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group theory
the mathematical method of describing the symmetry of an object based on its geometry
symmetry element - geometric entity like a plane, axis, point, ect that a symmetry operation is centered on (around which the operation is defined) - referred to as an object
e.g. rotating around an AXIS, reflecting across a PLANE, etc.
symmetry operation - transformations of an object into a configuration that is INDISTINGUISHABLE from the original - changing the original in a way that the transformed object looks identical to the original post-transformation
any 2 atoms interchanged by a symmetry operation are equivalent
symmetry elements
identity - E
proper rotation - Cn
reflection - sigma (σ)
improper rotation - Sn
inversion - i
identity - E
basically just a full 360 deg rotaion
trivial
every molecule has an E operation
proper rotation axis - Cn
rotation by 360/n deg, with n being an integer and replaced by the chosen integer when writing C
e.g. C2, C5, etc.
C2 = 180, C3 = 120, C4 = 90, and so on
molecules have different Cn axes of different n values at different locations
principle rotation axis (PRA) = highest order n of a molecule
z axis by convention
primes (like the ‘ applied to a Cn) - sometimes primes are used to rank and group different Cn axes
coincident (lie exactly on top of each other) with the principle rotation axis - ?
passes through more atoms - ?
mirror plane - σ
reflection across a mirror plane
3 types:
σn - horizontal, perpendicular to the PRA
σv - vertical, parallel to the PRA and actually contains it (as every axis of symmetry must cross the center of the atom) as well as a perpendicular C2 or whatever axis - makes sense, sig v always drawn in line with molecule spokes
σd - dihedral, contains PRA and cuts the space between perpendicular C2 or whatever axes
which is the “contains” in the notes doc referring to ?
molecules can have more than one σv or σd, but only ONE σh
usually going to have mirror planes between each spoke formed by an outer atom bonded to a central atom
that operation represented an Nσv, with N representing how many of this type of mirror plane there are
improper rotation axis - Sn
rotation by 350/n followed up by a reflection through a plane perpendicular to the rotation axis
works best with stuff coming off of 2 central atoms, like 2 Cs, bonded together (staggered ethane, kind of dumbell shape)
Sn of CH4 ?
inversion center
best for stuff like a cyclobutane (square ring) with alternating groups off the corners variably sticking up or down
more examples in the notes
point group
summary of all symmetry operations for a particular object
represented by a point group symbol, a shorthand name
can be used to derive all possible operations by using a character table
point group symbol ID
Does the molecule have a unique PRA, and what is the n?
Does the molecule have any C2 perpendicular to the PRA?
yes = symbol starts with D
no = symbol starts with C
Does the molecule have σh?
yes = symbol is Dnh or Cnh
no = proceed to step 4
Does the molecule have any other mirror planes?
yes = symbol is Dnd or Cnv
no = symbol is Dn or Cn
a good portion of molecules end up being C2v
high symmetries
some molecules have very high symmetries
tend to lack a unique PRA, but their point group symbols are usually easy to find
Td, Oh, Ih, Cinfv, Dinfv
inf = infinity
Td - tetrahedral, the 4 C3s running along each bond to the central atom
Oh - octahedral - C3s along each bond ?
Cinfv - linear between 2 atoms, axis is along the bond, can spin around at any angle and still look the same
no perpendicular C2
Dinfh - linear between 3 atoms
perpendicular C2
low symmetries
some molecules have very low symmetries
either have just E or E with a mirror plane or inversion center
C1 - asymmetric - e.g. tetra with all diff groups
Cs - E and σ - e.g. tetra with all but 2 diff groups
Ci - E and i, e.g. weird square ring thing
cyclic groups
C (as in the point group symbol)
do not have perpendicular C2 axes relative to the PRA
can be rotated but appear different if flipped over
dissymmetric
dihedral groups
D
have perpendicular C2 axes relative to the PRA
molecular properties
chiral molecules - only have one proper axis of rotation
possible point groups = Cn, Dn
polar molecules - only have one Cn axis and no σn
possible point groups = Cn, Cnv
anatomy of a character table
yeah I ain’t writing all dat
read it in the notes, page 7
some highlights
value of +1 indicates no change
value -1 = exact opposite
p and d orbitals assigned to one of the symmetry patterns that the molecule has
irreducible representations and their names
a basic pattern of symmetry transformations
most basic representation - cannot be further broken down
?
