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Chapter 5 Robust Performance Tailoring with Tuning - SSL - MIT

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Table 6.6: Primary mirror properties.<br />

Name Description Value Units Source<br />

dPM mirror diameter 3.5 m JPL<br />

ρM material density 2210 kg/m 3 ULE Glass<br />

EM Young’s Modulus 67.6 GPa ULE glass<br />

νM Poisson’s Ratio 0.17 none ULE glass<br />

ρa areal density 40 kg/m 2 JPL estimate<br />

mount properties are listed in Table 6.7 for reference.<br />

Table 6.7: Primary mirror mount properties.<br />

Name Description Value Units Source<br />

ρPM material density 1830 kg/m 3 low CTE MJ55<br />

EPM Young’s Modulus 111.7 GPa low CTE MJ55<br />

νPM Poisson’s Ratio 0.3 none low CTE MJ55<br />

rPM cross-sectional radius .05 m frequency estimates<br />

The combiner consists of the combining optics, supporting structure, a cryo-cooler,<br />

and thermal and mechanical controls and is located at the center of the interferometric<br />

array. All of these elements are modelled together as a concentrated mass (250 kg)<br />

<strong>with</strong> no inertia. The mass of the combiner is based on the CBE from JPL. The<br />

combiner mass is located at the origin of the spacecraft coordinate system and is<br />

connected to the bus <strong>with</strong> a rigid element. All of the finite elements that make up<br />

the instrument model are listed in Table 6.8.<br />

Optical <strong>Performance</strong><br />

The performance metrics of interest are the optical path differences (OPD) between<br />

the reference collector, collector 1, and the other three apertures as shown schemati-<br />

cally in Figure 6-6. Similar to the development model the OPD calculation is based<br />

only on the perturbations of the center node of the collector primary mirrors since<br />

there is no optical train detail in the model.<br />

When the interferometer is in its nominal configuration, i.e. the collectors and<br />

combiners are not perturbed from their locations, the path lengths from the star to<br />

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