Jump to
S1C2
Energy calculated at B3LYP/cc-pVQZ
| | hartrees |
| Energy at 0K | -79.870539 |
| Energy at 298.15K | -79.876440 |
| HF Energy | -79.870539 |
| Nuclear repulsion energy | 42.276054 |
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 B3LYP/cc-pVQZ
| 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 |
3025 |
2931 |
0.00 |
321.84 |
0.00 |
0.01 |
| 2 |
A1g |
1423 |
1379 |
0.00 |
0.28 |
0.69 |
0.82 |
| 3 |
A1g |
995 |
964 |
0.00 |
11.74 |
0.20 |
0.34 |
| 4 |
A1u |
304 |
294 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
3026 |
2932 |
60.12 |
0.00 |
0.00 |
0.00 |
| 6 |
A2u |
1414 |
1369 |
1.01 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3069 |
2974 |
0.00 |
134.08 |
0.75 |
0.86 |
| 7 |
Eg |
3069 |
2974 |
0.00 |
134.07 |
0.75 |
0.86 |
| 8 |
Eg |
1503 |
1456 |
0.00 |
13.52 |
0.75 |
0.86 |
| 8 |
Eg |
1503 |
1456 |
0.00 |
13.52 |
0.75 |
0.86 |
| 9 |
Eg |
1223 |
1185 |
0.00 |
0.14 |
0.75 |
0.86 |
| 9 |
Eg |
1223 |
1185 |
0.00 |
0.14 |
0.75 |
0.86 |
| 10 |
Eu |
3094 |
2998 |
65.28 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3094 |
2998 |
65.28 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1506 |
1459 |
8.85 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1506 |
1459 |
8.85 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
827 |
801 |
3.75 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
827 |
801 |
3.75 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 16316.5 cm
-1
Scaled (by 0.9688) Zero Point Vibrational Energy (zpe) 15807.4 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 B3LYP/cc-pVQZ
Point Group is D3d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.764 |
| C2 |
0.000 |
0.000 |
-0.764 |
| H3 |
0.000 |
1.015 |
1.161 |
| H4 |
-0.879 |
-0.508 |
1.161 |
| H5 |
0.879 |
-0.508 |
1.161 |
| H6 |
0.000 |
-1.015 |
-1.161 |
| H7 |
-0.879 |
0.508 |
-1.161 |
| H8 |
0.879 |
0.508 |
-1.161 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5271 | 1.0904 | 1.0904 | 1.0904 | 2.1756 | 2.1756 | 2.1756 |
C2 | 1.5271 | | 2.1756 | 2.1756 | 2.1756 | 1.0904 | 1.0904 | 1.0904 | H3 | 1.0904 | 2.1756 | | 1.7589 | 1.7589 | 3.0843 | 2.5336 | 2.5336 | H4 | 1.0904 | 2.1756 | 1.7589 | | 1.7589 | 2.5336 | 2.5336 | 3.0843 | H5 | 1.0904 | 2.1756 | 1.7589 | 1.7589 | | 2.5336 | 3.0843 | 2.5336 | H6 | 2.1756 | 1.0904 | 3.0843 | 2.5336 | 2.5336 | | 1.7589 | 1.7589 | H7 | 2.1756 | 1.0904 | 2.5336 | 2.5336 | 3.0843 | 1.7589 | | 1.7589 | H8 | 2.1756 | 1.0904 | 2.5336 | 3.0843 | 2.5336 | 1.7589 | 1.7589 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.354 |
|
C1 |
C2 |
H7 |
111.354 |
| C1 |
C2 |
H8 |
111.354 |
|
C2 |
C1 |
H3 |
111.354 |
| C2 |
C1 |
H4 |
111.354 |
|
C2 |
C1 |
H5 |
111.354 |
| H3 |
C1 |
H4 |
107.525 |
|
H3 |
C1 |
H5 |
107.525 |
| H4 |
C1 |
H5 |
107.525 |
|
H6 |
C2 |
H7 |
107.525 |
| H6 |
C2 |
H8 |
107.525 |
|
H7 |
C2 |
H8 |
107.525 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/cc-pVQZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.263 |
|
|
|
| 2 |
C |
-0.263 |
|
|
|
| 3 |
H |
0.088 |
|
|
|
| 4 |
H |
0.088 |
|
|
|
| 5 |
H |
0.088 |
|
|
|
| 6 |
H |
0.088 |
|
|
|
| 7 |
H |
0.088 |
|
|
|
| 8 |
H |
0.088 |
|
|
|
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 |
-15.013 |
0.000 |
0.000 |
| y |
0.000 |
-15.013 |
0.000 |
| z |
0.000 |
0.000 |
-15.718 |
|
| Traceless |
| | x | y | z |
| x |
0.353 |
0.000 |
0.000 |
| y |
0.000 |
0.353 |
0.000 |
| z |
0.000 |
0.000 |
-0.705 |
|
| Polar |
