Lesson 4 of 6 · Reaction wheels and thrusters
Turn by exchanging momentum
9 minute lesson · 3 checks along the way
Your goal for this lessonDistinguish internal momentum exchange from external force and torque.
In this lesson 4 sections · 3 checks
Using archive links & definitions
Words with a dotted underline open a short definition right here in the lesson.
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Turn by exchanging angular momentum
A changes its spin to exchange angular momentum with the rest of the spacecraft. In an ideal isolated system, total angular momentum is conserved. The wheel and body respond in opposite senses. This can change pointing without expelling propellant, within the wheel’s speed and torque limits.
An internal wheel cannot by itself change the translational momentum of the spacecraft’s center of mass. A propulsion maneuver requires an external momentum exchange, such as expelling propellant. Keep the words rotation and translation separate when interpreting a diagram.
Check 1 of 3
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Read & understand
Work a simple momentum exchange
Suppose a fictional spacecraft body has moment of inertia 200 kg·m² about one axis. A wheel gains 4 kg·m²/s of angular momentum, and external torque is negligible. The rest of the body loses 4 kg·m²/s, so its angular changes by −4 / 200 = −0.02 rad/s in this ideal model.
The sign indicates the opposite sense to the wheel’s gain. The example neglects changes in geometry and treats the stated body inertia as constant. It demonstrates conservation, rather than specifying a real vehicle’s commanded turn or settling behavior.
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Wheels have limits
Persistent external disturbances can drive wheel speed toward a limit. transfers accumulated angular momentum out of the wheel-spacecraft system using an external torque. Thrusters can provide it; magnetic actuators can exchange torque with a suitable planetary magnetic field. Available methods depend on the mission environment.
An actuator’s command must be checked against its geometry. A force whose line of action misses the center of mass can create both translation and rotation. A balanced pair can produce a torque with little net force in an ideal arrangement. Real alignment and performance errors require measurement and correction.
Account for both sides of the exchange
Single axis · constant body inertia · negligible external torque WHEEL GAINS ANGULAR MOMENTUM ΔL(wheel) = +4 kg·m²/s The rest of the body must lose the same amount. BODY RESPONSE: I = 200 kg·m² Δω(body) = −4 ÷ 200 = −0.02 rad/s The opposite sign follows from momentum conservation. Unloading the combined system requires an appropriate external torque.
Open full-size diagram in a new tab: Account for both sides of the exchangeCheck 2 of 3
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Close the feedback loop
A controller compares desired with an estimate and commands a response. Sensor delay, structural flexibility and actuator limits affect the outcome. A larger command is not automatically a faster or better settled maneuver. Test the transient response as well as the final angle.
If a wheel reaches its speed limit, restarting the same pointing command does not create unlimited momentum capacity. The system needs an appropriate unloading action or a changed operating plan. This is where the physics of conservation becomes a practical scheduling constraint.
Check 3 of 3
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Put it together
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