Does a gyroscope centripetal force?

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Discussion Overview

The discussion revolves around the mechanics of gyroscopic precession, specifically focusing on the role of centripetal force in gyroscopes and their behavior under various conditions, including friction and support structures. Participants explore theoretical concepts, practical examples, and specific cases like the Levitron toy.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant questions how centripetal force is provided when a gyroscope's center of mass moves in a circular path, suggesting that friction with a support may play a role.
  • Another participant describes a gyroscope suspended from a string, noting that it rotates around the support point rather than its center of mass, and speculates on the forces involved.
  • A participant expresses confusion about the conditions under which a gyroscope can precess without friction, raising the question of whether air friction contributes to the behavior of a Levitron top.
  • Some participants discuss the implications of centripetal acceleration and the application of Newton's second law (F=ma) in the context of gyroscopic motion.
  • There is mention of videos demonstrating gyroscopic behavior, with participants analyzing the forces at play and questioning how gravity interacts with the support structure.
  • Concerns are raised about whether the centrifugal force generated by the rotation of the center of mass can be calculated and its significance in the overall dynamics of the gyroscope.

Areas of Agreement / Disagreement

Participants express varying views on the necessity of friction for gyroscopic precession, with some asserting that it is essential while others question its role. The discussion remains unresolved regarding the exact nature of forces acting on gyroscopes in different scenarios.

Contextual Notes

Some participants highlight the complexity of forces involved, including the potential for small forces to influence the behavior of gyroscopes, and the need for clearer diagrams or explanations to visualize these interactions. There is also uncertainty about the implications of different support structures on gyroscopic stability.

hamilton111
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After reading in specialized Physics books and different articles, I’m still thinking about gyroscopical precession. I understand everything about angular momentum, torques…, but if center of masses makes a circular movement, Where does it provide centripetal force? Could it be for the axe friction with the vertical tower? In that case, I wonder, Could it make precessing a top or a gyroscope over a no frictional floor?
I’m waiting forward to listening to you or maybe you propose me any link about this question.
Thanks a lot from Spain. (Sorry about my English)
 
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I've seen gyroscopes suspended by a string from one end, and when the gyroscope's main axis is horizontal, it doesn't rotate about it's center of mass, but instead rotates approximately around the support point, with the center of mass traveling in a circle. My guess is that the string is being pulled slightly outwards by the precession of the gyroscope, and that the inwards horizontal component of tension in the string (due to gravity) counter acts this.

Need an expert here to explain this.
 
hamilton111 said:
<snip>
but if center of masses makes a circular movement, Where does it provide centripetal force? Could it be for the axe friction with the vertical tower? In that case, I wonder, Could it make precessing a top or a gyroscope over a no frictional floor?

On a smooth surface, the gyroscope still precesses, but its centre of gravity does not travel in a circle. Instead the tips of the axis moves in circles. You can try spinning a toy top (gyroscope) on a piece of glass to see.

Wai Wong
 
I understand the examples you explain. So, my doubt is still with me. We imagine a gyroscope with horizontal precess which receives a first impulsion to avoid the nutation as the one in the picture.
It’s right for me that center of mass moves with angular and constant velocity around fulcrum. Is it right? So, it makes that it will have centripetal acceleration towards this fulcrum. Is it right? And, finally, if it’s like that and we use the equation F=Ma(center of mass) I wonder where is this force created in case that the fulcrum hasn’t got friction. Is it OK for me to apply this equation in this case? I think it would be right.
Sincerely

Alberto
 

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In order for the gyroscope to precess about the fulcrum, the fulcrum must provide a centripetal component of force. If it doesn't, the gyroscope will slide off the support.
 
I agree with you, but that makes me doubt again. If no friction makes to slide the gyroscope, How does it precess the top of LEVITRON if the axe hasn’t got friction? Is it made by the friction with the air? It’s difficult for me to understand it.
Alberto
 
I don't have one of those Levitron toys handy, but I know what you are referring to. Question: When the top precesses, does its center of mass move?
 
