Jump to
S1C2
Energy calculated at M06-2X/6-31G
| | hartrees |
| Energy at 0K | -79.755406 |
| Energy at 298.15K | -79.761341 |
| HF Energy | -79.755406 |
| Nuclear repulsion energy | 42.175177 |
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 M06-2X/6-31G
| 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 |
3083 |
3083 |
0.00 |
219.61 |
0.01 |
0.03 |
| 2 |
A1g |
1471 |
1471 |
0.00 |
8.62 |
0.74 |
0.85 |
| 3 |
A1g |
1039 |
1039 |
0.00 |
10.60 |
0.30 |
0.46 |
| 4 |
A1u |
305 |
305 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
3084 |
3084 |
51.10 |
0.00 |
0.00 |
0.00 |
| 6 |
A2u |
1468 |
1468 |
7.11 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3147 |
3147 |
0.00 |
134.98 |
0.75 |
0.86 |
| 7 |
Eg |
3147 |
3147 |
0.00 |
134.73 |
0.75 |
0.86 |
| 8 |
Eg |
1554 |
1554 |
0.00 |
47.61 |
0.75 |
0.86 |
| 8 |
Eg |
1554 |
1554 |
0.00 |
47.59 |
0.75 |
0.86 |
| 9 |
Eg |
1257 |
1257 |
0.00 |
4.73 |
0.75 |
0.86 |
| 9 |
Eg |
1257 |
1257 |
0.00 |
4.70 |
0.75 |
0.86 |
| 10 |
Eu |
3172 |
3172 |
62.75 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3172 |
3172 |
62.76 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1558 |
1558 |
13.58 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1558 |
1558 |
13.58 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
858 |
858 |
7.43 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
858 |
858 |
7.43 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 16769.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 16769.9 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 M06-2X/6-31G
Point Group is D3d
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 |
1.020 |
1.160 |
| H4 |
-0.883 |
-0.510 |
1.160 |
| H5 |
0.883 |
-0.510 |
1.160 |
| H6 |
0.000 |
-1.020 |
-1.160 |
| H7 |
-0.883 |
0.510 |
-1.160 |
| H8 |
0.883 |
0.510 |
-1.160 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5302 | 1.0937 | 1.0937 | 1.0937 | 2.1788 | 2.1788 | 2.1788 |
C2 | 1.5302 | | 2.1788 | 2.1788 | 2.1788 | 1.0937 | 1.0937 | 1.0937 | H3 | 1.0937 | 2.1788 | | 1.7663 | 1.7663 | 3.0895 | 2.5348 | 2.5348 | H4 | 1.0937 | 2.1788 | 1.7663 | | 1.7663 | 2.5348 | 2.5348 | 3.0895 | H5 | 1.0937 | 2.1788 | 1.7663 | 1.7663 | | 2.5348 | 3.0895 | 2.5348 | H6 | 2.1788 | 1.0937 | 3.0895 | 2.5348 | 2.5348 | | 1.7663 | 1.7663 | H7 | 2.1788 | 1.0937 | 2.5348 | 2.5348 | 3.0895 | 1.7663 | | 1.7663 | H8 | 2.1788 | 1.0937 | 2.5348 | 3.0895 | 2.5348 | 1.7663 | 1.7663 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.183 |
|
C1 |
C2 |
H7 |
111.183 |
| C1 |
C2 |
H8 |
111.183 |
|
C2 |
C1 |
H3 |
111.183 |
| C2 |
C1 |
H4 |
111.183 |
|
C2 |
C1 |
H5 |
111.183 |
| H3 |
C1 |
H4 |
107.707 |
|
H3 |
C1 |
H5 |
107.707 |
| H4 |
C1 |
H5 |
107.707 |
|
H6 |
C2 |
H7 |
107.707 |
| H6 |
C2 |
H8 |
107.707 |
|
H7 |
C2 |
H8 |
107.707 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.447 |
|
|
|
| 2 |
C |
-0.447 |
|
|
|
| 3 |
H |
0.149 |
|
|
|
| 4 |
H |
0.149 |
|
|
|
| 5 |
H |
0.149 |
|
|
|
| 6 |
H |
0.149 |
|
|
|
| 7 |
H |
0.149 |
|
|
|
| 8 |
H |
0.149 |
|
|
|
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 |
-14.838 |
0.000 |
0.000 |
| y |
0.000 |
-14.838 |
0.000 |
| z |
0.000 |
0.000 |
-15.253 |
|
| Traceless |
| | x | y | z |
| x |
0.208 |
0.000 |
0.000 |
| y |
0.000 |
0.208 |
0.000 |
| z |
0.000 |
0.000 |
-0.416 |
|
| Polar |
| 3z2-r2 | -0.832 |
| 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 |
