Zumdahl - PowerPoint PPT Presentation

1 / 31
About This Presentation
Title:

Zumdahl

Description:

Zumdahl s Chapter 9 Covalent Bonding Orbitals Chapter Contents Hybridization and LE dnspm Molecular Orbitals Bond Order Bonding in Homonuclear Diatomics ... – PowerPoint PPT presentation

Number of Views:170
Avg rating:3.0/5.0
Slides: 32
Provided by: chrisp
Category:

less

Transcript and Presenter's Notes

Title: Zumdahl


1
Zumdahls Chapter 9
  • Covalent Bonding
  • Orbitals

2
Chapter Contents
  • Hybridization and LE
  • dnspm
  • Molecular Orbitals
  • Bond Order
  • Bonding in Homonuclear Diatomics
  • Paramagnetism
  • Heteronuclear Bonding
  • LE MO

3
Atomic Orbital Hybridization
  • VSEPR postulates repulsion geometries, but are
    atomic wavefunctions flexible enough to supply?
  • A key to wave mechanics is superposition,
    creating new waves from interference of old ones.
  • Degenerate (same energy) wavefunctions can mix
    arbitrarily to give new degenerate sets. ?
  • If energy lowering is possible, even
    near-degenerate (similar energy) sets of ? can
    mix to new sets.

4
The Joys of Promotion
  • Minimization of electron repulsion is the motive
    for mixing a set of AOs (Atomic Orbitals) that
    produces new AOs in the VSEPR directions.
  • In addition, paired electrons in AOs are already
    satisfied and need no stinking bonds, but if
    these partners are split up, more bonding is
    possible, at the bargain expense of promotion to
    higher energy orbitals. Extra bond energies pay
    it back.

5
Carbon Wins Big
  • The electronic configuration of carbon is
  • He 2s2 2p2 or He ?? ? ?
  • As such, only CH2 or two valence bonds are
    possible for carbon. Not for long.
  • Using the energy accessible from bond formation,
    carbon promotes an s e to a p orbital
  • He 2s1 2p3 or He ? ? ? ?
  • Making CH4 and other four valence molecules.

6
Blending the l out of it.
  • Promotion is necessary but not sufficient we
    must still mix spxpypz in ways like VSEPR.
  • The electron density follows the new orbital
    directions and the nuclei obey the bonding
    geometry.
  • We neednt blend all of the available orbitals!
  • We can mix s?px and leave py and pz for lone
    pair.
  • That would give us linear XAX bonding.
  • And that results from constructive interference
    in ?.

7
Wave Mixture Geometries
2s
2px
8
sp Hybridization
  • Starting with two AOs, mixing must generate no
    more than nor no fewer than two hybrids.
  • The s px combination points up the x-axis while
    the s px combination points down the x-axis.
  • Together they give linear XAX molecules (BeF2).
  • Also, the sp hybrid is elongated in its bonding
    direction for better penetration and lower energy.

9
Trigonal Planar Hybridization, sp2
and
mixed with
and 2 other combinations
gives
10
sp2 Hybridization
  • As with sp, the leftover p orbital(s) are
    available for electrons as either lone pairs or ?
    bonds.
  • In contrast, the single bonds created with the
    hybrids are called ? bonds, where ? is the Greek
    s and ? is the Greek p.
  • All 3 sp2 together look like

If your browser supports VRML, try
http//www.chm.davidson.edu/vrml/ao/ for details
of hybrid orbitals.
11
sp3 Tetrahedral Hybridization
  • The sp2 are even more penetrating than the sp but
    less so than sp3. The more the p character, the
    more directional the hybrid. Duhh.
  • Carbon can hybridize sp3, but so can N and O the
    difference is in how many hybrids have only one
    electron. Those bond the others lone pair.
  • The four sp3 together look like

12
Hybridization Beyond spn
  • The sp3 hybrid orbitals permit a valence of up to
    4 and the expected octet.
  • Violating the octet demands incorporation of d
    orbitals as in dsp3, d2sp3, etc.
  • They use dz²
  • and dx²y²

13
Trigonal Bipyramidal dsp3
  • Mixing dz² with sp3 gives five orbitals, two of
    which are axial and three equatorial.

Only one each of the two kinds are shown here,
but the other axial is just down the Z while the
other two equatorials are around Z at 120 to the
one shown.
14
Octahedral d²sp³
  • Mixing dx²y² with the five dsp³ gives the six
    identical d²sp³ orbitals in Cartesian directions.
  • This picture is merely diagrammatic it is not an
    accurate representation of the d²sp³
    wave-functions. (It is a group of spheres and
    cones.)
  • Still, if your browser is equipped with VRML, you
    can play with my first 3d world construction at
  • http//www.utdallas.edu/parr/chm1315/d2sp3.wrl

15
How Chemists Use Hybrids
  • Hybrid orbitals are great shorthand notations for
    building up a molecules geometry center by
    center part of every molecular model kit.
  • The skeletal structure so developed is called the
    ? skeleton because in-line overlap of adjacent
    bonding hybrids are cylindrically symmetrical
    about the internuclear axis and thus have no
    (axial) angular momentum (like s for an atom).

