Reconciling the Coriolis Force Contradiction on a Spinning Disk

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SUMMARY

The discussion centers on the apparent contradiction involving the Coriolis force on a frictionless spinning disk. Participants clarify that in the inertial frame, a ball remains stationary, while in the rotating frame, it appears to move in a circle due to the centrifugal force acting outward and the Coriolis force acting inward. The Coriolis force is defined as -2Ω x v, where v = Ωr, and is essential for reconciling the forces acting on the ball. Ultimately, the centrifugal force and the Coriolis force together account for the necessary centripetal acceleration in the rotating frame.

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  • Understanding of inertial and non-inertial reference frames
  • Familiarity with fictitious forces, specifically centrifugal and Coriolis forces
  • Basic knowledge of angular velocity and circular motion
  • Ability to apply Newton's laws in rotating frames
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  • Study the derivation of the Coriolis force in rotating systems
  • Explore applications of the Coriolis effect in meteorology and oceanography
  • Learn about the mathematical formulation of fictitious forces in non-inertial frames
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Physics students, educators, and professionals interested in classical mechanics, particularly those studying rotational dynamics and non-inertial reference frames.

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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