Derivatives and equilibrium position of a spring

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SUMMARY

The equilibrium position of a spring can be determined by taking the derivative of the potential energy function U(r) and solving for r, as this method accounts for the arbitrary constant in potential energy. Setting U(r) to zero may yield correct results in simple systems, but it is not a reliable method due to the nature of potential energy being unique up to a constant. For more complex scenarios, such as time-varying forces, minimizing potential energy through its derivative is the preferred approach. Thus, using derivatives is essential for accurate calculations in physics.

PREREQUISITES
  • Understanding of potential energy functions in physics
  • Knowledge of derivatives and their application in finding equilibrium
  • Familiarity with the concept of net force and tension in springs
  • Basic principles of energy conservation in mechanical systems
NEXT STEPS
  • Study the application of derivatives in potential energy functions
  • Learn about the equilibrium position of springs using force balance equations
  • Explore the concept of energy conservation in dynamic systems
  • Investigate the effects of time-varying forces on spring systems
USEFUL FOR

Physics students, mechanical engineers, and anyone studying dynamics and energy conservation in mechanical systems will benefit from this discussion.

lonewolf219
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I determined the equilibrium point of a spring by setting the potential energy function U(r) equal to zero and solving for r. But I just looked at the guided solution, and they took the derivative of U(r) first, then solved for r.

Is my approach correct? Can we solve for the equilibrium position of a spring without taking any derivatives?
 
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hi lonewolf219! :smile:
lonewolf219 said:
I determined the equilibrium point of a spring by setting the potential energy function U(r) equal to zero and solving for r.

you must somehow have chosen your constant in such a way that that happened to work

potential energy is only unique up to a constant

eg with gravitational potential energy we often set it equal to 0 "at infinity", or at the level of the lab floor :wink:
 
Thanks Tiny Tim! But I thought that a spring has zero potential energy and maximum kinetic energy at the equilibrium position ? Am I wrong?
 
lonewolf219 said:
Is my approach correct? Can we solve for the equilibrium position of a spring without taking any derivatives?

Solving for the zero of the potential energy function is bogus, because you can always add an arbitrary constant to the potential energy without changing any physics. So if you got the right answer, you got lucky in your choice of zero point (which is pretty easy to do in a lot of simple systems). On the other hand, adding an arbitrary constant won't affect the derivative, so if you're going to use energy methods the derivative approach is always correct (which may be why they're teaching it to you).

If you want a derivative-free solution, you can set the net force on the end of the spring to zero, solve for the tension in the spring required to meet that condition. That can be very hard to do in the general case of time-varying forces acting on the spring, such as if there's a weight bouncing around on the end. For that problem, you'll likely find that minimizing the potential energy by looking for the zeroes of the first derivative is easiest.
 
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Nugatory said:
Solving for the zero of the potential energy function is bogus …

bogus! that's the word i was looking for!

thanks, Nugatory :smile:
lonewolf219 said:
Thanks Tiny Tim! But I thought that a spring has zero potential energy and maximum kinetic energy at the equilibrium position ? Am I wrong?

it only has has zero potential energy at the equilibrium position if you define it that way …

and if you know enough about the equilibrium position in the first place, to define it that way, then why did you ever need to solve anything?

bogus! :rolleyes:
 
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Okay, thanks guys. I noticed it worked for another problem but as Nugatory mentioned, it must be luck with simple systems
 

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