Jump to
S1C2
Energy calculated at PBE1PBE/6-31G
| | hartrees |
| Energy at 0K | -79.702586 |
| Energy at 298.15K | -79.708523 |
| HF Energy | -79.702586 |
| Nuclear repulsion energy | 42.165077 |
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 PBE1PBE/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 |
3067 |
2932 |
0.00 |
223.09 |
0.01 |
0.02 |
| 2 |
A1g |
1467 |
1402 |
0.00 |
8.80 |
0.72 |
0.84 |
| 3 |
A1g |
1043 |
997 |
0.00 |
8.96 |
0.28 |
0.44 |
| 4 |
A1u |
306 |
292 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
3065 |
2929 |
58.67 |
0.00 |
0.00 |
0.00 |
| 6 |
A2u |
1464 |
1400 |
8.05 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3135 |
2997 |
0.00 |
135.22 |
0.75 |
0.86 |
| 7 |
Eg |
3135 |
2997 |
0.00 |
135.22 |
0.75 |
0.86 |
| 8 |
Eg |
1550 |
1482 |
0.00 |
45.53 |
0.75 |
0.86 |
| 8 |
Eg |
1550 |
1482 |
0.00 |
45.53 |
0.75 |
0.86 |
| 9 |
Eg |
1255 |
1200 |
0.00 |
3.65 |
0.75 |
0.86 |
| 9 |
Eg |
1255 |
1200 |
0.00 |
3.65 |
0.75 |
0.86 |
| 10 |
Eu |
3162 |
3023 |
67.18 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3162 |
3023 |
67.18 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1552 |
1484 |
14.96 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1552 |
1484 |
14.96 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
860 |
822 |
8.96 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
860 |
822 |
8.97 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 16720.1 cm
-1
Scaled (by 0.9559) Zero Point Vibrational Energy (zpe) 15982.8 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 PBE1PBE/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 | | 1.5270 | 1.0957 | 1.0957 | 1.0957 | 2.1791 | 2.1791 | 2.1791 |
C2 | 1.5270 | | 2.1791 | 2.1791 | 2.1791 | 1.0957 | 1.0957 | 1.0957 | H3 | 1.0957 | 2.1791 | | 1.7679 | 1.7679 | 3.0930 | 2.5379 | 2.5379 | H4 | 1.0957 | 2.1791 | 1.7679 | | 1.7679 | 2.5379 | 2.5379 | 3.0930 | H5 | 1.0957 | 2.1791 | 1.7679 | 1.7679 | | 2.5379 | 3.0930 | 2.5379 | H6 | 2.1791 | 1.0957 | 3.0930 | 2.5379 | 2.5379 | | 1.7679 | 1.7679 | H7 | 2.1791 | 1.0957 | 2.5379 | 2.5379 | 3.0930 | 1.7679 | | 1.7679 | H8 | 2.1791 | 1.0957 | 2.5379 | 3.0930 | 2.5379 | 1.7679 | 1.7679 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.318 |
|
C1 |
C2 |
H7 |
111.318 |
| C1 |
C2 |
H8 |
111.318 |
|
C2 |
C1 |
H3 |
111.318 |
| C2 |
C1 |
H4 |
111.318 |
|
C2 |
C1 |
H5 |
111.318 |
| H3 |
C1 |
H4 |
107.563 |
|
H3 |
C1 |
H5 |
107.563 |
| H4 |
C1 |
H5 |
107.563 |
|
H6 |
C2 |
H7 |
107.563 |
| H6 |
C2 |
H8 |
107.563 |
|
H7 |
C2 |
H8 |
107.563 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.494 |
|
|
|
| 2 |
C |
-0.494 |
|
|
|
| 3 |
H |
0.165 |
|
|
|
| 4 |
H |
0.165 |
|
|
|
| 5 |
H |
0.165 |
|
|
|
| 6 |
H |
0.165 |
|
|
|
| 7 |
H |
0.165 |
|
|
|
| 8 |
H |
0.165 |
|
|
|
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 |
-14.730 |
0.000 |
0.000 |
| y |
0.000 |
-14.730 |
0.000 |
| z |
0.000 |
0.000 |
-15.127 |
|
| Traceless |
| | x | y | z |
| x |
0.199 |
0.000 |
0.000 |
| y |
0.000 |
0.199 |
0.000 |
| z |
0.000 |
0.000 |
-0.397 |
|
| Polar |
| 3z2-r2 | -0.794 |
| 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 |
3.292 |
