Reconciling the Coriolis Force Contradiction on a Spinning Disk

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Discussion Overview

The discussion revolves around the apparent contradictions involving the Coriolis force and centrifugal force on a spinning disk, particularly focusing on a ball that remains stationary in an inertial frame while appearing to move in a rotating frame. Participants explore the implications of switching reference frames and the nature of fictitious forces in this context.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Technical explanation

Main Points Raised

  • Some participants assert that in the rotating frame, the ball appears to spin with speed w * r, despite being stationary in the inertial frame.
  • Others argue that without movement in the inertial frame, one cannot claim the presence of centrifugal force or any real force acting on the ball.
  • It is noted that centrifugal force is a fictitious force arising from the non-inertial frame, and participants discuss the implications of this in terms of apparent acceleration.
  • Some participants suggest that the Coriolis force must be considered to account for the net inward force required for circular motion, while others maintain that the Coriolis force is zero in the inertial frame.
  • A later reply emphasizes that the centrifugal force points outward, while the Coriolis force, which is argued to be significant, points inward and must balance the forces for uniform circular motion.

Areas of Agreement / Disagreement

Participants express differing views on the role and existence of the Coriolis force and centrifugal force in this scenario. There is no consensus on how these forces interact or whether the Coriolis force is necessary to explain the motion of the ball in the rotating frame.

Contextual Notes

The discussion highlights the complexities of switching between inertial and non-inertial frames, particularly regarding the definitions and implications of fictitious forces. There are unresolved assumptions about the nature of forces acting on the ball and the conditions under which these forces are considered.

Electric to be
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Imagine there is a frictionless disk that spins with angular speed w. There is a ball on it that sits motionless at some radius r from the center. Now, switch to the frame of the rotating disk. In this frame the ball should be spinning with speed w * r. Edit: To be clear, the ball is NOT moving in the original, inertial frame. Only in the non inertial frame.

Since the ball is undergoing apparent circular motion, the net "force" (fictitous included) should be mv^2/r. The centrifugal force provides this force exactly. However, since in this frame the ball also has some velocity relative to the frame, there is also a Coriolis force that is parallel to the centrifugal. As a result the net forces (fictitious included) cannot be mv^2/r. So how is this possible?

At first I thought that the V in the Coriolis force equation must only refer to V in the radial direction. However, wikipedia and other sources said v is simply the total relative velocity. As a result I'm very confused.

Maybe if somebody could show an easy derivation (like on this kind of spinning disk for the Coriolis force) it would help my confusion. However, it still wouldn't reconcile this seeming contradiction.
 
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Electric to be said:
Imagine there is a frictionless disk that spins with angular speed w. There is a ball on it that sits motionless at some radius r from the center. Now, switch to the frame of the rotating disk. In this frame the ball should be spinning with speed w * r.

if the disk is frictionless ... then the ball isn't likely to be put into motion
 
davenn said:
if the disk is frictionless ... then the ball isn't likely to be put into motion

That's the point. In the inertial frame, the ball isn't moving. It is only moving upon switching to the non inertial frame of the spinning disk.
 
Electric to be said:
That's the point. In the inertial frame, the ball isn't moving. It is only moving upon switching to the non inertial frame of the spinning disk.

but with no movement of the ball you can't say it is under centrifugal force or any force for that matter
the spinning disk isn't supplying any force to the ball

really need some one else to explain your reference frames clearer

@DrakkithDave
 
davenn said:
but with no movement of the ball you can't say it is under centrifugal force or any force for that matter
the spinning disk isn't supplying any force to the ball

really need some one else to explain your reference frames clearer

@DrakkithDave

Well centrifugal force isn't a real force to begin with, it's fictitious, an artifact from switching to a non inertial frame. In the non inertial frame the ball seems to be accelerating, these fictitious forces are made up to explain this, even though no real forces act on the ball.
 
Electric to be said:
Imagine there is a frictionless disk that spins with angular speed w. There is a ball on it that sits motionless at some radius r from the center. Now, switch to the frame of the rotating disk. In this frame the ball should be spinning with speed w * r. Edit: To be clear, the ball is NOT moving in the original, inertial frame. Only in the non inertial frame.

Since the ball is undergoing apparent circular motion, the net "force" (fictitous included) should be mv^2/r. The centrifugal force provides this force exactly. .

This is where you go wrong. The centrifugal force is pointed outwards, but the acceleration of the ball is towards the center, so there has to be another force, pointed towards the center, twice the size of the centrifugal force. This happens to be the coriolis force.
 
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I don't understand the confusion. The coriolis force is zero. In the inertial frame, the ball is not moving. In the rotating frame, the ball is traveling in a circle under the influence of the centrifugal force.
 
Vanadium 50 said:
I don't understand the confusion. The coriolis force is zero. In the inertial frame, the ball is not moving. In the rotating frame, the ball is traveling in a circle under the influence of the centrifugal force.
But the centrifugal force is pointed away from the center. The ball can only move in a circle because of the Coriolis force, which is twice the size of the centrifugal force, and pointed inwards. The coriolis force is -2 Ω x v, where v = Ω r.
 
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I think I don't understand the setup.
 
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Vanadium 50 said:
I think I don't understand the setup.
There's a rotating frame, and a ball that's stationary in an inertial frame, so it's moving in a circle in the rotating frame.
Since there are no external forces on it, the sum of the Centrifugal force and the Coriolis force must account for the centripetal acceleration in the rotaging frame.
 
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  • #11
The setup is as follows: there is a ball which is at rest in an inertial frame, consider it's motion in a rotating frame.

@willem2 has it exactly correct. In the rotating frame the motion of the ball is uniform circular motion, therefore there is a net inwards pointing force. The centrifugal force points outwards. The Coriolis force points inwards with a magnitude exactly sufficient to make the net force the correct direction and magnitude.
 

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