What happens to energy in a gyro vs. flywheel problem?

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Discussion Overview

The discussion revolves around the dynamics of a system involving a gyro and a flywheel, specifically focusing on the conservation of angular momentum and energy during precession. Participants explore the implications of the gyro's motion when its gimbal is released and the flywheel is already in motion, considering both theoretical and practical aspects of the problem.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant describes the initial conditions and constraints of the system, noting the angular moment of inertia and angular velocities involved.
  • Another participant discusses the nature of precession, suggesting that while the total angular momentum's magnitude remains constant, its direction changes due to the applied torque.
  • A participant proposes a hypothetical scenario where the flywheel rotates without the gyro being spun up, concluding that no significant changes would occur in that case.
  • One participant claims to have solved the problem, suggesting that the gyro tilts forward and gains energy from the flywheel, which subsequently comes to a stop.
  • Another participant questions how total angular momentum is conserved if the gyro spins while the flywheel stops.
  • It is noted that the gyro's angular velocity increases slightly, indicating that the flywheel's energy is relatively small compared to that of the gyro.
  • A later reply introduces the idea of varying moments of inertia and angular velocities, questioning whether the flywheel would stop under different conditions.
  • One participant suggests that if the flywheel has more angular momentum than the gyro, it will continue to turn, with the gyro aligning itself with the flywheel's rotational axis.

Areas of Agreement / Disagreement

Participants express differing views on the conservation of angular momentum and energy, with some proposing solutions while others raise questions about the implications of those solutions. The discussion remains unresolved regarding the exact outcomes of the system's dynamics.

Contextual Notes

Participants acknowledge the complexity of the interactions between the gyro and flywheel, including the effects of torque and the conditions under which energy and momentum are conserved. There are unresolved aspects regarding the precise calculations and assumptions made in the analysis.

Ryoko
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I have a problem which got me thinking, but I'm unable to solve to my satisfaction. The problem involves a gyro attached to a platform which in turn is attached to a flywheel. (See image below)

gyro.png


The constraints are as follow: The platform & flywheel are solidly attached to each other and can only rotate about the global X-axis. The gyro gimbal has one axis of freedom about the local Y-axis. There is no friction.

The system has the following properties: The gyro has an angular moment of inertia of 0.25 slug-ft^2 and is spinning at 1000 rad/sec (angular momentum of 250 lbf-ft-sec). The platform/flywheel has an angular moment of inertia of 80 slug-ft^2.

The initial conditions are that the gyro is spun up with its gimbal is locked in place. The platform is then spun about the x-axis to an angular velocity of 1 rad/sec. The gyro's gimbal is released when the gyro's spin axis is exactly vertical (aligned with the z-axis). What happens to the system?

I know that the gyro will immediately precess. But I'm having trouble with conserving both angular momentum and total energy. As I understand it, if the gyro precesses, it will take angular momentum away from the flywheel so that the total angular momentum along the x-axis is conserved. However, if any momentum is taken from the flywheel, it's energy drops. Where does this energy go? I seem to remember that precession doesn't change the angular momentum of the gyro, which means the gyro didn't gain the energy lost from the flywheel when it's momentum changed. What am I overlooking? How do I conserve both angular momentum and energy?
 
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Ryoko said:
I seem to remember that precession doesn't change the angular momentum of the gyro, [...]

Hang on - the state of precessing motion is a state where the total angular momentum is changing all the time. During gyroscopic precession the gyroscope wheel is subject to a torque, and that torque is continuously changing the total angular momentum.

The thing that doesn't change in the friction-free case is the magnitude of the total angular momentum. In the case of friction-free gyroscopic precession the magnitude of the spin rate does not change and the magnitude of the precession rate does not change.

I'm just responding to this detail. I haven't looked whether this affects the outcome of your reasoning.
 
One way to think about this is what would happen if the flywheel were rotated but the gyro was not spun up at all...
 
If the gyro was not spinning, then nothing of interest would happen. The flywheel would just continue to spin without any changes.

Hang on - the state of precessing motion is a state where the total angular momentum is changing all the time.

The direction of the angular momentum vector is changing, but it's magnitude remains constant. The direction of the angular momentum vector is changing because the precession is producing a torque reaction which is being countered by the gimbal mount. However ...

I do think I have solved the problem. If I did the math correctly, it looks like the gyro tilts forward about 18.7 degrees, gains the energy from the flywheel turning it into additional spin momentum, and the flywheel comes to a stop. I know I said that the gyro doesn't gain spin momentum from a precession. And that's true for a simple circular movement. But in this case, the gyro is being forced to move in a somewhat complicated motion which allows torque to be applied to the spin axis.
 
Ryoko said:
I do think I have solved the problem. If I did the math correctly, it looks like the gyro tilts forward about 18.7 degrees, gains the energy from the flywheel turning it into additional spin momentum, and the flywheel comes to a stop. I know I said that the gyro doesn't gain spin momentum from a precession. And that's true for a simple circular movement. But in this case, the gyro is being forced to move in a somewhat complicated motion which allows torque to be applied to the spin axis.

If finally only gyro spins and flywheel stops how is total angular momentum conserved?
 
The gyro tilts forward so its angular momentum along the x-axis replaces the missing momentum from the flywheel.
 
Ryoko said:
The gyro tilts forward so its angular momentum along the x-axis replaces the missing momentum from the flywheel.

What was your answer for final rpm of gyro?
 
The gyro angular velocity only increased a little to 1000.16 r/s. The reason is that the flywheel had very little energy compared to the gyro.
 
Ryoko said:
The gyro angular velocity only increased a little to 1000.16 r/s. The reason is that the flywheel had very little energy compared to the gyro.

Right. An interesting modification is to see whether the flywheel would stop rotating at all combinations of Moments of Inertia and angular velocities?
 
  • #10
If I understand what's happening correctly, if the flywheel has more angular momentum than the gyro, the flywheel will continue turning (albeit slower) and the gyro will align itself with the flywheel's rotational axis (x-axis).
 

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