Yes the center of mass is jumping the whole time between two points.
Look at the video
 

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That jumping around doesn't look anything like precession to me. I suspect it's due to magnetic forces acting on the top--realize that the top is a precessing magnet suspended in a non-uniform magnetic field.
 
  • #10
I can say after these answers that are impossible the precession without friction and with vacuum?
 
  • #11
Look at this video:

http://demolab.phys.virginia.edu/demos/pictures/1q50-23.mpg

This system doesn't appear to rotate about the center of mass, but instead around the point of support. I suspect a small outwards angle on the string as the bicycle tire rotates around.
 
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  • #12
This video answers the question: A heavy gyro suspended from a string at one end of the gyro. Rather than rotate about it's center of mass, it orbits around the support point. The orbit varies in radius, larger if the gyro is tilts downwards, smaller if the gyro tilts upwards. The explanation given is that the center of mass will maintain an altitude (I assume this would only be true if the gyro wasn't slowing down due to friction), so if the gyro tilts upwards, the orbit gets smaller because the angle of the inscribed cone becomes smaller so that the center of mass remains at the same altitude and vice versa when the gyro tilts downwards.

As previously posted by others here, the rotation of the center of mass generates an outwards force, but if the rotational rate is small, so is the outwards force. Towards the end of this video, the gyro is slowed down, and at the slower speed, it does seem to rotate about it's center of mass (or nearly so) while horizontal, then again, this isn't much different than stopping the gyro, and spinning it perpendicular to it's main axis, sort of like twirling a rope.

http://www.gyros.biz/lecture/wmv/9.wmv

Another video, gyro suspended by string:

http://www.gyroscopes.org/video/1hi.wmv

More videos:

http://www.gyros.biz/lecture/wmv/5.wmv

http://www.gyros.biz/lecture/wmv/7.wmv

main web page for these videos:

http://www.gyroscopes.org/1974lecture.asp
 
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  • #13
Doc Al said:
In order for the gyroscope to precess about the fulcrum, the fulcrum must provide a centripetal component of force. If it doesn't, the gyroscope will slide off the support.
Doc Al is correct. If you look at a typical gyroscope, the end points are shaped like balls, and the tower tops are cup like to provide the small amount of centripal force to keep the gyro from sliding off.

As seen in the case of the gyros suspended by string, there is an outwards force due to the rotation of the center of mass.
 
  • #14
Thanks a lot for the videos.Unfortunately my english is not so good and I cannot understand whet they say.
It´s right for me that the center of mass rotation makes a centrifugal force. All of you say that it´s very small,but is it possible to be calculated through mv2/r or is it smaller that mv2/r ?
On video 7.wmv how can it be gyroscope not falling?
Why isn´t the force of gravity "mg" transmited by the support point to the floor?
It´s surprising for me.
Sincerely
Alberto
 
  • #15
hamilton111 said:
It´s right for me that the center of mass rotation makes a centrifugal force. All of you say that it´s very small,but is it possible to be calculated through mv2/r or is it smaller that mv2/r ?
It's mv^2 / r, but v is very low in these cases.

On video 7.wmv how can it be gyroscope not falling? Why isn´t the force of gravity "mg" transmited by the support point to the floor?
Because the gyroscope is creating a torque force, in the direction that is upwards on the non supported point, and downwards on the supported point. The net result is there is a downwards force that equal (on average) to the weight of the gyroscope at the support point, not at the gyroscopes center of mass, so the platform doesn't fall.

Here's another example of this princple:

http://www.gyros.biz/lecture/wmv/8.wmv
 
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  • #16
I don’t understand quite well a question. If the platform doesn’t fall is because the force on the top of the tower is very small, isn’t it? Much smaller than the weight of the gyroscope. If the tower makes another equal reaction upwards, is it right that the F=ma(cm)? If the gyroscope is under the action of weight (downwards) and a small reaction (upwards), the center of mass should fall or not? Could you send me a forces’diagram?
What I watch in videos 7, 8, does it happen with a simple toy gyroscope (non articulated)? I think in this case the gyroscope would make the platform fall.
Sincerely. Alberto.
 

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