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Title: Molecular Orbitals


1
Molecular Orbitals
  • Chapter 5

2
Molecular Orbital Theory
  • Molecular orbital theory uses the methods of
    group theory to describe bonding. Symmetry and
    relative energies largely determine how they
    interact to form molecular orbitals.
  • If the total energy of the electrons in the
    molecular orbitals is less than in the atomic
    orbitals, the molecule is predicted to form and
    be stable.

3
Molecular Orbital TheoryApproximations to the MO
Theory
  • Born-Oppenheimer approximation
  • ?(r,R)?el(r)?(R)
  • ?el(r) describes the electrons and ?(R) describes
    the nuclei.
  • (R) describes the nuclear coordinates and (r)
    describes the electron coordinates.
  • Nuclei are much heavier and move slowly relative
    to the electrons. The motion of the electrons
    can be separated out.
  • ?el(r) will be uniquely considered

4
Molecular Orbital TheoryApproximations to the MO
Theory
  • Orbital Approximation
  • It is not possible to find an exact solution for
    the electronic wavefunction in a many-electron
    system. It can be expressed as a product of
    one-electron wavefunctions.
  • ?el(e1,e2en)?1(e1)?2(e2),?n(en) where ?i are
    the molecular orbitals of the system.
  • In this expression, electron-electron
    interactions are neglected. More complicated
    expressions treat the interactions between
    electrons for a many-electron system.

5
Molecular Orbital TheoryApproximations to the MO
Theory
  • Linear combinations of atomic orbitals, LCAO
    approximation.
  • where cij is the weight or
    amplitude of the atomic orbital, ?j, in the
    molecular orbital, ?i.
  • Usually the atomic orbitals are known and only
    the coefficients need to be determined.
  • ?1c11?1c12?2
  • ?2c21?1c22?2 The coefficients can be positive
    or negative.

6
Molecular Orbital TheoryApproximations to the MO
Theory
  • Linear combinations of atomic orbitals, LCAO
    approximation.
  • Minimal basis set (how many AOs are used).
  • Orbitals describing core electrons are ignored
    (coefficients are extremely small).
  • The sum includes all valence electron orbitals.
  • H, O, and Na

7
Three Conditions for Overlap/Combining of Atomic
Orbitals
  • Symmetry of the orbitals must be such that
    regions with the same sign of ? overlap.
  • Overlap of s atomic orbital with p atomic
    orbitals
  • Energies of the overlapping orbitals must be
    similar.
  • The distance between overlapping orbitals must be
    short to be effective.

8
Construction of Molecular Orbitals
  • The molecular orbital for diatomic hydrogen, H2.
  • ?Nca?(1sa) cb?(1sb) LCAO for bonding
  • ?-Nca?(1sa) - cb?(1sb) LCAO for antibonding
  • ca and cb are adjustable coefficients to reflect
    the contribution to bonding. Here, we assume
    that the coefficients are the same for the
    bonding and antibonding. Since the orbitals are
    idential, cacb, and these can be set equal to 1.
  • The normalization constant, N, is introduced to
    verify that the integral, ,
    is equal to 1.
  • The probability density (location of the
    electron), is obtained by squaring the
    wavefunction. The electron has to be located
    somewhere in space.

9
Construction of Molecular Orbitals
  • ?(ca?(1sa) cb?(1sb))2 ca2?2(1sa)cb2?2(1sb)
    2cacb?(1sa)?(1sb)
  • ca2?2(1sa) is the probability of finding the
    electron on the 1sa atomic orbital.
  • 2cacb?(1sa)?(1sb) is the interaction term and
    relates to the probability of finding the
    electron between the atoms.
  • The positive term indicates bonding between the
    atoms.

10
Construction of Molecular Orbitals
  • ?(ca?(1sa) - cb?(1sb))2 ca2?2(1sa)cb2?2(1sb)-
    2cacb?(1sa)?(1sb)
  • ca2?2(1sa) is the probability of finding the
    electron on the 1sa atomic orbital.
  • In this situation, -2cacb?(1sa)?(1sb) is the
    interaction term. The electrons in this orbital
    are excluded from the region between the atoms.
  • The negative term indicates antibonding between
    the atoms. The surface where the electron is
    excluded is called a nodal surface. Make sure
    that you understand Figure 5-1.

