
Reaction wheels of varying sizes
General
- Primary attitude control actuators on most spacecraft
- Reaction wheel failures a common problem for many space missions
- Extra reaction wheels for redundancy
- Failure of one reaction wheel often followed by failure of others of same design
- Four reaction wheels failed on the Far Ultraviolet Spectroscopy Explorer (FUSE) in 2001, 2002, 2004 and 2007
Characteristics
- Reaction wheel assembly contains:
- Rotating flywheel (supported by ball bearings)
- Internal brushless DC electric motor
- Associated electronics
- Wide range of capabilities:
- Max. torque from 0.01 to 1.0 Nm
- Max. angular momentum from 2 to 250 Nms
- Max. rotational speeds from 1,000 to 6,000 rpm
- Back electromotive force at high speeds
- Difficult to provide high angular momentum and high torque in the same wheel
- Motor drives command inputs
- Torque command
- Internal closed-loop controller
- Holds reaction wheel speed at commanded value
- Control electronics located in separate box or integral with the wheel unit
- Generally provided with digital and/or tachometer → reading of wheel’s rotational speed
- Wheel friction
$$
L_{drag}^w=-\tau_v\omega^w-\tau_c\space sign(\omega^w)
$$
$\tau_v$ and $\tau_c$ are empirically determined, can exhibit temperature dependence
- Not a good model for friction at low speeds, especially when crossing zero speed
- Dynamic model of friction incorporating hysteresis is required to represent these phenomena adequately
- History of friction modelling
- 1st dynamic friction model → Dahl model (1968)
- Many models developed since → LuGre model (developed by Lund and Grenoble)
- Frictional forces larger at low speeds (Stribeck effect or “stiction”)
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⚠️ Increasing drag torque is often an indication of potential wheel failure. General practice to monitor drag torque on reaction wheels on orbiting spacecraft.
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Disturbances
- Reaction wheels are onw of the major sources of attitude disturbances
- 4 classifications:
- Radial forces
- Axial forces
- Radial moments
- Axial moments
- Perturb spacecraft attitude by creating an $r\times F$ torque
- $r$ is vector from spacecraft’s centre of mass to the point of application of the force
- Effect of reaction wheel force disturbances minimized by locating wheel close to spacecraft’s center of mass
- Effects of disturbance moments are independent of the location of the wheel