Molecular interactions - PowerPoint PPT Presentation

1 / 32
About This Presentation
Title:

Molecular interactions

Description:

Complete valence shells are still able to interact with one another. Van der Waals ... frequency response of various dielectric mechanisms in terms of the real and ... – PowerPoint PPT presentation

Number of Views:430
Avg rating:3.0/5.0
Slides: 33
Provided by: ylee2
Category:

less

Transcript and Presenter's Notes

Title: Molecular interactions


1
Molecular interactions
  • Yongsik lee
  • June 2009

2
Residual interaction
  • Complete valence shells are still able to
    interact with one another
  • Van der Waals
  • Hydrogen bodning

3
Interaction 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

4
frequency 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

5
Polarizability, 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

7
Electrical Dipole Moments
8
Dipole 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

9
Polar vs. non-polar molecules
10
Estimating µ
  • Pauling electronegativities
  • µ/D ??
  • If an atom attracts the electrons more strongly,
    the more electronegative atom is (-) of µ

11
Dispersion of Refractive Index
12
Total Dipole moments mol geometry
13
Interactions between Dipoles
14
a 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.

15
(No Transcript)
16
Intermolecular forces between µ
17
Induced 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

18
Polarizability volumes, a
  • Dimensions of volume
  • a a/(4peo)
  • Difference between HOMO and LUMO

19
Dipole-induced dipole interaction
  • Induced dipole, µ, follows the changing
    orientation of the permanent dipole, µ
  • V -µ12a2/pe0r6

20
Induced 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

21
(No Transcript)
22
quadrupole
  • Electric quadrupole
  • Magnetic quadrupole

23
Dipole-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? ???
  • ?? ???

25
Molecular 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.

26
Overall Potential Energy
27
Various Models for Overall Potential
28
Morse potential
29
Morse 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

30
Lennard-Jones potential
  • between a pair of neutral atoms or molecules.
  • John Lennard-Jones(1924)

31
Lennard-Jones 12,6 Potential
32
Potential energy surface
Write a Comment
User Comments (0)
About PowerShow.com