Frictionless Disk Supported by Massless String

In summary, the author of a book provided a solution to a problem involving a frictionless disc supported by a massless string. One of the solutions stated that the tension in the string was equal to Mg/2, which may seem counterintuitive since the string is supporting the entire mass of the disc. However, this is because each half of the string is supporting half of the mass, resulting in half the tension at each end. This is further supported by the fact that in another setup where both ends of the string are attached to the ceiling, the tension is also half of Mg. The net vertical force must be zero, so the tension in the two strings would still sum to mg even if the disc was rotating with friction.
  • #1
hringsak
In the following diagram, a frictionless disc is supported by a massless string. This problem was given by the author of a book, and a solution was given to some questions that were asked about this diagram. One thing the author said in one of the solutions, was that the tension in the string was equal to Mg/2. Why is this? I would have thought that since the one string is supporting the entire mass of the disc that it should just be Mg.
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  • #2
hringsak said:
One thing the author said in one of the solutions, was that the tension in the string was equal to Mg/2. Why is this? I would have thought that since the one string is supporting the entire mass of the disc that it should just be Mg.
Consider three setups:
1) The one in your diagram.
2) The one in your diagram, except that we've permanently fixed the string to the disk with a glob of glue at the lowest point.
3) Like #2, except that instead of one string passing through the glob of glue we have two strings both ending in the glob of glue and held onto the disk by the glue.

In #3 we clearly have two strings. Is the tension going to be the same or different in the three cases?
 
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  • #3
Okay, that makes sense that each half of the string is supporting half of the mass. Instead of one end of the string being attached to the ceiling and one end to the disc, where the tension would be Mg, you have just half of the tension at each end. However, because in the midpoint of the string there is no glob of glue, which would provide a balancing force to both halves of the string as in setup #2, doesn't one half pull on the end of the other half, therefore making the tension Mg?

I do get your point that the glue in the middle in setup #2 is not even necessary, but isn't that because the tension from one half is balanced by tension from the other half?
 
  • #4
Wait, I get it now - because both ends are attached to the ceiling, they each are pulling with just half the force as in the example where just one end is attached to the ceiling. In that example you have the full force of Mg pulling in opposite directions. The fact that in the above diagram, both ends are attached to the ceiling, that results in just half the tension in the string.
 
  • #5
The object isn't accelerating so the net force in any direction must be zero. Therefore the vertical forces must sum to zero.
 
  • #6
If the cylinder was rotating and there was friction the net vertical force would still be zero. The tension in the two strings wouldn't be the same but would still sum to mg.
 

FAQ: Frictionless Disk Supported by Massless String

1. What is a frictionless disk supported by a massless string?

A frictionless disk supported by a massless string is a theoretical concept in physics and engineering. It refers to a disk that is able to rotate freely without any resistance or friction, and is held in place by a string that has no mass and therefore does not contribute to the forces acting on the disk.

2. How is a frictionless disk supported by a massless string different from a regular disk?

The main difference between a frictionless disk supported by a massless string and a regular disk is the absence of friction and the weight of the string. In a regular disk, friction and the weight of the string can affect the motion and stability of the disk, while these factors are eliminated in a frictionless disk supported by a massless string.

3. Is a frictionless disk supported by a massless string possible in real life?

No, a frictionless disk supported by a massless string is a theoretical concept and is not possible in real life. This is because all objects have some level of friction and all strings have some level of mass, even if they are very small. However, this concept is often used in physics and engineering to simplify calculations and understand the behavior of objects in ideal conditions.

4. What are some real-life applications of a frictionless disk supported by a massless string?

While a frictionless disk supported by a massless string is not possible in real life, the concept has practical applications in engineering and physics. For example, it can be used to analyze the motion of satellites in space, the behavior of objects in a vacuum, or the ideal motion of a pendulum.

5. How does the tension in a massless string affect a frictionless disk?

In a frictionless disk supported by a massless string, the tension in the string does not affect the motion of the disk. This is because the string has no mass and therefore does not contribute to the forces acting on the disk. The only forces acting on the disk are the centripetal force, which keeps the disk moving in a circular path, and the normal force, which keeps the disk from falling through the string.

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