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Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

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Page 1: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Chapter 9Molecular Geometriesand Bonding Theories

Page 2: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Molecular Shapes• we’ve learned to draw Lewis structures and

account for all the valence electrons in a molecule.

• But: Lewis structures are two dimensional and molecules are 3 dimensional objects.

• The 3D structure is absolutely critical for understanding molecules.

Page 3: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Molecular Shapes• geometry & shape of

molecule critical• we can easily predict

the 3D structure of a molecule just by adding up:

• bound atoms + lone pairs

Page 4: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

What Determines the Shape of a Molecule?

• atoms and lone pairs take up space and prefer to be as far from each other as possible

• shape can be predicted from simple geometry

lone pair

bonds

Page 5: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

“Things”

• The central atom has four “things” around it. A “thing” is an atom or a lone pair of electrons.

• # things = atoms plus lone pairs

Page 6: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Valence Shell Electron Pair Repulsion Theory

(VSEPR)“The best arrangement of a given number of things is the one that minimizes the repulsions among them.”

Page 7: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Geometries

These are the geometries for two through six things around a central atom.

number of things arrangement geometry bond angles

Page 8: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Geometries

• All one must do is count the number of “things” in the Lewis structure.

• The geometry will be that which corresponds to that number of “things.”

Page 9: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

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Molecular Geometries

• The geometry is often not the shape of the molecule, however.

• The “shape” is defined by the positions of only the atoms in the molecules, not the lone pairs.

Page 10: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Geometries vs. shape

Within each geometry, there might be more than one shape.

Page 11: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Linear geometrytwo things

• In this geometry, there is only one molecular geometry: linear.

• NOTE: If there are only two atoms in the molecule, the molecule will be linear no matter what the geometry is.

things geometry atoms lone pairs shape example

Page 12: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Trigonal Planar Electron Domain3 things

• There are two molecular geometries:– Trigonal planar, if there are no lone pairs– Bent, if there is a lone pair.

things geometry atoms lone pairs shape example

Page 13: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Lone pairs and Bond Angle

• Lone pairs are physically larger than atoms.

• Therefore, their repulsions are greater; this tends to decrease bond angles in a molecule.

Page 14: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Multiple Bonds and Bond Angles

• Double and triple bonds place greater electron density on one side of the central atom than do single bonds.

• Therefore, they also affect bond angles.

Page 15: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Tetrahedral geometry 4 things

• There are three molecular geometries:– Tetrahedral, if no lone pairs– Trigonal pyramidal if one is a nonbonding pair– Bent if there are two nonbonding pairs

Things geometry atoms lone pairs shape example

Page 16: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Trigonal Bipyramidal geometry5 things

• There are two distinct positions in this geometry:– Axial– Equatorial

Page 17: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Trigonal Bipyramidal geometry

Lower-energy conformations result from having lone pairs in equatorial, rather than axial, positions in this geometry.

Page 18: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Trigonal Bipyramidal geometry• There are four

distinct molecular geometries in this domain:– Trigonal

bipyramidal– Seesaw– T-shaped– Linear

Things geometry atoms lone pairs shape example

Page 19: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Octahedral geometry 6 things

• All positions are equivalent in the octahedral domain.• There are three molecular geometries:

Things geometry atoms lone shape example pairs

Page 20: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Larger MoleculesIn larger molecules, we talk about the geometry about a particular atom rather than the geometry of the molecule as a whole.

Page 21: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

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Larger Molecules

The structure of the whole molecule is only clear when we look at the whole molecule. But the geometry about each atom still follows the same rules!

Page 22: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

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Polarity

• In Chapter 8 we discussed bond dipoles.

• polar bonds versus polar molecules. We must think about the molecule as a whole.

Page 23: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Polarity

By adding the individual bond dipoles, one can determine the overall dipole moment for the molecule.

Page 24: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Polarity“The tractor pull”

Page 25: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Overlap and Bonding• covalent bonds form when electrons are “shared.”• But how, when the electrons are in these atomic

orbitals? Do atomic orbitals overlap?• Yes.

Page 26: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Overlap and Bonding• Increased overlap brings

the electrons and nuclei closer together while simultaneously decreasing electron-electron repulsion.

• However, if atoms get too close, the internuclear repulsion greatly raises the energy.

