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TPF-I SWG Report - Exoplanet Exploration Program - NASA

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C HAPTER 5<br />

secondary mirror along the optical axis may exceed 1 nm over much of the spectrum, as shown by the<br />

uppermost trace in Figure 5-16. Below 28 Hz, the amplitude varies, but it peaks at more than 10 nm near<br />

17 Hz. Also between 60 and 80 Hz, amplitudes are large. They exceed the rate that can be corrected by<br />

the fringe tracker, and they are in the section of the beamtrain that is not monitored by laser metrology,<br />

which stops near the FOR mirror. An error budget for the beamtrain has not been developed, but it is<br />

likely to be significantly less than 1 nm for frequencies greater than a few hertz. However, on the positive<br />

side, the vibration amplitudes are sufficiently small that it is possible that vibration mitigation efforts<br />

would reduce them sufficiently. Such mitigations might be (for example) improved isolation of reaction<br />

wheels, or no reaction wheels, and spacecraft controlled by proportional thrusters or another low vibration<br />

system. In the worst case, a laser metrology system could be added to the telescopes to measure much of<br />

the unmonitored path. Primary-mirror vibrations were typically an order of magnitude smaller, so they are<br />

much less likely to cause concern. Additional work to look at the major bending modes of the primary is<br />

also desirable.<br />

5.7 Mission Description<br />

The current concept of the <strong>TPF</strong>-I mission begins with the launch of a single heavy-class launch vehicle<br />

from Kennedy Space Center. The complete observatory, traveling as one integrated assembly, is flown to<br />

the Sun–Earth L2 point. At the L2 point the observatory is inserted into a halo orbit. L2 was chosen over<br />

an Earth drift-away orbit like that used by the Spitzer mission because L2 offers simpler<br />

telecommunications geometry, a lower insertion energy requirement, and the option to launch groundbased<br />

spare spacecraft to the orbit after the deployment of the original formation.<br />

Figure 5-17 depicts a concept for the cruise stage. The cruise stage is used to transport the formation as<br />

packaged for launch from Earth to L2. The cruise stage also protects the optics from some potential<br />

contamination sources during launch. The stage includes a separate propulsion system, solar panels, and a<br />

mechanical structure. The electronics on the combiner spacecraft are used to control the cruise stage. On<br />

Cruise Stage Enclosure<br />

Section separates to<br />

expose Collector #2 for<br />

deployment<br />

Combiner<br />

Spacecraft<br />

Collector Spacecraft (4)<br />

Aft Prop Module /<br />

Collector Enclosure<br />

Section 1 separates to<br />

expose Collector #1 for<br />

deployment<br />

Cruise Stage Position and<br />

Attitude maintained by<br />

Combiner S/C using<br />

Cruise Stage Forward<br />

RCS<br />

Cruise Stage<br />

Collector #1 Separates<br />

from S/C aft attach<br />

fitting, deploys with<br />

gentle spring push off<br />

Cruise Stage sustains launch<br />

loads and provides<br />

contamination protection for<br />

optics during launch and<br />

cruise phases<br />

Figure 5-17. Cruise Stage (RCS is Reaction Control System).<br />

116

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