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Molecular Orbitals 5 N 2 NH 3 H 2 O Why do they make chemical bonds ?

Why do they make chemical bonds ? Molecular Orbitalsbh.knu.ac.kr/~leehi/index.files/Molecular_Orbitals.pdf · 2018-10-24 · Types of Chemical Bonds . Covalent Bond • A molecule

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  • Molecular Orbitals 5

    N2 NH3 H2O

    Why do they make chemical bonds ?

  • Stabilization

    Bond energy

    Why do they make chemical bonds?

  • Metallic Bond Ionic Bond Covalent Bond

    Types of Chemical Bonds

  • Covalent Bond

    • A molecule is composed of atoms that are bound together by sharing pairs of electrons using the atomic orbitals of the bound atoms.

    •Description of valence electron arrangement

    •Description of atomic orbital types used to share electrons or hold lone pairs.

    •Prediction of geometry

    •Analogous to atomic orbitals for atoms, MOs are the quantum mechanical solutions to the organization of valence electrons in molecules.

    •Electron pairs in the molecule are assumed to be localized on a particular atom or in the space between two atoms

    •Electron pairs localized on an atom : lone pairs

    •Electron pairs found in the space between the atoms : bonding pairs

  • Covalent Bond

    Fact: O2 is paramagnetic!

    O OLewis structure VSEPR Valence bond theory

    •sp2 hybridized •lone pairs in sp2 hybrid orbitals •bonding pairs in σ and π bonds

    All show all electrons paired.

    LE is great to predict bondings and structures and geometries of molecules.

    BUT, there are some short points. •No concept of resonance. No paramagnetic properties. No information of bond energy.

    In contrast to LE, molecular orbitals describe how electrons spread over all the atoms in a molecule and bind them together, which can give correct views of

    • concept of resonance. paramagnetic properties. bond energy.

  • Formation of Molecular Orbitals from Atomic Orbitals

    H2 – 2 protons and 2 electrons Schroedinger Eq => Molecular orbitals

    But, no way to solve => LCAO (linear combination of atomic orbitals)

    => Approximate solutions of Schroedinger Eq

    H – 1 proton and 1 electron Schröedinger Eq => Atomic orbitals

    f+

    f+2

    Constructive overlap ⇒ enhance e- density between the nuclei

    ⇒ attract the nuclei ⇒ bonding orbital

    fA fB A B

    fA

    fB

    A B f- f-2

    destructive overlap ⇒ node(s) between the nuclei

    ⇒ repel each other ⇒ antibonding orbital

    +

    – –

    ++

    +

    Overlap of wavefunctions (constructive Overlap)

    (destructive Overlap)

  • φ+

    φ+2

    φΑ φΒ Α Β

    φΑ

    φΒ

    Α Β φ− φ−2

    Higher energy state

    Lower energy state

    Constructive overlap ⇒ enhance e- density between the nuclei

    ⇒ attract the nuclei ⇒ bonding orbital

    destructive overlap ⇒ node(s) between the nuclei

    ⇒ repel each other ⇒ antibonding orbital

    Ψ = caψa + cbψb

    Formation of Molecular Orbitals from Atomic Orbitals

  • )]1()1([2

    1)]1()1([)( babbaa ssscscN ψψψψσ +=+=Ψ

    )]1()1([2

    1)]1()1([*)( babbaa ssscscN ψψψψσ −=−=Ψ

    Formation of Molecular Orbitals from Atomic Orbitals Molecular Orbitals from s Orbitals

    H2

    σ*1s antibonding m.o. (higher energy than separate atoms)

    σ1s bonding m.o. (lower energy than separate atoms)

    σ (C2 symmetric about the line connecting the nuclei)

  • Formation of Molecular Orbitals from Atomic Orbitals Molecular Orbitals from p Orbitals

    π (C2 antisymmetric about the line connecting the nuclei)

  • Formation of Molecular Orbitals from Atomic Orbitals Molecular Orbitals from d Orbitals

    No interaction

  • Classification of Covalent Bonds (by symmetry)

    σ bond (C2 symmetric about z- axis)

    π bond (C2 antisymmetric about z- axis)

    δ bond (C4 antisymmetric about z- axis)

    φ bond (C6 antisymmetric about z- axis)

    U2, HTa2+ (in calculation)

    0 node

    1 node

    2 node

    3 node

    Node(s) at z-axis

  • 3 Things to Consider to Form Molecular Orbitals

    N atomic orbitals => N molecular orbitals Symmetry match of atomic orbitals Relative energy of atomic orbitals

    Forming nonbonding orbitals

    Remember ! The more nodes, the higher energy.