Page 27: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

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Hybrid Orbitals

But how do you get tetrahedral, trigonal bipyramidal, and other geometries when the atomic orbitals seem to be at right angles from each other all the time?

Page 28: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

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Hybrid Orbitals

• Consider beryllium:– In its ground electronic

state, it would not be able to form bonds because it has no singly-occupied orbitals.

Page 29: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

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Hybrid Orbitals

But if it absorbs the small amount of energy needed to promote an electron from the 2s to the 2p orbital, it can form two bonds.

Page 30: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

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Hybrid Orbitals• Mixing the s and p orbitals yields two degenerate

orbitals that are hybrids of the two orbitals.– These sp hybrid orbitals have two lobes like a p orbital.– One of the lobes is larger and more rounded as is the s

orbital.

Page 31: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

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Hybrid Orbitals• These two degenerate orbitals would align

themselves 180 from each other.• This is consistent with the observed geometry of

beryllium compounds: linear.

Page 32: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

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Hybrid Orbitals

• With hybrid orbitals the orbital diagram for beryllium would look like this.

• The sp orbitals are higher in energy than the 1s orbital but lower than the 2p.

Page 33: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Hybrid Orbitals

Using a similar model for boron leads to…

Page 34: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Hybrid Orbitals

…three degenerate sp2 orbitals.

Page 35: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Hybrid Orbitals

With carbon we get…

Page 36: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Hybrid Orbitals…four degenerate

sp3 orbitals.

Page 37: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Hybrid Orbitals

For geometries involving expanded octets on the central atom, we must use d orbitals in our hybrids.

Page 38: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Hybrid Orbitals

This leads to five degenerate sp3d orbitals…

…or six degenerate sp3d2 orbitals.

Page 39: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Hybrid Orbitals

Once you know the number of things around an atom, you know the hybridization state of the atom if you can count letters up to six.

Page 40: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Exam 3 topics• Chapter 7, periodic properties• Chapter 8, covalent and ionic bonding• Chapter 8, electronegativity• Chapter 8, polar bonds• Chapter 8, Lewis structures

– standard lewis structures– formal charge– resonance– less than an octet– more than an octet

• Chapter 9, geometry and shape of molecules• Chapter 9, polarity/dipole moments of whole molecules• Chapter 9, introduction to covalent bonding, diatomics

Page 41: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Exam 3 topics• Chapter 9, hybridization sp, sp2, sp3, sp3d, sp3d2

Page 42: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Chapter 7

• Periodic trends• Effective nuclear charge• trends in atomic radius• trends in ion radius• Ionization energy, trends• electron affinity, trends.

Page 43: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Effective Nuclear Charge

The effective nuclear charge, Zeff, is:

Zeff = Z − S

where Z = atomic number S = screening constant, usually close to the number of inner (n-1) electrons.

Na

Page 44: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Valence electrons:

How many valence electrons in:

OO2-

CoCo2+

Page 45: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Bonding atomic radius tends to… …decrease from left to right across a row due to increasing Zeff.

…increase from top to bottom of a column due to increasing value of n

Sizes of Atoms

increasing Eff incre

asing n

Page 46: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Sizes of Ions

Ionic size depends upon:

Nuclear charge.

Number of electrons.

Orbitals in which electrons reside.

Page 47: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Trends in First Ionization EnergiesOn a smaller scale, there are two jags in each line. Why?

Page 48: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Trends in Electron Affinity

There are also two discontinuities in this trend.

Page 49: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Page 50: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Exam 3 topics• Chapter 8, covalent and ionic

bonding– What is ionic bonding? What

holds the atoms together?– Energetics of ionic bonding– Lattice energy

Page 51: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Exam 3 topics• Chapter 8, electronegativity

– What is electronegativity?– What are the trends on the

periodic table?

• Chapter 8, polar bonds

Page 52: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Exam 3 topics• Chapter 8, Lewis structures

– standard lewis structures– formal charge– resonance– less than an octet– more than an octet

XeF2 XeF6, CO3-, NO2, ClO4

-, SbF5, SO2, SO32-, H2O2

Page 53: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Exam 3 topics• Chapter 8, bond enthalpies

– use bond enthalpy table to calculate a H of reaction

– bonds broken - bonds made = enthapy of reaction.

