Jump to
S1C2
Energy calculated at M06-2X/3-21G
| | hartrees |
| Energy at 0K | -79.342264 |
| Energy at 298.15K | -79.348210 |
| HF Energy | -79.342264 |
| Nuclear repulsion energy | 42.037735 |
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/3-21G
| 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 |
3090 |
2963 |
0.00 |
175.83 |
0.01 |
0.03 |
| 2 |
A1g |
1469 |
1408 |
0.00 |
8.08 |
0.74 |
0.85 |
| 3 |
A1g |
996 |
955 |
0.00 |
9.12 |
0.29 |
0.45 |
| 4 |
A1u |
310 |
297 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
3093 |
2965 |
34.90 |
0.00 |
0.00 |
0.00 |
| 6 |
A2u |
1474 |
1414 |
9.51 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3144 |
3014 |
0.00 |
109.21 |
0.75 |
0.86 |
| 7 |
Eg |
3144 |
3014 |
0.00 |
109.05 |
0.75 |
0.86 |
| 8 |
Eg |
1576 |
1511 |
0.00 |
44.69 |
0.75 |
0.86 |
| 8 |
Eg |
1576 |
1511 |
0.00 |
44.68 |
0.75 |
0.86 |
| 9 |
Eg |
1262 |
1209 |
0.00 |
4.15 |
0.75 |
0.86 |
| 9 |
Eg |
1262 |
1209 |
0.00 |
4.11 |
0.75 |
0.86 |
| 10 |
Eu |
3169 |
3038 |
40.96 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3169 |
3038 |
40.60 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1577 |
1512 |
13.66 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1577 |
1512 |
13.70 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
866 |
831 |
8.92 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
866 |
831 |
8.94 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 16810.4 cm
-1
Scaled (by 0.9587) Zero Point Vibrational Energy (zpe) 16116.2 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 M06-2X/3-21G
Point Group is D3d
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 |
1.023 |
1.160 |
| H4 |
-0.886 |
-0.511 |
1.160 |
| H5 |
0.886 |
-0.511 |
1.160 |
| H6 |
0.000 |
-1.023 |
-1.160 |
| H7 |
-0.886 |
0.511 |
-1.160 |
| H8 |
0.886 |
0.511 |
-1.160 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5430 | 1.0939 | 1.0939 | 1.0939 | 2.1853 | 2.1853 | 2.1853 |
C2 | 1.5430 | | 2.1853 | 2.1853 | 2.1853 | 1.0939 | 1.0939 | 1.0939 | H3 | 1.0939 | 2.1853 | | 1.7712 | 1.7712 | 3.0925 | 2.5351 | 2.5351 | H4 | 1.0939 | 2.1853 | 1.7712 | | 1.7712 | 2.5351 | 2.5351 | 3.0925 | H5 | 1.0939 | 2.1853 | 1.7712 | 1.7712 | | 2.5351 | 3.0925 | 2.5351 | H6 | 2.1853 | 1.0939 | 3.0925 | 2.5351 | 2.5351 | | 1.7712 | 1.7712 | H7 | 2.1853 | 1.0939 | 2.5351 | 2.5351 | 3.0925 | 1.7712 | | 1.7712 | H8 | 2.1853 | 1.0939 | 2.5351 | 3.0925 | 2.5351 | 1.7712 | 1.7712 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
110.794 |
|
C1 |
C2 |
H7 |
110.794 |
| C1 |
C2 |
H8 |
110.794 |
|
C2 |
C1 |
H3 |
110.794 |
| C2 |
C1 |
H4 |
110.794 |
|
C2 |
C1 |
H5 |
110.794 |
| H3 |
C1 |
H4 |
108.116 |
|
H3 |
C1 |
H5 |
108.116 |
| H4 |
C1 |
H5 |
108.116 |
|
H6 |
C2 |
H7 |
108.116 |
| H6 |
C2 |
H8 |
108.116 |
|
H7 |
C2 |
H8 |
108.116 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.589 |
|
|
|
| 2 |
C |
-0.589 |
|
|
|
| 3 |
H |
0.196 |
|
|
|
| 4 |
H |
0.196 |
|
|
|
| 5 |
H |
0.196 |
|
|
|
| 6 |
H |
0.196 |
|
|
|
| 7 |
H |
0.196 |
|
|
|
| 8 |
H |
0.196 |
|
|
|
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 |
-14.817 |
0.000 |
0.000 |
| y |
0.000 |
-14.817 |
0.000 |
| z |
0.000 |
0.000 |
-15.233 |
|
| Traceless |
| | x | y | z |
| x |
0.208 |
0.000 |
0.000 |
| y |
0.000 |
0.208 |
0.000 |
| z |
0.000 |
0.000 |
-0.415 |
|
| Polar |
| 3z2-r2 | -0.831 |
| 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 |