3.298 |
0.000 |
0.000 |
| y |
0.000 |
3.304 |
0.003 |
| z |
0.000 |
0.003 |
3.445 |
<r2> (average value of r
2) Å
2
| <r2> |
30.697 |
| (<r2>)1/2 |
5.540 |
Jump to
S1C1
Energy calculated at M06-2X/6-31G
| | hartrees |
| Energy at 0K | -79.751206 |
| Energy at 298.15K | |
| HF Energy | -79.751206 |
| Nuclear repulsion energy | 42.025658 |
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 M06-2X/6-31G
| 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' |
3086 |
3086 |
0.00 |
|
|
|
| 2 |
A1' |
1492 |
1492 |
0.00 |
|
|
|
| 3 |
A1' |
1032 |
1032 |
0.00 |
|
|
|
| 4 |
A1" |
305i |
305i |
0.00 |
|
|
|
| 5 |
A2" |
3079 |
3079 |
53.04 |
|
|
|
| 6 |
A2" |
1463 |
1463 |
7.29 |
|
|
|
| 7 |
E' |
3166 |
3166 |
49.48 |
|
|
|
| 7 |
E' |
3166 |
3166 |
49.70 |
|
|
|
| 8 |
E' |
1563 |
1563 |
15.67 |
|
|
|
| 8 |
E' |
1563 |
1563 |
15.52 |
|
|
|
| 9 |
E' |
928 |
928 |
7.89 |
|
|
|
| 9 |
E' |
928 |
928 |
7.95 |
|
|
|
| 10 |
E" |
3146 |
3146 |
0.00 |
|
|
|
| 10 |
E" |
3146 |
3146 |
0.00 |
|
|
|
| 11 |
E" |
1550 |
1550 |
0.00 |
|
|
|
| 11 |
E" |
1550 |
1550 |
0.00 |
|
|
|
| 12 |
E" |
1211 |
1211 |
0.00 |
|
|
|
| 12 |
E" |
1210 |
1210 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16486.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 16486.9 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 M06-2X/6-31G
Point Group is D3h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.771 |
| C2 |
0.000 |
0.000 |
-0.771 |
| H3 |
0.000 |
1.016 |
1.174 |
| H4 |
-0.880 |
-0.508 |
1.174 |
| H5 |
0.880 |
-0.508 |
1.174 |
| H6 |
0.000 |
1.016 |
-1.174 |
| H7 |
0.880 |
-0.508 |
-1.174 |
| H8 |
-0.880 |
-0.508 |
-1.174 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5426 | 1.0928 | 1.0928 | 1.0928 | 2.1946 | 2.1946 | 2.1946 |
C2 | 1.5426 | | 2.1946 | 2.1946 | 2.1946 | 1.0928 | 1.0928 | 1.0928 | H3 | 1.0928 | 2.1946 | | 1.7595 | 1.7595 | 2.3480 | 2.9341 | 2.9341 | H4 | 1.0928 | 2.1946 | 1.7595 | | 1.7595 | 2.9341 | 2.9341 | 2.3480 | H5 | 1.0928 | 2.1946 | 1.7595 | 1.7595 | | 2.9341 | 2.3480 | 2.9341 | H6 | 2.1946 | 1.0928 | 2.3480 | 2.9341 | 2.9341 | | 1.7595 | 1.7595 | H7 | 2.1946 | 1.0928 | 2.9341 | 2.9341 | 2.3480 | 1.7595 | | 1.7595 | H8 | 2.1946 | 1.0928 | 2.9341 | 2.3480 | 2.9341 | 1.7595 | 1.7595 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.624 |
|
C1 |
C2 |
H7 |
111.624 |
| C1 |
C2 |
H8 |
111.624 |
|
C2 |
C1 |
H3 |
111.624 |
| C2 |
C1 |
H4 |
111.624 |
|
C2 |
C1 |
H5 |
111.624 |
| H3 |
C1 |
H4 |
107.235 |
|
H3 |
C1 |
H5 |
107.235 |
| H4 |
C1 |
H5 |
107.235 |
|
H6 |
C2 |
H7 |
107.235 |
| H6 |
C2 |
H8 |
107.235 |
|
H7 |
C2 |
H8 |
107.235 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.456 |
|
|
|
| 2 |
C |
-0.456 |
|
|
|
| 3 |
H |
0.152 |
|
|
|
| 4 |
H |
0.152 |
|
|
|
| 5 |
H |
0.152 |
|
|
|
| 6 |
H |
0.152 |
|
|
|
| 7 |
H |
0.152 |
|
|
|
| 8 |
H |
0.152 |
|
|
|
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 |
-14.815 |
0.000 |
0.000 |
| y |
0.000 |
-14.815 |
0.000 |
| z |
0.000 |
0.000 |
-15.173 |
|
| Traceless |
| | x | y | z |
| x |
0.179 |
0.000 |
0.000 |
| y |
0.000 |
0.179 |
0.000 |
| z |
0.000 |
0.000 |
-0.358 |
|
| Polar |
| 3z2-r2 | -0.717 |
| 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 |
3.215 |
0.000 |
0.000 |
| y |
0.000 |
3.207 |
0.000 |
| z |
0.000 |
0.000 |
3.362 |
<r2> (average value of r
2) Å
2
| <r2> |
30.929 |
| (<r2>)1/2 |
5.561 |