Orbitals and Covalent Bond

Orbitals and Covalent Bond Molecular Orbitals  The overlap of atomic orbitals from separate atoms makes molecular orbitals  Each molecular orbita...
Author: Miles Hunt
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Orbitals and Covalent Bond

Molecular Orbitals  The overlap of atomic orbitals from separate atoms

makes molecular orbitals  Each molecular orbital has room for two electrons  Two types of MO  Sigma ( σ ) between atoms  Pi ( π ) above and below atoms

Sigma bonding orbitals  From s orbitals on separate atoms +

+

s orbital s orbital

+ +

+ +

Sigma bonding molecular orbital

Sigma bonding orbitals  From p orbitals on separate atoms ⊕



p orbital

p orbital









Sigma bonding molecular orbital

Pi bonding orbitals ⊕ ⊕





⊕ ⊕

 p orbitals on separate atoms

Pi bonding molecular orbital

Sigma and pi bonds  All single bonds are sigma bonds  A double bond is one sigma and one pi bond  A triple bond is one sigma and two pi bonds.

Atomic Orbitals Don’t Work  to explain molecular geometry.  In methane, CH4 , the shape s tetrahedral.  The valence electrons of carbon should be two in s,

and two in p.  the p orbitals would have to be at right angles.  The atomic orbitals change when making a molecule

Hybridization  We blend the s and p orbitals of the valence electrons

and end up with the tetrahedral geometry.  We combine one s orbital and 3 p orbitals.

 sp3 hybridization has tetrahedral geometry.

In terms of energy 2p Energy

Hybridization

2s

sp3

How we get to hybridization  We know the geometry from experiment.  We know the orbitals of the atom  hybridizing atomic orbitals can explain the

geometry.  So if the geometry requires a tetrahedral shape, it is sp3 hybridized  This includes bent and trigonal pyramidal molecules because one of the sp3 lobes holds the lone pair.

2 sp

hybridization

 C2H4

 Double bond acts as one pair.  trigonal planar  Have to end up with three blended orbitals.

 Use one s and two p orbitals to make sp2 orbitals.  Leaves one p orbital perpendicular.

In terms of energy 2p Energy

Hybridization

2s

2p sp2

Where is the P orbital?  Perpendicular  The overlap of orbitals

makes a sigma bond (σ bond)

Two types of Bonds  Sigma bonds from overlap of orbitals.  Between the atoms.  Pi bond (π bond) above and below atoms  Between adjacent p orbitals.  The two bonds of a

double bond.

H

H C

H

C H

2 sp

hybridization

 When three things come off atom.  trigonal planar  120º  One π bond, σ + lp =3

What about two  When two things come off.  One s and one p hybridize.  linear

sp hybridization  End up with two lobes 180º apart.  p orbitals are at right angles  Makes room for two π bonds and

two sigma bonds.  A triple bond or two double bonds.

In terms of energy 2p Energy

Hybridization

2s

2p sp

CO2

 C can make two σ and two π  O can make one σ and one π

O

C O

N2

N2

Breaking the octet  PCl5

 The model predicts that we must use the d orbitals.  dsp3 hybridization

 There is some controversy about how involved the d

orbitals are.

3 dsp  Trigonal bipyrimidal  can only σ bond.  can’t π bond.  basic shape for five

things.

PCl5 Can’t tell the hybridization of Cl Assume sp3 to minimize repulsion of electron pairs.

2 3 d sp  gets us to six things around  Octahedral  Only σ bond

Molecular Orbital Model  Localized Model we have learned explains much about    

bonding. It doesn’t deal well with the ideal of resonance, unpaired electrons, and bond energy. The MO model is a parallel of the atomic orbital, using quantum mechanics. Each MO can hold two electrons with opposite spins Square of wave function tells probability

What do you get?  Solve the equations for H2  HA HB

 get two orbitals  MO2 = 1sA - 1sB  MO1 = 1sA + 1sB

The Molecular Orbital Model • The molecular orbitals are centered on a line through the nuclei

