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Covalent bonding #3

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<strong>Covalent</strong> <strong>bonding</strong><br />

uThere are many different approaches to<br />

describing covalent bonds<br />

– which one you pick is often a compromise<br />

between ease of use and accuracy<br />

uMolecular orbital theory is the best<br />

approach if good agreement with<br />

experiment is needed<br />

Lewis theory<br />

uLewis’ theory of <strong>bonding</strong> was one one the<br />

earliest to have any success<br />

uBased on the octet rule<br />

– main group elements like to have eight<br />

electrons when they form compounds (except<br />

hydrogen)<br />

Bond order<br />

uIn many cases Lewis structures can be used<br />

to calculate bond orders that correlate well<br />

with experimentally measured bond<br />

strengths and lengths<br />

– :N:::N: triple bond<br />

– O::O double bond<br />

1


Formal charges<br />

uA molecule may have more than one<br />

plausible Lewis structure<br />

uThe best Lewis structure is the one that has<br />

the least charge separation<br />

Resonance structures<br />

uMolecules and ions with more than one<br />

distinct but equivalent (by rotation or<br />

reflection etc.) Lewis structures can occur<br />

the real structure is usually an average of<br />

these different resonance forms<br />

Failures of the Lewis model<br />

uA number of molecules with odd numbers<br />

of electrons exist (no octet) e.g. NO<br />

uAn atom may not have enough electrons to<br />

complete its octet without having ridiculous<br />

formal charges e.g. BF 3<br />

uA central atom may clearly have more than<br />

8 electrons e.g. SF 6<br />

uO 2 is paramagnetic!!<br />

2


Molecular Orbital theory<br />

uIn principle, the electronic structure of<br />

molecules can be worked out in the same<br />

way as for atoms<br />

– solve the schrodinger equation<br />

uThis gives molecular orbitals rather than<br />

atomic orbitals<br />

uHowever, it is difficult to solve the<br />

Schrodinger equation for molecular species<br />

LCAO approximation<br />

uGood approximations to the molecular<br />

orbitals can be obtained by taking linear<br />

combinations of atomic orbitals<br />

Rules for use of MOs<br />

uWhen two AOs mix to give MOs, two MOs<br />

will be produced<br />

uFor mixing AOs must have similar energies<br />

uEach orbital can have two electrons max<br />

uFill lowest energy orbitals first<br />

uIf you have unpaired electrons they should<br />

be spin parallel (Hund’s rule)<br />

uBond order is number of <strong>bonding</strong> pairs<br />

minus number of anti<strong>bonding</strong> pairs<br />

3


Period 1 diatomics<br />

Overlapping p-orbitals<br />

Oxygen and fluorine<br />

4


Nitrogen<br />

Bond orders<br />

Experimental verification<br />

uUV-photoelectron spectroscopy can be used<br />

to verify the MO diagrams.<br />

– Molecules are ionized using monochromatic<br />

light<br />

» N 2(g) + h•---> N 2<br />

+<br />

(g) + e -<br />

– The kinetic energy of the resulting<br />

photoelectrons is measured<br />

5


PES spectrum for N 2<br />

Heteronuclear diatomics<br />

uMO diagrams for heteronuclear species are<br />

constructed in a similar fashion to those for<br />

homonuclear species<br />

– However, the AO energies are different<br />

Molecular shapes<br />

uThe prediction of molecular shapes can be<br />

done in a number of ways<br />

– MO theory is very effective. However, it<br />

requires complicated calculations<br />

– VSEPR (Valence Shell Electron Pair<br />

Repulsion) theory is good for main group<br />

compounds and predictions can be made easily<br />

6


VSEPR<br />

uVSEPR does not have a solid theoretical<br />

foundation<br />

uIt is based on the idea that pairs of valence<br />

electrons (either <strong>bonding</strong> or lone pairs) will<br />

try and avoid each other as much as<br />

possible<br />

– molecule adopts a geometry that allows<br />

electron pairs to be as far apart as possible<br />

Electron pair count and geometry<br />

uTwo pairs on central atom - linear<br />

uThree pairs on central atom - trigonal<br />

