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TPF-C Technology Plan - Exoplanet Exploration Program - NASA

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Chapter 4<br />

surface polish is nonetheless required to minimize fixed pattern noise. This test cannot measure<br />

thermally induced wavefront changes on the order of λ/10,000, (the magnitude of change that is<br />

relevant to successful coronagraph operation). If the spherical mirror is manufactured to λ/100<br />

rms at MSF, then it is possible that thermally induced changes on the order of λ/1000 can be<br />

tracked. Thus, this test is a thermal “overdrive test,” and the results can be correlated with the<br />

thermal system model. Likewise, simulated wheel noise excitation of the testbed can only be an<br />

overdrive test.<br />

An alternative approach is to employ the TDM in a separate test that addresses mirror stability in<br />

a room-temperature vacuum chamber. The test (like the baseline approach) requires highprecision<br />

thermal control of the mirror and the ability to apply localized, measurable temperature<br />

gradients on it. The wavefront measurement interferometer/camera is placed at the center of<br />

curvature, and its position is monitored with laser metrology, as with the baseline. The<br />

advantage of this approach is that it separates the mirror stability test from the complications<br />

presented by the cold thermal-vac chamber and hardware in the Sunshield/Isothermal enclosure<br />

testbed. Testing would entail heating the mirror in a known, measurable way while monitoring<br />

the shape of the optic. Depending on camera-to-mirror metrology precision, focus may not be<br />

measurable, but other low-order aberrations (e.g., astigmatism, coma) can be measured and<br />

compared to model predictions. The test yields the sensitivity of the mirror to thermal<br />

deformations and validates our modeling approach. However, the advantages are somewhat<br />

offset by the long radius of curvature of TDM: 7.2 m. This means that the vacuum facility is an<br />

8–9-m-long vertical vacuum chamber. This test also does not allow the mirror to see a cold<br />

background nor is it as highly integrated as the baseline test in the cold chamber.<br />

Progress to Date<br />

To date, work has resulted only in the definition of the measurement goals and the conceptual<br />

design of the testbed. See the Sub-scale EM Sunshield and Isothermal Enclosure discussion in<br />

Section 4.2.4 for information on the development of that portion of the testbed.<br />

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