Jump to
S1C2
Energy calculated at B1B95/TZVP
| | hartrees |
| Energy at 0K | -79.796276 |
| Energy at 298.15K | -79.802192 |
| HF Energy | -79.796276 |
| Nuclear repulsion energy | 42.400340 |
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/TZVP
| 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 |
3061 |
2929 |
0.00 |
291.14 |
0.01 |
0.01 |
| 2 |
A1g |
1429 |
1368 |
0.00 |
2.54 |
0.74 |
0.85 |
| 3 |
A1g |
1022 |
978 |
0.00 |
11.29 |
0.25 |
0.40 |
| 4 |
A1u |
312 |
299 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
3061 |
2929 |
58.73 |
0.00 |
0.00 |
0.00 |
| 6 |
A2u |
1407 |
1347 |
2.35 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3119 |
2984 |
0.00 |
142.37 |
0.75 |
0.86 |
| 7 |
Eg |
3119 |
2984 |
0.00 |
142.37 |
0.75 |
0.86 |
| 8 |
Eg |
1507 |
1442 |
0.00 |
26.63 |
0.75 |
0.86 |
| 8 |
Eg |
1507 |
1442 |
0.00 |
26.63 |
0.75 |
0.86 |
| 9 |
Eg |
1220 |
1168 |
0.00 |
0.66 |
0.75 |
0.86 |
| 9 |
Eg |
1220 |
1168 |
0.00 |
0.66 |
0.75 |
0.86 |
| 10 |
Eu |
3143 |
3008 |
63.45 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3143 |
3008 |
63.45 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1508 |
1443 |
11.75 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1508 |
1443 |
11.75 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
826 |
791 |
4.43 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
826 |
791 |
4.43 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 16469.9 cm
-1
Scaled (by 0.9569) Zero Point Vibrational Energy (zpe) 15760.0 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/TZVP
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 |
1.015 |
1.156 |
| H4 |
-0.879 |
-0.507 |
1.156 |
| H5 |
0.879 |
-0.507 |
1.156 |
| H6 |
0.000 |
-1.015 |
-1.156 |
| H7 |
-0.879 |
0.507 |
-1.156 |
| H8 |
0.879 |
0.507 |
-1.156 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5183 | 1.0895 | 1.0895 | 1.0895 | 2.1676 | 2.1676 | 2.1676 |
C2 | 1.5183 | | 2.1676 | 2.1676 | 2.1676 | 1.0895 | 1.0895 | 1.0895 | H3 | 1.0895 | 2.1676 | | 1.7572 | 1.7572 | 3.0767 | 2.5255 | 2.5255 | H4 | 1.0895 | 2.1676 | 1.7572 | | 1.7572 | 2.5255 | 2.5255 | 3.0767 | H5 | 1.0895 | 2.1676 | 1.7572 | 1.7572 | | 2.5255 | 3.0767 | 2.5255 | H6 | 2.1676 | 1.0895 | 3.0767 | 2.5255 | 2.5255 | | 1.7572 | 1.7572 | H7 | 2.1676 | 1.0895 | 2.5255 | 2.5255 | 3.0767 | 1.7572 | | 1.7572 | H8 | 2.1676 | 1.0895 | 2.5255 | 3.0767 | 2.5255 | 1.7572 | 1.7572 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.383 |
|
C1 |
C2 |
H7 |
111.383 |
| C1 |
C2 |
H8 |
111.383 |
|
C2 |
C1 |
H3 |
111.383 |
| C2 |
C1 |
H4 |
111.383 |
|
C2 |
C1 |
H5 |
111.383 |
| H3 |
C1 |
H4 |
107.494 |
|
H3 |
C1 |
H5 |
107.494 |
| H4 |
C1 |
H5 |
107.494 |
|
H6 |
C2 |
H7 |
107.494 |
| H6 |
C2 |
H8 |
107.494 |
|
H7 |
C2 |
H8 |
107.494 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.340 |
|
|
|
| 2 |
C |
-0.340 |
|
|
|
| 3 |
H |
0.113 |
|
|
|
| 4 |
H |
0.113 |
|
|
|
| 5 |
H |
0.113 |
|
|
|
| 6 |
H |
0.113 |
|
|
|
| 7 |
H |
0.113 |
|
|
|
| 8 |
H |
0.113 |
|
|
|
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 |
-14.859 |
0.000 |
0.000 |
| y |
0.000 |
-14.859 |
0.000 |
| z |
0.000 |
0.000 |
-15.532 |
|
| Traceless |
| | x | y | z |
| x |
0.336 |
0.000 |
0.000 |
| y |
0.000 |
0.336 |
0.000 |
| z |
0.000 |
0.000 |
-0.672 |
|
| Polar |
| 3z2-r2 | -1.345 |
