Difference between W=-(ΔU) and negative U.

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Discussion Overview

The discussion centers on the relationship between the equation W=-ΔU and the concept of potential energy being negative when the reference point is set at infinity. Participants explore whether these two statements convey the same message or if they are distinct concepts within the context of gravitational potential energy and work-energy principles.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Technical explanation

Main Points Raised

  • Some participants question whether W=-ΔU and the statement about potential energy being negative at infinity convey the same meaning.
  • Others argue that the statement about potential energy being negative is not universally true, as some systems can have positive potential energy even with the reference point at infinity.
  • It is noted that the sign in W=-ΔU is a convention, with some participants emphasizing that positive work is defined as work done by the system.
  • Some participants assert that W=-ΔU is derived from the law of conservation of energy, particularly in the context of adiabatic processes, while others challenge the relevance of this derivation.
  • There is a distinction made between W=-ΔU referring to work done and ΔU representing the difference in potential energy between two states, with some suggesting that this applies only under specific conditions.
  • Participants discuss the implications of setting the reference point for potential energy and whether it can be positive or negative depending on the chosen reference.
  • Some participants mention that the equation W=-ΔU is independent of the reference point used for potential energy.
  • There is a suggestion that certain systems may allow for a reference point where potential energy is defined as positive without leading to infinite values.

Areas of Agreement / Disagreement

Participants express differing views on the relationship between W=-ΔU and the concept of potential energy at infinity. There is no consensus on whether these statements are equivalent, and multiple competing interpretations of potential energy and work exist throughout the discussion.

Contextual Notes

Some participants highlight that the discussion is not related to thermodynamic systems undergoing adiabatic processes, but rather focuses on gravitational potential energy. There are also mentions of varying conventions in definitions and interpretations of energy and work across different contexts.

donaldparida
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Is there any difference between the meaning of the equation W=-ΔU and the meaning of the statement that potential energy of system is always negative when the reference point(zero point) is taken to be located at infinity or do they both convey the same message?
 
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I see no link between the two statements.

Note also that the statement that "the potential energy of system is always negative when the reference point(zero point) is taken to be located at infinity" is not absolutely true. There are systems that can have positive potential energy even in that case.
 
I should also point out that the sign in W=-ΔU is also a convention, that positive work is work done by the system, not on the system. That convention is far from universal.
 
Doesn't W=-ΔU come from the law of conservation of energy?(when there is positive increase in K.E. there must be negative increase or simply decrease in the P.E. so that the total energy remains constant.)
 
donaldparida said:
Doesn't W=-ΔU come from the law of conservation of energy?(when there is positive increase in K.E. there must be negative increase or simply decrease in the P.E. so that the total energy remains constant.)
It comes from conservation of energy when dealing with adiabatic processes. But my point was about the sign in the equation, which is somewhat arbitrary.
 
There is a difference.
While W=-ΔU talks about the work done W is the difference between two states of the potential energy ΔU (if both end results are at rest is the only time it really applies, on other occasions it is W=-(ΔU+ΔE[kinetic]) ).
The other says that when you consider a two body system under the influence of a conservative force, that is there is potential energy, the reference point of infinity is taken as the point of 0 energy. However the statement is inaccurate because negative energy in such a case happens in a system with at least two bodies bound to one another.
 
##\Delta U## is the change in internal energy, not just potential energy. It includes kinetic energy.
 
Dale said:
##\Delta U## is the change in internal energy, not just potential energy. It includes kinetic energy.
For some reason our professors said otherwise. Guess either they mistook or convention is not the same in every place. Some people use j as the sqrt(-1) on single plane complex numbers, where as others use i for instance.
 
@donaldparida can you clarify the context? Is this for a thermodynamic system undergoing an adiabatic process, or something else?
 
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  • #10
No, this question is not related to a thermodynamic system undergoing adiabatic process. It is related to the gravitational potential energy of a system.
 
  • #11
Ah, please ignore my comments above. They were in the wrong context.

The equation has nothing whatsoever to do with setting the reference at infinity. In fact, it shows that any reference can be used since ##\Delta U## is independent of the reference.
 
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  • #12
Is it correct to say that if the reference point is set at infinity only then the potential energy is negative and if we select any other reference point, the potential energy is positive?
 
  • #13
if the reference point is set at infinity only then the potential energy is ALWAYS negative and if we select any other reference point, the potential energy is SOMETIMES positive
 
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  • #14
donaldparida said:
No, this question is not related to a thermodynamic system undergoing adiabatic process. It is related to the gravitational potential energy of a system.
Then ignore my comments. For me, W = -ΔU is a thermodynamical statement.

It is always useful to state the context of the question :smile:
 
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  • #15
@Dale , so in conclusion, the equation W=-ΔU (meaning that the work done is the negative of the change in potential energy) and the fact that the potential energy of a system when the reference point is taken at infinity is always negative have no relation with each other and the equation W=-ΔU comes from the work-energy theorem and the law of conservation of energy. Right? Also is there any reference point for which the potential energy of a system always comes out to be positive?
 
  • #16
donaldparida said:
in conclusion, the equation W=-ΔU (meaning that the work done is the negative of the change in potential energy) and the fact that the potential energy of a system when the reference point is taken at infinity is always negative have no relation with each other
Correct.
donaldparida said:
Also is there any reference point for which the potential energy of a system always comes out to be positive?
R=0, but in practice that is never used because it would be positive and infinite everywhere.
 
  • #17
Dale said:
R=0, but in practice that is never used because it would be positive and infinite everywhere.
For 1/r^2 forces yes.
 
  • #18
  • #19
In forces such as coulomb's law and Newton's formula for gravity, notice that r is in the denominator. r refers to the distance between the object and the source. In the case of these two forces, the two objects feel each other of course. If you try to find the limit of 1/r as r approaches 0, you will find the result gets bigger and bigger and diverges to infinity.
However do note, that is true for point objects, in reality if you know the force in every single location there are some physical systems where the force does not diverge when r=0, and again it depends on the problem. In certain systems you can define r=0 as the point of 0 potential energy and not have the result infinite everywhere.
Systems such as distributed charge in a sphere, or an object with its mass distributed in a certain configuration in space, would not necessarily yield infinity when r=0.
 

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