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1
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- Orbitals and Covalent Bond
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2
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- The overlap of atomic orbitals from separate atoms makes molecular
orbitals
- Each molecular orbital has room for two electrons
- Two types of MO
- Sigma ( s ) between atoms
- Pi ( p ) above and below
atoms
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3
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- From s orbitals on separate atoms
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4
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- From p orbitals on separate atoms
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5
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- p orbitals on separate atoms
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6
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- 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.
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7
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- 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
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8
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- 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.
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9
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10
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11
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12
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13
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- 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.
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14
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- 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.
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15
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16
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17
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18
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19
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- Perpendicular
- The overlap of orbitals makes a
sigma bond (s bond)
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20
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- Sigma bonds from overlap of orbitals.
- Between the atoms.
- Pi bond (p bond) above and below atoms
- Between adjacent p orbitals.
- The two bonds of a double bond.
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21
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22
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- When three things come off atom.
- trigonal planar
- 120º
- One p bond, s + lp =3
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23
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- When two things come off.
- One s and one p hybridize.
- linear
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24
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25
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- End up with two lobes 180º apart.
- p orbitals are at right angles
- Makes room for two p bonds and two sigma bonds.
- A triple bond or two double bonds.
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26
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27
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- C can make two s and two p
- O can make one s and one p
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28
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29
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30
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- PCl5
- The model predicts that we must use the d orbitals.
- dsp3 hybridization
- There is some controversy about how involved the d orbitals are.
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31
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32
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- Trigonal bipyrimidal
- can only s bond.
- can’t p bond.
- basic shape for five things.
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33
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34
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- gets us to six things around
- Octahedral
- Only σ bond
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35
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- 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
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36
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- Solve the equations for H2
- HA HB
- get two orbitals
- MO2 = 1sA - 1sB
- MO1 = 1sA + 1sB
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37
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- 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
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38
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- 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
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39
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40
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- We use labels to indicate shapes, and whether the MO’s are bonding or
antibonding.
- MO1 = s1s
- MO2 = s1s* (* indicates antibonding)
- Can write them the same way as atomic orbitals
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41
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- 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.
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42
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43
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- The difference between the number of bonding electrons and the number of
antibonding electrons divided by two
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44
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- The 1s orbital is much smaller than the 2s orbital
- When only the 2s orbitals are involved in bonding
- Don’t use the s1s or s1s* for Li2
- Li2 = (s2s)2
- In order to participate in bonds the orbitals must overlap in space.
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45
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- Need to use Homonuclear so that we know the relative energies.
- Li2-
- (s2s)2 (s2s*)1
- Be2
- (s2s)2 (s2s*)2
- What about the p orbitals? How do they form orbitals?
- Remember that orbitals must be conserved.
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46
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47
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48
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49
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50
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- (s2s)2(s2s*)2 (s2p)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.
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51
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- 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.
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52
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- The energies of of the p2p and the s2p are
reversed by p and s interacting
- The s2s and the s2s* are no longer equally spaced.
- Here’s what it looks like.
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53
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54
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55
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- 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.
- Movie.
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56
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- Ferromagnetic strongly attracted
- Paramagnetic weakly attracted
- Diamagnetic weakly repelled
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57
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58
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- Simple type has them in the same energy level, so can use the orbitals
we already know.
- Slight energy differences.
- NO
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59
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60
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- 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
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61
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62
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- Paramagnetic
- Since 2p is lower in energy, favored by electrons.
- Electrons spend time closer to fluorine.
- Compatible with polarity and electronegativity.
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63
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- sp orbitals are called the Localized electron model
- s and p Molecular orbital model
- Localized is good for geometry, doesn’t deal well with resonance.
- seeing s bonds as localized works well
- It is the p bonds in the resonance structures that can move.
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64
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65
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66
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