11
Finding the Normalization Constant
  • The electron must be somewhere in space.

12
Nonbonding Orbitals
  • Nonbonding orbitals occur when there is not a
    corresponding orbital of the correct symmetry.
  • There is no net overlap between the wavefunctions
    or the wavefunctions are orthogonal.
  • The energy of the nonbonding orbital is
    essentially equal to the atomic orbital.
  • Illustrate the combining of an s orbital with the
    three p orbitals.
  • Nonbonding orbitals may also result because of
    the energy differences of combining orbitals. It
    may also occur if the separation between atoms is
    too great.

13
Formation of Molecular Orbitals from p Atomic
Orbitals
  • Illustrate with the different p orbitals.
  • ? and ? bonding molecular orbitals.
  • The symmetry properties of the orbitals must
    match (e.g. C2 rotation) for the wavefunctions to
    combine.
  • The character tables reveal the symmetry of
    particular orbitals indicating if they will or
    will not combine.
  • If there is no symmetry match for an orbital, the
    orbital is nonbonding.
  • When overlapping regions have the same sign,
    there will be an increased probability in the
    overlap region. If opposite signs exist, the
    combination produces decreased electron
    probability in the overlap region.

14
Formation of Molecular Orbitals from d Atomic
Orbitals
  • The same rules apply for the combination of d
    orbitals.
  • Types of bonding with d orbitals.
  • ? bonding with dz2 orbitals
  • ? bonding with dyz and dxz orbitals
  • ? bonding (new) with and dxy orbitals.
  • This type of bonding is invoked to account for
    quadruple bonds.
  • Discuss nodal surfaces and their locations.
    These can be illustrated with orbital viewer
    software.

15
Homonuclear Diatomics
  • Figure 5-5 illustrates a simplified molecular
    orbital diagram for homonuclear diatomics.
  • Aufbau, Hunds, and Pauli-exclusion
  • Bond order ½( of bonding electrons - of
    antibonding electrons.
  • g and u stand for gerade and ungerade which
    relate to the inversion symmetry operation.
    Gerade, g, indicates that the orbital is
    symmetric with respect to the inversion
    operation.
  • Illustrate this with a few orbitals.

16
Orbital Mixing
  • The diagram shown in Fig. 5-5 is not entirely
    correct homonuclear diatomics since other
    orbitals of appropriate symmetry may interact.
  • ?ici,2sa?(2sa) ci,2sb?(2sb) ci,2pa?(2pa)
    ci,2pb?(2pb)
  • How many molecular orbitals would be produced
    from this combination?
  • ?1c1,2sa?(2sa)c2,2sb?(2sb) c3,2pa?(2pa)
    c4,2pb?(2pb)
  • This is an example of one of the s-type orbitals.
  • The result of this mixing is that the lowest
    energy orbitals move lower and the higher energy
    orbitals move higher in energy. The mixing
    inverts the order of the ?g and ?u bonding
    orbitals (Examine Fig. 5-6).
  • When overlapping the AOs the valence shell
    orbitals are commonly the only orbitals
    considered. This is called the minimal basis
    set. Illustrate for N.

17
Electron Configurations for Homonuclear Diatomics
  • The mixing effect decreases as a progression is
    made across the periodic table.
  • The order of ?g and ?u switch back at O2.
  • The electron configurations for some homonuclear
    diatomics.
  • H2, C2, and O2
  • The frontier orbitals (HOMO and LUMO)
  • Important when considering bonding and
    reactivity.
  • Paramagnetic versus diamagnetic.

18
Photoelectron Spectroscopy
  • Method for determining orbital energies.
  • O2(g) h?(photon)?O2(g) e-
  • Ionization energy h?-KE (of expelled electron)
  • Figures 5-10 and 5-11. The ionization energies
    of the low-energy orbitals are indicated.
  • The fine structure is a result of the interaction
    between the electron energy and the vibration
    energy. The peaks with pronounced vibration
    structure are involved strongly in bonding.

