Time independent potential and mechanical energy conservatio

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Discussion Overview

The discussion revolves around a problem from Taylor Mechanics concerning time-dependent potentials and the implications for mechanical energy conservation. Participants explore the mathematical properties of work integrals and potential energy definitions in the context of forces that depend on time.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant notes that the work integral evaluated at a specific time is independent of the path taken, suggesting a relationship between force and potential energy.
  • Another participant proposes treating time as a fixed parameter when considering potential energy, questioning whether this approach reflects realistic motion.
  • Concerns are raised about the implications of an object moving a finite distance without a change in time, which some argue is impossible and undermines the conservation of mechanical energy.
  • Participants discuss the limitations of the definition of time-dependent potential energy in guaranteeing conservation of energy for realistic trajectories.

Areas of Agreement / Disagreement

Participants express differing views on the implications of time-dependent potential energy for mechanical energy conservation, with no consensus reached on the validity of the arguments presented.

Contextual Notes

Participants highlight the dependence of the discussion on the treatment of time as a fixed parameter and the implications for realistic motion, indicating unresolved assumptions about the nature of the trajectories involved.

Who May Find This Useful

This discussion may be of interest to students and educators in mechanics, particularly those exploring the nuances of potential energy and conservation laws in time-dependent systems.

C. Lee
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Hi,

I was woking on a problem from Taylor Mechanics.(4.27) It reads:

Suppose that the force F(r , t) depends on the time t but stillsatisfies ∇ × F = 0. It is a mathematical fact that the work integral ∫12F(r , t) ⋅ dr (evaluated at anyone time t) is independent of the path taken between the points 1 and 2. Use this to show that the time-dependent PE defined by (4.48) -∫r0rF(r' , t) ⋅ dr', for any fixed time t, has the claimed property that F(r , t) = -∇U(r , t). Can you see what goes wrong with the argument leading to Equation (4.19), that is, conservation of energy?

Equation (4.19) is nothing but Δ(T + U) = 0.
I tried to write down the gradient of (4.48) directly, but I failed because I do not know how to handle ∇∫r0rF(r' , t) ⋅ dr'. And, I think, thus I cannot see what goes wrong with the argument leading to (4.19). (I am aware of the fact that mechanical energy is no longer conserved since potential energy U depends on time)
Can somebody help me with that gradient part, or is there any other way to do this?
 
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For the potential energy you can just consider t as unknown but fixed parameter.

C. Lee said:
Can you see what goes wrong with the argument leading to Equation (4.19), that is, conservation of energy?
The work integral is evaluated at a specific time. Does this represent realistic motion?
 
mfb said:
For the potential energy you can just consider t as unknown but fixed parameter.

The work integral is evaluated at a specific time. Does this represent realistic motion?

Alright. So in the case where r0 ≠ r, that means the object should move finite distance without change in time. This is impossible, so therefore this definition of time-dependent potential energy cannot lead to conservation of mechanical energy.

Is this right?
 
C. Lee said:
Alright. So in the case where r0 ≠ r, that means the object should move finite distance without change in time. This is impossible
Right.
C. Lee said:
so therefore this definition of time-dependent potential energy cannot lead to conservation of mechanical energy.
At least you cannot guarantee conservation of energy for a realistic trajectory that needs some time.
 
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