Page 54: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Exam 3 topics• Chapter 9, geometry and shape of molecules, VSEPR.• Chapter 9, polarity/dipole moments of whole molecules

• Give the geometry, shape and predict the dipole moment of each:

• XeF2, ClO4-, SF4, BrO2

-

Page 55: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Exam 3 topicsChapter 9, introduction to

covalent bonding, diatomics

covalent bonds form when electrons are “shared.”But how, when the electrons are in these atomic orbitals? Do atomic orbitals overlap?Yes.

Page 56: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Exam 3 answers

F

Xe F

BrF

F

F

.. ..

..TBP, linear, nonpolar

..

F octahedral, square pyramid, polar

S

F

F F

F

: TBP, See saw, polar

Page 57: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

C

trigonal planar,trigonal planar, nonpolar

..O

OO ....

:

: :--.. ..

C

O

OO ....

:

:

-

-.. ..

..:

C

O

O..

:

:

-..:

O.. :-..

15.

Page 58: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

CEM 151 Exam 2 FS07

0

5

10

15

20

25

5 20 30 40 50 60 70 80 90 100

Score

Frequency

Bin Frequency5 1

15 220 525 230 735 2240 1345 750 1755 1060 1865 1770 1775 2180 1385 1190 1695 8

100 3105 2

Mean 59.53774Median 61.5Mode 32SD 21.4384Range 101Minimum 3Maximum 104Count 212

Exam 3

Note: 53 4 points (better than 80%)

Page 59: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Regrade policy

• See your T.A. at recitation.• Must be more than 7 points• Entire exam will be regraded.• We’re giving back points for direction of

polarity on most of the problems where it is an issue BEFORE we give exam back.

• 12, 13, 15, 19, 20• You only draw arrows for 2 problems.

Page 60: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

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Valence Bond Theory

• Hybridization is a major player in this approach to bonding.

• There are two ways orbitals can overlap to form bonds between atoms.

Page 61: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

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Sigma () Bonds

• Sigma bonds are characterized by– Head-to-head overlap.– Cylindrical symmetry of electron density about the

internuclear axis.

Page 62: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

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Pi () Bonds

• Pi bonds are characterized by– Side-to-side overlap.– Electron density

above and below the internuclear axis.

Page 63: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

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Single Bonds

Single bonds are always bonds, because overlap is greater, resulting in a stronger bond and more energy lowering.

Page 64: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Multiple Bonds

In a multiple bond one of the bonds is a bond and the rest are bonds.

Page 65: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

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Multiple Bonds

• Example: formaldehyde an sp2 orbital on carbon overlaps in fashion with the corresponding orbital on the oxygen.

• The unhybridized p orbitals overlap in fashion.

Page 66: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

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Multiple Bonds

In triple bonds, as in acetylene, two sp orbitals form a bond between the carbons, and two pairs of p orbitals overlap in fashion to form the two bonds.

Page 67: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

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Delocalized Electrons: Resonance

When writing Lewis structures for species like the nitrate ion, we draw resonance structures to more accurately reflect the structure of the molecule or ion.

- - -

+ + +

Page 68: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

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Delocalized Electrons: Resonance

• each of the four atoms in the nitrate ion has a p orbital.

• The p orbitals on all three oxygens overlap with the p orbital on the central nitrogen.

Page 69: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

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Delocalized Electrons: Resonance

This means the electrons are not localized between the nitrogen and one of the oxygens, but rather are delocalized throughout the ion.

Page 70: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

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Resonance

The organic molecule benzene has six bonds and a p orbital on each carbon atom.

Page 71: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

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Resonance

• In reality the electrons in benzene are not localized, but delocalized.

• The even distribution of the electrons in benzene makes the molecule unusually stable.

Page 72: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

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Molecular Orbital (MO) Theory

Valence bond theory works very well for most observed properties of ions and molecules, but there are some concepts better represented by molecular orbital theory.

Page 73: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

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Molecular Orbital (MO) Theory

• In MO theory, we invoke the wave nature of electrons.

• If waves interact constructively, the resulting orbital is lower in energy: a bonding molecular orbital.

Page 74: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

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Molecular Orbital (MO) Theory

If waves interact destructively, the resulting orbital is higher in energy: an antibonding molecular orbital.

Page 75: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

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Molecular Orbital (MO) Theory• Valence bond theory:• atomic orbitals are mixed in each

individual atom before bonding.

