Reconciling the Coriolis Force Contradiction on a Spinning Disk

In summary, the conversation discusses a frictionless disk spinning with angular speed w and a stationary ball on it. Upon switching to the rotating frame, the ball is seen to be moving with speed w * r due to the fictitious centrifugal force. However, there is also a Coriolis force that counteracts the centrifugal force and allows for the ball's circular motion. This leads to confusion and a request for a clearer explanation of reference frames. Ultimately, the conversation concludes that the centrifugal force and the Coriolis force account for the ball's circular motion in the rotating frame.
  • #1
Electric to be
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6
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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  • #2
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
 
  • #3
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.
 
  • #4
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
 
  • #5
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.
 
  • #6
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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  • #7
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.
 
  • #8
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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  • #9
I think I don't understand the setup.
 
  • #10
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.
 

1. What is the Coriolis Force Contradiction?

The Coriolis Force Contradiction is a paradox that arises when trying to reconcile the Coriolis force, a fictitious force that appears to act on objects moving in a rotating reference frame, with the principle of inertia, which states that an object will continue to move in a straight line unless acted upon by a force.

2. How does the Coriolis Force Contradiction arise?

The contradiction arises because the Coriolis force appears to act on objects that are moving in a straight line, which seems to go against the principle of inertia. This is because the Coriolis force is only observed in a rotating reference frame, where the principle of inertia is no longer valid.

3. Is the Coriolis Force Contradiction a real phenomenon?

No, the Coriolis Force Contradiction is not a real phenomenon. It is simply a paradox that arises due to the difference in reference frames and does not affect the actual behavior of objects in motion.

4. How is the Coriolis Force Contradiction resolved?

The Coriolis Force Contradiction is resolved by understanding that the principle of inertia still holds true in a rotating reference frame, but the Coriolis force must be taken into account when analyzing the motion of objects. This means that the Coriolis force does not contradict the principle of inertia, but rather complements it.

5. What are some real-world examples of the Coriolis Force Contradiction?

One example of the Coriolis Force Contradiction is the path of a projectile launched from a rotating platform. From the perspective of someone on the platform, the projectile appears to follow a curved path due to the Coriolis force. However, from an outside observer's perspective, the projectile still follows a straight line according to the principle of inertia. Another example is the trajectory of hurricanes, which are affected by the Coriolis force due to the Earth's rotation, but still follow the laws of motion.

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