Jump to
S1C2
Energy calculated at wB97X-D/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -79.833211 |
| Energy at 298.15K | -79.839126 |
| HF Energy | -79.833211 |
| Nuclear repulsion energy | 42.330014 |
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 wB97X-D/aug-cc-pVTZ
| 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 |
3051 |
2919 |
0.00 |
349.02 |
0.00 |
0.01 |
| 2 |
A1g |
1431 |
1369 |
0.00 |
0.00 |
0.28 |
0.44 |
| 3 |
A1g |
1014 |
970 |
0.00 |
12.29 |
0.18 |
0.30 |
| 4 |
A1u |
305 |
292 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
3050 |
2917 |
58.22 |
0.00 |
0.00 |
0.00 |
| 6 |
A2u |
1411 |
1350 |
1.97 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3107 |
2973 |
0.00 |
119.37 |
0.75 |
0.86 |
| 7 |
Eg |
3107 |
2973 |
0.00 |
119.57 |
0.75 |
0.86 |
| 8 |
Eg |
1509 |
1444 |
0.00 |
8.26 |
0.75 |
0.86 |
| 8 |
Eg |
1509 |
1444 |
0.00 |
8.29 |
0.75 |
0.86 |
| 9 |
Eg |
1226 |
1173 |
0.00 |
0.07 |
0.75 |
0.86 |
| 9 |
Eg |
1226 |
1173 |
0.00 |
0.06 |
0.75 |
0.86 |
| 10 |
Eu |
3131 |
2995 |
61.04 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3131 |
2995 |
61.19 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1509 |
1444 |
10.18 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1509 |
1444 |
10.19 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
832 |
796 |
3.99 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
832 |
795 |
3.99 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 16445.4 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 15731.7 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 wB97X-D/aug-cc-pVTZ
Point Group is D3d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.762 |
| C2 |
0.000 |
0.000 |
-0.762 |
| H3 |
0.000 |
1.016 |
1.157 |
| H4 |
-0.880 |
-0.508 |
1.157 |
| H5 |
0.880 |
-0.508 |
1.157 |
| H6 |
0.000 |
-1.016 |
-1.157 |
| H7 |
-0.880 |
0.508 |
-1.157 |
| H8 |
0.880 |
0.508 |
-1.157 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5233 | 1.0903 | 1.0903 | 1.0903 | 2.1711 | 2.1711 | 2.1711 |
C2 | 1.5233 | | 2.1711 | 2.1711 | 2.1711 | 1.0903 | 1.0903 | 1.0903 | H3 | 1.0903 | 2.1711 | | 1.7599 | 1.7599 | 3.0796 | 2.5273 | 2.5273 | H4 | 1.0903 | 2.1711 | 1.7599 | | 1.7599 | 2.5273 | 2.5273 | 3.0796 | H5 | 1.0903 | 2.1711 | 1.7599 | 1.7599 | | 2.5273 | 3.0796 | 2.5273 | H6 | 2.1711 | 1.0903 | 3.0796 | 2.5273 | 2.5273 | | 1.7599 | 1.7599 | H7 | 2.1711 | 1.0903 | 2.5273 | 2.5273 | 3.0796 | 1.7599 | | 1.7599 | H8 | 2.1711 | 1.0903 | 2.5273 | 3.0796 | 2.5273 | 1.7599 | 1.7599 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.263 |
|
C1 |
C2 |
H7 |
111.263 |
| C1 |
C2 |
H8 |
111.263 |
|
C2 |
C1 |
H3 |
111.263 |
| C2 |
C1 |
H4 |
111.263 |
|
C2 |
C1 |
H5 |
111.263 |
| H3 |
C1 |
H4 |
107.622 |
|
H3 |
C1 |
H5 |
107.622 |
| H4 |
C1 |
H5 |
107.622 |
|
H6 |
C2 |
H7 |
107.622 |
| H6 |
C2 |
H8 |
107.622 |
|
H7 |
C2 |
H8 |
107.622 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.771 |
|
|
|
| 2 |
C |
-0.771 |
|
|
|
| 3 |
H |
0.257 |
|
|
|
| 4 |
H |
0.257 |
|
|
|
| 5 |
H |
0.257 |
|
|
|
| 6 |
H |
0.257 |
|
|
|
| 7 |
H |
0.257 |
|
|
|
| 8 |
H |
0.257 |
|
|
|
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 |
-14.801 |
0.000 |
0.000 |
| y |
0.000 |
-14.801 |
0.000 |
| z |
0.000 |
0.000 |
-15.517 |
|
| Traceless |
| | x | y | z |
| x |
0.358 |
0.000 |
0.000 |
| y |
0.000 |
0.358 |
0.000 |
| z |
0.000 |
0.000 |
-0.717 |
|
| Polar |
| 3z2-r2 | -1.434 |