| 3z2-r2 | -1.410 |
| 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 |
3.990 |
0.000 |
0.000 |
| y |
0.000 |
3.990 |
0.000 |
| z |
0.000 |
0.000 |
4.522 |
<r2> (average value of r
2) Å
2
| <r2> |
30.789 |
| (<r2>)1/2 |
5.549 |
Jump to
S1C1
Energy calculated at B3LYP/cc-pVQZ
| | hartrees |
| Energy at 0K | -79.866355 |
| Energy at 298.15K | |
| HF Energy | -79.866355 |
| Nuclear repulsion energy | 42.113749 |
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 B3LYP/cc-pVQZ
| 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' |
3041 |
2946 |
0.00 |
|
|
|
| 2 |
A1' |
1439 |
1394 |
0.00 |
|
|
|
| 3 |
A1' |
992 |
961 |
0.00 |
|
|
|
| 4 |
A1" |
297i |
288i |
0.00 |
|
|
|
| 5 |
A2" |
3034 |
2940 |
61.68 |
|
|
|
| 6 |
A2" |
1411 |
1367 |
0.68 |
|
|
|
| 7 |
E' |
3102 |
3006 |
55.01 |
|
|
|
| 7 |
E' |
3102 |
3006 |
55.02 |
|
|
|
| 8 |
E' |
1511 |
1464 |
10.39 |
|
|
|
| 8 |
E' |
1511 |
1464 |
10.39 |
|
|
|
| 9 |
E' |
899 |
871 |
2.85 |
|
|
|
| 9 |
E' |
899 |
871 |
2.85 |
|
|
|
| 10 |
E" |
3080 |
2984 |
0.00 |
|
|
|
| 10 |
E" |
3080 |
2984 |
0.00 |
|
|
|
| 11 |
E" |
1503 |
1456 |
0.00 |
|
|
|
| 11 |
E" |
1503 |
1456 |
0.00 |
|
|
|
| 12 |
E" |
1175 |
1138 |
0.00 |
|
|
|
| 12 |
E" |
1175 |
1138 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16079.6 cm
-1
Scaled (by 0.9688) Zero Point Vibrational Energy (zpe) 15577.9 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 B3LYP/cc-pVQZ
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 |
1.011 |
1.175 |
| H4 |
-0.876 |
-0.506 |
1.175 |
| H5 |
0.876 |
-0.506 |
1.175 |
| H6 |
0.000 |
1.011 |
-1.175 |
| H7 |
0.876 |
-0.506 |
-1.175 |
| H8 |
-0.876 |
-0.506 |
-1.175 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5410 | 1.0892 | 1.0892 | 1.0892 | 2.1923 | 2.1923 | 2.1923 |
C2 | 1.5410 | | 2.1923 | 2.1923 | 2.1923 | 1.0892 | 1.0892 | 1.0892 | H3 | 1.0892 | 2.1923 | | 1.7519 | 1.7519 | 2.3491 | 2.9305 | 2.9305 | H4 | 1.0892 | 2.1923 | 1.7519 | | 1.7519 | 2.9305 | 2.9305 | 2.3491 | H5 | 1.0892 | 2.1923 | 1.7519 | 1.7519 | | 2.9305 | 2.3491 | 2.9305 | H6 | 2.1923 | 1.0892 | 2.3491 | 2.9305 | 2.9305 | | 1.7519 | 1.7519 | H7 | 2.1923 | 1.0892 | 2.9305 | 2.9305 | 2.3491 | 1.7519 | | 1.7519 | H8 | 2.1923 | 1.0892 | 2.9305 | 2.3491 | 2.9305 | 1.7519 | 1.7519 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.776 |
|
C1 |
C2 |
H7 |
111.776 |
| C1 |
C2 |
H8 |
111.776 |
|
C2 |
C1 |
H3 |
111.776 |
| C2 |
C1 |
H4 |
111.776 |
|
C2 |
C1 |
H5 |
111.776 |
| H3 |
C1 |
H4 |
107.071 |
|
H3 |
C1 |
H5 |
107.071 |
| H4 |
C1 |
H5 |
107.071 |
|
H6 |
C2 |
H7 |
107.071 |
| H6 |
C2 |
H8 |
107.071 |
|
H7 |
C2 |
H8 |
107.071 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/cc-pVQZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.269 |
|
|
|
| 2 |
C |
-0.269 |
|
|
|
| 3 |
H |
0.090 |
|
|
|
| 4 |
H |
0.090 |
|
|
|
| 5 |
H |
0.090 |
|
|
|
| 6 |
H |
0.090 |
|
|
|
| 7 |
H |
0.090 |
|
|
|
| 8 |
H |
0.090 |
|
|
|
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 |
-14.997 |
0.000 |
0.000 |
| y |
0.000 |
-14.997 |
0.000 |
| z |
0.000 |
0.000 |
-15.703 |
|
| Traceless |
| | x | y | z |
| x |
0.353 |
0.000 |
0.000 |
| y |
0.000 |
0.353 |
0.000 |
| z |
0.000 |
0.000 |
-0.706 |
|
| Polar |
| 3z2-r2 | -1.412 |
| 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 |
3.960 |
0.000 |
0.000 |
| y |
0.000 |
3.960 |
0.000 |
| z |
0.000 |
0.000 |
4.502 |
<r2> (average value of r
2) Å
2
| <r2> |
31.054 |
| (<r2>)1/2 |
5.573 |