inorganic bonding - molecular orbital theory Flashcards

(64 cards)

1
Q

what is molecular orbital theory?

A

the idea that during bonding, electrons are placed into multicentre molecular orbitals, and are delocalised over the whole molecule

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2
Q

give 2 approximations that MO theory requires

A

1- orbital approximation - that the overall wavefunction of a molecule with N electrons can be written as the product of N single-electron wavefunctions
2- the linear combination of atomic orbitals - as atomic orbitals are single electron wavefunctions that can interact with each other, MOs are formed from weighted sums of atomic orbitals (in-phase by addition, out-of-phase by subtraction)

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3
Q

molecular orbital definition

A

the single electron wave functions in molecules

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4
Q

what is the purpose of a normalisation constant, N?

A

for the linear combination of atomic orbitals, a normalisation constant must be used to ensure the wave function remains a single electron wavefunction

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5
Q

bonding orbital definition

A

the molecular orbital created from the in-phase combination of similar orbitals

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6
Q

what does it mean if electron density is enhanced between the nuclei?

A

bond formation

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7
Q

what does it mean if electron density is reduced between nuclei?

A

bond is broken/no bond is formed

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8
Q

antibonding orbital definition

A

molecular orbital created from out-of-phase combination of orbitals

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9
Q

what orbitals are given from the in-phase and out-of-phase combinations of 2 1s orbitals?

A

1 orbitals are formed:
in-phase gives σg bonding MO
out-of-phase gives σu* antibonding MO

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10
Q

what does σ mean in terms of orbitals?

A

refers to single/standard bonding/antibonding MOs - a σ orbital has cylindrical symmetry, it can be rotated about the internuclear axis with no change in appearance

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11
Q

what do g and u mean in terms of orbitals?

A

this refers to symmetry about an inversion centre, they are parity labels
g = gerade, meaning the orbital stays the same on inversion (symmetrical)
u = ungerade, meaning the orbital changes on inversion (not symmetrical)

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12
Q

what does * mean in terms of orbitals?

A

this indicated the presence of a nodal plane between the nuclei, this means it is an antibonding orbital

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13
Q

give the notation for single bonding and antibonding orbtials

A

bonding - σg
antibonding - σu*

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14
Q

describe the energetic differences between bonding and antibonding MOs

A

bonding MOs are always at a lower energy than the initial atomic orbitals, indicating stability
antibonding MOs are always at a higher energy to the initial atomic orbitals

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15
Q

what does π mean in terms of orbitals?

A

π refers to directional interactions of p-orbitals, such as sideways overlap - indicated double/triple bonds

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16
Q

how do π orbitals differ to σ orbitals?

A

π bonding orbitals are asymmetric when inverted
π antibonding orbitals are symmetric when inverted
- this is opposite to σ orbitals
therefore bonding = πu and antibonding = πg*

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17
Q

how do p-orbitals interact to form MOs?

A

p-orbitals are directional so they don’t all interact the same way:
pz orbitals interact in-phase to form σg bonding orbitals, and out-of-phase to form σu* antibonding orbitals
py and px orbitals can interact in-phase to form πu bonding orbitals, and out-of-phase to form πg* antibonding orbitals

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18
Q

what is the difference between π orbitals created from sideways overlap of px orbitals and py orbitals?

A

there is no difference, other than direction
both sets of πu/πg* MOs are degenerate

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19
Q

describe the energetic differences between π and σ bonding and antibonding MOs

A

π interactions are less efficient than σ interactions, so π MOs are stabilised/destabilised to a lesser degree than σ MOs

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20
Q

can 2 different types of p-orbitals interact to form π bonds?

A

no, must be px+px/py+py, cannot be px+py/pz
this is because p-orbitals are directional, so there is no net interaction between 2 different types of p-orbital as they cannot overlap without the interaction cancelling out (essentially, fully in-phase or out-of-phase interaction is not possible)

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21
Q

π-bonds are most common for period 2 elements, why?

A

π interactions are more sensitive to distance than σ interactions, and π-bonds/double bonds are much shorter, so best suit period 2 elements which have small atomic radii

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22
Q

how is bond order calculated?

