Jump to
S1C2
Energy calculated at B1B95/cc-pVDZ
| | hartrees |
| Energy at 0K | -79.768418 |
| Energy at 298.15K | -79.774333 |
| HF Energy | -79.768418 |
| Nuclear repulsion energy | 42.198282 |
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 B1B95/cc-pVDZ
| 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 |
3065 |
2946 |
0.00 |
264.35 |
0.01 |
0.01 |
| 2 |
A1g |
1414 |
1359 |
0.00 |
3.71 |
0.75 |
0.86 |
| 3 |
A1g |
1039 |
999 |
0.00 |
10.04 |
0.28 |
0.44 |
| 4 |
A1u |
321 |
309 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
3062 |
2944 |
58.08 |
0.00 |
0.00 |
0.00 |
| 6 |
A2u |
1382 |
1328 |
0.08 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3132 |
3010 |
0.00 |
153.42 |
0.75 |
0.86 |
| 7 |
Eg |
3132 |
3010 |
0.00 |
153.42 |
0.75 |
0.86 |
| 8 |
Eg |
1478 |
1420 |
0.00 |
29.43 |
0.75 |
0.86 |
| 8 |
Eg |
1478 |
1420 |
0.00 |
29.43 |
0.75 |
0.86 |
| 9 |
Eg |
1204 |
1157 |
0.00 |
0.81 |
0.75 |
0.86 |
| 9 |
Eg |
1204 |
1157 |
0.00 |
0.81 |
0.75 |
0.86 |
| 10 |
Eu |
3156 |
3033 |
55.12 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3156 |
3033 |
55.12 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1478 |
1421 |
8.50 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1478 |
1421 |
8.49 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
820 |
788 |
5.29 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
820 |
788 |
5.29 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 16408.9 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 15772.3 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 B1B95/cc-pVDZ
Point Group is D3d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.759 |
| C2 |
0.000 |
0.000 |
-0.759 |
| H3 |
0.000 |
1.022 |
1.162 |
| H4 |
-0.885 |
-0.511 |
1.162 |
| H5 |
0.885 |
-0.511 |
1.162 |
| H6 |
0.000 |
-1.022 |
-1.162 |
| H7 |
-0.885 |
0.511 |
-1.162 |
| H8 |
0.885 |
0.511 |
-1.162 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5179 | 1.0988 | 1.0988 | 1.0988 | 2.1761 | 2.1761 | 2.1761 |
C2 | 1.5179 | | 2.1761 | 2.1761 | 2.1761 | 1.0988 | 1.0988 | 1.0988 | H3 | 1.0988 | 2.1761 | | 1.7705 | 1.7705 | 3.0955 | 2.5392 | 2.5392 | H4 | 1.0988 | 2.1761 | 1.7705 | | 1.7705 | 2.5392 | 2.5392 | 3.0955 | H5 | 1.0988 | 2.1761 | 1.7705 | 1.7705 | | 2.5392 | 3.0955 | 2.5392 | H6 | 2.1761 | 1.0988 | 3.0955 | 2.5392 | 2.5392 | | 1.7705 | 1.7705 | H7 | 2.1761 | 1.0988 | 2.5392 | 2.5392 | 3.0955 | 1.7705 | | 1.7705 | H8 | 2.1761 | 1.0988 | 2.5392 | 3.0955 | 2.5392 | 1.7705 | 1.7705 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.527 |
|
C1 |
C2 |
H7 |
111.527 |
| C1 |
C2 |
H8 |
111.527 |
|
C2 |
C1 |
H3 |
111.527 |
| C2 |
C1 |
H4 |
111.527 |
|
C2 |
C1 |
H5 |
111.527 |
| H3 |
C1 |
H4 |
107.339 |
|
H3 |
C1 |
H5 |
107.339 |
| H4 |
C1 |
H5 |
107.339 |
|
H6 |
C2 |
H7 |
107.339 |
| H6 |
C2 |
H8 |
107.339 |
|
H7 |
C2 |
H8 |
107.339 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.100 |
|
|
|
| 2 |
C |
-0.100 |
|
|
|
| 3 |
H |
0.033 |
|
|
|
| 4 |
H |
0.033 |
|
|
|
| 5 |
H |
0.033 |
|
|
|
| 6 |
H |
0.033 |
|
|
|
| 7 |
H |
0.033 |
|
|
|
| 8 |
H |
0.033 |
|
|
|
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 |
-14.706 |
0.000 |
0.000 |
| y |
0.000 |
-14.706 |
0.000 |
| z |
0.000 |
0.000 |
-15.277 |
|
| Traceless |
| | x | y | z |
| x |
0.286 |
0.000 |
0.000 |
| y |
0.000 |
0.286 |
0.000 |
| z |
0.000 |
0.000 |
-0.571 |
|
| Polar |
| 3z2-r2 | -1.143 |
