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

Physical Chemistry I: Phase Equilibrium at The Richard Stockton College of New Jersey, Study notes of Physical Chemistry

A lecture note from the richard stockton college of new jersey's chemistry program, school of natural sciences and mathematics, for the course chem 3410: physical chemistry i, fall 2008. The lecture focuses on phase equilibrium, discussing key concepts such as minimized free energy, chemical potential, and molar entropy and volume of different phases. The document also introduces the concept of phase diagrams and their significance in understanding the temperature and pressure dependence of phase stability.

Typology: Study notes

Pre 2010

Uploaded on 08/08/2009

koofers-user-hzp-1
koofers-user-hzp-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 17, 2008
Lecture 20: Phase equilibrium
References
1. Levine, Physical Chemistry, Sections 7.1–7.3
Key Concepts
At equilibrium, the free energy is minimized. Therefore, the phase with the lowest chemical potential
will be stable.
For a single component system, µ=G
n=G.
The key question is how µdepends on Tand P. We can find this dependence by writing (dG for a
single component system) out in two different ways:
dG = =SdT +V dP
=∂µ
∂T P
dT +∂µ
∂P T
dP
which gives us:
∂µ
∂T P
=Sand ∂µ
∂P T
=V
We can now see how µvaries with Tand Pby comparing the molar entropy and volume of different
phases.
The molar entropy of a gas phase is much greater than the molar entropy of a solid or liquid phase.
This is due to the large number of different ways to arrange molecules in the gas phase (i.e. the vast
number of configurations leads to high entropy. Using a similar argument, the molar entropy of the
solid phase will be the smallest since there are a much more limited number of possible configurations,
leading to a low entropy phase.
So, in a plot of µversus T, a curve for the gas phase will have the steepest negative slope, while a solid
phase will have a much shallower negative slope.
If we polt µversus Tat a fixed pressure, the most stable phase at a particular temperature is the
phase with the lowest µ. If the chemical potential of two phases is equal, the two phase coexist at that
temperature and pressure, i.e. they are in equilibrium.
To determine the effect of pressure on the stability of phases, we need to examine the differences the
molar volume (V) of each phase. Gases typically have the largest molar volumes, so changing the
pressure would have a large impact on the chemical potential of a gas phase, while it is a much smaller
impact when dealing with a condensed phase, such as a liquid or solid.
If we want to capture both the temperature and pressure dependence of the stability of phases we can
plot Pversus Tand generate a phase diagram for the single component system. The phase diagram
is a map that indicates which phase(s) is(are) most stable under particular Tand Pconditions.
When we construct these single-component or unary phase diagrams, we will see regions when single
phases are stable, lines where two phases are in equilibrium, and one single point (the triple point)
where all three phases are in equilibrium.

Partial preview of the text

Download Physical Chemistry I: Phase Equilibrium at The Richard Stockton College of New Jersey 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 17, 2008

Lecture 20: Phase equilibrium

References

  1. Levine, Physical Chemistry, Sections 7.1–7.

Key Concepts

  • At equilibrium, the free energy is minimized. Therefore, the phase with the lowest chemical potential will be stable.
  • For a single component system, μ = Gn = G.
  • The key question is how μ depends on T and P. We can find this dependence by writing dμ (dG for a single component system) out in two different ways:

dG = dμ = −SdT + V dP

dμ =

∂μ ∂T

P

dT +

∂μ ∂P

T

dP

which gives us: (^) ( ∂μ ∂T

P

= −S and

∂μ ∂P

T

= V

  • We can now see how μ varies with T and P by comparing the molar entropy and volume of different phases.
  • The molar entropy of a gas phase is much greater than the molar entropy of a solid or liquid phase. This is due to the large number of different ways to arrange molecules in the gas phase (i.e. the vast number of configurations leads to high entropy. Using a similar argument, the molar entropy of the solid phase will be the smallest since there are a much more limited number of possible configurations, leading to a low entropy phase.
  • So, in a plot of μ versus T , a curve for the gas phase will have the steepest negative slope, while a solid phase will have a much shallower negative slope.
  • If we polt μ versus T at a fixed pressure, the most stable phase at a particular temperature is the phase with the lowest μ. If the chemical potential of two phases is equal, the two phase coexist at that temperature and pressure, i.e. they are in equilibrium.
  • To determine the effect of pressure on the stability of phases, we need to examine the differences the molar volume (V ) of each phase. Gases typically have the largest molar volumes, so changing the pressure would have a large impact on the chemical potential of a gas phase, while it is a much smaller impact when dealing with a condensed phase, such as a liquid or solid.
  • If we want to capture both the temperature and pressure dependence of the stability of phases we can plot P versus T and generate a phase diagram for the single component system. The phase diagram is a map that indicates which phase(s) is(are) most stable under particular T and P conditions.
  • When we construct these single-component or unary phase diagrams, we will see regions when single phases are stable, lines where two phases are in equilibrium, and one single point (the triple point) where all three phases are in equilibrium.