Conservation of energy - olympiad problem

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Discussion Overview

The discussion revolves around the conservation of energy in the context of a rubber balloon being inflated, specifically addressing the relationship between work done, elastic energy, and pressure differences. Participants explore the mathematical expressions related to the elastic energy and the forces involved in the inflation process.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant presents a formula for elastic energy and questions the validity of equating work done to the change in energy, suggesting that the correct relationship is dW = -dU.
  • Another participant challenges this assertion, asking for clarification on why dW would equal -dU.
  • Further contributions clarify the distinction between elastic force and the forces associated with pressure differences, with one participant stating that the force needed to expand the balloon is equal and opposite to the elastic force.
  • Participants discuss the implications of using different forms of the energy conservation equation, with some advocating for dW = dU instead of dW = -dU.
  • There is a suggestion that the mathematical representation of elastic force may not fully capture the physical reality of the forces acting on the balloon's surface.

Areas of Agreement / Disagreement

Participants express differing views on the correct formulation of the work-energy relationship, with no consensus reached on whether dW should equal -dU or dU. The discussion remains unresolved regarding the best approach to represent the forces involved.

Contextual Notes

There are unresolved assumptions regarding the definitions of elastic force and the conditions under which the equations apply. The discussion also highlights the complexity of explaining the relationship between work and energy in this specific context.

jpas
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When a rubber balloon of spherical shape with un-stretched radius 0 r is inflated to a sphere of radius r ( ≥ r0 ), the balloon surface contains extra elastic energy due to the stretching. In a simplistic theory, the elastic energy at constant temperature T can be expressed by[tex]U= 4\Pi {r_0}^2kRT(2 {\lambda}^2+\frac{1}{\lambda^4}-3)[/tex]

(c) Express ΔP in terms of parameters given in Eq. (2.2), and sketch ΔP as a function of λ = [tex]\frac {r}{r_0}[/tex]In the solution the problem is solved calculating the work, dW, and then making it equal to

[tex]\frac {dU}{dr}.dr[/tex]

But this isn't true. The true equation is

dW=-dU.

Are the solutions wrong?
 
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Why do you think dW=-dU? :smile:
 
jpas said:
But this isn't true. The true equation is

dW=-dU.
Careful. While the force associated with the potential--in this case an elastic force--is given by F = - dU/dr, the change in potential energy is the work done against this force.
 
Hi,

I think I got it. I'm calculating the force associated with the pressure difference, not the force associated with the potential. These have different directions. Then, because

[tex]F_{elastic}=-\frac{dU}{dr}[/tex] (hooke's law)

[tex]\Delta P A = \frac{dU}{dr}[/tex]

Is that it?
 
That's right. The force needed to expand the balloon is equal and opposite to the elastic force.
 
Doc Al said:
That's right. The force needed to expand the balloon is equal and opposite to the elastic force.

I think we need to clarify "elastic force" here a bit. The "elastic force" we derive from F=-dU/dr is a mathematical quantity equal to -delta(P)*A, while the actual elastic force is tangent to the surface. For that reason, I think we should avoid using F=-dU/dr and instead, use the energy conservation equation dW=dU.
 
hikaru1221 said:
I think we need to clarify "elastic force" here a bit. The "elastic force" we derive from F=-dU/dr is a mathematical quantity equal to -delta(P)*A, while the actual elastic force is tangent to the surface.
Good point. My point was that the force required to expand the balloon will equal dU/dr, not -dU/dr.
For that reason, I think we should avoid using F=-dU/dr and instead, use the energy conservation equation dW=dU.
My point was that dW equals (dU/dr)dr , not (-dU/dr)dr. (Equivalent to what you're saying, I think.)
 
Doc Al said:
My point was that dW equals (dU/dr)dr , not (-dU/dr)dr. (Equivalent to what you're saying, I think.)

Yes, they're equivalent; both leads to the same result. I just wanted to advise the OP not choose the harder path as it's more complicated to explain the term "elastic force", though your explanation goes to the root.
 

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