Jump to
S1C2
Energy calculated at B3PW91/6-31G*
| | hartrees |
| Energy at 0K | -79.801762 |
| Energy at 298.15K | -79.807671 |
| HF Energy | -79.801762 |
| Nuclear repulsion energy | 42.170485 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at B3PW91/6-31G*
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1g |
3057 |
2924 |
0.00 |
|
|
|
| 2 |
A1g |
1450 |
1387 |
0.00 |
|
|
|
| 3 |
A1g |
1025 |
981 |
0.00 |
|
|
|
| 4 |
A1u |
313 |
300 |
0.00 |
|
|
|
| 5 |
A2u |
3057 |
2925 |
58.17 |
|
|
|
| 6 |
A2u |
1424 |
1362 |
1.41 |
|
|
|
| 7 |
Eg |
3117 |
2982 |
0.00 |
|
|
|
| 7 |
Eg |
3117 |
2982 |
0.00 |
|
|
|
| 8 |
Eg |
1529 |
1462 |
0.00 |
|
|
|
| 8 |
Eg |
1529 |
1462 |
0.00 |
|
|
|
| 9 |
Eg |
1230 |
1177 |
0.00 |
|
|
|
| 9 |
Eg |
1230 |
1177 |
0.00 |
|
|
|
| 10 |
Eu |
3141 |
3005 |
66.33 |
|
|
|
| 10 |
Eu |
3141 |
3005 |
66.34 |
|
|
|
| 11 |
Eu |
1532 |
1466 |
9.57 |
|
|
|
| 11 |
Eu |
1532 |
1466 |
9.56 |
|
|
|
| 12 |
Eu |
831 |
795 |
6.00 |
|
|
|
| 12 |
Eu |
831 |
795 |
6.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16542.3 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 15826.0 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at B3PW91/6-31G*
Point Group is D3d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.763 |
| C2 |
0.000 |
0.000 |
-0.763 |
| H3 |
0.000 |
1.021 |
1.162 |
| H4 |
-0.884 |
-0.510 |
1.162 |
| H5 |
0.884 |
-0.510 |
1.162 |
| H6 |
0.000 |
-1.021 |
-1.162 |
| H7 |
-0.884 |
0.510 |
-1.162 |
| H8 |
0.884 |
0.510 |
-1.162 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5256 | 1.0961 | 1.0961 | 1.0961 | 2.1790 | 2.1790 | 2.1790 |
C2 | 1.5256 | | 2.1790 | 2.1790 | 2.1790 | 1.0961 | 1.0961 | 1.0961 | H3 | 1.0961 | 2.1790 | | 1.7678 | 1.7678 | 3.0937 | 2.5389 | 2.5389 | H4 | 1.0961 | 2.1790 | 1.7678 | | 1.7678 | 2.5389 | 2.5389 | 3.0937 | H5 | 1.0961 | 2.1790 | 1.7678 | 1.7678 | | 2.5389 | 3.0937 | 2.5389 | H6 | 2.1790 | 1.0961 | 3.0937 | 2.5389 | 2.5389 | | 1.7678 | 1.7678 | H7 | 2.1790 | 1.0961 | 2.5389 | 2.5389 | 3.0937 | 1.7678 | | 1.7678 | H8 | 2.1790 | 1.0961 | 2.5389 | 3.0937 | 2.5389 | 1.7678 | 1.7678 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.381 |
|
C1 |
C2 |
H7 |
111.381 |
| C1 |
C2 |
H8 |
111.381 |
|
C2 |
C1 |
H3 |
111.381 |
| C2 |
C1 |
H4 |
111.381 |
|
C2 |
C1 |
H5 |
111.381 |
| H3 |
C1 |
H4 |
107.496 |
|
H3 |
C1 |
H5 |
107.496 |
| H4 |
C1 |
H5 |
107.496 |
|
H6 |
C2 |
H7 |
107.496 |
| H6 |
C2 |
H8 |
107.496 |
|
H7 |
C2 |
H8 |
107.496 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.503 |
|
|
|
| 2 |
C |
-0.503 |
|
|
|
| 3 |
H |
0.168 |
|
|
|
| 4 |
H |
0.168 |
|
|
|
| 5 |
H |
0.168 |
|
|
|
| 6 |
H |
0.168 |
|
|
|
| 7 |
H |
0.168 |
|
|
|
| 8 |
H |
0.168 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
-0.008 |
0.000 |
0.000 |
0.008 |
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.604 |
0.000 |
0.000 |
| y |
0.000 |
-14.604 |
0.000 |
| z |
0.000 |
0.000 |
-15.115 |
|
| Traceless |
| | x | y | z |
| x |
0.255 |
0.000 |
0.000 |
| y |
0.000 |
0.255 |
0.000 |
| z |
0.000 |
0.000 |
-0.510 |
|
| Polar |
| 3z2-r2 | -1.021 |
| x2-y2 | 0.000 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.334 |
0.000 |
0.000 |
| y |
0.000 |
3.334 |
0.000 |
| z |
0.000 |
0.000 |
3.564 |
<r2> (average value of r