| 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 |
3.498 |
0.000 |
0.000 |
| y |
0.000 |
3.498 |
0.000 |
| z |
0.000 |
0.000 |
3.889 |
<r2> (average value of r
2) Å
2
| <r2> |
30.589 |
| (<r2>)1/2 |
5.531 |
Jump to
S1C1
Energy calculated at B1B95/cc-pVDZ
| | hartrees |
| Energy at 0K | -79.763664 |
| Energy at 298.15K | |
| HF Energy | -79.763664 |
| Nuclear repulsion energy | 42.041209 |
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 B1B95/cc-pVDZ
| 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' |
3079 |
2960 |
0.00 |
|
|
|
| 2 |
A1' |
1423 |
1368 |
0.00 |
|
|
|
| 3 |
A1' |
1037 |
996 |
0.00 |
|
|
|
| 4 |
A1" |
313i |
301i |
0.00 |
|
|
|
| 5 |
A2" |
3069 |
2950 |
60.40 |
|
|
|
| 6 |
A2" |
1377 |
1324 |
0.03 |
|
|
|
| 7 |
E' |
3161 |
3038 |
43.41 |
|
|
|
| 7 |
E' |
3161 |
3038 |
43.41 |
|
|
|
| 8 |
E' |
1481 |
1424 |
10.64 |
|
|
|
| 8 |
E' |
1481 |
1424 |
10.63 |
|
|
|
| 9 |
E' |
885 |
850 |
4.39 |
|
|
|
| 9 |
E' |
885 |
850 |
4.39 |
|
|
|
| 10 |
E" |
3141 |
3019 |
0.00 |
|
|
|
| 10 |
E" |
3141 |
3019 |
0.00 |
|
|
|
| 11 |
E" |
1475 |
1418 |
0.00 |
|
|
|
| 11 |
E" |
1475 |
1418 |
0.00 |
|
|
|
| 12 |
E" |
1153 |
1109 |
0.00 |
|
|
|
| 12 |
E" |
1153 |
1109 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16131.4 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 15505.5 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 B1B95/cc-pVDZ
Point Group is D3h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.765 |
| C2 |
0.000 |
0.000 |
-0.765 |
| H3 |
0.000 |
1.018 |
1.177 |
| H4 |
-0.881 |
-0.509 |
1.177 |
| H5 |
0.881 |
-0.509 |
1.177 |
| H6 |
0.000 |
1.018 |
-1.177 |
| H7 |
0.881 |
-0.509 |
-1.177 |
| H8 |
-0.881 |
-0.509 |
-1.177 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5309 | 1.0977 | 1.0977 | 1.0977 | 2.1928 | 2.1928 | 2.1928 |
C2 | 1.5309 | | 2.1928 | 2.1928 | 2.1928 | 1.0977 | 1.0977 | 1.0977 | H3 | 1.0977 | 2.1928 | | 1.7627 | 1.7627 | 2.3538 | 2.9407 | 2.9407 | H4 | 1.0977 | 2.1928 | 1.7627 | | 1.7627 | 2.9407 | 2.9407 | 2.3538 | H5 | 1.0977 | 2.1928 | 1.7627 | 1.7627 | | 2.9407 | 2.3538 | 2.9407 | H6 | 2.1928 | 1.0977 | 2.3538 | 2.9407 | 2.9407 | | 1.7627 | 1.7627 | H7 | 2.1928 | 1.0977 | 2.9407 | 2.9407 | 2.3538 | 1.7627 | | 1.7627 | H8 | 2.1928 | 1.0977 | 2.9407 | 2.3538 | 2.9407 | 1.7627 | 1.7627 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
112.012 |
|
C1 |
C2 |
H7 |
112.012 |
| C1 |
C2 |
H8 |
112.012 |
|
C2 |
C1 |
H3 |
112.012 |
| C2 |
C1 |
H4 |
112.012 |
|
C2 |
C1 |
H5 |
112.012 |
| H3 |
C1 |
H4 |
106.815 |
|
H3 |
C1 |
H5 |
106.815 |
| H4 |
C1 |
H5 |
106.815 |
|
H6 |
C2 |
H7 |
106.815 |
| H6 |
C2 |
H8 |
106.815 |
|
H7 |
C2 |
H8 |
106.815 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.101 |
|
|
|
| 2 |
C |
-0.101 |
|
|
|
| 3 |
H |
0.034 |
|
|
|
| 4 |
H |
0.034 |
|
|
|
| 5 |
H |
0.034 |
|
|
|
| 6 |
H |
0.034 |
|
|
|
| 7 |
H |
0.034 |
|
|
|
| 8 |
H |
0.034 |
|
|
|
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 |
-14.696 |
0.000 |
0.000 |
| y |
0.000 |
-14.696 |
0.000 |
| z |
0.000 |
0.000 |
-15.266 |
|
| Traceless |
| | x | y | z |
| x |
0.285 |
0.000 |
0.000 |
| y |
0.000 |
0.285 |
0.000 |
| z |
0.000 |
0.000 |
-0.570 |
|
| Polar |
| 3z2-r2 | -1.140 |
| 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 |
3.426 |
0.000 |
0.000 |
| y |
0.000 |
3.426 |
0.000 |
| z |
0.000 |
0.000 |
3.838 |
<r2> (average value of r
2) Å
2
| <r2> |
30.853 |
| (<r2>)1/2 |
5.555 |