Will M1 Spin Around M2 When Rope is Cut?

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Discussion Overview

The discussion revolves around the dynamics of two masses, M1 and M2, connected by a rope, when the rope is cut while the system is spinning around a center of mass. Participants explore whether M1 will spin around M2 after the rope is severed, considering various factors such as tangential velocities and the nature of the connection between the masses.

Discussion Character

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

Main Points Raised

  • One participant suggests that M1 and M2 will start rotating around their center of mass after the rope is cut, maintaining their tangential speeds just before the break.
  • Another participant argues that the use of a rope complicates the situation, proposing that a rigid bar would lead to different dynamics, and expresses doubt that M1 and M2 will spin about their mutual center of mass due to the nature of the rope's tension.
  • Some participants discuss the implications of the rope's elasticity and tension, suggesting that the non-rigid nature of the rope could lead to oscillatory motion rather than a stable spinning motion.
  • There is a consideration of the scenario where M1 and M2 are free from the rope, leading to parallel motion with M2 moving faster, which raises questions about the effects of the rope on their velocities and the resulting motion.
  • One participant emphasizes that the angular momentum of the system relative to its center of mass is conserved, suggesting that this conservation principle is crucial to understanding the motion after the cut.

Areas of Agreement / Disagreement

Participants express differing views on whether M1 and M2 will spin around each other after the rope is cut, with some supporting the idea and others challenging it based on the complexities introduced by the rope. The discussion remains unresolved, with multiple competing perspectives presented.

Contextual Notes

Participants note that the assumptions about the rope's rigidity and the nature of the forces involved may significantly affect the outcome, and there are unresolved questions regarding the velocities of M1 and M2 immediately after the rope is cut.

Davidindenver
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Ok this device is spinning around the center of mass(CM).

CW------CM--------------M1---M2

while at full speed the roap is cut like so
CW------CM-------------- M1---M2

does M1 spin around M2?

It seems simple enough but I can't find the answer.
 
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I think yes, they do spin.

An instant before the break, M1 has a tangential speed v1, and M2 has v2>v1. That should be the same an instant after the break, therefore M1 and M2 will start rotating around their center of mass while going away from the rest of the device.

The rest of the device, unless the point "CM" was fixed in space, will also be shoot away (opposite direction of course) so as the center of mass (the point in space where "CM" was before, but now "CM" is not the center of mass anymore) will remain the same. And the rest of the device will spin too (same verse as M1-M2) so that the angular momentum is conserved.
 
The fact that a rope is used makes this very complicated. If you replace th erope with a solid (massless?) bar then yes they would spin around each other, but not necessarily about their centre of mass.

At the instant the bar is cut, M2 will have a higher tangental velocity as:

v_{\perp} = r\frac{d\phi}{d\t} (where \phi is the angle in the plane of motion)

I don't think however that they'll spin about their mutual centre of mass as the spinning motion is intialised only buy the velocity gradient between M1 and M2. This is why I say the bar must be rigid to cause any kind of spinning motion, as if it were rope there would not be constant tension across it as there would in a spin. There would be come sort of ocillatory motion in their spinning.

I hope what I've said makes sense, they're my thoughts, I'm happy to be corrected.
 
neu said:
The fact that a rope is used makes this very complicated. If you replace th erope with a solid (massless?) bar then yes they would spin around each other, but not necessarily about their centre of mass.

At the instant the bar is cut, M2 will have a higher tangental velocity as:

v_{\perp} = r\frac{d\phi}{d\t} (where \phi is the angle in the plane of motion)

I don't think however that they'll spin about their mutual centre of mass as the spinning motion is intialised only buy the velocity gradient between M1 and M2. This is why I say the bar must be rigid to cause any kind of spinning motion, as if it were rope there would not be constant tension across it as there would in a spin. There would be come sort of ocillatory motion in their spinning.

I hope what I've said makes sense, they're my thoughts, I'm happy to be corrected.

Uhm...

I think the rope is just as good. The only difference (not considering needlessly complicating issues like rope linear elasticity) is that if the 2 masses were going towards each other, the rope wouldn't prevent it and the distance between M1 and M2 could become less than the original distance. But this is not the case here, M1 and M2 tend to have their distance increase after the break due to tangential speeds, and we can safely assume that the rope in this case guarantees the distance is therefore always the same.

And of course they spin around their new center of mass... what else? That would be true even if the distance wasn't fixed, so even if they were linked with a spring.
 
Consider that the two masses are free when released, i.e. there's no rope linking them. Obviously they would travel parallel to each other with M2 having a greater velocity.

Now, back to being connected by the rope. M2 will want to carry on moving at v2 but will be resisted by M1 and be pulled back and diagonally. Hence M2 will slow, and M1 will be accelerated by the rope tension. As the rope is not rigid, there will be times when either M1 or M2 are near free objects as the tension in the rope will be negligable (I think), as the relative velocities of M1 & M2 oscillates. In this scenario a centre of mass would be a crude aproximation.

Now this may or may not be the case depending on the difference in velocity between M1 & M2. You can call this pedantry, but I think it would be a significant effect.
 
neu said:
Consider that the two masses are free when released, i.e. there's no rope linking them. Obviously they would travel parallel to each other with M2 having a greater velocity.

Now, back to being connected by the rope. M2 will want to carry on moving at v2 but will be resisted by M1 and be pulled back and diagonally. Hence M2 will slow, and M1 will be accelerated by the rope tension. As the rope is not rigid, there will be times when either M1 or M2 are near free objects as the tension in the rope will be negligable (I think), as the relative velocities of M1 & M2 oscillates. In this scenario a centre of mass would be a crude aproximation.

Now this may or may not be the case depending on the difference in velocity between M1 & M2. You can call this pedantry, but I think it would be a significant effect.

IMHO, you are overcomplicating.

You can also figure out what is the angular momentum of the system M1+M2 relative to its own center of mass (not "CM") one instant before the rope is cut. Such momentum is not zero, and is conserved after the cut.
 

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