Gyroscopic precession force diagram

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Discussion Overview

The discussion revolves around the forces acting on a gyroscope, particularly focusing on the concept of gyroscopic precession and the equilibrium of forces. Participants explore the relationship between gravity, normal force, and torque, as well as the mathematical representation of angular relationships.

Discussion Character

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

Main Points Raised

  • One participant expresses confusion about what force keeps the flywheel of a gyroscope in the air, noting the roles of gravity and normal force.
  • Another participant suggests that the torque from gravity causes precession rather than a force keeping the flywheel up.
  • A participant clarifies that normal force cancels gravity, indicating a force equilibrium without the need for additional forces.
  • There is a discussion about whether the normal force is equal to the gravitational force, with some participants affirming that they must be equal if there is no vertical acceleration.
  • One participant mentions that while normal force cancels gravity, they interpreted the question as asking what counters the torque that would cause a gyroscope to fall.
  • Another participant highlights that the video shared explains the concepts in terms of linear forces and accelerations, which may be more intuitive than discussing torque and angular momentum.
  • A participant reiterates their inquiry about force equilibrium, expressing gratitude for the responses received.

Areas of Agreement / Disagreement

Participants generally agree on the concept of force equilibrium between normal force and gravity, but there remains some uncertainty regarding the role of torque and the interpretation of the original question about forces acting on the gyroscope.

Contextual Notes

Some participants note the distinction between angular momentum and torque, indicating potential confusion in terminology. The discussion also touches on the complexity of relating linear and angular concepts, which may not be fully resolved.

Elias Waranoi
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Hi, I've been learning about gyroscopic precession recently and I feel like I get it. I understand that when the flywheel of a gyroscope is spinning its angular moment plus the angular moment created by the torque from the force of gravity makes it turn. But I were thinking about the forces in a gyroscope and couldn't figure out what force is keeping the flywheel up. I know of the force of gravity and the normal force on the pivot connected to the rod connecting to the flywheel but to me that doesn't seem to be enough to keep the flywheel in the air. What's the other forces?

And bonus question, my physics book showed me that dθ = dL / L. I can understand this in a trigonometric way with tanθ = opposite / adjacent = dL / L. I can't make the connection between my knowledge in trigonometry and dθ = dL / L. The tanθ != dθ is what's bothering me.
 
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Elias Waranoi said:
Hi, I've been learning about gyroscopic precession recently and I feel like I get it. I understand that when the flywheel of a gyroscope is spinning its angular moment plus the angular moment created by the torque from the force of gravity makes it turn. But I were thinking about the forces in a gyroscope and couldn't figure out what force is keeping the flywheel up. I know of the force of gravity and the normal force on the pivot connected to the rod connecting to the flywheel but to me that doesn't seem to be enough to keep the flywheel in the air. What's the other forces?

And bonus question, my physics book showed me that dθ = dL / L. I can understand this in a trigonometric way with tanθ = opposite / adjacent = dL / L. I can't make the connection between my knowledge in trigonometry and dθ = dL / L. The tanθ != dθ is what's bothering me.
It's not that there is a force keeping it up; it's that the torque from gravity, which is what you'd expect to make it fall over, has the paradoxical effect of making it precess instead.

By the way, you wrote of the gyroscope's angular moment (which is mormally termed angular momentum) and the angular moment (which should be just "moment") of gravity. I.e. you made them sound like they are dimensionally the same, but they are different. Angular momentum is ML2T-1, whereas torque is ML2T-2.
 
Elias Waranoi said:
I know of the force of gravity and the normal force on the pivot connected to the rod connecting to the flywheel but to me that doesn't seem to be enough to keep the flywheel in the air.
Normal force cancels gravity, so there is a force equilibrium. No other forces are needed. The video below might help you.

 
A.T. said:
Normal force cancels gravity, so there is a force equilibrium. No other forces are needed.
So if there is force equilibrium does that mean that the normal force from the pivot is the same size as the force from gravity?
 
Elias Waranoi said:
So if there is force equilibrium does that mean that the normal force from the pivot is the same size as the force from gravity?
The vertical forces must be equal but opposite if there is no vertical acceleration of the center of mass. Since the center of mass moves slowly in circles, the pivot must also provide a small horizontal centripetal force.
 
A.T. said:
Normal force cancels gravity, so there is a force equilibrium. No other forces are needed
True, but I interpreted the question as asking what counters the torque, which would make a pencil, e.g., fall over.
@Elias Waranoi , which were you asking? Maybe it was both.
 
I was asking about force equilibrium. But I appreciate all the responses I get!
 
Elias Waranoi said:
I was asking about force equilibrium. But I appreciate all the responses I get!
The video I posted explains the issue in terms of linear forces and accelerations, which are more intuitive to most people, than torque and angular momentum.
 

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