describes how an object/set of objects, like an orbital, changes under each of the symmetry operations in that point group
need to memorize naming rules ?
sigma
h has to be perp to a C2
v parallel to C2
don’t put a sigma where another C2 could go
octahedral
C2’ and “
sig v and d?
tetrahedral
S4
also C3 and C2 and sigv
i = S2
i is the same as rotating 180 and then flipping
more EN atoms
get the axial regions
need less room on trig bi
very high symmetry
probably no principal rotation axis
Cinfv
if the ends of the linear molecule are DIFFERENT
if onyl have E
is a C1
asymmetric
chiral with symmetry
Cn or Dn
dissymmetric
S operations
look for alternating up/down parts
complex MO diagrams solving steps
find the molecular structure - if it has a resonance form then use that one. Use FC to confirm that the form is right.
Find the symmetry of the structure and its corresponding character table
Prep MO diagram. Put central atom to the left and terminal atoms to the right. Put the combo in the middle.
Use the periodic table to find the valence orbitals (whichever ones are on the lowest row). Position those of the more EN atom closer to the bottom. Any nonbonding S has to be the lowest of all
Use the character table to find the letter designation for each central orbital.
Calc number code for terminal atom designation by testing each symmetry operation (+1 if don’t move, 0 if they do). Find the letter designations with the codes that add to the calculated number code.
Note down how many of each central bond MO there should be and tally those.
Write in the a1s first them go from there. All sets should be spaced equally relative to the AOs that form them. The bonding should be below the lowest AO that forms it and the anti above the highest, with the nobondings in between. Nonbonding should be straight across their corresponding AO. Draw lines between corresponding MO and AOs
Fill in the e-
tally up bonding (first of any MO set), antibonding (last of any set) and nonbonding (the rest and any s that were nonbonding to begin with).
Compare results to lewis structure from before.
reducible and irreducible representations
the number code you calculate for the terminal atom AO designations is a reducible representation
the codes you add up to figure out the corresponding letter designations are all IRreducible
the act of identifying the irreducible representations is called decomposing
the combo of letters you get from the calculation defining the terminal AO types is called a SALC, or symmetry adopted linear combinations
ions
ionic molecules are going to add or take away from your e- total
don’t forget this!
degeneracy
a and b are single
e is doubly degenerate - each MO has 2 orbital slots
t is triply degenerate
nonbonding effect
the orbital ends up spread across the molecule and doesn’t strongly contribute 1 way or another to bonding
discounted in BO calc
H terminal atoms
usually its 1s AO orbital is midway between the 2p and 2s AOs of the central atom
repeat MO designations
multiple AOs may call for the same MO designation
just put it once - they’re just both contributing to the same MO
if the terminal atom valence is 3p, for example
4s is likely too high energy to interact with 3p
will still be sandwiching the terminal 3p between the central 3p and 3s
e orbital position
usually listed above a1
bs also usually higher e than a1
nonbonding tally
any terminal s orbitals that are too low E to interact with the rest of the AO are also considered nonbonding
1e
probably above the lower central s AO
gonna be placed higher than any AOs not contributing to the e MO
for every bonding orbital
there must be an anti
picture of bond shading drawings
4/5/2025
number of bonding orbitals and BO
the number of bonding orbitals will only correctly predict the number of molecular bonds if the BO is a whole number!
this will also screw up the lone pair count
diatomics
since there’s only 2 atoms involved, you can get the MO letter designations of both from the table, since there isn’t the same “central-terminal” relationship going on