  • Homonuclear Diatomic Molecules

    bond order = (no. of e– in bonding m.o.s) - (no. of e– in antibonding m.o.s)

    2

    b.o. = 1

    H2

    1st Row Diatomic Molecules

    σg2(1s)

    b.o. > 0 (i.e., lower energy than separate atoms)

    b.l = 74.1 pm BE = 436 kJ/mol

    b.o. = 0.5

    H2+

    σg1(1s)

    b.l = 105.2 pm BE = 258 kJ/mol

    b.o. = 0

    He2

    σg2σu*2 (1s)

    *detected at very low T and P *BE = 0.01 J/mol

    b.o. = 0.5

    He2+

    σg2σu*1 (1s)

    b.l. =108 pm BE = 233 kJ/mol

    )]1()1([)( bbaa scscN ψψσ +=Ψ

    )]1()1([*)( bbaa scscN ψψσ −=Ψ

  • Homonuclear Diatomic Molecules 2st Row Diatomic Molecules

    Not big

    No mixing (O2, F2, Ne2)

    Mixing (Li2 - N2)

    )]2()2()2()2([ bcacbbaa pcpcscscN ψψψψ +++=Ψ

  • Homonuclear Diatomic Molecules 2st Row Diatomic Molecules

    b.o. = 1

    Li2

    σg2(2s)

    * found in gas phase

    b.o. = 0

    Be2

    σg2σu*2 (2s)

    b.o. = 1

    B2

    σg2σu*2 (2s)πu1πu1(2p)

    * B12 (solid phase) * Paramagnetic (gas phase)

    b.o. = 2 (π)

    C2

    σg2σu*2 (2s)πu2πu2(2p)

    * Found in gas phase * rare * C22- is more common C2 d(C-C) 124.2 pm (b.o. = 2) CaC2 d(C-C) 119.1 pm (b.o. = 3) C2H2 d(C-C) 120.5 pm (b.o. = 3)

    b.o. = 3 (2π+σ)

    N2

    σg2σu*2(2s) πu2πu2σg2 (2p)

    b.l. = 109.8 pm BE = 942 kJ/mol

  • Homonuclear Diatomic Molecules 2st Row Diatomic Molecules

    b.o. = 2

    O2

    σg2σu*2(2s)σg2πu2πu2πg*1πg*1(2p)

    b.l. = 120.8 pm * Paramagnetic

    Other forms of O2n O2+ b.o = 2.5, b.l = 111.6 pm O2- b.o = 1.5, b.l = 135 pm O22- b.o = 1, b.l = 149 pm

    b.o. = 1

    F2

    σg2σu*2(2s)σg2πu2πu2πg*2πg*2(2p)

    b.o. = 0

    Ne2

    σg2σu*2(2s)σg2πu2πu2πg*2πg*2σu*2 (2p)

  • Homonuclear Diatomic Molecules 2st Row Diatomic Molecules

    Big triumph of MO theory

    HOMO (highest occupied molecular orbital)

    LUMO (lowest unoccupied molecular orbital)

    SOMO (singly occupied molecular orbital)

    Frontier orbitals

  • Homonuclear Diatomic Molecules Bond Lengths

    Bond length Covalent radius

    H-X H-B H-C H-N H-O H-F

    Length (pm) 120 109 101.2 96 91.8

    1

    1. Any trend found? OK with electronegativity difference

    2

    2. Any trend found? Don’t be fooled by the text book. Covalent radii are defined in X-X single bond (Table 2-8).

  • Homonuclear Diatomic Molecules How to measure the energy levels of MOs ? (Photoelectron spectroscopy)

    photoelectron v

    A + hν A+ + e- Ionization energy = hν - ½ mv2

    IE

    hν = UV UPS : outer electrons hν = X-ray XPS : inner electrons

  • Homonuclear Diatomic Molecules How to measure the energy levels of MOs ? (Photoelectron spectroscopy)

    N2 O2

    Ionization energy = hν - ½ mv2

    N2 O2

    Why fine structure?

