Length of a massive elastic string hung by it's end

Click For Summary

Homework Help Overview

The problem involves a homogeneous elastic string of mass M and length L, which is hung by one end in a constant gravitational field. Participants are tasked with determining the new length L' of the string when subjected to these conditions, utilizing concepts from elasticity and gravitational potential energy.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the application of Hooke's law and the conditions for equilibrium in the context of gravitational and elastic forces. There are inquiries about the uniformity of stretching and how to mathematically minimize potential energy. The role of the string's mass and the definition of the spring constant for infinitesimal sections are also debated.

Discussion Status

The discussion is active, with participants exploring various interpretations of the problem. Some have proposed potential relationships between the forces and the string's length, while others are seeking clarification on the application of Hooke's law and the implications of the string's mass. There is no explicit consensus, but several productive lines of reasoning have emerged.

Contextual Notes

Participants are navigating the complexities of the problem, including the non-uniform stretching of the string and the implications of the string's mass on the overall behavior of the system. The discussion reflects the constraints of the homework context, where complete solutions are not provided.

Heirot
Messages
145
Reaction score
0

Homework Statement



Given a homogenous string of mass M, length L and elasticity k, find the length L' when it's hung by one end in a constant gravity field.

Homework Equations



Hooke's law.

The Attempt at a Solution



I don't know how to apply Hooke's law in this situation. Please help.
Thanks
 
Physics news on Phys.org
Hi Heirot! :smile:

It will be in equilibrium when its total potential energy (gravitational plus spring) is a minimum. :wink:

(can you see why?)
 
Yes, I can see that :) I just don't know what to minimize mathematically because the streching won't be uniform.
 
Heirot said:
… the streching won't be uniform.

Yes it will …

consider a small section of spring from rest-length x to x + dx …

the external forces on it are T(x + dx) and -T(x) and Mgdx/L, so … ? :smile:
 
So dT = - Mg/L dx -> T(x) = Mg/L (L-x) if x is measured form the top. But this we already knew. How does this help in calculating the streaching?
 
Now use Hooke's law
 
But spring constant k is a global property of the string, not local. Recall that if we cut the string in half, the new constant is 2k, not k. So, what would be the string constant for an infinitesimal part of the string?
 
Do it for the (L-x) part of the spring
 
Well, all below x, we can replace by an external force Mg (L-x)/L. If the upper part of the string were massless, we would have Mg(L-x)/L= k L/x s, where s is the displacement. I can't figure out how to include the mass of the string.
 
  • #10
I'm confused … where does Hooke's law (which is only concerned with internal tension) come into that? …

and what does the mass have to do with it? :confused:
 
  • #11
Can you please show me your solution so that I can precisely tell you where I think the problem lies?
 
  • #12
After having thought about it for a week, still not being able to solve it, I was thinking about your approach. Would you say that L' = L + Mg/k?
 
Last edited:
  • #13
Yup! … gravitational force = elastic force (so net force = 0) … Mg = (L' - L)k. :smile:
 
  • #14
It just occurred to me now, if we divide the unstreched length L into equal parts of length dx then the spring constant for that part is k'=kL/dx. On the other hand, a change in the length dl(x) of dx at some point x is dl(x) = F(x)/k'. Integration gives L' = L + Mg/2k as is pretty much expected.

Thanks for your help, tiny-tim :)
 

Similar threads

  • · Replies 7 ·
Replies
7
Views
3K
  • · Replies 1 ·
Replies
1
Views
2K
Replies
17
Views
2K
  • · Replies 1 ·
Replies
1
Views
3K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 5 ·
Replies
5
Views
2K
Replies
13
Views
2K
  • · Replies 25 ·
Replies
25
Views
4K
  • · Replies 6 ·
Replies
6
Views
2K