Conservation of Mechanical Energy Requirement

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Discussion Overview

The discussion revolves around the conditions for the conservation of mechanical energy, particularly the role of conservative and non-conservative forces. Participants explore the definitions and implications of these forces in relation to work done and energy conservation, as well as the potential for time-dependent forces to be classified as conservative.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants assert that mechanical energy is conserved when the net work done by non-conservative forces is zero, while momentum conservation requires the external net force to be zero.
  • One participant clarifies that conservative forces can be defined by a scalar potential, and provides a mathematical formulation of energy conservation using Newton's second law.
  • Another participant questions how non-conservative forces can produce zero net work, suggesting that their work may be finite but negligibly small, or that the algebraic signs of the work done may cancel out.
  • There is a discussion about whether time-dependent forces can be considered conservative, with some participants arguing that a time-dependent force cannot have a scalar potential due to path dependence.
  • One participant emphasizes that the curl of a vector field must be zero for it to be expressible as a gradient, which is a requirement for defining a scalar potential.
  • Another participant points out that the concept of curl does not apply to time-dependent forces in the same way, suggesting that such forces are inherently path-dependent and thus not conservative.

Areas of Agreement / Disagreement

Participants express differing views on the nature of time-dependent forces and their classification as conservative. While there is some agreement on the definitions of conservative and non-conservative forces, the implications of time dependence remain contested.

Contextual Notes

The discussion includes assumptions about the definitions of conservative forces and the mathematical properties of vector fields, which may not be universally accepted. The implications of time dependence on force classification are also not resolved.

fog37
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Hello Forum,
Conservation of mechanical energy ME= KE+PE happens when the net work done by the non conservative forces is zero. Conservation of total momentum, instead, happens when the external net force is zero (or close to zero).

In the case of mechanical energy, the non-conservative forces are also external forces to the system and can be nonzero. If the other external forces are conservative, the ME is conserved but not momentum.
But what we care about is the work they produce. How can nonconservative forces produce zero work? I guess their work may be finite but negligibly small. Maybe the total sum of the work done by the nonconservative force is zero...

Is that correct?

fog37
 
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First you should clarify the definitions. A conservative force is given by a time-independnet scalar potential,
$$\vec{F}(\vec{x})=-\vec{\nabla} V(\vec{x}).$$
Then you take Newton's 2nd Law, multiply it by ##\dot{\vec{x}}## and integrate over time to get the energy-conservation law
$$\frac{m}{2} \dot{\vec{x}}^2+V(\vec{x})=\text{const}.$$
Then there are forces that do no work. An example is the motion in an external magnetic field. The Lorentz force is always perpendicular to ##\dot{\vec{x}}## and thus it doesn't contribute to the work.
$$\vec{F} \cdot \dot{\vec{x}}=q (\dot{\vec{x}} \times \vec{B}) \cdot \dot{\vec{x}}=0.$$
 
Sure, so there are two types of forces: conservative and non-conservative. Both types of force can perform work. What matters for the mechanical energy to be conserved is that the net work done by the nonconservative forces is zero. How can that happen? If the nonconservative forces act perpendicularly to the object's path or if the algebraic signs of the works produce a net zero work...

As you mention, conservative forces admit a potential function V(x), which is a function of position. Can a time-dependent force be conservative? I don't think so. But why? What is the rigorous argument to explain that?

Thanks!
fog37
 
Conservative force means that we can define a scalar potential function for that force. To be able to define a scalar function for a vector field the curl (wrt space coordinates) of the vector field should be 0 because curl of a gradient should be always 0. Since force can be written as gradient when we take curl of it, we should obtain 0.
 
Sure, wherever the curl F = 0 we can express F= Delta V, i.e. we can use a scalar potential V.

but what if the force F was F(t), i.e. a function of time?
 
I think you cannot talk about curl of a time dependent function (without fixing time) because now your force is four vector but curl is defined on 3D. Also notice that if you define a potential when you follow different paths in space between two points, you may not reach same potential due to time dependence which makes your force path dependent . So I don't think a time dependent force is conservative. However, in a fixed time your force can be considered as a conservative force if the curl of it wrt space coordinates 0.
 

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