Docsity
Docsity

Prepare for your exams
Prepare for your exams

Study with the several resources on Docsity


Earn points to download
Earn points to download

Earn points by helping other students or get them with a premium plan


Guidelines and tips
Guidelines and tips

Chemical Potential of an Ideal Gas - Lecture Notes | CHEM 3410, Study notes of Physical Chemistry

Material Type: Notes; Professor: Richard; Class: PHYSICAL CHEMISTRY I; Subject: Chemistry; University: The Richard Stockton College of New Jersey; Term: Fall 2008;

Typology: Study notes

Pre 2010

Uploaded on 08/08/2009

koofers-user-lc5-1
koofers-user-lc5-1 🇺🇸

5

(1)

10 documents

1 / 1

Toggle sidebar

This page cannot be seen from the preview

Don't miss anything!

bg1
The Richard Stockton College of New Jersey
Chemistry Program, School of Natural Sciences and Mathematics
PO Box 195, Pomoma, NJ
CHEM 3410: Physical Chemistry I Fall 2008
October 6, 2008
Lecture 15: Chemical potential of an ideal gas
References
1. Levine, Physical Chemistry, Sections 4.6–4.8, 6.1–6.2
Key Concepts
For a single component system consisting of an ideal gas, we were able to arrive at an expression for
the chemical potential by integrating our expression for dG for a single component system at constant
temperature (dG =V dP ) between some reference pressure Pand the pressure of interest P:
µ(T, P ) = µ(T) + RT ln P
P
where µ(T) is the chemical potential of the pure gas in the reference state (usually P= 1 bar)
We can now arrive at expressions for related quantities such as S, since we know that S=∂G
∂T P,n = µ
∂T P,n
(where the bar above the quantity means per mole, or the molar entropy).
For an ideal gas in a mixture, we have to account for the actual amount of each gas in the system using
the mole fraction and/or partial pressure. These two quantities are related. For component A, if we
denote the partial pressures as PAand the mole fraction as XA, then we can write the following:
PA=XAPT OT AL
By doing some more integrating from a starting state of the pure gas at the reference pressure, to
the partial pressure of the gas in the mixture, we arrived at the following expression for the chemical
potential of a gas (i) in a mixture of gases:
µmixture
i(T, P ) = µpure
i(T, P ) + RT ln XA
item The mixing of ideal gases is completely driven by entropy. There is no interaction between gas
atoms/molecules in an ideal gas, therefore Hmix = 0.Going from the unmixed to mixed state results
in an increase in entropy (∆Smix >0) meaning that Gmix <0 (∆G= HTS).
Based on our expression for the chemical potential of an ideal gas in a mixture, we were able to arrive
at an expression for the free energy of mixing of ideal gases. In general for a system of igases and
then for a two-compoennt system (A & B) we wrote:
Gmix =RT XXiln Xi
Gmix =RT (XAln XA+XBln XB)
Related Exercises in Levine
Exercises: 4.40, 6.1

Partial preview of the text

Download Chemical Potential of an Ideal Gas - Lecture Notes | CHEM 3410 and more Study notes Physical Chemistry in PDF only on Docsity!

The Richard Stockton College of New Jersey

Chemistry Program, School of Natural Sciences and Mathematics PO Box 195, Pomoma, NJ

CHEM 3410: Physical Chemistry I — Fall 2008

October 6, 2008

Lecture 15: Chemical potential of an ideal gas

References

  1. Levine, Physical Chemistry, Sections 4.6–4.8, 6.1–6.

Key Concepts

  • For a single component system consisting of an ideal gas, we were able to arrive at an expression for the chemical potential by integrating our expression for dG for a single component system at constant temperature (dG = V dP ) between some reference pressure P ◦^ and the pressure of interest P :

μ(T, P ) = μ◦(T ) + RT ln

P

P ◦

where μ◦(T ) is the chemical potential of the pure gas in the reference state (usually P = 1 bar)

  • We can now arrive at expressions for related quantities such as S, since we know that −S =

∂G ∂T

P,n

∂μ ∂T

P,n (where the bar above the quantity means per mole, or the molar entropy).

  • For an ideal gas in a mixture, we have to account for the actual amount of each gas in the system using the mole fraction and/or partial pressure. These two quantities are related. For component A, if we denote the partial pressures as PA and the mole fraction as XA, then we can write the following:

PA = XAPT OT AL

  • By doing some more integrating from a starting state of the pure gas at the reference pressure, to the partial pressure of the gas in the mixture, we arrived at the following expression for the chemical potential of a gas (i) in a mixture of gases:

μmixturei (T, P ) = μpurei (T, P ) + RT ln XA

item The mixing of ideal gases is completely driven by entropy. There is no interaction between gas atoms/molecules in an ideal gas, therefore ∆Hmix = 0. Going from the unmixed to mixed state results in an increase in entropy (∆Smix > 0) meaning that ∆Gmix < 0 (∆G = ∆H − T ∆S).

  • Based on our expression for the chemical potential of an ideal gas in a mixture, we were able to arrive at an expression for the free energy of mixing of ideal gases. In general for a system of i gases and then for a two-compoennt system (A & B) we wrote:

∆Gmix = RT

Xi ln Xi

∆Gmix = RT (XA ln XA + XB ln XB )

Related Exercises in Levine

Exercises: 4.40, 6.