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

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Figure 10-6. AC Magnetic Shielding – Payload TestThermal fluctuations of both the SQUID and its electronics correlate with bias variations of the readout system;we therefore control the temperature of both. (Thermal fluctuations also correlate with gain fluctuations, butthe associated requirements are straightforward to meet). In addition, we minimize the sensitivity of the systemto any residual thermal variations. We must limit to 20 nΦ o the bias variations which mimic the science data.We have measured the thermal sensitivity of isolated SQUIDs and have found a coefficient of approximately 10mΦ o /K. Although we do not fully understand the cause, in some cases the thermal sensitivity of the completereadout system can be as much as 1 Φ o /K.Temporarily raising the temperature of the superconductive signal cable above its transition temperaturerestores the sensitivity to approximately 10 mΦ o /K. Furthermore, 2 μK temperature control of the SQUID hasbeen achieved using two nested feedback control loops. In addition, the temperature of the liquid helium bath isregulated and there are various passive control elements. We have measured the electronics sensitivity tothermal fluctuations. We achieved an electronics temperature coefficient of 50 μΦ o /K during early testing andhave reached 20 μΦ o /K by selecting electronic components with little temperature sensitivity. A 20 μΦ o /Ktemperature coefficient implies a 1 mK temperature control requirement for the electronics at roll frequency.For each SQUID, the measured bias temperature coefficient is less than the required 0.01 Φ 0 /K, as shown inTable 10-2 and Figure 10-7 below. The trend in the data taken between 2.92 K and 4.35 K indicates the biastemp-co will meet specification for all four SQUIDS over the full science range of 2.7 to 3.0 K.290 March 2007 Chapter 10 — SQUID Readout Subsystem (SRE) Analysis

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