19
Molecular Orbitals of Polar Bonds
  • A greater nuclear charge shifts the atomic energy
    levels lower in energy. The atomic orbitals have
    different energies and a given MO receives
    unequal contributions from the atomic orbitals.
  • Orbital energies are given in Table 5-1 and Fig.
    5-13.
  • The contribution of an atomic orbital to a
    molecular orbital is directly related to the
    energy. Generally, the MO has the most character
    of the AO closest to it in energy (i.e. it will
    have the greatest coefficient value).

20
The Molecular Orbitals for CO
  • The symmetry of the molecule will be reduced to
    C2v for easier discussion.
  • The px and py orbitals have this symmetry.
  • Combination of orbitals with the same symmetry.
  • s and pz have A1 symmetry (character table).
  • px and py possess B1 and B2 symmetry,
    respectively.
  • Compare with C?v (px and py, together, behave
    like the E1 representation).
  • Energies of the orbitals and MO orbitals were
    derived from Spartan using semi-empirical
    calculations.
  • Examine the MO diagram and PES.

21
The Molecular Orbitals for CO
  • Molecular orbitals derived from Spartan (semi).
  • ?-40.0,2?0.82?(O2s)-0.21?(O2pz)0.41?(C2s)0.34
    ?(C2pz)
  • ?-20.7,2?-0.48?(O2s)-0.66?(O2pz)0.56?(C2s)
  • ?-16.2,1?-0.85?(O2px)-0.51?(C2px)
  • ?-16.2,1?0.85?(O2py)0.51?(C2py)
  • ?-13.0,3?-0.46?(O2pz)-0.66?(C2s)0.59?(C2pz)
  • ?1.0,1?0.51?(O2px)-0.85?(C2px)
  • Discuss and understand the various contributions
    to the MOs. Examine the MOs. The character of
    the MO is determined by the relative amounts of
    contribution from the combining orbitals.
  • Atomic orbital contributions with small
    coefficients are ignored (lt0.13).

22
The Molecular Orbitals for CO
  • The MOs of greatest interest are the frontier
    orbitals. Identify these in the diagram.
  • HOMO contributes electrons in reactions and LUMO
    accepts electrons (future discussion).
  • For the HOMO, the greater electron density is on
    the carbon (larger lobe).
  • Actual bonding in most compounds is M-C-O. In
    fact, a higher overall electron density is on the
    carbon (show with Spartan). Why?
  • Examine the fine structure in the PES. Why is
    there the fine structure originating from the 1?
    orbitals.

23
The Molecular Orbitals for LiF
  • Examine the diagram for LiF.
  • Small interactions due to poor energy overlap.
  • In a real compound, each Li is surrounded by six
    F- ions. A modification to this simple picture
    is needed (developed later).
  • Utilize Spartan to construct correct MO energy
    diagrams for HF and HI.

24
Molecular Orbitals for Larger Molecules
  • Determine the point group of the molecule.
  • Linear D?h ? D2h and C?v ? C2v
  • Assign x, y, and z axes.
  • The principal rotation axis is chosen as the
    z-axis.
  • In non-linear molecules, the y axes of the outer
    atoms point toward the central atom.
  • Find the characters of the representations for
    the combination of atomic orbitals on the outer
    atoms.
  • Reduce each representation to its irreducible
    representations.
  • This determines the groups orbitals or SALCs.

25
Molecular Orbitals for Larger Molecules
  • Identify the appearance and character of the
    SALCs by using the projection technique.
  • For nonlinear molecules
  • Find the orbitals on the central atom with the
    same symmetries as the SALCs.
  • Combine the atomic orbitals of the central atom
    with the SALCs of the same symmetry to produce
    the MOs.
  • Energy similarities are also considered to
    determine amount of contribution in a particular
    MO.

26
Linear Molecule, FHF-
  • The symmetry is D?h but we shall use D2h.
  • This retains the symmetry of the p orbitals.
  • Examine the D2h character table and identify the
    IRs that the same symmetry as the AOs.
  • The z-axis is down the internuclear axis.
  • Fig. 5-16 illustrates the group orbitals (i.e.
    SALCs) that form on the fluorine atoms.
  • Make sure that you can identify the symmetry or
    IR.
  • There does not have to be direct boding between
    the outer orbitals.

