Jump to
S1C2
Energy calculated at B2PLYP=FULLultrafine/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -79.784471 |
| Energy at 298.15K | |
| HF Energy | -79.652256 |
| Nuclear repulsion energy | 42.348174 |
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 B2PLYP=FULLultrafine/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 |
3055 |
2930 |
0.00 |
349.42 |
0.00 |
0.01 |
| 2 |
A1g |
1435 |
1376 |
0.00 |
0.03 |
0.44 |
0.61 |
| 3 |
A1g |
1010 |
968 |
0.00 |
13.02 |
0.18 |
0.30 |
| 4 |
A1u |
306 |
294 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
3055 |
2930 |
56.72 |
0.00 |
0.00 |
0.00 |
| 6 |
A2u |
1421 |
1363 |
0.88 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3103 |
2976 |
0.00 |
119.70 |
0.75 |
0.86 |
| 7 |
Eg |
3103 |
2976 |
0.00 |
119.70 |
0.75 |
0.86 |
| 8 |
Eg |
1520 |
1458 |
0.00 |
8.29 |
0.75 |
0.86 |
| 8 |
Eg |
1520 |
1458 |
0.00 |
8.29 |
0.75 |
0.86 |
| 9 |
Eg |
1234 |
1184 |
0.00 |
0.07 |
0.75 |
0.86 |
| 9 |
Eg |
1234 |
1184 |
0.00 |
0.07 |
0.75 |
0.86 |
| 10 |
Eu |
3127 |
2999 |
60.09 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3127 |
2999 |
60.09 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1522 |
1459 |
8.54 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1522 |
1459 |
8.54 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
830 |
796 |
3.25 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
830 |
796 |
3.25 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 16477.1 cm
-1
Scaled (by 0.9591) Zero Point Vibrational Energy (zpe) 15803.2 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 B2PLYP=FULLultrafine/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 |
1.015 |
1.157 |
| H4 |
-0.879 |
-0.507 |
1.157 |
| H5 |
0.879 |
-0.507 |
1.157 |
| H6 |
0.000 |
-1.015 |
-1.157 |
| H7 |
-0.879 |
0.507 |
-1.157 |
| H8 |
0.879 |
0.507 |
-1.157 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5243 | 1.0888 | 1.0888 | 1.0888 | 2.1711 | 2.1711 | 2.1711 |
C2 | 1.5243 | | 2.1711 | 2.1711 | 2.1711 | 1.0888 | 1.0888 | 1.0888 | H3 | 1.0888 | 2.1711 | | 1.7573 | 1.7573 | 3.0780 | 2.5271 | 2.5271 | H4 | 1.0888 | 2.1711 | 1.7573 | | 1.7573 | 2.5271 | 2.5271 | 3.0780 | H5 | 1.0888 | 2.1711 | 1.7573 | 1.7573 | | 2.5271 | 3.0780 | 2.5271 | H6 | 2.1711 | 1.0888 | 3.0780 | 2.5271 | 2.5271 | | 1.7573 | 1.7573 | H7 | 2.1711 | 1.0888 | 2.5271 | 2.5271 | 3.0780 | 1.7573 | | 1.7573 | H8 | 2.1711 | 1.0888 | 2.5271 | 3.0780 | 2.5271 | 1.7573 | 1.7573 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.277 |
|
C1 |
C2 |
H7 |
111.277 |
| C1 |
C2 |
H8 |
111.277 |
|
C2 |
C1 |
H3 |
111.277 |
| C2 |
C1 |
H4 |
111.277 |
|
C2 |
C1 |
H5 |
111.277 |
| H3 |
C1 |
H4 |
107.606 |
|
H3 |
C1 |
H5 |
107.606 |
| H4 |
C1 |
H5 |
107.606 |
|
H6 |
C2 |
H7 |
107.606 |
| H6 |
C2 |
H8 |
107.606 |
|
H7 |
C2 |
H8 |
107.606 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.729 |
|
|
|
| 2 |
C |
-0.729 |
|
|
|
| 3 |
H |
0.243 |
|
|
|
| 4 |
H |
0.243 |
|
|
|
| 5 |
H |
0.243 |
|
|
|
| 6 |
H |
0.243 |
|
|
|
| 7 |
H |
0.243 |
|
|
|
| 8 |
H |
0.243 |
|
|
|
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 |
-15.008 |
0.000 |
0.000 |
| y |
0.000 |
-15.008 |
0.000 |
| z |
0.000 |
0.000 |
-15.767 |
|
| Traceless |
| | x | y | z |
| x |
0.380 |
0.000 |
0.000 |
| y |
0.000 |
0.380 |
0.000 |
| z |
0.000 |
0.000 |
-0.759 |
|
| Polar |
| 3z2-r2 | -1.518 |