| 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 |
3.755 |
0.000 |
0.000 |
| y |
0.000 |
3.755 |
0.000 |
| z |
0.000 |
0.000 |
4.096 |
<r2> (average value of r
2) Å
2
| <r2> |
30.536 |
| (<r2>)1/2 |
5.526 |
Jump to
S1C1
Energy calculated at B1B95/TZVP
| | hartrees |
| Energy at 0K | -79.791887 |
| Energy at 298.15K | |
| HF Energy | -79.791887 |
| Nuclear repulsion energy | 42.241856 |
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/TZVP
| 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' |
3077 |
2944 |
0.00 |
|
|
|
| 2 |
A1' |
1447 |
1384 |
0.00 |
|
|
|
| 3 |
A1' |
1020 |
976 |
0.00 |
|
|
|
| 4 |
A1" |
301i |
288i |
0.00 |
|
|
|
| 5 |
A2" |
3070 |
2938 |
63.40 |
|
|
|
| 6 |
A2" |
1406 |
1345 |
2.67 |
|
|
|
| 7 |
E' |
3151 |
3015 |
52.38 |
|
|
|
| 7 |
E' |
3151 |
3015 |
52.38 |
|
|
|
| 8 |
E' |
1515 |
1450 |
14.18 |
|
|
|
| 8 |
E' |
1515 |
1450 |
14.17 |
|
|
|
| 9 |
E' |
901 |
862 |
4.02 |
|
|
|
| 9 |
E' |
901 |
862 |
4.01 |
|
|
|
| 10 |
E" |
3129 |
2994 |
0.00 |
|
|
|
| 10 |
E" |
3129 |
2994 |
0.00 |
|
|
|
| 11 |
E" |
1505 |
1440 |
0.00 |
|
|
|
| 11 |
E" |
1505 |
1440 |
0.00 |
|
|
|
| 12 |
E" |
1170 |
1120 |
0.00 |
|
|
|
| 12 |
E" |
1170 |
1120 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16229.5 cm
-1
Scaled (by 0.9569) Zero Point Vibrational Energy (zpe) 15530.0 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/TZVP
Point Group is D3h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.766 |
| C2 |
0.000 |
0.000 |
-0.766 |
| H3 |
0.000 |
1.010 |
1.171 |
| H4 |
-0.875 |
-0.505 |
1.171 |
| H5 |
0.875 |
-0.505 |
1.171 |
| H6 |
0.000 |
1.010 |
-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 | | 1.5313 | 1.0885 | 1.0885 | 1.0885 | 2.1844 | 2.1844 | 2.1844 |
C2 | 1.5313 | | 2.1844 | 2.1844 | 2.1844 | 1.0885 | 1.0885 | 1.0885 | H3 | 1.0885 | 2.1844 | | 1.7497 | 1.7497 | 2.3421 | 2.9235 | 2.9235 | H4 | 1.0885 | 2.1844 | 1.7497 | | 1.7497 | 2.9235 | 2.9235 | 2.3421 | H5 | 1.0885 | 2.1844 | 1.7497 | 1.7497 | | 2.9235 | 2.3421 | 2.9235 | H6 | 2.1844 | 1.0885 | 2.3421 | 2.9235 | 2.9235 | | 1.7497 | 1.7497 | H7 | 2.1844 | 1.0885 | 2.9235 | 2.9235 | 2.3421 | 1.7497 | | 1.7497 | H8 | 2.1844 | 1.0885 | 2.9235 | 2.3421 | 2.9235 | 1.7497 | 1.7497 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.867 |
|
C1 |
C2 |
H7 |
111.867 |
| C1 |
C2 |
H8 |
111.867 |
|
C2 |
C1 |
H3 |
111.867 |
| C2 |
C1 |
H4 |
111.867 |
|
C2 |
C1 |
H5 |
111.867 |
| H3 |
C1 |
H4 |
106.973 |
|
H3 |
C1 |
H5 |
106.973 |
| H4 |
C1 |
H5 |
106.973 |
|
H6 |
C2 |
H7 |
106.973 |
| H6 |
C2 |
H8 |
106.973 |
|
H7 |
C2 |
H8 |
106.973 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.358 |
|
|
|
| 2 |
C |
-0.358 |
|
|
|
| 3 |
H |
0.119 |
|
|
|
| 4 |
H |
0.119 |
|
|
|
| 5 |
H |
0.119 |
|
|
|
| 6 |
H |
0.119 |
|
|
|
| 7 |
H |
0.119 |
|
|
|
| 8 |
H |
0.119 |
|
|
|
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 |
-14.845 |
0.000 |
0.000 |
| y |
0.000 |
-14.845 |
0.000 |
| z |
0.000 |
0.000 |
-15.512 |
|
| Traceless |
| | x | y | z |
| x |
0.333 |
0.000 |
0.000 |
| y |
0.000 |
0.333 |
0.000 |
| z |
0.000 |
0.000 |
-0.667 |
|
| Polar |
| 3z2-r2 | -1.334 |
| 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 |
3.718 |
0.000 |
0.000 |
| y |
0.000 |
3.718 |
0.000 |
| z |
0.000 |
0.000 |
3.913 |
<r2> (average value of r
2) Å
2
| <r2> |
30.797 |
| (<r2>)1/2 |
5.550 |