• Molecular orbital theory:• no prebonding mixing. Molecular

orbitals are computed after bonding.

Page 76: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

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MO Theory

• In H2 the two electrons go into the bonding molecular orbital.

• The bond order is one half the difference between the number of bonding and antibonding electrons.

Page 77: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

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MO Theory

For hydrogen, with two electrons in the bonding MO and none in the antibonding MO, the bond order is

12

(2 - 0) = 1

Page 78: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

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MO Theory

• In the case of He2, the bond order would be

12

(2 - 2) = 0

• Therefore, He2 does not exist.

Page 79: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

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Rules for making and filling molecular orbitals

• 1. The number of MO’s equals the #of Atomic orbitals• 2. The overlap of two atomic orbitals gives two

molecular orbitals, 1 bonding, one antibonding• 3. Atomic orbitals combine with other atomic orbitals of

similar energy.• 4. Degree of overlap matters. More overlap means

bonding orbital goes lower in E, antibonding orbital goes higher in E.

• 5. Each MO gets two electrons• 6. Orbitals of the same energy get filled 1 electron at a

time until they are filled.

Page 80: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

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MO Theory

• For atoms with both s and p orbitals, there are two types of interactions:– The s and the p orbitals

that face each other overlap in fashion.

– The other two sets of p orbitals overlap in fashion.

Page 81: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

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MO Theory

• The resulting MO diagram looks like this.• There are both and bonding molecular orbitals

and * and * antibonding molecular orbitals.

Page 82: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

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MO Theory

• The earlier p-block elements in the second period have a sizeable interaction between the s and p orbitals.

• This flips the order of the and molecular orbitals in these elements.

Page 83: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

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Second-Row MO Diagrams

Page 84: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Heterodiatomic molecules

COC

CO has a triple bond

Page 85: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Heterodiatomic molecules

NO is paramagneticradical

Page 86: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

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Why MO theory?

MO theory explains things that Valence Bond theory does not.

1. Magnetism

2. Color of molecules

3. Excited states of molecules.

Page 87: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

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MagnetismWe learned that electrons have magnetic quantum number ms “spin”.

Electrons have magnetic moment.

Electrons cause magnetism.

Three kinds of magnetism:

1. Diamagnetism2. Paramagnetism3. Ferromagnetism

Page 88: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Diamagnetic Paramagnetic

Electrons all paired Unpaired electrons

Page 89: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Oxygen O2 is Paramagnetic!

O O.. ..

.... Why?

Page 90: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

MO to the rescue

Page 91: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Ferromagnetism

Like iron, pulled to a magnet.

Long range order of spins in material

N

S

Page 92: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

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MO theory and color

Remember, elements produced color because of electronsMoving from higher to lower energy levels.

With MO theory, color of molecules is explained the same way

Page 93: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

Conjugated polyenes have MO’s that give rise to colors energy is absorbed, electrons go to higher energy levels.

Page 94: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

How do we see color?

Qu

ickTim

e™

an

d a

TIF

F (

Un

com

pre

ssed

) de

com

pre

sso

rare

need

ed

to s

ee

th

is p

ictu

re.

Rhodopsin

Isomerization wiggles the rest of the protein, sends nerve signal

Page 95: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

and Bonding

How does Color Vision work?

Each rhodopsin (Rod, Blue, Green, Red) protein exhibits a different wavelength

maxima as a result of 11cis-retinal binding as a protonated Schiff base (PSB)

via a lysine residue. It is these interactions that lead to color vision and allow us

to see the whole visible spectrum.

11-cis-retinal : ~ 380 nm

11-cis-retinal SB : ~ 365 nm

11-cis-retinal PSB : ~ 440 nm

PSB in Blue Rhodopsin : ~ 410 nm

PSB in Green Rhodopsin : ~ 530 nm

PSB in Red Rhodopsin : ~ 560 nm

PSB in Rod Rhodopsin : ~ 500 nm

400 nm

700 nm

Wavelength (nm)

NH

Page 96: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

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and Bonding

QuickTime™ and aTIFF (Uncompressed) decompressor

are needed to see this picture.

You can change the energy of the MO’s of retinal by changing the environment around the molecule.

Page 97: Molecular Geometries and Bonding Chapter 9 Molecular Geometries and Bonding Theories

MolecularGeometries

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