Find the Smallest Possible Tension in a Massless String Supporting a Disk

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The discussion revolves around the mechanics of a disk suspended by a massless string, focusing on the tension at various points and the effects of friction. The tension at the lowest point of the string, T(π/2), is questioned, particularly regarding its value of Mg/2 and the implications of the angle π/2. Participants clarify that the disk rests in the loop of the string and explore how the tension in the vertical segments may differ due to friction and angles. The conversation highlights the complexities of tension distribution in a non-uniform system and the need for a clear understanding of the forces at play. Overall, the analysis emphasizes the importance of considering all forces and angles when determining tension in such mechanical setups.
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A disk of mass M and radius R is held up by a massless string. (The two ends of the string are connected to a ceiling and the disk rests on the bottom of the string.) The coefficient of friction between the disk is μ. What is the smallest possible tension in the string at its lowest point?

This is from "Introduction to Classical Mechanics" by David Morin. I am confused as to how T(∏/2) = Mg/2. T(∏/2) refers to the tension in the rightmost point of the disk where the string does not touch the disk anymore.)
 
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What does the ##\pi/2## refer to?

I take it, by "in the bottom" you mean the disk rests in the loop of the string?

If the disk were just held up by two vertical lengths of string - what would the tension in each string be?
 
They would be mg/2. In the problem, why do the tensions in the vertical lengths have to be equal? The tension in the string increases opposite the direction of friction so from this argument, I see that the vertical lengths have different tensions. What am I missing?
 
How do you see that the vertical lengths have different tensions?
Are they hanging at different angles?
Is the disk spinning?

Remember - I cannot see any diagram you may be looking at.
 
Topic about reference frames, center of rotation, postion of origin etc Comoving ref. frame is frame that is attached to moving object, does that mean, in that frame translation and rotation of object is zero, because origin and axes(x,y,z) are fixed to object? Is it same if you place origin of frame at object center of mass or at object tail? What type of comoving frame exist? What is lab frame? If we talk about center of rotation do we always need to specified from what frame we observe?

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