Results for the exercise
For the work in the exercise 6.2 I found that the work differential for an ideal fas in a powe-potential tramp was:
We can use this to get the work differential for an ideal gas in a 3D container by subtitude d=3 thatis the dimensions, obtaining:
Seeing this we can say that the parameter a is going to represent the volume:
know, if we take the limit when n goes to infinity, we can write:
That applying the limit is:
or that is also equal to:
That is the work differential for an ideal gas in a 3D container, which relates to the equation mentioned in the exercise as it was for a 1D container.
We can use this to get the work differential for an ideal gas in a 3D container by subtitude d=3 thatis the dimensions, obtaining:
Seeing this we can say that the parameter a is going to represent the volume:
know, if we take the limit when n goes to infinity, we can write:
or that is also equal to:
That is the work differential for an ideal gas in a 3D container, which relates to the equation mentioned in the exercise as it was for a 1D container.






You should remember that this is not the work differential for an ideal gas.
ResponderBorrarI am starting to get worried about how little many of you seem to remember from their thermodynamics course and from previous exercises about the ideal gas :-)