Which thread breaks first when subjected to different forces?

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Discussion Overview

The discussion revolves around the behavior of two threads, A and B, when subjected to different types of forces: a gradually increasing force and an impulsive force. Participants explore the implications of these forces on which thread is likely to break first, considering concepts from Newton's laws and shockwave propagation.

Discussion Character

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

Main Points Raised

  • The original poster (OP) proposes that thread B breaks first under gradual force and thread A breaks first under impulsive force, using Newton's second law to support this reasoning.
  • Some participants agree with the OP's reasoning, suggesting that the assumptions made about acceleration are valid.
  • One participant introduces the concept of shock waves, explaining how the propagation of force through the threads could affect which thread breaks first, depending on the rate of force increase.
  • Another participant questions the OP's assumption about the acceleration being very large when thread A is pulled suddenly, seeking clarification on this point.
  • Some participants discuss the implications of the system not being in equilibrium when the string is pulled suddenly, noting that the acceleration experienced by the mass may be significant.
  • There is a suggestion that if the acceleration equals gravitational acceleration, both threads could break simultaneously, assuming they are identical.
  • One participant emphasizes that the key issue may not be the acceleration of the block but rather the comparison of shockwave propagation speed to the rate of force increase.

Areas of Agreement / Disagreement

Participants generally express agreement with the OP's reasoning, but there remains uncertainty about the implications of acceleration when thread A is pulled suddenly. Multiple competing views exist regarding the mechanics involved, particularly concerning shockwave propagation and equilibrium conditions.

Contextual Notes

Participants express uncertainty about the assumptions made regarding acceleration and the conditions under which the threads break. The discussion includes varying interpretations of force dynamics and the role of shockwaves, indicating a complex interplay of factors that are not fully resolved.

Vibhor
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Hello ,

Please see the attached image , in first case thread A is pulled with gradually increasing force while in second case an impulsive force is applied on thread A ? Which one breaks first in the two cases ?

I think in the first case , thread B breaks . In second case , thread A breaks first .

This is my reasoning -

Consider the mass and apply Newton's II law to it .Downwards is taken positive .

∑F = ma
FA - FB + mg = ma

FA - FB = m(a-g)

Case 1 ) When the thread is pulled slowly, acceleration 'a' would be negligible and we get ,

FA - FB = -mg < 0
FA < FB

Hence B breaks first .

Case 2) But if A is pulled very fast than 'a' would be very large and we get ,

FA - FB = m(a-g) >0 . Now here I am assuming that 'a' > g ( Is this correct ??)

FA > FB

Hence A breaks first .

Is the above reasoning correct ? I am a little unsure in Case 2) where I am considering 'a' to be very large when the sudden force is applied on thread A . Is it right to take 'a' very large ??

Many Thanks
 

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Yes,what you have done is correct.
 
When you pull the string suddenly what happens is that the system won't be in equilibrium.Also note that when you pull the string suddenly the rock accelerates for a very short time(in this time we can assume that the both the strings won't be following hooke's law) the acceleration is for a very short time but is so huge that the force is very high on string A and it breaks.An interesting case would be when a=g.Then the force on both strings are the same and we can expect both of them to break together(assuming they are identical strings).
 
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I think the answer is correct.
We can think of it in terms of shock waves. An increase of force travels through matter as a shockwave and it propagates at the speed of sound in that material. So an increase of force travels through the lower thread at the speed of sound in thread, say ##CT##, until it hits the block, then travels through the block at speed ##CB##, the speed of sound in the block. Let the length of the lower thread be ##L## and the thickness of the block be ##D##. Let the time rate of increase of force be ##J##.

Then the time for a shock wave to travel from the bottom of thread A to the bottom of thread B is ##\left(\frac L{CT}+\frac D{CB}\right)##. It follows that the tension at the bottom of thread B minus the tension at the bottom of thread A is
$$mg-J\left(\frac L{CT}+\frac D{CB}\right)$$
If ##J## is small this will be positive, so that the tension is higher at the bottom of the upper thread, so that thread breaks first. If ##J>\frac{mg}{\frac L{CT}+\frac D{CB}}## it is negative so that the the tension is higher at the bottom of the lower thread, so that thread breaks first.
 
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But do you think the reasoning in the OP is also correct ??
 
If your string A breaks it means,force on it was larger than that on B.This would imply a>g,hence I think your reasoning is correct.
 
I am still unable to convince myself fully that acceleration of mass would be very large when A is pulled suddenly . Do you mind explaining ?
 
I think the difficulty here lies in imagining anything accelerating greater than g without moving too much.Good way of looking at this would be to imagine that when you pull the string suddenly the bottom and lower string elongating a bit.The force causes the string A to elongate and break faster than that of B;once string A breaks no more force acts and the system is again in equilibrium.
 
Vibhor said:
I am still unable to convince myself fully that acceleration of mass would be very large when A is pulled suddenly . Do you mind explaining ?
I don't think acceleration of the block is the key issue, or at least, it's not the easiest way to understand the problem. The comparison of the speed of propagation of the shockwave to the rate of increase in force is the key issue, as per the above equation. If a sufficiently savage jerk were applied to one end of a thread that was unattached at the other end, it would break.
 

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