Jump to
S1C2
Energy calculated at wB97X-D/cc-pVTZ
| | hartrees |
| Energy at 0K | -79.832723 |
| Energy at 298.15K | -79.838639 |
| HF Energy | -79.832723 |
| Nuclear repulsion energy | 42.325555 |
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 wB97X-D/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 |
3052 |
2918 |
0.00 |
292.90 |
0.01 |
0.01 |
| 2 |
A1g |
1433 |
1370 |
0.00 |
0.89 |
0.74 |
0.85 |
| 3 |
A1g |
1014 |
969 |
0.00 |
11.53 |
0.22 |
0.36 |
| 4 |
A1u |
306 |
293 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
3051 |
2917 |
58.31 |
0.00 |
0.00 |
0.00 |
| 6 |
A2u |
1413 |
1351 |
1.94 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3110 |
2973 |
0.00 |
132.63 |
0.75 |
0.86 |
| 7 |
Eg |
3110 |
2973 |
0.00 |
132.86 |
0.75 |
0.86 |
| 8 |
Eg |
1510 |
1444 |
0.00 |
17.41 |
0.75 |
0.86 |
| 8 |
Eg |
1510 |
1444 |
0.00 |
17.42 |
0.75 |
0.86 |
| 9 |
Eg |
1226 |
1172 |
0.00 |
0.34 |
0.75 |
0.86 |
| 9 |
Eg |
1226 |
1172 |
0.00 |
0.34 |
0.75 |
0.86 |
| 10 |
Eu |
3133 |
2995 |
62.43 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3133 |
2995 |
62.52 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1511 |
1445 |
9.68 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1511 |
1445 |
9.72 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
832 |
796 |
4.19 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
832 |
796 |
4.19 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 16457.2 cm
-1
Scaled (by 0.956) Zero Point Vibrational Energy (zpe) 15733.1 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 wB97X-D/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 |
1.016 |
1.157 |
| H4 |
-0.880 |
-0.508 |
1.157 |
| H5 |
0.880 |
-0.508 |
1.157 |
| H6 |
0.000 |
-1.016 |
-1.157 |
| H7 |
-0.880 |
0.508 |
-1.157 |
| H8 |
0.880 |
0.508 |
-1.157 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5237 | 1.0903 | 1.0903 | 1.0903 | 2.1713 | 2.1713 | 2.1713 |
C2 | 1.5237 | | 2.1713 | 2.1713 | 2.1713 | 1.0903 | 1.0903 | 1.0903 | H3 | 1.0903 | 2.1713 | | 1.7600 | 1.7600 | 3.0798 | 2.5273 | 2.5273 | H4 | 1.0903 | 2.1713 | 1.7600 | | 1.7600 | 2.5273 | 2.5273 | 3.0798 | H5 | 1.0903 | 2.1713 | 1.7600 | 1.7600 | | 2.5273 | 3.0798 | 2.5273 | H6 | 2.1713 | 1.0903 | 3.0798 | 2.5273 | 2.5273 | | 1.7600 | 1.7600 | H7 | 2.1713 | 1.0903 | 2.5273 | 2.5273 | 3.0798 | 1.7600 | | 1.7600 | H8 | 2.1713 | 1.0903 | 2.5273 | 3.0798 | 2.5273 | 1.7600 | 1.7600 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.253 |
|
C1 |
C2 |
H7 |
111.253 |
| C1 |
C2 |
H8 |
111.253 |
|
C2 |
C1 |
H3 |
111.253 |
| C2 |
C1 |
H4 |
111.253 |
|
C2 |
C1 |
H5 |
111.253 |
| H3 |
C1 |
H4 |
107.632 |
|
H3 |
C1 |
H5 |
107.632 |
| H4 |
C1 |
H5 |
107.632 |
|
H6 |
C2 |
H7 |
107.632 |
| H6 |
C2 |
H8 |
107.632 |
|
H7 |
C2 |
H8 |
107.632 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.246 |
|
|
|
| 2 |
C |
-0.246 |
|
|
|
| 3 |
H |
0.082 |
|
|
|
| 4 |
H |
0.082 |
|
|
|
| 5 |
H |
0.082 |
|
|
|
| 6 |
H |
0.082 |
|
|
|
| 7 |
H |
0.082 |
|
|
|
| 8 |
H |
0.082 |
|
|
|
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 |
-14.791 |
0.000 |
0.000 |
| y |
0.000 |
-14.791 |
0.000 |
| z |
0.000 |
0.000 |
-15.471 |
|
| Traceless |
| | x | y | z |
| x |
0.340 |
0.000 |
0.000 |
| y |
0.000 |
0.340 |
0.000 |
| z |
0.000 |
0.000 |
-0.680 |
|
| Polar |
| 3z2-r2 | -1.360 |