16
? and the remainders
  • The ? skeleton sets hybridization for each of the
    molecules central atoms.
  • Bonded to 3 things? No lone pair? You are sp2!
  • I not only expect 120 bonds from you but also an
    unhybridized p orbital ? to that plane.
  • Since the rest of your octet isnt a lone pair,
    you must be ? bonding to one or more of your
    partners.
  • Bonded to 3 with a lone pair? Youre sp3!
  • I expect 109.43 bond angles or there abouts.

17
? bonds? Piece of cake.
  • Unhybridized p orbitals on adjacent bonding
    centers can overlap (inefficiently) sideways.
  • Density not cylindrically symmetric (like ?) but
    does allow for buildup between nuclei (off
    line-of-centers).
  • ? bonds weaker than ? but add 1 to the bond
    order.
  • Off axis, theyre vulnerable to chemical attack
    ? bonds are reactive while ? are relatively
    inert.
  • Unsaturated fats have ?s to permit metabolic
    degrade.

18
Vitamin B12
19
Vitamin B12 withits multiple bonds
20
Molecular Orbital (MO) Theory
  • Electrons dont ignore all other nuclei beyond
    the adjacent bonding pair. Theyre really
    global.
  • Instead of building molecules atom by atom, well
    pour electrons onto a nuclear skeleton.
  • Hess assures us that when all the electrons are
    finally present, the (binding) energies will be
    the same either way.
  • So how do electrons respond differently this way?

21
Add electrons to proton framework
  • They see a wavefunction that spans molecule!
  • First approximation model to that is LCAO, Linear
    Combination of Atomic Orbitals.
  • Study the diatomics for simplicity. The
    advantages to MO will become apparent even there.
  • Thus, H2s MOs are LC of 1sA and 1sB where A and
    B are the labels for the two hydrogen atoms.
  • 1s? ? 1sA 1sB while 1s? ? 1sA 1sB (2 in 2
    out)

22
1s? H2
A
B
Fortunately, this MO holds both electrons.
See http//www.chm.davidson.edu/vrml/mo/h2/h2.html
23
1s? H2 MO
A
B
Any electron in this antibonding MO reduces BO by
½.
24
Bond Order (BO) in MO
  • MOs come in constructive (e.g., 1s?) and
    destructive (e.g., 1s?) combinations as regards
    the internuclear region.
  • Since they must mimic lone pairs as well, there
    are nonbonding MOs, but they do not influence
    BO.
  • BO ½ (? electrons MO ? electrons MO )
  • First surprising consequence H2 has BO ½
  • A stable one-electron bond is possible.
  • Correlates with Diss. E. and negatively with Bond
    R.

25
Using p AOs
  • If internuclear axis is Z, then 2pZA 2pZB binds
    and is called 2pz?. The combo antibinds.
  • More interesting are PX and PY which combine off
    the internuclear axis as ? MOs.
  • 2pX? ? 2pXA 2pXB for example.
  • Note that some combinations are meaningless
    because they do not overlap in bonding regions
    e.g., 2pXA 2pYB produces no MO.

26
Degenerate MOs
  • The energies of 2pX? and 2pY? are identical.
  • Hunds Rule applies to MOs just as it did AOs.
  • 1s?2 1s?2 2s?2 2s?2 2pZ?2 2pX?1 (C2)
  • is followed by
  • 1s?2 1s?2 2s?2 2s?2 2pZ?2 2pX?1 2pY?1 (C2)
  • Implying not only CC but also ? ? or a
    paramagnetic C2 diatom.

27
Decline of Bond Order
  • The pinnacle of A2 (2nd row generic diatom) comes
    at N2 with electronic configuration
  • Be2 2pZ?2 2pX?2 2pY?2 and bond order 3, N?N.
  • Weve run out of bonding MOs of the 2 shell.
  • Starting with O2, antibonding highest occupied
    MOs (HOMO) diminish BO.
  • Be2 2pZ?2 2pX?2 2pY?2 2pX?1 2pY?1
  • Only bond order 2 but paramagnetic.

See http//www.chem.technion.ac.il/ElBookOrb/molec
ule.htm
28
Formic Acid, HCO2H
  • Lewis Structure would have resonance in the
    conjugate base with the C-O bonds at 1.5 order.
  • MO generates this naturally by mixing 2pX from
    both oxygens and the carbon to create

An example of the delocalized nature of ?
bonding.
? bonding is better described as local.
29
Benzene, a textbook delocalization
Their mixing generates these double bonds.
  • After hybridizing sp2 for the ? skeleton,
  • Yes, you can build MOs from hybridized AOs.
  • The 6 leftover pX orbitals mix to give global
    MOs ? the plane of the nuclei.
  • Before mixing they are

30
C6H6 ? Bonding
  • After mixing, six new MOs arise, 3 bonding and 3
    antibonding.
  • Best case at top, and worst case at bottom.
  • The 6 electrons from each carbons p pair up in
    the 3 bonding ?s.

31
Knowing Where the Electrons are is
  • POWER

PC Spartan
Write a Comment
User Comments (0)
About PowerShow.com