Opposing Forces on an Ideal Spring

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Discussion Overview

The discussion revolves around the behavior of ideal springs, particularly massless springs, under various conditions such as opposing forces, compression, and energy dynamics. Participants explore theoretical aspects, problem-solving techniques, and the implications of mass on spring behavior.

Discussion Character

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

Main Points Raised

  • One participant questions whether two unequal forces can be exerted on opposite sides of a massless spring, to which another responds that this is not possible in a steady state.
  • There is a request for more information on solving problems involving springs with and without mass.
  • A participant poses a question about whether a massless spring, when compressed and released, will overshoot its uncompressed length and where the stored energy goes.
  • Another participant asserts that a massless spring cannot overshoot its uncompressed length, citing conservation of energy, and discusses the conversion of stored energy to kinetic energy.
  • A later post presents a calculation involving a massless spring with added mass, concluding that the spring will overshoot its uncompressed length as the mass approaches zero, while detailing the energy exchange during oscillation.
  • There is a correction regarding the angular frequency of the system, with a participant acknowledging an error in their previous calculation.

Areas of Agreement / Disagreement

Participants express differing views on whether a massless spring can overshoot its uncompressed length, leading to an unresolved debate on the implications of mass and energy conservation in this context.

Contextual Notes

Some discussions involve assumptions about the nature of massless springs and the conditions under which energy conservation applies. The mathematical treatment of angular frequency and energy dynamics is also subject to refinement and correction.

Who May Find This Useful

This discussion may be of interest to those studying mechanics, particularly in the context of oscillatory motion and energy dynamics in springs, as well as individuals looking to understand the theoretical limits of spring behavior.

peeyush_ali
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can we exert 2 unequal forces in opposite directions on the two sides of an ideal<mass less> spring?
 
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can u tell me some more facts abt springs..how to solve problems involving springs with mass and without mass..??
 
A massless spring is compressed then suddenly released. Does it overshoot its uncompressed length? Where does the stored energy go?
 
YorkLarry said:
A massless spring is compressed then suddenly released. Does it overshoot its uncompressed length? Where does the stored energy go?

It can not overshoot its uncompressed length,because it's not accord with conversation of energy. when you release the massless spring,the stored energy switch the spring's kinetic energy,or else why the spring can kinetic without energy
 
I did some calculations after the last post. I've never seen an actual massless spring, and I don't know how to make one or where to buy one, so I added some mass m by gluing a mass m/2 to each end of the spring. I worked out the dynamics and then took the limit as m approaches zero.

If the spring with relaxed length Lo is compressed to length L1 and then released, it will oscillate with amplitude (Lo - L1) independent of m. It has angular frequency sqrt(k/m). The potential and kinetic energy exchange during the motion so as to keep the total energy constant. The maximum kinetic energy equals the maximum potential energy.

As the limit of small m is approached, the angular frequency increases, and the ends of the spring move faster and faster. So the spring will overshoot its uncompressed length regardless of how small m is. The stored energy goes into kinetic energy during the motion, except at the extremes of spring length.

If the mass m is distributed along the length of the spring instead of being concentrated at the ends, the argument is the same. Slices of mass other than at the ends move more slowly than the ends so the kinetic energy formulas are slightly different. The amplitude is still Lo - L1. The angular frequency is still proportional to sqrt(k/m) with the proportionality constant dependent on details of the mass distribution. Behavior in the massless limit is the same.

I can provide details if anyone is interested.
 
Apologies re the previous post - the angular frequency should be 2 sqrt(k/m). I dropped the factor of two.
 

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