| 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 |
3.838 |
0.000 |
0.000 |
| y |
0.000 |
3.837 |
0.000 |
| z |
0.000 |
0.000 |
4.288 |
<r2> (average value of r
2) Å
2
| <r2> |
30.572 |
| (<r2>)1/2 |
5.529 |
Jump to
S1C1
Energy calculated at wB97X-D/cc-pVTZ
| | hartrees |
| Energy at 0K | -79.828492 |
| Energy at 298.15K | |
| HF Energy | -79.828492 |
| Nuclear repulsion energy | 42.157419 |
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 wB97X-D/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' |
3072 |
2937 |
0.00 |
|
|
|
| 2 |
A1' |
1454 |
1390 |
0.00 |
|
|
|
| 3 |
A1' |
1011 |
966 |
0.00 |
|
|
|
| 4 |
A1" |
288i |
276i |
0.00 |
|
|
|
| 5 |
A2" |
3065 |
2930 |
60.03 |
|
|
|
| 6 |
A2" |
1414 |
1352 |
1.33 |
|
|
|
| 7 |
E' |
3145 |
3007 |
53.21 |
|
|
|
| 7 |
E' |
3145 |
3007 |
52.95 |
|
|
|
| 8 |
E' |
1521 |
1455 |
11.28 |
|
|
|
| 8 |
E' |
1521 |
1455 |
11.21 |
|
|
|
| 9 |
E' |
913 |
873 |
3.16 |
|
|
|
| 9 |
E' |
913 |
873 |
3.17 |
|
|
|
| 10 |
E" |
3123 |
2986 |
0.00 |
|
|
|
| 10 |
E" |
3123 |
2986 |
0.00 |
|
|
|
| 11 |
E" |
1511 |
1445 |
0.00 |
|
|
|
| 11 |
E" |
1511 |
1445 |
0.00 |
|
|
|
| 12 |
E" |
1180 |
1128 |
0.00 |
|
|
|
| 12 |
E" |
1180 |
1128 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16257.8 cm
-1
Scaled (by 0.956) Zero Point Vibrational Energy (zpe) 15542.4 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 wB97X-D/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 |
1.012 |
1.171 |
| H4 |
-0.877 |
-0.506 |
1.171 |
| H5 |
0.877 |
-0.506 |
1.171 |
| H6 |
0.000 |
1.012 |
-1.171 |
| H7 |
0.877 |
-0.506 |
-1.171 |
| H8 |
-0.877 |
-0.506 |
-1.171 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5376 | 1.0892 | 1.0892 | 1.0892 | 2.1879 | 2.1879 | 2.1879 |
C2 | 1.5376 | | 2.1879 | 2.1879 | 2.1879 | 1.0892 | 1.0892 | 1.0892 | H3 | 1.0892 | 2.1879 | | 1.7533 | 1.7533 | 2.3416 | 2.9253 | 2.9253 | H4 | 1.0892 | 2.1879 | 1.7533 | | 1.7533 | 2.9253 | 2.9253 | 2.3416 | H5 | 1.0892 | 2.1879 | 1.7533 | 1.7533 | | 2.9253 | 2.3416 | 2.9253 | H6 | 2.1879 | 1.0892 | 2.3416 | 2.9253 | 2.9253 | | 1.7533 | 1.7533 | H7 | 2.1879 | 1.0892 | 2.9253 | 2.9253 | 2.3416 | 1.7533 | | 1.7533 | H8 | 2.1879 | 1.0892 | 2.9253 | 2.3416 | 2.9253 | 1.7533 | 1.7533 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.661 |
|
C1 |
C2 |
H7 |
111.661 |
| C1 |
C2 |
H8 |
111.661 |
|
C2 |
C1 |
H3 |
111.661 |
| C2 |
C1 |
H4 |
111.661 |
|
C2 |
C1 |
H5 |
111.661 |
| H3 |
C1 |
H4 |
107.196 |
|
H3 |
C1 |
H5 |
107.196 |
| H4 |
C1 |
H5 |
107.196 |
|
H6 |
C2 |
H7 |
107.196 |
| H6 |
C2 |
H8 |
107.196 |
|
H7 |
C2 |
H8 |
107.196 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.248 |
|
|
|
| 2 |
C |
-0.248 |
|
|
|
| 3 |
H |
0.083 |
|
|
|
| 4 |
H |
0.083 |
|
|
|
| 5 |
H |
0.083 |
|
|
|
| 6 |
H |
0.083 |
|
|
|
| 7 |
H |
0.083 |
|
|
|
| 8 |
H |
0.083 |
|
|
|
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 |
-14.783 |
0.000 |
0.000 |
| y |
0.000 |
-14.783 |
0.000 |
| z |
0.000 |
0.000 |
-15.435 |
|
| Traceless |
| | x | y | z |
| x |
0.326 |
0.000 |
0.000 |
| y |
0.000 |
0.326 |
0.000 |
| z |
0.000 |
0.000 |
-0.653 |
|
| Polar |
| 3z2-r2 | -1.305 |
| 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 |
3.803 |
0.000 |
0.000 |
| y |
0.000 |
3.802 |
0.000 |
| z |
0.000 |
0.000 |
4.261 |
<r2> (average value of r
2) Å
2
| <r2> |
30.843 |
| (<r2>)1/2 |
5.554 |