  • Homonuclear Diatomic Molecules How to measure the energy levels of MOs ? (Photoelectron spectroscopy)

    Ionization energy = hν - ½ mv2

    Franck-Condon Principle: Classically, the Franck–Condon principle is the approximation that an electronic transition is most likely to occur without changes in the positions of the nuclei in the molecular entity and its environment. The resulting state is called a Franck–Condon state, and the transition involved, a vertical transition.

    Mnucleus >> Melectron e-: faster motion

    Ionization energy = hν - ½ mv2 – Evib+

  • Homonuclear Diatomic Molecules How to measure the energy levels of MOs ? (Photoelectron spectroscopy)

    Ionization energy = hν - ½ mv2 – Evib+

    N2 O2

    stronger bonding involved less bonding involved

  • Heteronuclear Diatomic Molecules

    N atomic orbitals => N molecular orbitals Symmetry match of atomic orbitals Relative energy of atomic orbitals

    3 things to consider to form MOs

    |cA| = |cΒ|

    |cA| > |cΒ| |cA| >> |cΒ| |cA| = |cΒ|

    |cA| < |cΒ| |cA|

  • Heteronuclear Diatomic Molecules Polar Bonds

    Average potential energy of all terms

    Ex) E(C2p) = [E(1D) x 5 + E(3P) x 9 + E(1S) x 1]/15

  • Heteronuclear Diatomic Molecules CO

    Significant mixing between O2pz and C2s

  • Heteronuclear Diatomic Molecules CO

    Significant mixing with C2s

    C∞v

  • Heteronuclear Diatomic Molecules CO

    Significant mixing with C2s

    C∞v

    M – C≡O M – O≡C ?

  • Heteronuclear Diatomic Molecules Ionic Compounds and MOs

    LiF

    Li: 1s22s1 Li+: 1s2 F: 1s22s2sp5 F-: 1s22s22p6 Electrostatic interaction

    View of ionic interaction

    View of MO

    F2p character Transfer of Li2s e- to F2p orbital which is lowered

    Don’t forget that ionic interaction is omnidirectional and more accurate MO description requires bands.

  • Heteronuclear Diatomic Molecules Ionic Compounds and MOs

    LiF

    Li: 1s22s1 Li+: 1s2 F: 1s22s2sp5 F-: 1s22s22p6

    View of ionic interaction

    Is this process really helpful?

    Thermodynamically unfavorable!!

    Lattice enthalpy is the deriving force.

  • MOs for Larger Molecules

    1. Determine the point group of molecules. (D∞h D2h, C∞v C2v) 2. Assign x, y, z coordinates. 3. Find reducible representations for ns orbitals on the outer atoms. Repeat for np

    orbitals in the same symmetry. (valence orbitals) 4. Reduce the reducible representations of step 3 to derive group orbitals or

    symmetry adapted linear combinations (SALCs) 5. Find the atomic orbitals of the central atoms with the same symmetries as those

    found in step 4. 6. Combine the atomic orbitals of the central atom and the SALCs of the outer atoms

    with the same symmetry and similar energy to form MOs.