A

no. filled bonding orbitals - no. filled antibonding orbitals

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23
Q

how are MOs filled?

A

electrons are places in MOs using aufbau + pauli principle + hunds first rule

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24
Q

why can UV radiation break bonds, in terms of molecular orbitals?

A

UV radiation is of high enough energy that it is able to promote an electron from the bonding to antibonding orbitals, thus the excited species is left with a bond order of 1 less than before, indicating that a bond was broken
e.g. bond order 1 -> bond order 0

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25
how can bond order be used to determine if molecules can exist?
a molecule can only exist if bond order between atoms is greater than 0 - if bond order = 0 or less, there is no stabilisation upon formation of the molecule, so it will not happen - does not have to be a whole number! just has to be >0
26
the bond dissociation enthalpy for Li2 is less than for H2, why?
Li2 involved interaction between 2s orbitals, whereas H2 uses 1s orbital interactions, 2s orbitals are more diffuse than 1s so their interaction in Li2 is less than the interaction in H2, so less energy is needed to break the bond
27
how can H2 become an electrical conductor?
electrons can hop in between H2+ ions when is it in the form of a metallic fluid, free flowing electrons means it can carry a charge - this metallic fluid is formed from H2 at very high pressures
28
HOMO definition
highest occupied molecular orbital
29
LUMO definition
lowest occupied molecular orbital
30
paramagnetism definition
an atoms weak attraction to a magnet
31
why does paramagnetism occur?
occurs when parallel electron spins are able to align with an applied magnetic field, so they behave as tiny magnets
32
give one use of paramagnetism
paramagnetism of O2 can be used to measure O2 content in air by measuring magnetism of the gas - this is used in premature baby incubators
33
diamagnetism definition
an atoms weak repulsion from a magnet - this is a much weaker effect than paramagnetism
34
when does diamagnetism occur?
occurs in atoms/molecules with fully paired electrons
35
why do peroxide O2^2- ions and superoxide ions O2^- have different BDEs?
they have different bond orders: peroxide bond order = 1 superoxide bond order = 1.5 so superoxide bond is stronger, so must have a greater BDE
36
outline the relationship between bond order and bond strength
the greater the bond order, the stronger the bond
37
isoelectronic definition
refers to 2 atoms/molecules which the same electronic structure + no. of valence electrons
38
s-p mixing definition
the interaction between σ orbitals derived from s and p atomic orbitals
39
how does s-p mixing affect the energies of MOs?
stabilises s based σu and establishes p based σ g therefore pushing σg orbital above πu orbitals π orbitals are unaffected by s-p mixing as they are of the wrong symmetry to interact with the σ orbitals
40
name 1 compound in which s-p mixing takes place
N2 - this is why σ and π orbitals are out of typical order also occurs in O2 and F2 but it is much weaker, and so isn't enough to move orbitals out of order
41
how does s-p mixing change across a period (L ->R) ?
across the period the s-p gap increases so s-p mixing becomes less significant - the s-p gap increases because increasing nuclear charge pulls electrons towards nucleus, Zeff increases across a period, which stabilises s and p orbitals, but s orbitals are stabilised to a greater extent than p as s is more penetrating
42
how are energies for individual MOs calculated?
ionisation energy is measured using photoelectron spectroscopy - the sample is bombarded with photons and kinetic energy of expelled electrons is measured photon energy = IE + electron kinetic energy
43
give the 3 possible interactions of d-orbitals
end on interaction gives σ orbitals edge on interaction gives π orbitals face on interaction gives δ orbitals
44
how can stability of atomic orbitals be determined for heteronuclear diatomics?
the more electronegative atom has its valence orbitals at lower energy
45
give the wavefunction for a heteronuclear diatomic molecule
bonding orbital: Ψ = N[Cxϕx + Cyϕy] for molecule X-Y, where Cx and Cy are unequal constants antibonding : Ψ* = N*[C'xϕx - C'yϕy] where C'x and C'y are unequal constants
46
how are Cx and Cy affected by electronegativity?