27
Linear Molecule, FHF-
  • For a linear species, these representations do
    not need to be reduced to IRs (but you can do it
    his way).
  • Only the 1s atomic orbital is considered for
    hydrogen, and it has an Ag type symmetry.
  • Two SALCs have the correct symmetry to interact
    with the the hydrogen atom.
  • The SALC from the 2s atomic orbital is too low in
    energy. The H 1s atomic orbital interacts most
    strongly with the SALC from the 2pz orbitals on
    fluorine.
  • (-13.6 eV and -18.7 eV).
  • Five of the SALCs do not interact with the
    central atom. These are essentially nonbonding.

28
Linear Molecule, FHF-
  • The MO picture illustrates a 3-center, 2-electron
    bond(s). This is different than the Lewis
    approach which utilizes a localized description
    of bonding between 2 atoms.
  • Involving a large number of atoms coordinated to
    a central atom usually decreases the bonding
    orbitals even further.

29
Bonding in the CO2 Molecule
  • The molecule reduces to D2h symmetry for easier
    analysis.
  • Construct the group orbitals as before and
    determine their symmetry (Fig. 5-19).
  • Determine the symmetry of the C atomic orbitals
    and group interactions to determine MOs.
  • Label the interactions according to symmetry
    taking into account the energy differences.
    Discuss these interactions.
  • A large energy difference indicates that the
    interaction is probably insignificant.

30
Bonding in the CO2 Molecule
  • Construct the MO diagram from the combinations
    determined previously.
  • Notice the multitude of 3-center, 2-electron
    orbitals.
  • All the bonding orbitals are occupied as well as
    two nonbonding MOs.
  • Identify the ?-type and ?-type bonds. Where is
    the electron density for the nonbonding
    electrons?
  • Note Use capital when describing symmetry and
    lower case letter when describing the actual
    orbitals (see diagram).
  • A1g versus alg

31
H2O A Nonlinear Molecule
  • The point group is C2v.
  • C2 axis is determined as the z axis and as the xz
    plane of the molecule.
  • Only the 1s orbital will be considered on the
    hydrogens so it is not necessary to assign axes
    to hydrogen.
  • Find the representation for the group orbitals.
  • The book utilizes transformation matrices to find
    the reducible representation for the SALCS. We
    will use a slightly different approach throughout
    the semester which is simpler (especially for
    larger molecules).

32
H2O A Nonlinear Molecule
  • The book largely finds the IRs of ? by
    inspection. We will reduce the RR into its
    component IRs by a systematic approach.
  • Transformation matrix exist which will reduce the
    matrix to one consisting of blocks along the
    diagonal. Each of these matrices belongs to an
    IR.
  • Find the Irs and normalize the SALCs.

33
H2O A Nonlinear Molecule
  • Determine the central atomic orbitals that can
    combine with the SALCs.
  • The 2pz and 2s possess A1 symmetry and the px
    orbital possesses B2 symmetry. What about the py
    central atomic orbital?
  • Combine the central atomic orbitals with the
    SALCs considering the differences in potential
    energy.
  • How many MOs will form?
  • How many a1orbitals will form? Why? Roughly
    determine the contribution of the SALC and the
    center pz and 2s atomic orbitals to each al MO
    (discuss this in some detail).

34
H2O A Nonlinear Molecule
  • ?1-0.88?(O2s)-0.11?(O2pz)-0.33?(Ha)-0.33?(Hb)
  • or c1?(O2s)c2(?(Ha)?(Hb)) (ignoring the O2pz
    contrib.)
  • ?20.77?(O2px)0.45?(Ha)-0.45?(Hb)
  • Or c3?(O2s)c4(?(Hb)-?(Ha))
  • ?3-0.33?(O2s)0.83?(O2pz)0.31?(Ha)0.31?(Hb)
  • ?41.00?(O2py)
  • ?5-0.34?(O2s)-0.54?(O2pz)0.54?(Ha)0.54?(Hb)
  • ?6-0.64?(O2px)0.54?(Ha)-0.54?(Hb)
  • The 2py atomic orbital is nonbonding (1b2).
  • Examine Table 5-3 and Fig. 5-29. All four MOs
    are different. What are the major differences
    when compared to the Lewis structure? Can also
    view the MOs with Spartan.

