Why U is a State Function if W(adiabatic) Does Not Depend on State?

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Discussion Overview

The discussion centers on the nature of state functions in thermodynamics, specifically addressing why internal energy (U) is considered a state function while work (W) is not, particularly in the context of adiabatic processes. Participants explore the implications of these definitions and the mathematical underpinnings of state functions.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants assert that while internal energy is a state function, work is not, leading to questions about the relationship between them during adiabatic processes.
  • Others propose that both heat (q) and work (w) are not state functions but rather depend on the process, prompting requests for mathematical explanations.
  • A participant introduces the concept of exact and inexact differentials to explain why the change in internal energy (dE) is an exact differential, while q and w are inexact, suggesting that their sum is what makes dE a state function.
  • Some argue that during an adiabatic process, since w equals U, it raises the question of whether work can be considered a state function in that specific context.
  • Another participant clarifies that the change in a state function does not depend on the path taken, using examples of different processes that yield the same change in internal energy but different values for q and w.
  • There is a suggestion that if one restricts to adiabatic paths, work could be expressed as a function of thermodynamic variables, but this does not imply that work itself is a state function.
  • One participant emphasizes that state functions can be measured independently of the process history, which is not the case for work.

Areas of Agreement / Disagreement

Participants generally disagree on whether work can be considered a state function in the context of adiabatic processes, with some asserting it cannot while others suggest it might under specific conditions. The discussion remains unresolved regarding the implications of work in these scenarios.

Contextual Notes

Participants express uncertainty about the definitions and implications of state functions, particularly in relation to different thermodynamic processes. There are unresolved questions about the mathematical treatment of work and heat in these contexts.

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if work is not a state function and internal energy is a state function,
then why does w(adiabatic)=U is a state function?
 
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well i think that in [tex]\Delta U = q+w[/tex] q and w are not state functions but processes, so you can ask the same question here i guess. although I am not sure how this can be, somebody please give a mathematical explanation?
 
The answer here might lie in the difference between exact and inexact differentials. An exact differential is the differential of a scalar function, call it F. For a function of two variables x and y, we have:
[tex]dF = P(x,y)dx + Q(x,y)dy[/tex]
By the commutation of second order partial derivatives, we find that if
[tex]\frac{\partial P}{\partial y} = \frac{\partial Q}{\partial x}[/tex]
then the quantity
[tex]Pdx + Qdy[/tex]
is an exact differential.
Now, say that x and y are also functions of some variables s and t. It may be true that dx = Ads + Bdt is not an exact differential. Likewise, dy = Cds + Ddt may also be inexact. However, if we add them together we can get an expression
[tex]Pdx + Qdy[/tex]
that is exact (that is, Pdx + Qdy = dF).

This is what's going on when one discusses the first law of thermodynamics:
[tex]dE = dQ + dW[/tex]
dE is an exact differential. dQ and dW are inexact, but their sum is exact. By the way, exact differentials are related to path independence in terms of integration. When you have more than two variables you are integrating over, there is a notion of "path". But because an exact differential can be reduced to the differential of a scalar function (ie just one variable now) there are no longer multiple paths--that is, all paths are equivalent.

Hope this helps!
 
thanks~
but during an adiabatic process, w=U, so how are you supposed to know whether w and U are or aren't state functions?
 
Because the change in a state function does not depend on the path taken. Suppose the adiabatic process was running an electric current through a resistor in a gas. Taking as the system the gas with the resistor in it, the only energy transfer is the electric work across the boundary, so the process is adiabatic. The temperature and pressure of the gas increase, but the volume remains the same. In this case [itex]\Delta U = w[/itex]. Now suppose that instead of having a current flow through it, the system is just heated the same final temperature and no work is done. In this case [itex]\Delta U = q[/itex]. In both cases [itex]\Delta U[/itex] is the same, but q and w are different depending on which path is taken. This is the difference: state functions do not depend on the path taken.
 
but is kinda seems like in an adiabatic function, work will then become a state function too...
 
No, work is not a state function, only U is. As said above:

U = Q + W

You can get the same value for U for many different combinations of Q and W. In this special case, Q = 0 so U = W.
 
Are state functions defined for entire thermodynamics or for certain processes? If last then it's possible to say that in adiabatic process work is state function.
 
This is what a state function means: I can walk into a room and look at a system and take measurements of things like temperature, pressure, volume, etc. I can then leave and come back later, having no idea what happened while I was gone, but just by taking measurements of the current state of the system I can tell how much any state function changed between the time I left and the time I came back. I can't do this with work because I don't know whether the process was adiabtic or not. Doing work can raise the temperature of a system. So can heating it. It is impossible for me to tell which it was by measuring the T, P, V... at the beginning and end of a process.
 
  • #10
so in a adiabatic process, work isn't a state function?
 
  • #11
Yes, if you are restrict yourself to adiabatic paths, then the work form can be written as the dw, where w is a function of thermodynamic variables.

This means the work done will only depend on the endpoints of the path -- as long as we are only considering paths along which dq = 0.
 
  • #12
i see... thanks! :)
 

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