if Y is more electronegative than X, Cy > Cx, meaning the more electronegative atom contributes more to the bonding orbital, distribution of electrons is towards Y
47
how are C'x and C'y affected by electronegativity?
if Y is more electronegative than X, C'x > C'y, meaning the more electropositive atom contributes more to the antibonding orbital
48
how are g/u MO labels changed for heteronuclear diatomics?
they are not used because inversion changes the positions of the nuclei (no symmetry)
49
how are atoms in molecules different to free atoms?
atoms in molecules can change the shapes/energies of their atomic orbitals to provide the best overlap + maximise bonding
50
how is energy conserved in MO theory?
total energy of new molecular orbital set must = total energy of original atomic orbitals
51
why is it difficult to extend MO theory from diatomic to polyatomics?
this is because it is difficult to identify which atomic orbitals have the correct symmetry to interact together, this is explained using group theory - exception is linear molecules
52
describe the bonding in a linear molecule AX2, where A is a group 2 element, using a valence bond theory approach
electronic configuration ends in s2, since molecule structure is linear, we know sp hybridisation will occur as 2 sp hybrid orbitals are 180 apart so s + pz -> 2 sp hybrids, + px + py new directional sp hybrid orbitals engage with X atoms forming 2 σ bonds and remaining p orbitals stay unoccupied
53
describe the bonding in a linear molecule AX2, where A is a group 2 element, using an MO theory approach
combinations of X orbitals can interact with A orbitals of the same symmetry, in-phase combinations have the correct symmetry to interact with A orbitals to give 2 sets of bonding/antibonding orbitals, px and py cannot interact with X orbitals so form non bonding orbitals MO diagram shows 2 lowest bonding orbitals are both occupied, one for each A-X bond, although these orbitals are different, the 2 A-X bonds are identical as electron density from both bonding orbitals contributes to each bond
54
what is the purpose of partial molecular orbital schemes?
can provide good understanding of bonding in a molecule, especially useful for explaining bonding in electron poor/rich compounds that do not obey the octet rule
55
hypervalent compounds definition
compounds in which the central atom breaks the octet rule - elements in period 3+ are capable of forming these
56
how are hypervalent compounds accounted for by valence bond theory?
d-orbitals are included in the hybridisation, allowing for geometries in which the octet has been expanded
57
what is the hybridisation in square planar complexes?
dsp2, involving dx2y2 / px / py / s
58
what is the hybridisation in trigonal bipyramidal complexes?
dsp3, involving dz2 / all p and s
59
what is the hybridisation in square pyramidal complexes?
dsp3, involving dx2y2 / all p and s
60
what is the hybridisation in octahedral complexes?
d2sp3, involving dx2y2 / dz2 / all p and s
61
why is MO theory preferred for modelling the bonding in hypervalent compounds?
valence bond theory approach can result in strange non whole number bond orders
62
how are hypervalent compounds accounted for using MO theory?
e.g. PF5 = trigonal bipyramidal molecule with 10 ve- equatorial bonds are based on sp2 (px+py) hybridisation of central P atom interacting with F p-orbitals, average bond order = 1 axial bonded F atoms interact with P both via pz orbitals (left over from hybridisation)
63
explain bridging of group 13 atoms like B using valence bond theory
B has 3 valence electrons each B = sp3 hybridised as tetrahedral 2 sp3 hybrid orbitals interact with with H 1s orbital forming B-H σ bonds - uses up 2 electrons from B remaining electron from B in 1 remaining sp3 orbital, the other is empty - both hybrid orbitals are involved with bridging H atoms, each bridge containing 1 electron (electrons are delocalised around the bridging)
64
explain bridging of group 13 atoms like B using MO theory
bonding orbital formed by in-phase combination of B and H orbitals antibonding orbital formed by out-of-phase combination of B and H orbitals out of phase combinations of B orbitals do not have the correct symmetry to interact with H 1s orbital therefore 2 leftover B sp3 orbitals from both B atoms form the bonding, antibonding and non bonding orbitals for bridge bonds, bond order = 1 total = 0.5 per bond