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                   212                       MEMS and Microstructures in Aerospace Applications


                   The MEMS technologies used for these systems are similar to those discussed in
                   Chapter 8.
                       In general, there are several design considerations that must be considered in
                   the design of spacecraft attitude sensors. Chief among these are the specific nature
                   of the control system application. The constraints associated with predicted en-
                   vironmental conditions such as the prelaunch handling, launch loads (mechanical
                   vibration or shock as well as acoustic exposure), pressure venting profiles, on-orbit
                   operating temperatures, particle contamination, EMI or EMC effects, and radiation
                   exposure (both the total dose and heavy ions) must be well understood and docu-
                   mented prior to the detailed design phase of the sensor.
                       Other system level, but no less important, considerations come into play with
                   spacecraft attitude sensors such as the specific placement and orientation of the
                   device on the spacecraft or platform structure to be controlled. Inadequate attention
                   to these details, especially on very lightweight highly flexible structures, can lead to
                   destabilizing (and, in extreme cases, possibly destructive) controls–structures inter-
                   action (CSI) problems for the GN&C designer.
                       The imminent introduction of the MEMS-based GN&C sensor technology into
                   the spacecraft designer’s inventory will herald a breakthrough in how the function
                   of medium-to-high accuracy attitude determination will be implemented in future
                   space missions.


                   10.3.1 MEMS MAGNETOMETERS
                   MEMS magnetometers have already been discussed in Chapter 7, Microtechnologies
                   for Science Instrumentation Applications. A magnetometer measures the three com-
                   ponents of the magnetic field and provides a measurement of the attitude relative to
                   inertial coordinates. Since only the direction of the magnetic field is sensitive to the
                   attitude, another vector measurement such as a sun sensor is required for attitude
                   determination. For magnetometers, the largest component of the random noise for
                   attitude determination arises not from the sensor itself, but from the magnetic field
                   model, which, for LEO orbits, can cause an error of 0.58 at the equator, and up to 38
                   near the magnetic poles. Therefore, the sensitivity requirements for magnetometers
                   as an attitude sensor are relatively weak and provide an opportunity for insertion of
                   MEMS devices. The performance requirements for attitude determination magnet-
                   ometers are a range of about +60 mT, with a sensitivity of +10 nT.
                       A number of miniature magnetometer developments have occurred in recent
                   years. For the SUNSAT-1 satellite, the magnetic observatory at Hermanus manu-
                   factured a miniature fluxgate magnetometer with this performance at a size of about
                   130 mm   90 mm   36 mm and a weight of 295 g.
                       The University of California, Los Angeles, has developed a miniature fluxgate
                   magnetometer for NASA’s NMP ST5 small satellite mission. The magnetometer
                   mass and power is kept low with a dual core series drive circuit. The magnetometer
                   has two commendable ranges, 64,000 and 1000 nT. The dynamic range is changed
                   from 64,000 to 1000 nT by altering the closed loop response from 64,000 to 5000
                   nT, and then amplifying the signal to get to a 1000 nT range. This method keeps the





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