3.081 |
0.000 |
0.000 |
| y |
0.000 |
3.087 |
0.003 |
| z |
0.000 |
0.003 |
3.287 |
<r2> (average value of r
2) Å
2
| <r2> |
30.829 |
| (<r2>)1/2 |
5.552 |
Jump to
S1C1
Energy calculated at M06-2X/3-21G
| | hartrees |
| Energy at 0K | -79.337979 |
| Energy at 298.15K | |
| HF Energy | -79.337979 |
| Nuclear repulsion energy | 41.879546 |
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/3-21G
| 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' |
3057 |
2931 |
0.00 |
|
|
|
| 2 |
A1' |
1486 |
1425 |
0.00 |
|
|
|
| 3 |
A1' |
986 |
946 |
0.00 |
|
|
|
| 4 |
A1" |
311i |
298i |
0.00 |
|
|
|
| 5 |
A2" |
3052 |
2926 |
35.32 |
|
|
|
| 6 |
A2" |
1464 |
1404 |
8.77 |
|
|
|
| 7 |
E' |
3127 |
2998 |
30.37 |
|
|
|
| 7 |
E' |
3127 |
2998 |
30.54 |
|
|
|
| 8 |
E' |
1582 |
1517 |
15.80 |
|
|
|
| 8 |
E' |
1582 |
1516 |
15.64 |
|
|
|
| 9 |
E' |
929 |
890 |
9.02 |
|
|
|
| 9 |
E' |
929 |
890 |
9.04 |
|
|
|
| 10 |
E" |
3107 |
2978 |
0.00 |
|
|
|
| 10 |
E" |
3106 |
2978 |
0.00 |
|
|
|
| 11 |
E" |
1569 |
1505 |
0.00 |
|
|
|
| 11 |
E" |
1569 |
1505 |
0.00 |
|
|
|
| 12 |
E" |
1210 |
1160 |
0.00 |
|
|
|
| 12 |
E" |
1210 |
1160 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16389.8 cm
-1
Scaled (by 0.9587) Zero Point Vibrational Energy (zpe) 15712.9 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/3-21G
Point Group is D3h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.778 |
| C2 |
0.000 |
0.000 |
-0.778 |
| H3 |
0.000 |
1.019 |
1.174 |
| H4 |
-0.882 |
-0.509 |
1.174 |
| H5 |
0.882 |
-0.509 |
1.174 |
| H6 |
0.000 |
1.019 |
-1.174 |
| H7 |
0.882 |
-0.509 |
-1.174 |
| H8 |
-0.882 |
-0.509 |
-1.174 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5562 | 1.0930 | 1.0930 | 1.0930 | 2.2019 | 2.2019 | 2.2019 |
C2 | 1.5562 | | 2.2019 | 2.2019 | 2.2019 | 1.0930 | 1.0930 | 1.0930 | H3 | 1.0930 | 2.2019 | | 1.7646 | 1.7646 | 2.3478 | 2.9370 | 2.9370 | H4 | 1.0930 | 2.2019 | 1.7646 | | 1.7646 | 2.9370 | 2.9370 | 2.3478 | H5 | 1.0930 | 2.2019 | 1.7646 | 1.7646 | | 2.9370 | 2.3478 | 2.9370 | H6 | 2.2019 | 1.0930 | 2.3478 | 2.9370 | 2.9370 | | 1.7646 | 1.7646 | H7 | 2.2019 | 1.0930 | 2.9370 | 2.9370 | 2.3478 | 1.7646 | | 1.7646 | H8 | 2.2019 | 1.0930 | 2.9370 | 2.3478 | 2.9370 | 1.7646 | 1.7646 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.232 |
|
C1 |
C2 |
H7 |
111.232 |
| C1 |
C2 |
H8 |
111.232 |
|
C2 |
C1 |
H3 |
111.232 |
| C2 |
C1 |
H4 |
111.232 |
|
C2 |
C1 |
H5 |
111.232 |
| H3 |
C1 |
H4 |
107.654 |
|
H3 |
C1 |
H5 |
107.654 |
| H4 |
C1 |
H5 |
107.654 |
|
H6 |
C2 |
H7 |
107.654 |
| H6 |
C2 |
H8 |
107.654 |
|
H7 |
C2 |
H8 |
107.654 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.598 |
|
|
|
| 2 |
C |
-0.598 |
|
|
|
| 3 |
H |
0.199 |
|
|
|
| 4 |
H |
0.199 |
|
|
|
| 5 |
H |
0.199 |
|
|
|
| 6 |
H |
0.199 |
|
|
|
| 7 |
H |
0.199 |
|
|
|
| 8 |
H |
0.199 |
|
|
|
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 |
-14.803 |
0.000 |
0.000 |
| y |
0.000 |
-14.803 |
0.000 |
| z |
0.000 |
0.000 |
-15.130 |
|
| Traceless |
| | x | y | z |
| x |
0.164 |
0.000 |
0.000 |
| y |
0.000 |
0.164 |
0.000 |
| z |
0.000 |
0.000 |
-0.328 |
|
| Polar |
| 3z2-r2 | -0.655 |
| 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 |
3.016 |
0.000 |
0.000 |
| y |
0.000 |
3.010 |
0.000 |
| z |
0.000 |
0.000 |
3.272 |
<r2> (average value of r
2) Å
2
| <r2> |
31.075 |
| (<r2>)1/2 |
5.574 |