2) Å
2
| <r2> |
30.567 |
| (<r2>)1/2 |
5.529 |
Jump to
S1C1
Energy calculated at B3PW91/6-31G*
| | hartrees |
| Energy at 0K | -79.797282 |
| Energy at 298.15K | |
| HF Energy | -79.797282 |
| Nuclear repulsion energy | 42.009122 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at B3PW91/6-31G*
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1' |
3072 |
2939 |
0.00 |
|
|
|
| 2 |
A1' |
1472 |
1408 |
0.00 |
|
|
|
| 3 |
A1' |
1023 |
979 |
0.00 |
|
|
|
| 4 |
A1" |
305i |
292i |
0.00 |
|
|
|
| 5 |
A2" |
3065 |
2932 |
59.88 |
|
|
|
| 6 |
A2" |
1424 |
1362 |
1.31 |
|
|
|
| 7 |
E' |
3148 |
3011 |
54.85 |
|
|
|
| 7 |
E' |
3148 |
3011 |
54.85 |
|
|
|
| 8 |
E' |
1538 |
1472 |
10.94 |
|
|
|
| 8 |
E' |
1538 |
1472 |
10.94 |
|
|
|
| 9 |
E' |
912 |
872 |
5.60 |
|
|
|
| 9 |
E' |
912 |
872 |
5.60 |
|
|
|
| 10 |
E" |
3127 |
2992 |
0.00 |
|
|
|
| 10 |
E" |
3127 |
2992 |
0.00 |
|
|
|
| 11 |
E" |
1528 |
1462 |
0.00 |
|
|
|
| 11 |
E" |
1528 |
1462 |
0.00 |
|
|
|
| 12 |
E" |
1181 |
1130 |
0.00 |
|
|
|
| 12 |
E" |
1181 |
1130 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16309.7 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 15603.5 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at B3PW91/6-31G*
Point Group is D3h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.770 |
| C2 |
0.000 |
0.000 |
-0.770 |
| H3 |
0.000 |
1.016 |
1.177 |
| H4 |
-0.880 |
-0.508 |
1.177 |
| H5 |
0.880 |
-0.508 |
1.177 |
| H6 |
0.000 |
1.016 |
-1.177 |
| H7 |
0.880 |
-0.508 |
-1.177 |
| H8 |
-0.880 |
-0.508 |
-1.177 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5391 | 1.0950 | 1.0950 | 1.0950 | 2.1961 | 2.1961 | 2.1961 |
C2 | 1.5391 | | 2.1961 | 2.1961 | 2.1961 | 1.0950 | 1.0950 | 1.0950 | H3 | 1.0950 | 2.1961 | | 1.7601 | 1.7601 | 2.3545 | 2.9397 | 2.9397 | H4 | 1.0950 | 2.1961 | 1.7601 | | 1.7601 | 2.9397 | 2.9397 | 2.3545 | H5 | 1.0950 | 2.1961 | 1.7601 | 1.7601 | | 2.9397 | 2.3545 | 2.9397 | H6 | 2.1961 | 1.0950 | 2.3545 | 2.9397 | 2.9397 | | 1.7601 | 1.7601 | H7 | 2.1961 | 1.0950 | 2.9397 | 2.9397 | 2.3545 | 1.7601 | | 1.7601 | H8 | 2.1961 | 1.0950 | 2.9397 | 2.3545 | 2.9397 | 1.7601 | 1.7601 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.862 |
|
C1 |
C2 |
H7 |
111.862 |
| C1 |
C2 |
H8 |
111.862 |
|
C2 |
C1 |
H3 |
111.862 |
| C2 |
C1 |
H4 |
111.862 |
|
C2 |
C1 |
H5 |
111.862 |
| H3 |
C1 |
H4 |
106.978 |
|
H3 |
C1 |
H5 |
106.978 |
| H4 |
C1 |
H5 |
106.979 |
|
H6 |
C2 |
H7 |
106.978 |
| H6 |
C2 |
H8 |
106.978 |
|
H7 |
C2 |
H8 |
106.979 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.512 |
|
|
|
| 2 |
C |
-0.512 |
|
|
|
| 3 |
H |
0.171 |
|
|
|
| 4 |
H |
0.171 |
|
|
|
| 5 |
H |
0.171 |
|
|
|
| 6 |
H |
0.171 |
|
|
|
| 7 |
H |
0.171 |
|
|
|
| 8 |
H |
0.171 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.589 |
0.000 |
0.000 |
| y |
0.000 |
-14.589 |
0.000 |
| z |
0.000 |
0.000 |
-15.038 |
|
| Traceless |
| | x | y | z |
| x |
0.225 |
0.000 |
0.000 |
| y |
0.000 |
0.225 |
0.000 |
| z |
0.000 |
0.000 |
-0.450 |
|
| Polar |
| 3z2-r2 | -0.899 |
| x2-y2 | 0.000 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.266 |
0.000 |
0.000 |
| y |
0.000 |
3.266 |
0.000 |
| z |
0.000 |
0.000 |
3.484 |
<r2> (average value of r
2) Å
2
| <r2> |
30.823 |
| (<r2>)1/2 |
5.552 |