0.000 |
0.000 |
| y |
0.000 |
3.292 |
0.000 |
| z |
0.000 |
0.000 |
3.464 |
<r2> (average value of r
2) Å
2
| <r2> |
30.628 |
| (<r2>)1/2 |
5.534 |
Jump to
S1C1
Energy calculated at PBE1PBE/6-31G
| | hartrees |
| Energy at 0K | -79.698303 |
| Energy at 298.15K | |
| HF Energy | -79.698303 |
| Nuclear repulsion energy | 42.025771 |
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 PBE1PBE/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' |
3081 |
2945 |
0.00 |
|
|
|
| 2 |
A1' |
1491 |
1425 |
0.00 |
|
|
|
| 3 |
A1' |
1039 |
993 |
0.00 |
|
|
|
| 4 |
A1" |
298i |
285i |
0.00 |
|
|
|
| 5 |
A2" |
3071 |
2935 |
61.74 |
|
|
|
| 6 |
A2" |
1462 |
1398 |
8.48 |
|
|
|
| 7 |
E' |
3167 |
3027 |
55.33 |
|
|
|
| 7 |
E' |
3167 |
3027 |
55.33 |
|
|
|
| 8 |
E' |
1561 |
1492 |
16.85 |
|
|
|
| 8 |
E' |
1561 |
1492 |
16.85 |
|
|
|
| 9 |
E' |
938 |
897 |
9.12 |
|
|
|
| 9 |
E' |
938 |
897 |
9.12 |
|
|
|
| 10 |
E" |
3145 |
3006 |
0.00 |
|
|
|
| 10 |
E" |
3145 |
3006 |
0.00 |
|
|
|
| 11 |
E" |
1549 |
1481 |
0.00 |
|
|
|
| 11 |
E" |
1549 |
1481 |
0.00 |
|
|
|
| 12 |
E" |
1210 |
1157 |
0.00 |
|
|
|
| 12 |
E" |
1210 |
1157 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16492.1 cm
-1
Scaled (by 0.9559) Zero Point Vibrational Energy (zpe) 15764.8 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 PBE1PBE/6-31G
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 |
1.017 |
1.175 |
| H4 |
-0.881 |
-0.508 |
1.175 |
| H5 |
0.881 |
-0.508 |
1.175 |
| H6 |
0.000 |
1.017 |
-1.175 |
| H7 |
0.881 |
-0.508 |
-1.175 |
| H8 |
-0.881 |
-0.508 |
-1.175 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5384 | 1.0948 | 1.0948 | 1.0948 | 2.1942 | 2.1942 | 2.1942 |
C2 | 1.5384 | | 2.1942 | 2.1942 | 2.1942 | 1.0948 | 1.0948 | 1.0948 | H3 | 1.0948 | 2.1942 | | 1.7610 | 1.7610 | 2.3504 | 2.9369 | 2.9369 | H4 | 1.0948 | 2.1942 | 1.7610 | | 1.7610 | 2.9369 | 2.9369 | 2.3504 | H5 | 1.0948 | 2.1942 | 1.7610 | 1.7610 | | 2.9369 | 2.3504 | 2.9369 | H6 | 2.1942 | 1.0948 | 2.3504 | 2.9369 | 2.9369 | | 1.7610 | 1.7610 | H7 | 2.1942 | 1.0948 | 2.9369 | 2.9369 | 2.3504 | 1.7610 | | 1.7610 | H8 | 2.1942 | 1.0948 | 2.9369 | 2.3504 | 2.9369 | 1.7610 | 1.7610 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.767 |
|
C1 |
C2 |
H7 |
111.767 |
| C1 |
C2 |
H8 |
111.767 |
|
C2 |
C1 |
H3 |
111.767 |
| C2 |
C1 |
H4 |
111.767 |
|
C2 |
C1 |
H5 |
111.767 |
| H3 |
C1 |
H4 |
107.081 |
|
H3 |
C1 |
H5 |
107.081 |
| H4 |
C1 |
H5 |
107.081 |
|
H6 |
C2 |
H7 |
107.081 |
| H6 |
C2 |
H8 |
107.081 |
|
H7 |
C2 |
H8 |
107.081 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/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 |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.710 |
0.000 |
0.000 |
| y |
0.000 |
-14.710 |
0.000 |
| z |
0.000 |
0.000 |
-15.048 |
|
| Traceless |
| | x | y | z |
| x |
0.169 |
0.000 |
0.000 |
| y |
0.000 |
0.169 |
0.000 |
| z |
0.000 |
0.000 |
-0.338 |
|
| Polar |
| 3z2-r2 | -0.676 |
| 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 |
3.216 |
0.000 |
0.000 |
| y |
0.000 |
3.216 |
0.000 |
| z |
0.000 |
0.000 |
3.371 |
<r2> (average value of r
2) Å
2
| <r2> |
30.847 |
| (<r2>)1/2 |
5.554 |