  • MOs for Larger Molecules FHF-

    F(2px)+F(2px) 2 -2 0 0 0 0 2 -2

    F(2py)+F(2py) 2 -2 0 0 0 0 -2 2

    F(2pz)+F(2pz) 2 2 0 0 0 0 2 2

    F(2s) + F(2s) 2 2 0 0 0 0 2 2

    B3u + B2g

    B2u + B3g Ag + B1u Ag + B1u

    D∞h D2h

    Very strong H-bonding

  • MOs for Larger Molecules FHF-

    H: 1s orbital

    Ag

    F---F: SALCs

    D∞h D2h

    can combine to form MOs

  • MOs for Larger Molecules FHF-

    D∞h D2h

    (-18.65 eV)

    (-40.17 eV)

    (-13.61 eV) H 1s

    H 1s will strongly interact with F2Pzs (Ag). Don't forget if F2s contributes, 3 MOs are formed.

  • MOs for Larger Molecules FHF-

    D∞h D2h

    bonding

    antibonding

    non-bonding * there are slight long-range interactions.

    MO 3-center 2-electron bond

    Lewis structure

    F H F

  • MOs for Larger Molecules CO2

    D∞h D2h

    2 -2 0 0 0 0 2 -2

    2 -2 0 0 0 0 -2 2

    2 2 0 0 0 0 2 2

    O(2px)+O(2px) O(2py)+O(2py) O(2pz)+O(2pz) O(2s) + O(2s) 2 2 0 0 0 0 2 2

    B3u + B2g

    B2u + B3g Ag + B1u Ag + B1u

  • MOs for Larger Molecules CO2

    D∞h D2h

    O---O: SALCs C: valence orbitals

    combine to form MOs

  • MOs for Larger Molecules CO2

    D∞h D2h

    Effective to form MOs

  • MOs for Larger Molecules CO2

    D∞h D2h

  • MOs for Larger Molecules CO2

    non-bonding σ

    bonding σ

    bonding π

    non-bonding π

    16 valence e-'s

    O=C=O

    Lewis structure

    3-center 2 electron bond

    2-center 2 electron bond

  • MOs for Larger Molecules H2O

    H(1s)+H(1s) 2 0 2 0 A1 + B1

    H------H: SALCs

    H H H H

    Ψa1= (1/√2){φa(H1s)+φb(H1s)}

    Ψb1= (1/√2){φa(H1s)-φb(H1s)}

    Α1 Β1

    O: valence orbitals

    2s A1 2px B1

    2pz A1 2py B2

  • MOs for Larger Molecules H2O

    H------H: SALCs

    H H

    H H

    Α1

    Β1

    O: valence orbitals

    2s A1

    2px B1

    2pz A1

    2py B2

    1b1 bonding 2b1 antibonding

    3a1 nearly non-bonding

    4a1 antibonding 2a1 bonding

    O

    H 1b2 non-bonding

    H2O MOs

  • MOs for Larger Molecules H2O

    Ψ1 Ψ3 Ψ5 Ψ2 Ψ6 Ψ4

    Very weak contribution of H group orbital (1s) weak contribution of O(2pz)

  • MOs for Larger Molecules H2O

    Lewis structure

    •Two lone pairs are equivalent (2 x sp3). •Two O-H bonds are equvalent [2 x (sp3 + H(1s))].

    MO

    lone pairs O-H bonds

  • MOs for Larger Molecules H2O

    O A1

    2s 2pz sp sp

    H----H SALCs

    A1 B1

    B2 B1

    Other approach

    b1

    b2

    b1

  • MOs for Larger Molecules H2O

    104.5°

    Why 104.5o in MO theory?

    Walsh Diagram - a diagram showing the variation of orbital energy with molecular geometry

  • MOs for Larger Molecules H2O

    Walsh Diagram - a diagram showing the variation of orbital energy with molecular geometry

    * When x-, y- axes are defined differently, B1 and B2 symmetries are exchanged.

  • MOs for Larger Molecules NH3

    3H(1s) 3 0 1 A1 + E

    A1

    E

    )]()()([3

    1cba HHH ψψψ ++=Ψ

    )]()()(2[6

    1cba HHH ψψψ −−=Ψ )]()([2

    1cb HH ψψ −=Ψ

    3H SALCs

    A1 A1

    E

    s pz

    px py

    N

  • MOs for Larger Molecules NH3

    3H(1s) 3 0 1 A1 + E

    Projection Operator Method : Group orbitals are constructed by summing the resulting orbitals of symmetry operations of an orbital A1

    E

    )]()()([3

    1cba HHH ψψψ ++=Ψ

    )]()()(2[6

    1cba HHH ψψψ −−=Ψ )]()([2

    1cb HH ψψ −=Ψ

    3H SALCs

    Ha

    E px py

    By inspecting N px, py orbitals, 2nd E (SALC) orbital is obtained.

