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Simple Mixtures Continued

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Since there is no interaction between molecules in a perfect gas, DHMIX=0. ... 946. 756. 363. 205. P/Torr. 0.0024. 0.0019. 0.009. 0.005. x. Problem 7.15b(a) ... – PowerPoint PPT presentation

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Title: Simple Mixtures Continued


1
Simple Mixtures Continued
2
Gibbs Energy of Mixing of Perfect Gases
  • Recall, mmolar Gibbs Energy

3
Entropy and Enthalpy of Mixing
  • Mole fractions are always lt0. Therefore, DSMIX
    is always gt0.
  • Since there is no interaction between molecules
    in a perfect gas, DHMIX0.

4
Note the form of the Curves
5
Problem 7.13b
6
Chemical Potentials of Ideal Solutions
  • When A(l) is in equilibrium with A(g) at a
    partial pressure PA, then
  • Recall, mA for a vapor is
  • Therefore, at equilibrium

7
Chemical Potentials of Ideal Solutions
  • Raoults Law
  • Measured the partial vapor pressure of each
    component in a mixture
  • Discovered that the partial pressure of the
    solvent of a solution was lower than the pressure
    of the pure solvent

8
Chemical Potentials of Ideal Solutions
  • Using Raoults Law, substitute for PA

Constants for a given substance at a given
temperature
9
Problem 7.9b
10
Ideal Binary Solutions
  • Raoults Law applies to each component (A and B)
  • The total pressure of the system follows Daltons
    Law

11
Ideal-Dilute Solutions
  • A solute lowers the chemical potential of a
    solvent
  • increases the disorder of the solvent
  • The disorder of a solvent of a solution is higher
    but it has a lower tendency to achieve disorder
    than the pure solvent.
  • this reduction in potential is m lower than m.

12
Ideal-Dilute Solutions
  • Raoults Law describes properties of an almost
    pure solvent in a real solution.
  • Raoults Law does not work well in describing the
    partial vapor pressure of the solute.
  • Since it its the minor component, the solute is
    far from its pure state
  • However, it is known that the partial vapor
    pressure of the solute is proportional to the
    mole fraction of the solute.
  • The slope of this line is different that what
    Raoults Law describes

13
Henrys Law
  • The vapor pressure of a volatile solute (b), is
    equal to its mole fraction in solution times a
    constant characteristic of the solute
  • KB is the pressure at xB1 determined by a line
    that is tangential to the point at xB0

14
Limitations
Limitations
  • Raoults and Henrys Laws are valid only at low
    concentrations of solute and solvent,
    respectively.

15
Problem
  • Estimate Henrys Law constant for methylene
    chloride given the following data

16
Problem 7.15b(a)
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