Title: Molecular interactions
1Molecular interactions
2Residual interaction
- Complete valence shells are still able to
interact with one another - Van der Waals
- Hydrogen bodning
3Interaction between partial charges
- Coulombs law
- V q1q2/4peor (in vacuum)
- Where qi the partial charge
- Where r the separation
- Where e permittivity of the medium
4frequency response of e
- frequency response of various dielectric
mechanisms in terms of the real and imaginary
parts of the permittivity. - Image used with the consent of Prof. Kenneth A.
Mauritz
5Polarizability, Relative Permittivity, Refractive
Index
Clausius-Mossotti equation
6- Permittivity e ereo
- Where er is relative permittivity
- Where eo is vacuum permittivity
- At room temperature, er is 78
7Electrical Dipole Moments
8Dipole moment
- µ qR
- Represent by an arrow (vector)
- Length magnitude of dipole moment
- Pointing (-) charge to () charge
- But the other way is still used
- Unit
- D (debye)
- 1 D 3.33564 x 10-30 Cm
- Electric chages e and e by 100 pm 4.8 D
9Polar vs. non-polar molecules
10Estimating µ
- Pauling electronegativities
- µ/D ??
- If an atom attracts the electrons more strongly,
the more electronegative atom is (-) of µ
11Dispersion of Refractive Index
12Total Dipole moments mol geometry
13Interactions between Dipoles
14a charge interacts with a dipole
- calculate all the interactions as if they were
merely a series of point charges. We start with
the Coulombic potential energy of two charges - We need to add up all the attractions and
repulsions in this three charge system to arrive
at a potential of a system pictured above of a
charge q2 and a dipole µ1 with charges q1.
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16Intermolecular forces between µ
17Induced dipole moments
- Temporary induced dipole moment, µ
- Result of the influence of an electric field
- Electron distribution of the molecule
- Polarizable
- Magnitude of µ
- µ a?
- Polarizability (a) depends on the distortion
caused by E
18Polarizability volumes, a
- Dimensions of volume
- a a/(4peo)
- Difference between HOMO and LUMO
19Dipole-induced dipole interaction
- Induced dipole, µ, follows the changing
orientation of the permanent dipole, µ - V -µ12a2/pe0r6
20Induced dipole induced dipole
- Dispersion force (London force)
- the attraction
- between temporarily induced dipoles in non-polar
molecules - often disappear within an instant).
- The polarization can be induced either
- by a polar molecule
- by the repulsion of negatively charged electron
clouds in non-polar molecules - At any given point in time the electrons may be
more concentrated in an electron cloud closer to
one atom, causing a fractional, momentary
negative charge
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22quadrupole
23Dipole-Dipole interaction (Keesom
interaction) Dipole-Induced dipole
interaction (Debye interaction) Induced
dipole-Induced dipole interaction) (London
interaction, Dispersion) Total Van der Waals
attractive interaction Keesom Debye London
Additional hydrogen-bonding can be considered.
24- Dipole moment? polarizability? ??? ?? VDW? ??
- ? ??? ??? ?? Keesom, Debye, London? ?? ??
- London interaction? ???
- ?? ???
25Molecular structure
- All bonds are stronger than all intermolecular
forces. - Systems that use bonding only will have the
strongest structures. - Systems that use bonding and intermolecular
forces will have weaker structures, where the
strength will depend upon the type of
intermolecular force being used. - Systems that use intermolecular forces and no
bonding will have the weakest structures known
examples of these would be Noble Gases.
26Overall Potential Energy
27Various Models for Overall Potential
28Morse potential
29Morse potential
- The Morse potential
- Philip M. Morse
- a convenient model for the PE of a diatomic
molecule - a better approximation for the vibrational
structure of the molecule - the quantum harmonic oscillator
- Property
- bond breaking, such as the existence of unbound
states - the anharmonicity of real bonds
- the non-zero transition probability for overtone
and combination bands
30Lennard-Jones potential
- between a pair of neutral atoms or molecules.
- John Lennard-Jones(1924)
31Lennard-Jones 12,6 Potential
32Potential energy surface