| 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 |
4.053 |
0.000 |
0.000 |
| y |
0.000 |
4.053 |
0.000 |
| z |
0.000 |
0.000 |
4.610 |
<r2> (average value of r
2) Å
2
| <r2> |
30.581 |
| (<r2>)1/2 |
5.530 |
Jump to
S1C1
Energy calculated at wB97X-D/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -79.829046 |
| Energy at 298.15K | |
| HF Energy | -79.829046 |
| Nuclear repulsion energy | 42.159075 |
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 wB97X-D/aug-cc-pVTZ
| 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' |
3071 |
2938 |
0.00 |
|
|
|
| 2 |
A1' |
1453 |
1390 |
0.00 |
|
|
|
| 3 |
A1' |
1011 |
967 |
0.00 |
|
|
|
| 4 |
A1" |
288i |
276i |
0.00 |
|
|
|
| 5 |
A2" |
3063 |
2930 |
60.73 |
|
|
|
| 6 |
A2" |
1413 |
1352 |
1.25 |
|
|
|
| 7 |
E' |
3144 |
3007 |
52.53 |
|
|
|
| 7 |
E' |
3144 |
3007 |
52.75 |
|
|
|
| 8 |
E' |
1521 |
1455 |
11.85 |
|
|
|
| 8 |
E' |
1521 |
1455 |
11.82 |
|
|
|
| 9 |
E' |
913 |
874 |
2.99 |
|
|
|
| 9 |
E' |
913 |
874 |
2.96 |
|
|
|
| 10 |
E" |
3122 |
2986 |
0.00 |
|
|
|
| 10 |
E" |
3122 |
2986 |
0.00 |
|
|
|
| 11 |
E" |
1510 |
1445 |
0.00 |
|
|
|
| 11 |
E" |
1510 |
1445 |
0.00 |
|
|
|
| 12 |
E" |
1181 |
1130 |
0.00 |
|
|
|
| 12 |
E" |
1181 |
1130 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16252.6 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 15547.2 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 wB97X-D/aug-cc-pVTZ
Point Group is D3h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.769 |
| C2 |
0.000 |
0.000 |
-0.769 |
| H3 |
0.000 |
1.012 |
1.171 |
| H4 |
-0.877 |
-0.506 |
1.171 |
| H5 |
0.877 |
-0.506 |
1.171 |
| H6 |
0.000 |
1.012 |
-1.171 |
| H7 |
0.877 |
-0.506 |
-1.171 |
| H8 |
-0.877 |
-0.506 |
-1.171 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5375 | 1.0892 | 1.0892 | 1.0892 | 2.1877 | 2.1877 | 2.1877 |
C2 | 1.5375 | | 2.1877 | 2.1877 | 2.1877 | 1.0892 | 1.0892 | 1.0892 | H3 | 1.0892 | 2.1877 | | 1.7534 | 1.7534 | 2.3413 | 2.9250 | 2.9250 | H4 | 1.0892 | 2.1877 | 1.7534 | | 1.7534 | 2.9250 | 2.9250 | 2.3413 | H5 | 1.0892 | 2.1877 | 1.7534 | 1.7534 | | 2.9250 | 2.3413 | 2.9250 | H6 | 2.1877 | 1.0892 | 2.3413 | 2.9250 | 2.9250 | | 1.7534 | 1.7534 | H7 | 2.1877 | 1.0892 | 2.9250 | 2.9250 | 2.3413 | 1.7534 | | 1.7534 | H8 | 2.1877 | 1.0892 | 2.9250 | 2.3413 | 2.9250 | 1.7534 | 1.7534 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.654 |
|
C1 |
C2 |
H7 |
111.654 |
| C1 |
C2 |
H8 |
111.654 |
|
C2 |
C1 |
H3 |
111.654 |
| C2 |
C1 |
H4 |
111.654 |
|
C2 |
C1 |
H5 |
111.654 |
| H3 |
C1 |
H4 |
107.203 |
|
H3 |
C1 |
H5 |
107.203 |
| H4 |
C1 |
H5 |
107.203 |
|
H6 |
C2 |
H7 |
107.203 |
| H6 |
C2 |
H8 |
107.203 |
|
H7 |
C2 |
H8 |
107.203 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.775 |
|
|
|
| 2 |
C |
-0.775 |
|
|
|
| 3 |
H |
0.258 |
|
|
|
| 4 |
H |
0.258 |
|
|
|
| 5 |
H |
0.258 |
|
|
|
| 6 |
H |
0.258 |
|
|
|
| 7 |
H |
0.258 |
|
|
|
| 8 |
H |
0.258 |
|
|
|
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 |
-14.791 |
0.000 |
0.000 |
| y |
0.000 |
-14.791 |
0.000 |
| z |
0.000 |
0.000 |
-15.492 |
|
| Traceless |
| | x | y | z |
| x |
0.351 |
0.000 |
0.000 |
| y |
0.000 |
0.351 |
0.000 |
| z |
0.000 |
0.000 |
-0.702 |
|
| Polar |
| 3z2-r2 | -1.403 |
| 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 |
4.023 |
0.000 |
0.000 |
| y |
0.000 |
4.022 |
0.000 |
| z |
0.000 |
0.000 |
4.633 |
<r2> (average value of r
2) Å
2
| <r2> |
30.856 |
| (<r2>)1/2 |
5.555 |