Net work done on Earth-object system and potential energy

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Discussion Overview

The discussion revolves around the concept of work done on an Earth-object system and its relation to potential energy, particularly in the context of lifting an object against gravity. Participants explore the implications of the work-energy theorem, the definitions of net work, and the roles of conservative and non-conservative forces in energy changes.

Discussion Character

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

Main Points Raised

  • One participant questions why the author of a textbook states that only the external force does net work on the system, suggesting that the work done by gravity should also be included.
  • Another participant argues that the effect of gravity is already accounted for through the concept of potential energy.
  • There is a suggestion that using the term "net non-conservative work" instead of "net work" could clarify the discussion and avoid confusion.
  • A participant notes that according to the work-kinetic energy theorem, the net work done by all forces is equal to the change in kinetic energy, raising a question about the implications when there is no change in kinetic energy but a change in potential energy.
  • Another participant confirms that the more general version of the work-energy relationship includes changes in both kinetic and potential energy, indicating that net work can be zero while other forms of energy change.
  • Discussion includes the possibility of changes in internal energy, particularly in systems involving friction or other forms of potential energy, such as a mass on a spring.
  • Participants acknowledge that the discussion is extending into areas beyond the typical application of the work-energy theorem, hinting at thermodynamic considerations.

Areas of Agreement / Disagreement

Participants express differing views on the definitions and implications of net work and potential energy, with no consensus reached on the interpretation of the work-energy theorem in relation to changes in energy forms. The discussion remains unresolved regarding the inclusion of various forms of energy and the applicability of the work-energy theorem in complex scenarios.

Contextual Notes

Participants highlight limitations in the traditional work-energy theorem when applied to systems with multiple forms of energy, such as internal energy and potential energy, and suggest that the theorem may not account for all energy changes in certain contexts.

NoahCygnus
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My book says:
"Let us derive an expression for the potential energy associated with an object at a given location above the surface of earth. Consider an external agent lifting an object of mass ##m## from an initial height ##y_{i}##above the ground to a final height ##y_{f}##. We assume the lifting is done slowly with no acceleration so the applied force from the agent can be modeled as being equal to in magnitude to the gravitational force on the object. The work done by the external agent on the earth-object system as the object undergoes this upward displacement is given by : ##W_{net} = \vec{Fapp}\cdot \Delta \vec{r} = mg\hat{j}\cdot[(y_{f} - y_{i})\hat{j}] = mgy_{f} - mgy_{i}##

Where this result is the net work done on the system because the applied force is only force by the environment. The equation represents a transfer of energy into the system and the energy appears in a different form called potential energy. Therefore we call the quantity ##mgy## as the gravitational potential energy ##U_{g}##. ##U_{g} \equiv mgy##.
Therefore ##W_{net} = \Delta U_{g}##."


What I don't understand is , why has the author stated that only the external force does net work done on the system? Why didn't the author include the work done due to gravity in the net work? Shouldn't the net work done on the system be ##W_{net} = W_{app} + W_{g}## , which is the sum of all the works done by both external and internal forces?
 
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NoahCygnus said:
Why didn't the author include the work done due to gravity in the net work?
The effect of gravity is already included via the potential energy.

Alternatively, you can ignore the concept of potential energy and include the work done by gravity explicitly.

When you use potential energy, one really should use a term like "net non-conservative work" (##W_{\rm{nc}}##) instead of "net work", in order to avoid confusions like this.
 
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jtbell said:
The effect of gravity is already included via the potential energy.

Alternatively, you can ignore the concept of potential energy and include the work done by gravity explicitly.

When you use potential energy, one really should use a term like "net non-conservative work" (##W_{\rm{nc}}##) instead of "net work", in order to avoid confusions like this.
Got it. One more question, work done on a system is the change in its energy, and according to work-kinetic energy theorem, net work done by all the forces , both conservative and non conservative, external or internal is equal to change in kinetic energy. In the above situation we see there is no change in kinetic energy, so net work done on the system is 0. But there is a change in potential energy, due to the work done by gravity ,even though the net work done is 0. Does that mean work-kinetic energy theorem is not a general statement and does not account for changes in the other types of energy by the individual work done by the forces?
 
Correct, the more general version is ##\Delta E = W_{\rm{nc}}## where:

  • ##\Delta E## is the change in the object's mechanical energy (kinetic + potential): ##\Delta E = \Delta K + \Delta U##
  • ##W_{\rm{nc}}## is the net work done by non-conservative forces (forces that don't have potential energy associated with them)
 
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jtbell said:
Correct, the more general version is ##\Delta E = W_{\rm{nc}}## where:

  • ##\Delta E## is the change in the object's mechanical energy (kinetic + potential): ##\Delta E = \Delta K + \Delta U##
  • ##W_{\rm{nc}}## is the net work done by non-conservative forces (forces that don't have potential energy associated with them)
So in a system, the net work done by all the forces may be zero, but there can still be changes in the other forms of energy except the kinetic energy?
 
NoahCygnus said:
but there can still be changes in the other forms of energy except the kinetic energy?
Yes, if you have more than one form of potential energy. Consider a mass hanging on a spring.
 
jtbell said:
Yes, if you have more than one form of potential energy. Consider a mass hanging on a spring.
But it can be internal energy too, as in case of a block that we push on a table having friction with a constant speed, the net work done is zero, as suggested by work kinetic energy theorem, but still there is a change in internal energy caused by the work done by the frictional force, am I correct?
 
Sure, in that case you have to consider the internal energy of both the block and the surface it's sliding on. They both warm up, right?

I think this is getting beyond the scope of the usual work-energy theorem. It's normally applied in situations where we can ignore the effects of the object's internal structure. This situation is sliding (:-p) over towards thermodynamics.
 
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jtbell said:
Sure, in that case you have to consider the internal energy of both the block and the surface it's sliding on. They both warm up, right?

I think this is getting beyond the scope of the usual work-energy theorem. It's normally applied in situations where we can ignore the effects of the object's internal structure. This situation is sliding (:-p) over towards thermodynamics.
You have been a big help. Finally I can rest. Thank you very much.
 

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