| 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 |
4.041 |
0.000 |
0.000 |
| y |
0.000 |
4.041 |
0.000 |
| z |
0.000 |
0.000 |
4.632 |
<r2> (average value of r
2) Å
2
| <r2> |
30.714 |
| (<r2>)1/2 |
5.542 |
Jump to
S1C1
Energy calculated at B2PLYP=FULLultrafine/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -79.780184 |
| Energy at 298.15K | |
| HF Energy | -79.647812 |
| Nuclear repulsion energy | 42.181797 |
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 B2PLYP=FULLultrafine/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' |
3070 |
2944 |
0.00 |
|
|
|
| 2 |
A1' |
1452 |
1393 |
0.00 |
|
|
|
| 3 |
A1' |
1007 |
966 |
0.00 |
|
|
|
| 4 |
A1" |
302i |
290i |
0.00 |
|
|
|
| 5 |
A2" |
3062 |
2937 |
58.85 |
|
|
|
| 6 |
A2" |
1419 |
1361 |
0.51 |
|
|
|
| 7 |
E' |
3135 |
3007 |
50.88 |
|
|
|
| 7 |
E' |
3135 |
3007 |
50.88 |
|
|
|
| 8 |
E' |
1529 |
1466 |
10.19 |
|
|
|
| 8 |
E' |
1529 |
1466 |
10.18 |
|
|
|
| 9 |
E' |
908 |
871 |
2.39 |
|
|
|
| 9 |
E' |
908 |
871 |
2.39 |
|
|
|
| 10 |
E" |
3112 |
2985 |
0.00 |
|
|
|
| 10 |
E" |
3112 |
2985 |
0.00 |
|
|
|
| 11 |
E" |
1521 |
1458 |
0.00 |
|
|
|
| 11 |
E" |
1521 |
1458 |
0.00 |
|
|
|
| 12 |
E" |
1188 |
1139 |
0.00 |
|
|
|
| 12 |
E" |
1188 |
1139 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16247.0 cm
-1
Scaled (by 0.9591) Zero Point Vibrational Energy (zpe) 15582.5 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 B2PLYP=FULLultrafine/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 |
1.011 |
1.171 |
| H4 |
-0.875 |
-0.505 |
1.171 |
| H5 |
0.875 |
-0.505 |
1.171 |
| H6 |
0.000 |
1.011 |
-1.171 |
| H7 |
0.875 |
-0.505 |
-1.171 |
| H8 |
-0.875 |
-0.505 |
-1.171 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5385 | 1.0877 | 1.0877 | 1.0877 | 2.1878 | 2.1878 | 2.1878 |
C2 | 1.5385 | | 2.1878 | 2.1878 | 2.1878 | 1.0877 | 1.0877 | 1.0877 | H3 | 1.0877 | 2.1878 | | 1.7506 | 1.7506 | 2.3421 | 2.9241 | 2.9241 | H4 | 1.0877 | 2.1878 | 1.7506 | | 1.7506 | 2.9241 | 2.9241 | 2.3421 | H5 | 1.0877 | 2.1878 | 1.7506 | 1.7506 | | 2.9241 | 2.3421 | 2.9241 | H6 | 2.1878 | 1.0877 | 2.3421 | 2.9241 | 2.9241 | | 1.7506 | 1.7506 | H7 | 2.1878 | 1.0877 | 2.9241 | 2.9241 | 2.3421 | 1.7506 | | 1.7506 | H8 | 2.1878 | 1.0877 | 2.9241 | 2.3421 | 2.9241 | 1.7506 | 1.7506 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.679 |
|
C1 |
C2 |
H7 |
111.679 |
| C1 |
C2 |
H8 |
111.679 |
|
C2 |
C1 |
H3 |
111.679 |
| C2 |
C1 |
H4 |
111.679 |
|
C2 |
C1 |
H5 |
111.679 |
| H3 |
C1 |
H4 |
107.176 |
|
H3 |
C1 |
H5 |
107.176 |
| H4 |
C1 |
H5 |
107.176 |
|
H6 |
C2 |
H7 |
107.176 |
| H6 |
C2 |
H8 |
107.176 |
|
H7 |
C2 |
H8 |
107.176 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.747 |
|
|
|
| 2 |
C |
-0.747 |
|
|
|
| 3 |
H |
0.249 |
|
|
|
| 4 |
H |
0.249 |
|
|
|
| 5 |
H |
0.249 |
|
|
|
| 6 |
H |
0.249 |
|
|
|
| 7 |
H |
0.249 |
|
|
|
| 8 |
H |
0.249 |
|
|
|
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 |
-14.993 |
0.000 |
0.000 |
| y |
0.000 |
-14.993 |
0.000 |
| z |
0.000 |
0.000 |
-15.759 |
|
| Traceless |
| | x | y | z |
| x |
0.383 |
0.000 |
0.000 |
| y |
0.000 |
0.383 |
0.000 |
| z |
0.000 |
0.000 |
-0.765 |
|
| Polar |
| 3z2-r2 | -1.531 |
| 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 |
4.007 |
0.000 |
0.000 |
| y |
0.000 |
4.007 |
0.000 |
| z |
0.000 |
0.000 |
4.651 |
<r2> (average value of r
2) Å
2
| <r2> |
30.983 |
| (<r2>)1/2 |
5.566 |