35
Ammonia NH3
  • Point group is C3v
  • The C3 axis is determined as the z-axis.
  • Find the RR (only consider the 1s atomic orbitals
    on the hydrogens).
  • Determine the IR components of the RR.
  • There are three SALCs, one with A1 symmetry and
    two (considered together) with E symmetry. What
    does the E representation indicate? The A1 SALC
    is easy to visualize. What about the two SALCs
    with E symmetry?
  • Sum of the squares of the coefficients for each
    AO must equal 1.
  • Symmetry of the central atom orbitals matches the
    symmetry of the SALCs. There must be one nodal
    surface in each E SALC.

36
Ammonia NH3
  • Determine the symmetry representations of the
    atomic orbitals on the central atom.
  • s and pz have A1 symmetry and px and py (as a
    pair) possess E symmetry.
  • Combine the central atomic orbitals with the
    SALCs of appropriate symmetry to form MOs.
  • Spartan helps in understanding the SALCs and MOs.
  • ?1e0.37?(2px)-0.63?(2py)0.58?(Ha)-0.28?(Hb)-0
    .27?(Hc)
  • ?1e0.63?(2px)0.37?(2py)0.49?(Hb)-0.48?(Hc)
  • SALCs

37
Ammonia NH3
  • MO diagram in Figure 5-31
  • A1 symmetry orbitals
  • A bonding, nonbonding, and antibonding MO
    (roughly)
  • E symmetry orbitals
  • These are doubly degenerate orbitals which means
    that there is a pair at low energies and a pair
    at high energies (the same energy).
  • Lone pair chemistry there is a lone pair of
    electrons largely located on the nitrogen atom.
    This can act as a Lewis base. The LUMO/HOMO
    chemistry will be discussed in detail later.
  • BF3 species

38
The Pi Bonding in C4H4
  • What is the point group?
  • Construction of the SALCs.
  • Find the RR and IRs.
  • The appearance of the SALCs may not be obvious
    when there is more than a two group atoms.
    Obviously, Spartan can be used to determine the
    wavefunctions and appearance of the orbitals.
    There is another way!!! This involves the use of
    projection operators.

39
Using the Projection Technique
  • The most important and frequent use for
    projection operators is to determine the proper
    way to combine atomic wave functions on
    individual atoms into Mos that correspond to the
    molecular symmetry.
  • A particular atomic orbital or wavefunction will
    be projected by the symmetry operations. Lets
    perform this for C4H4. This reveals how the
    atomic group orbitals combine to form the SALCs
    of a given symmetry determined earlier.

40
Phosphorus Pentafluoride, PF5
  • What is the point group?
  • Find the z-axis and determine the y-axes for the
    fluorine ligands.
  • Determine the RR representing the group orbitals
    from the fluorine ligands.
  • The axial and equatorial have to be considered
    separately since they are not interconverted by
    symmetry.
  • Determine the IRs components contained in ?.
  • How many SALCs will there be?
  • Website http//www.mpip-mainz.mpg.de/gelessus/g
    roup.html

41
Phosphorus Pentafluoride, PF5
  • Use the projection technique to determine the
    appearance of the group orbitals.
  • Determine the symmetry types of the central atom
    atomic orbitals.
  • Combine the SALCs and the atomic orbitals on
    phosphorus to make the MOs.
  • Draw the interaction diagram considering the
    potential energy differences.

42
Molecular Shapes
  • Determining the actual shapes of molecules using
    the MO approach usually involves the use of
    molecular modeling software (Spartan).
  • The overall energy at different bond distances
    and angles is calculated until the minimum is
    found. Any energy that is calculated will be
    equal to or greater than the true energy.

43
Hybrid Orbitals vs. Molecular Orbitals
  • The hybrid orbitals point from a central atom
    toward surrounding atoms or lone pairs.
  • Therefore, the symmetry properties of a set of
    hybrid orbitals will be identical to the
    properties of a set of vectors with origins at
    the nucleus of the central atom and pointing
    toward the surrounding atoms and lone pairs.
  • Td example in the book and PtCl42-
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