Coriolis effect vs common sense

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Discussion Overview

The discussion revolves around the Coriolis effect and its mathematical reasoning, particularly in the context of a spinning mass on a string where the radius is increased while maintaining constant angular velocity. Participants explore the implications of tangential and angular accelerations, torque, and the nature of fictitious forces in rotating frames of reference.

Discussion Character

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

Main Points Raised

  • One participant expresses confusion about the relationship between tangential acceleration and angular momentum, noting discrepancies in calculations derived from different sources.
  • Another participant clarifies the distinction between tangential linear acceleration and angular acceleration, suggesting that a torque is required when changing the radius while keeping tangential velocity constant.
  • A participant questions the implications of applying torque without a change in velocity, pondering the concept of effective mass in this scenario.
  • Further discussion highlights that the tangential component of force does not necessarily equal the change in tangential velocity, especially in non-inertial frames.
  • One participant proposes that the Coriolis force can be reconciled with common sense by considering the necessary tangential force to maintain constant tangential velocity while increasing the radius.
  • Another participant suggests that the work done on the string and the increase in kinetic energy should be considered in the analysis of forces involved.

Areas of Agreement / Disagreement

Participants express varying interpretations of the Coriolis effect and the associated forces, indicating that multiple competing views remain. The discussion does not reach a consensus on the correct approach or understanding of the concepts involved.

Contextual Notes

Participants note the complexity of the motions involved and the challenges of applying classical mechanics in non-inertial frames, which may lead to misunderstandings about the relationships between forces and accelerations.

guillefix
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Hello, I've long thought that the coriolis effect was something quite logical (i.e., things luck funny when in a rotating frame of reference), but interested in the mathematical reasoning behind it (because it, being a ficticious force is more about geomtry than physics), found that it was indeed one of the most counterintuitive things I know (at least in classical physics). My problem is the following:

Imagine you have a spinning mass (holded by a massless string say). And you increase the radius of the string with a constant rate, at the same time than exerting a perpendicular force on the mass so as to keep the angular velocity constant. Then tangential acceleration (tangential velocity is w*r) of the mass should be w*r' (as w is constant), where w is angular velocity and r' is the time derivative of the radius.

However, when I saw the same situation in Feynman's physics lectures book, I was dazzled. He, instead, considers the change in angular momentum, which is 2*m*r*r'*w, and that is equal to the torque, which is F*r. So te force exerted is 2*m*r'*w, and the acceleration, 2*r'*w.

So..how come this is double the previous result?? Where have I flawed my reasoning?

Thank you in advance
 
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You are confusing tangential linear acceleration (d(rw)/dt) with angular acceleration, in the sense that applies to torque and angular momentum. If the radius were increased with the tangential velocity constant, there would still be a torque required.
 
haruspex said:
If the radius were increased with the tangential velocity constant, there would still be a torque required.

Thanks! Altho I am still a bit confused. Imagine the case you propose: you have to exert a torque equal to m*r'*v, meaning that the force you have to apply is m*(r'/r)*v. However, the mass doesn't gain any velocity? Is in this system, the effective mass equal to infinity?

Also, in my case the 2*m*r*r'*w force, the Coriolis force, actually comes from the Coriolis acceleration 2*r'*w. So according to this acceleration, the tangential acceleration should be that, and not half of that!

Reference: http://en.wikipedia.org/wiki/Fictitious_force#Rotating_coordinate_systems
 
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guillefix said:
Thanks! Altho I am still a bit confused. Imagine the case you propose: you have to exert a torque equal to m*r'*v, meaning that the force you have to apply is m*(r'/r)*v. However, the mass doesn't gain any velocity? Is in this system, the effective mass equal to infinity?
I think in the case of constant tangnetial velocity and changing radius the mass still moves along a circular arc, but with a different center. The net force is still acting perpendicular to the velocity, so no work is done on the mass. But there still can be a tangential force component in respect to the original center, and hence a torque around it.
 
guillefix said:
Hello, I've long thought that the coriolis effect was something quite logical [..], but interested in the mathematical reasoning behind it [..]. My problem is the following:

Imagine you have a spinning mass (holded by a massless string say). And you increase the radius of the string with a constant rate, at the same time than exerting a perpendicular force on the mass so as to keep the angular velocity constant. Then tangential acceleration (tangential velocity is w*r) of the mass should be w*r' (as w is constant), where w is angular velocity and r' is the time derivative of the radius.

However, when I saw the same situation in Feynman's physics lectures book, I was dazzled. [..] force exerted is 2*m*r'*w, and the acceleration, 2*r'*w.

So..how come this is double the previous result?? Where have I flawed my reasoning?

Thank you in advance
in my case the 2*m*r*r'*w force, the Coriolis force, actually comes from the Coriolis acceleration 2*r'*w. So according to this acceleration, the tangential acceleration should be that, and not half of that!
To my regret I also find such complex motions confusing. However, here my 2cts: if you consider the acquired increase of kinetic energy when you stop increasing the radius, then I think that half of the force was used for the increase of kinetic energy of the mass and the other half for pulling the string outward. The mass is doing work on the string when it is moving outward, and much of that energy is provided by F. So, perhaps you did not sufficiently consider the radial motion and the work done on the string. With that you could lift a weight or activate a heater.
 
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Someone finally told me the missing piece in the puzzle: The tangential component of the force doesn't in general equal the change in the tangential component of velocity. (Because tangential and radial components are a non-inertial frame of reference, it doesn't work like using x and y coordinates) Think for example that in Uniform circular motion, the there is a radial acceleration, but the radial velocity isn't changing.

So taking this into account, coriolis force finally reconciles with common sense: Imagine the case in which the tangential velocity isn't changing, in that case the tangential force is omega x v. This is the acceleration needed so that the velocity doesn't change (as A.T. says, it is the acceleration needed so that the acceleration is perpendicular to the force). Well then, in my original case, I need to add the extra omega x v to have the change in tangential velocity as well as the increasing radius.
 
guillefix said:
Someone finally told me the missing piece in the puzzle: The tangential component of the force doesn't in general equal the change in the tangential component of velocity. (Because tangential and radial components are a non-inertial frame of reference, it doesn't work like using x and y coordinates) Think for example that in Uniform circular motion, the there is a radial acceleration, but the radial velocity isn't changing.

So taking this into account, coriolis force finally reconciles with common sense: Imagine the case in which the tangential velocity isn't changing, in that case the tangential force is omega x v. This is the acceleration needed so that the velocity doesn't change (as A.T. says, it is the acceleration needed so that the acceleration is perpendicular to the force). Well then, in my original case, I need to add the extra omega x v to have the change in tangential velocity as well as the increasing radius.
Yes, one can say the same thing in different ways. :smile:
 

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