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SuperNova / Acceleration Probe Thermal System Wes Ousley November 16, 2001.

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Presentation on theme: "SuperNova / Acceleration Probe Thermal System Wes Ousley November 16, 2001."— Presentation transcript:

1 SuperNova / Acceleration Probe Thermal System Wes Ousley November 16, 2001

2 SNAP Thermal P2 Wes Ousley Thermal Design Parameters High Earth Orbit, 3Re to 25Re, 3 day period Primary mirror diameter 2m  Hubble is 2.3m diameter OTA very sensitive to temperature changes  2 micron vertical shift would defocus image Detectors at 140K, area 0.3m 2, passively cooled

3 November 16, 2001 SNAP Thermal P3 Wes Ousley Overall View Spacecraft bus Detector radiator Solar array (alternating cells and OSR’s)

4 November 16, 2001 SNAP Thermal P4 Wes Ousley OTA Thermal Concept Hubble-type OTA thermal design Thermal control required for primary mirror, secondary mirror, and aft optics  No heaters baselined for secondary truss structure – must be very low CTE  Secondary mirror adjustments for significant changes in secondary structure temps Heater power estimate 100W  Scaled-down Hubble test result: 85W for primary and secondary mirrors TCS —Conduction loss thru primary structure significant  Power to heat aft optics: 15W

5 November 16, 2001 SNAP Thermal P5 Wes Ousley Instrument Diagram

6 November 16, 2001 SNAP Thermal P6 Wes Ousley Detectors Mounted to molybdenum plate  High-conductivity, low CTE Aluminum foil S-links couple plate to radiator (2m 2 ) Estimated 32W cooling required (D. Pankow)  Heat pipes recommended to raise efficiency of radiator Plate of 3mm thickness yields about 1.2C gradient among detectors  Finer control can be achieved by: —Thicker plate (higher mass) —Heat pipes mounted to plate (low mass, cost of ~200K) —More thermal control zones (higher cost)

7 November 16, 2001 SNAP Thermal P7 Wes Ousley Detector layout Moly plate

8 November 16, 2001 SNAP Thermal P8 Wes Ousley Conclusions Telescope thermal requirements met with 100W heater budget Detector temperatures at required level  Detector thermal gradients can be reduced by added mass or cost


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