 MO1 the greatest probability is between the nuclei  MO2 it is on either side of the nuclei

 this shape is called a sigma molecular orbital

The Molecular Orbital Model • In the molecule only the molecular orbitals exist, the

atomic orbitals are gone • MO1 is lower in energy than the 1s orbitals they came from.  This favors molecule formation  Called an bonding orbital

• MO2 is higher in energy

 This goes against bonding  antibonding orbital

The Molecular Orbital Model Energy

MO2 1s

H2

1s

MO1

The Molecular Orbital Model • We use labels to indicate shapes, and whether the MO’s are bonding or antibonding.  MO1 = σ1s

 MO2 = σ1s* (* indicates antibonding)

• Can write them the same way as atomic orbitals 2

 H2 = σ1s

The Molecular Orbital Model • Each MO can hold two electrons, but they must have opposite spins • Orbitals are conserved.

• The number of molecular orbitals must equal the

number atomic orbitals that are used to make them.

+

Energy

H2

σ1s* 1s

1s

σ1s

Bond Order  The difference between the number of bonding

electrons and the number of antibonding electrons divided by two

# bonding-#antibonding Bond Order = 2

Only outer orbitals bond  The 1s orbital is much smaller than the 2s orbital  When only the 2s orbitals

involved in bonding  Don’t use the σ1s or σ1s*  Li2 = (σ2s)2

are for Li2

 In order to participate in bonds the orbitals must

overlap in space.

Bonding in Homonuclear Diatomic Molecules

 Need to use Homonuclear so that we know the relative energies.  Li2-

 (σ2s)2 (σ2s*)1  Be2

 (σ2s)2 (σ2s*)2

 What about the p orbitals? How do they form orbitals?  Remember that orbitals must be conserved.

B2

B2 σ2p* σ2p π2p* π2p

Expected Energy Diagram 2p

σ2p* π2p* π2p* π2p π2p

2p

σ2p σ2s* 2s

σ2s

2s

B2 2p

2p

2s

2s

B2  (σ2s)2(σ2s*)2 (σ2p)2  Bond order = (4-2) / 2  Should be stable.  This assumes there is no interaction between the s and

p orbitals.  Hard to believe since they overlap  proof comes from magnetism.

Magnetism  Magnetism has to do with electrons.  Paramagnetism attracted by a magnet.  associated with unpaired electrons.  Diamagnetism attracted by a magnet.  associated with paired electrons.  B2 is paramagnetic.

Magnetism  The energies of of the π2p and the σ2p are reversed by

p and s interacting  The σ2s and the σ2s* are no longer equally spaced.  Here’s what it looks like.

Correct energy diagram σ2p* π2p* π2p*

2p

π2p

σ2p

π2p

2p

σ2s* 2s

2s σ2s

B2

σ2p* π2p* 2p

2p

σ2p π2p σ2s*

2s

2s σ2s

Patterns As bond order increases, bond energy increases. As bond order increases, bond length decreases. Supports basis of MO model. There is not a direct correlation of bond order to bond energy.  O2 is known to be paramagnetic.    

Magnetism  Ferromagnetic strongly attracted  Paramagnetic weakly attracted  Liquid Oxygen  Diamagnetic weakly repelled  Graphite  Water Frog

Examples  C2

 N2  O2  F2  P2

Heteronuclear Diatomic Species  Simple type has them in the same energy level, so can

use the orbitals we already know.  Slight energy differences.  NO

NO

2p

2p

2s 2s

You try  NO+  CN What if they come from completely different orbitals

and energy?  HF  Simplify first by assuming that F only uses one if its 2p orbitals.  F holds onto its electrons, so they have low energy

σ∗ 1s

2p σ

Consequences  Paramagnetic  Since 2p is lower in energy, favored by electrons.  Electrons spend time closer to fluorine.  Compatible with polarity and electronegativity.

Names  sp orbitals are called the Localized electron model  σ and π Μolecular orbital model  Localized is good for geometry, doesn’t deal well with

resonance.  seeing σ bonds as localized works well  It is the π bonds in the resonance structures that can move.

π delocalized bonding  C6H6

H

H H

H

H

H

H

H

H

H

H

H

C2 H 6

NO3-

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