  • MOs for Larger Molecules NH3

    A1

    E

    3H SALCs

    A1

    E

    s

    pz

    px

    py

    N

    A1

    mostly pz character

  • MOs for Larger Molecules BF3

    B F

    F

    F

    3F(2s) 3 0 1 3 0 1 A1' + E'

    3F(2px) 3 0 -1 3 0 -1 A2' + E'

    3F(2py) 3 0 1 3 0 1 A1' + E'

    3F(2pz) 3 0 -1 -3 0 1 A2'' + E''

  • MOs for Larger Molecules BF3

    B F

    F

    F

    3F(2s) A1' + E'

    A2' E'

    3F(2pz) A2'' + E'' 3F(2px) A2' + E' A1' E'

    3F(2py) A1' + E'

    A2'' E''

    A1' E'

    3F SALCs

    2s

    2px, 2py

    A2''

    A1'

    E'

    2pz

    B orbitals

  • MOs for Larger Molecules

    A2' E'

    A1' E'

    A1' E'

    A2'' E''

    3F(2px)

    3F(2py)

    3F(2pz)

    3F(2s) 3F SALCs

    BF3

    B orbitals

    2pz A2''

    2s A1'

    E'

    2py

    2px

  • MOs for Larger Molecules BF3

    bonding (a2”:slightly bonding)

    non-bonding almost non-bonding

    antibonding

    same for SO3, NO3-, CO32-

    Lewis ? VBT? ? σ and ? π

  • MOs for Larger Molecules SALCs

  • MOs for Larger Molecules SALCs

  • MOs for Larger Molecules SALCs

  • MOs for Larger Molecules Hybrid Orbitals

    One of the ways to predict the hybrid orbitals is..

    (Which atomic orbitals form hybrides?)

  • MOs for Larger Molecules Hybrid Orbitals

    Ex) CH4

    4 C-H bonds 4 1 0 0 2 A1+ T2 s, (px, py, pz) sp3

    why not d ? Ex) BF3

    B

    F

    F

    F

    3B-F bonds = 3F(2s) 3 0 1 3 0 1 A1' + E'

    s, (px, py) sp2

    슬라이드 번호 1Why do they make chemical bonds?Types of Chemical BondsCovalent BondCovalent BondFormation of Molecular Orbitals from Atomic Orbitals슬라이드 번호 7슬라이드 번호 8슬라이드 번호 9슬라이드 번호 10슬라이드 번호 11슬라이드 번호 12슬라이드 번호 13슬라이드 번호 14슬라이드 번호 15슬라이드 번호 16슬라이드 번호 17슬라이드 번호 18슬라이드 번호 19슬라이드 번호 20슬라이드 번호 21슬라이드 번호 22슬라이드 번호 23슬라이드 번호 24슬라이드 번호 25슬라이드 번호 26슬라이드 번호 27슬라이드 번호 28슬라이드 번호 29슬라이드 번호 30슬라이드 번호 31슬라이드 번호 32슬라이드 번호 33슬라이드 번호 34슬라이드 번호 35슬라이드 번호 36슬라이드 번호 37슬라이드 번호 38슬라이드 번호 39슬라이드 번호 40슬라이드 번호 41슬라이드 번호 42슬라이드 번호 43슬라이드 번호 44슬라이드 번호 45슬라이드 번호 46슬라이드 번호 47슬라이드 번호 48슬라이드 번호 49슬라이드 번호 50슬라이드 번호 51슬라이드 번호 52슬라이드 번호 53슬라이드 번호 54슬라이드 번호 55슬라이드 번호 56슬라이드 번호 57슬라이드 번호 58