Understanding the Difference Between pdV and Vdp

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SUMMARY

The discussion centers on the differences between pdV and Vdp in thermodynamic expressions, particularly in the context of the grand potential G. It establishes that while pdV represents the work done by or on a gas, Vdp is related to changes in internal energy at constant volume. The relationship dG = -pdV - Vdp is highlighted, showing that Vdp can be expressed as Vdp = SdT + Ndu, where S is entropy and u is the chemical potential. The conversation emphasizes the convenience of using specific forms of these equations in thermodynamic calculations.

PREREQUISITES
  • Understanding of thermodynamic principles, specifically the first law of thermodynamics.
  • Familiarity with the concepts of grand potential and state functions.
  • Knowledge of differential forms in thermodynamics, including dU, dQ, and dW.
  • Basic understanding of the relationships between heat capacities (Cp and Cv) and their implications in thermodynamic equations.
NEXT STEPS
  • Explore the derivation and applications of the grand potential in statistical mechanics.
  • Study the implications of state functions in thermodynamic systems, focusing on pressure and volume relationships.
  • Investigate the role of chemical potential in thermodynamic equations and its impact on system behavior.
  • Learn about the Euler equation and its significance in deriving thermodynamic identities.
USEFUL FOR

This discussion is beneficial for students and professionals in thermodynamics, particularly those studying physical chemistry, chemical engineering, and related fields. It provides insights for anyone looking to deepen their understanding of thermodynamic potentials and their applications in various systems.

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Homework Statement


The books often always present pdV but never Vdp. Why is that? surely it is present in expressions like dE or dG where G is the grand potential. Is it because we don't treat p as a variable? If so why not? For each of these function we can only have 3 variables? So having V and p both as variables would be a bit redundant? If so why?
 
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In a grand canonical ensemble is pressure constant for any system? Hence dp=0? The grand potential doesn't appear to have dp in it.
 
Is it also because P is a state function so dP can always be expressed as other variables just like dU can. However temperture is also a state function? but it is treated as a variable.
 
pivoxa15 said:

Homework Statement


The books often always present pdV but never Vdp. Why is that?
They mention VdP. VdP is related to the change in internal energy of the gas at constant volume. PdV is the work done by/on the gas. Together, VdP + PdV = nRdT. Since nCvdT is the heat flow at constant volume and nCpdT is the heat flow at constant pressure, and Cp-Cv = R, VdP + PdV = nRdT = n(Cp-Cv)dT

AM
 
Why don't they have Vdp in the expression of the grand potential?

G = grand potential = -pV

So dG = -pdV - Vdp = -SdT -pdV - Ndu

So -Vdp = -SdT - Ndu?

or Vdp = SdT + Ndu which must be true by definition would it? It's more convineint to use the right hand side instead of the left hand side?
 
pivoxa15 said:
Why don't they have Vdp in the expression of the grand potential?

G = grand potential = -pV

So dG = -pdV - Vdp = -SdT -pdV - Ndu

So -Vdp = -SdT - Ndu?

or Vdp = SdT + Ndu which must be true by definition would it? It's more convineint to use the right hand side instead of the left hand side?
Careful.

dQ = TdS
dU = nCvdT
dW = PdV

So the first law dQ = dU + dW can be written:

(1) TdS = nCvdT + PdV

Since d(PV) = VdP + PdV = d(nRT) = nRdT,

PdV = nRdT - VdP

So substituting this for PdV in (1):

(2) TdS = nCvdT + nRdT - VdP

(3) VdP = nCvdT + nRdT - TdS = nCpdT - TdS = nCpdT - dQ


So the first law can be written:

(4) dQ = nCpdT - VdP

AM
 
You haven't disproved Vdp = SdT + Ndu have you?
 
pivoxa15 said:
You haven't disproved Vdp = SdT + Ndu have you?
I am not sure what you mean by Ndu. I think it refers to added molecules.

From the Euler equation:

U = TS - PV

dU = d(TS) - d(PV) = (TdS + SdT) - (VdP + Pdv)

But the first law states that dU = dQ - PdV. Since dQ = TdS:

dU = TdS - PdV so

SdT - VdP = 0

AM
 
u stands for the chemical potential constant. If you have dU=dQ-Pdv you have not accounted for the chemical potential of particles entering and leaving the system. If you did then dU=TdS-pdV+udN. So

We have
U = TS - PV + uN

dU = d(TS) - d(PV) + d(uN)= (TdS + SdT) - (VdP + Pdv) + (Ndu + udN)

We have
dU=TdS-pdV+udN

So SdT - Vdp + Ndu = 0
hence Vdp = SdT + Ndu

Although why is U = TS - PV + uN?

Or even why is U = TS - PV when not accounting for chemical potential?

Is it more the fact that we first know the expressions for dU then work out U from those expressions?
 

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