Title: Real Gases
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2Real Gases
- Under some conditions, real gases do not follow
the ideal gas law. - Intermolecular forces of attraction cause the
measured pressure of a real gas to be less than
expected. - When molecules are close together, the volume of
the molecules themselves becomes a significant
fraction of the total volume of a gas.
3Real Gases
- Ideal gas equation (ideal gases)
- P (V ) nRT
- van der Waals equation (real gases)
- P (n2a)/V2 (V - nb) nRT
- a term is related to intermolecular force
strength. - b term is related to volume of the gas
molecules (in liters per mole). - Both a and b are empirical constants, determined
by experiment.
4van der Waals ConstantsFor Selected Gases
Force of attraction
Molecular volume
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8Volume of 1 mole of Gas at STP
9Ionic Bonds AsIntermolecular Forces
- There are no molecules in an ionic solid, and
therefore there cant be any intermolecular
forces. - There are simply inter-ionic attractions.
- Lattice energy is a measure of the strength of
inter-ionic attraction. - The attractive force between a pair of oppositely
charged ions increases as the charges on the ions
increase and as the ionic radii decrease. Lattice
energies increase accordingly.
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11Interionic Forces of Attraction
129.3
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14Ion-Dipole Forces in Dissolution
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16Hydrogen Bonds
- A hydrogen bond is an intermolecular force in
which a hydrogen atom covalently bonded to a
non-metal atom in one molecule is simultaneously
attracted to a non-metal atom of a neighboring
molecule. - The strongest hydrogen bonds are formed if the
non-metal atoms are small and highly
electronegative. - Usually occurs with nitrogen, oxygen, and
fluorine atoms. - Dotted lines are used to represent hydrogen bonds.
17Hydrogen Bonds in Water
18Intermolecular Hydrogen Bonds
19Intramolecular Hydrogen Bonds
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23Dispersion Forces
- A dispersion force is the force of attraction
between an instantaneous dipole and an induced
dipole. - Also called a London force after Fritz London who
offered a theoretical explanation of these forces
in 1928. - The polarizability of an atom or molecule is a
measure of the ease with which electron charge
density is distorted by an external electrical
field. - The greater the polarizability of molecules, the
stronger the intermolecular forces between them.
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26Volume of 1 mole of Gas at STP
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28Molecular Shapeand Polarizability
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32Predicting Physical Properties of Molecular
Substances
- Dispersion forces become stronger with increasing
molar mass and elongation of molecules. In
comparing nonpolar substances, molar mass and
molecular shape are the essential factors. - Dipole-dipole and dipole-induced dipole forces
are found in polar substances. The more polar the
substance, the greater the intermolecular force
is expected to be. - Because they occur in all molecular substances,
dispersion forces must always be considered.
Often they predominate.
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37Liquid-Vapor Equilibrium
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39Vapor Pressure Of Water
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41Vapor Pressure Curves
- Carbon disulfide CS2
- Methanol CH3OH
- Ethanol CH3CH2OH
- Water H2O
- Aniline C6H5NH2
- The temperature of the line P 760 mmHg with a
vapor pressure curve is the normal boiling point.
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44super-saturated
saturated (equilibrium)
unsaturated
45Equilibrium Vapor Pressure (mm Hg) T(oC) P T(oC
) P T(oC) P T(oC) P 0 4.58 21 18.65
35 42.2 92 567.0 5 6.54 22 19.83
40 55.3 94 610.9 10 9.21 23 21.07
45 71.9 96 657.6 12 10.52 24 22.38
50 92.5 98 707.3 14 11.99 25 23.76
55 118.0 100 760.0 16 13.63
26 25.21 60 149.4 102 815.9 17 14.53
27 26.74 65 187.5 104 875.1
18 15.48 28 28.35 70 233.7 106 937.9
19 16.48 29 30.04 80 355.1
108 1004.4 20 17.54 30 31.82
90 525.8 110 1074.6
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49Vaporization and Condensation
- Vaporization is the conversion of a liquid to a
gas. - The enthalpy of vaporization (DHvapn) is the
quantity of heat that must be absorbed to
vaporize a given amount of liquid at a constant
temperature. - Condensation (DHcondn) is the change of a gas to
a liquid. - Because enthalpy is a function of state, the
total enthalpy change between vaporization and
re-condensation at constant temperature must be
zero. - DHvapn DHcondn 0
- DHcondn - DHvapn
50Some Enthalpies of Vaporization
51Clausius-Clapeyron Equation ln(P) -?Hvap/RT
C ln(P1/P2) (?Hvap/R)(1/T2 - 1/T1)
Dependent on substance
atm
K
kJ/mol
0.0083143 kJ/molK
52ln(P) -?Hvap/RT C
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58Phase Changes Involving Solids
- The conversion of a solid to a liquid is called
melting, or fusion, and the temperature at which
a solid melts is its melting point. - The enthalpy of fusion, DHfusion, is the quantity
of heat required to melt a given amount of solid. - Sublimation is the process of a molecules passing
directly from the solid to the vapor state. - Enthalpy of sublimation, DHsubln, is the sum of
the enthalpies of fusion and vaporization. - The triple point is the point at which the vapor
pressure curve and the sublimation curve meet.
59Some Enthalpies of Fusion
60Generalized Phase Diagram
61Phase Diagram For H2O
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67Freeze Dried Coffee
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71Phase Diagram for Water
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75Specific Heats of Water
ice (-3oC) 2.092 J/gK ?ice
liquid(14.5oC) 4.184 J/gK ?liq
steam(100oC) 1.841 J/gK ?gas
76Specific Heat Capacities Table
77- Properties of Water
- Density 0.99987 g/ml _at_ 0oC Heat of
Fusion 6.008 kJ/mol _at_ 0oC - 1.00000 g/ml _at_ 4oC Heat of Vaporization 44.94
kJ/mol _at_ 0oC - 0.99707 g/ml _at_ 25oC 44.02 kJ/mol _at_ 25oC
- 0.95838 g/ml _at_ 100oC 40.67 kJ/mol _at_ 100oC
- Ion-Product, Kw 1.14 x 10-15 _at_ 0oC
Specific Heat ice (-3oC) 2.092 J/gK - 1.01 x 10-14 _at_ 25oC
liquid(14.5oC) 4.184 J/gK - 5.47 x 10-14 _at_ 50oC
steam(100oC) 1.841 J/gK - Equilibrium Vapor Pressure (mm Hg)
- T(oC) P T(oC) P T(oC) P T(oC) P
- 0 4.58 21 18.65 35 42.2 92 567.0
- 5 6.54 22 19.83 40 55.3 94 610.9
- 10 9.21 23 21.07 45 71.9 96 657.6
- 12 10.52 24 22.38 50 92.5 98 707.3
- 14 11.99 25 23.76 55 118.0 100 760.0
- 16 13.63 26 25.21 60 149.4 102 815.9
- 17 14.53 27 26.74 65 187.5 104 875.1
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80Surface Tension
- Surface tension (g) is the amount of work
required to extend a liquid surface and is
usually expressed in J / m2. - Adhesive forces are intermolecular forces between
unlike molecules. - Cohesive forces are intermolecular forces between
like molecules. - A meniscus is the interface between a liquid and
the air above it. - Viscosity is a measure of a liquids resistance
to flow. - Liquids which flow easily are said to mobile.
81Intermolecular Forces in a Liquid
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84Adhesive and Cohesive Forces
85Meniscus Formation
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87Capillary Action
88Measuring Viscosity
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