)AverageSummedWeightedCurrent (fA)AverageNoise(marcsec)MaximumNoise(marcsec)MinimumNoise(marcsec)Ration S /n EX-Axis, Side A 23.7 51.8 58.0 47.7 1.07Y-Axis, Side A 13.4 84.4 96.4 77.4 0.74X-Axis, Side B 15.4 74.0 84.0 68.2 0.82Y-Axis, Side B 16.7 109.7 127.3 99.8 0.46We can estimate the contribution of the photon/electron pair shot noise n S and of the electronic noise n E withthe following expression and the knowledge of the summed weighted currents of each of the detector pairs,which vary with the brightness of the star. The summed currents i S are plotted in Figure 11-15 throughFigure 11-18 as a function of time, again in days. The fit assumes the following model.2 2 SnT= nS+ nE= +iScciE2SEquation 11-4324 March 2007 Chapter 11 — Telescope Readout Subsystem (TRE) Analysis

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