Title: Simple Mixtures
1Chapter 7
2Partial Molar Volume
- The partial molar volume of a substance A in a
mixture is the change in volume per mole of A
added to a large volume of the mixture. - The partial molar volumes of the components of a
mixture vary with composition because the
environment of each type of molecule changes from
pure A to pure B. - This changing molecular environment, and the
consequential modification of the forces acting
between molecules, results in the variation of
the thermodynamic properties of a mixture as its
composition is changed.
3One way to measure partial molar volume is to
measure the dependence of the volume on the
composition and to fit the observed volume to a
function of the amount of substance by using a
curve fitting program. The slope of the function
can then be found by diffentiation.
Molar volumes can also be negative!
4Partial Molar Gibbs Energies
- For a pure substance, m G.
- For a substance in a mixture, the chemical
potential is the partial molar Gibbs Energy.
5Wider Significance of m
6Gibbs-Duhem Equation
The chemical potential of one component of a
mixture cannot change independently of the
chemical potentials of the other components In
a binary mixture, if one increases, the other
must decrease.
7Thermodynamics of Mixing
8Chemical Potentials of Liquids
- At equilibrium, the chemical potential of a
substance as a vapour must be equal to its
chemical potential in the liquid. - If a solute is present in the liquid
Raoults Law (after a series of experiments)
When components are structurally similar, they
follow Raoults Law
Mixtures that obey this law are ideal
9Raoults Law
- The rate at which A molecules leave the surface
is ? of them at the surface. - Rate of vaporization kxA
- The rate at which molecules condense ?
concentration in the gas phase which is ? to the
partial pressure. - Rate of condensation kpA
- At equilibrium they are equal.
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11Ideal-Dilute Solutions
- In ideal solutions, the solute and solvent obey
Raoults Law. - In a dilute solution the solvent molecules are in
an environment very much like the one they have
in the pure liquid. - In contrast, the solute molecules are surrounded
by solvent molecules, which is entirely
different. - Therefore, the solvent behaves like a pure liquid
and the solute behaves differently obeying
Henrys Law - For real solutions at low concentrations, Henrys
Law applies - pB xBKB where KB is an empirical constant.
12Liquid Mixtures
These are valid for ideal liquids. Gas perfection
/ solution ideality Perfect gas no interaction
between molecules and DH 0, driving force for
mixing is DS gt 0. Ideal solution A-B
interaction in mixture is the same as A-A and B-B
interaction. Real solutions These interactions
are very different. There may be an enthalpy
change in mixing and also and increased order,
decreasing entropy and DG gt 0. Then these liquids
do not mix or partially mix, meaning they are
miscible only over a certain range of composition.
13Excess Functions
- Excess functions, XE, is the difference between
the observed thermodynamic function of mixing and
the function for an ideal solution. (e.g.
SEDmixS - DmixSideal) - This indicates the extent to which solutions are
nonideal. - Regular solution is a solution for which HE 0
but SE 0.
14Colligative Properties
- Boiling-point elevation
- Freezing-point depression
- Osmotic pressure
- These properties depend only on the number of
solute particles present, not their identity. - Assumption 1 Solution is dilute.
- Assumption 2 Solute is not volatile
- Assumption 3 Solute does not dissolve in the
solid solvent. - All colligative properties stem from the
reduction of chemical potential of the liquid
solvent as a result of the presence of solute.
(mA to mA RT lnxA)
15Elevation of Boiling Point
Depression of Freezing Point
16Osmosis
Osmosis is the spontaneous passage of a pure
solvent into a solution separated from it by a
semi-permeable membrane. The osmotic pressure, P,
is the pressure that must be applied to the
solution to stop the influx of solvent. Osmometry
is the determination of molecular mass by the
measurement of osmotic pressure.
pP
p
mA(p)
mA(pP)
Equal at eq.
17 Vant Hoff equation
18Activities
- Deviations from ideal behaviour can be taken into
account by introducing activity.
19Solute Activity
20Activities in terms of Molalities
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