Massless string pulled by a force

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When a massless string is pulled by a force from one end, tension arises due to the internal forces acting between segments of the string. The tension is constant throughout the string if it is not accelerating, as shown by the equation T1 = T2, indicating that the net force on each segment is zero. If the string has mass and equal forces are applied at both ends, the tension remains equal to the applied force F, preventing acceleration. However, a truly massless string cannot exist under these conditions without leading to infinite acceleration. Ultimately, the discussion emphasizes the importance of recognizing simplifying assumptions in physics to avoid complex and unphysical scenarios.
  • #31
andyrk said:
And if I say that I am fine with infinite acceleration, then what would the tension be?
This just results in a math fail. It's like asking if God can create a rock so big he can't lift it. It doesn't have an answer. Indeed, even stating that you apply a force to this string is impossible. So you're going to have to decide what you want to get out of this problem.
 
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  • #32
In reality the string will have a small mass density ρ . Assuming that is moving with a finite acceleration a (because for example it is attached to other main bodies that do so) a length dx of the string will have a net force F=(ρdx)a=T(x+dx)-T(x)=dT as it follows from Newton's 2nd law. If the acceleration a is not too big such that the product ρa is small we can approximately say that the net force is zero from which it follows that dT=0 that is the tension along the string remain constant.

Finally i want to say something general that i find quite important when studying physics. It is quite often when studying physics that we do silent simplifying assumptions that simplify the calculations a lot and brighten only the key points of a phenomenon.If we don't make those assumption the study can become quite complex sometimes, so complex that we can't make any usefull conclusions.
 
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