uFour pairs on central atom - tetrahedral<br />

uFive pairs on central atom - trigonal<br />

bipyramidal<br />

uSix pairs on central atom - octahedral<br />

uSeven pairs - a number of possibilities<br />

Electron counting<br />

uFor molecules with single bonds to the<br />

central atom count all valence electrons of<br />

central atom plus one electron for each<br />

ligand atom<br />

– BCl 3 3 electrons from boron and 1 from each<br />

chlorine so there are 3 pairs of electrons<br />

uWhen there are double bonds present count<br />

the four electrons associated with the<br />

double bond as a single pair<br />

7


Linear geometry<br />

Trigonal geometry<br />

Tetrahedral geometry<br />

8


TBP geometry<br />

Octahedral geometry<br />

Seven coordinate species<br />

uIF 7 , XeF 6 , UF 7<br />

2-<br />

, NbF 7<br />

2-<br />

9


Species that violate VSEPR<br />

uLike nearly all truly useful sets of rules<br />

there are exceptions<br />

uSpecies that are sterically crowded often do<br />

not obey VSEPR<br />

» XeF 6 obeys VSEPR (7 pairs)<br />

» TeCl 6<br />

2-<br />

does not (7 pairs but is octahedral)<br />

Hybridization<br />

uThe <strong>bonding</strong> around atoms with different<br />

geometries is often pictures as consisting of<br />

overlapping hybrid orbitals<br />

– a hybrid orbital is a mixture of AOs<br />

– mixing in different ways gives different<br />

geometries<br />

Different types of hybridization<br />

10


How useful are hybrid orbitals<br />

uThe use of hybrid orbitals provides a<br />

picture of the <strong>bonding</strong> around an atom<br />

uHybridization arguments are not predictive,<br />

just descriptive<br />

uMO theory is predictive but complicated to<br />

use<br />

An MO view of H 2 O<br />

uMO theory predicts the lone pairs and<br />

bonds in H 2 O are not equivalent unlike the<br />

hybridization view<br />

Intermolecular forces<br />

uAttractive interactions between molecules<br />

allow the formation of molecular liquids<br />

and solids<br />

uThere are a number of different types of<br />

intermolecular forces<br />

– dispersion/London/van der Waals forces<br />

– dipolar interactions<br />

– hydrogen bonds<br />

11


Dispersion forces<br />

uAll molecular and atomic species are<br />

attracted to each other by dispersion forces<br />

uFluctuations in charge distribution polarize<br />

nearby atoms and molecules. This induced<br />

dipole interacts with the original uneven<br />

charge distribution<br />

The strength of dispersion forces<br />

uThe strength of the interaction depends on<br />

– number of electrons in atom or molecule<br />

– spatial extent of atom or molecule<br />

uIncreasing electron count tends to increase<br />

the strength of the interaction<br />

– more charge to move around<br />

uIncreasing spatial extent increase the<br />

interaction<br />

– can get better charge separation<br />

The BPs of MH 4 species<br />

12


Interactions between polar molecules<br />

uSome molecules have a permanent dipole<br />

moment<br />

– due to a low symmetry charge distribution<br />

uTo get low symmetry charge distribution<br />

you must have polar bonds<br />

– uneven distribution of charge between two<br />

bonded atoms<br />

uPolar bonds do not guarantee a polar<br />

molecule!<br />

Electronegativity<br />

uSome atoms are better at attracting<br />

electrons than others<br />

– the ability to attract electrons is called<br />

electronegativity<br />

uElectronegativity was quantified by Pauling<br />

Dipole-dipole versus dispersion<br />

uMolecular dipoles can give a significant<br />

contribution to intermolecular forces<br />

– CO (BP 82K) and N 2 (BP 77K)<br />

uHowever, dispersion forces are usually<br />

more important<br />

– HCl (BP 188K) and HBr (BP 206 K)<br />

13


The effect of hydrogen <strong>bonding</strong><br />

Hydrogen <strong>bonding</strong><br />

uVery polar molecules (HF, H 2 O, NH 3 ) often<br />

have anomalous properties<br />

uThe interactions between molecules are<br />

strong<br />

– intermolecular distances drop down into the<br />

region where a covalent contribution is to be<br />

expected<br />

14

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