Jump to
S1C2
Energy calculated at M06-2X/6-31G**
| | hartrees |
| Energy at 0K | -79.778386 |
| Energy at 298.15K | -79.784297 |
| HF Energy | -79.778386 |
| Nuclear repulsion energy | 42.235770 |
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 |
3079 |
2926 |
0.00 |
222.48 |
0.01 |
0.02 |
| 2 |
A1g |
1444 |
1372 |
0.00 |
7.17 |
0.75 |
0.85 |
| 3 |
A1g |
1029 |
978 |
0.00 |
10.26 |
0.30 |
0.47 |
| 4 |
A1u |
313 |
298 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
3081 |
2929 |
49.80 |
0.00 |
0.00 |
0.00 |
| 6 |
A2u |
1412 |
1342 |
0.77 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3145 |
2989 |
0.00 |
135.32 |
0.75 |
0.86 |
| 7 |
Eg |
3145 |
2989 |
0.00 |
134.98 |
0.75 |
0.86 |
| 8 |
Eg |
1521 |
1445 |
0.00 |
40.30 |
0.75 |
0.86 |
| 8 |
Eg |
1521 |
1445 |
0.00 |
40.24 |
0.75 |
0.86 |
| 9 |
Eg |
1225 |
1164 |
0.00 |
2.93 |
0.75 |
0.86 |
| 9 |
Eg |
1225 |
1164 |
0.00 |
2.96 |
0.75 |
0.86 |
| 10 |
Eu |
3167 |
3010 |
59.08 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3167 |
3010 |
58.94 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1524 |
1448 |
7.78 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1524 |
1448 |
7.79 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
825 |
784 |
4.57 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
825 |
784 |
4.57 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 16584.1 cm
-1
Scaled (by 0.9504) Zero Point Vibrational Energy (zpe) 15761.5 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 M06-2X/6-31G**
Point Group is D3d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.763 |
| C2 |
0.000 |
0.000 |
-0.763 |
| H3 |
0.000 |
1.019 |
1.159 |
| H4 |
-0.882 |
-0.509 |
1.159 |
| H5 |
0.882 |
-0.509 |
1.159 |
| H6 |
0.000 |
-1.019 |
-1.159 |
| H7 |
-0.882 |
0.509 |
-1.159 |
| H8 |
0.882 |
0.509 |
-1.159 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5261 | 1.0931 | 1.0931 | 1.0931 | 2.1755 | 2.1755 | 2.1755 |
C2 | 1.5261 | | 2.1755 | 2.1755 | 2.1755 | 1.0931 | 1.0931 | 1.0931 | H3 | 1.0931 | 2.1755 | | 1.7645 | 1.7645 | 3.0865 | 2.5324 | 2.5324 | H4 | 1.0931 | 2.1755 | 1.7645 | | 1.7645 | 2.5324 | 2.5324 | 3.0865 | H5 | 1.0931 | 2.1755 | 1.7645 | 1.7645 | | 2.5324 | 3.0865 | 2.5324 | H6 | 2.1755 | 1.0931 | 3.0865 | 2.5324 | 2.5324 | | 1.7645 | 1.7645 | H7 | 2.1755 | 1.0931 | 2.5324 | 2.5324 | 3.0865 | 1.7645 | | 1.7645 | H8 | 2.1755 | 1.0931 | 2.5324 | 3.0865 | 2.5324 | 1.7645 | 1.7645 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.250 |
|
C1 |
C2 |
H7 |
111.250 |
| C1 |
C2 |
H8 |
111.250 |
|
C2 |
C1 |
H3 |
111.250 |
| C2 |
C1 |
H4 |
111.250 |
|
C2 |
C1 |
H5 |
111.250 |
| H3 |
C1 |
H4 |
107.635 |
|
H3 |
C1 |
H5 |
107.635 |
| H4 |
C1 |
H5 |
107.635 |
|
H6 |
C2 |
H7 |
107.635 |
| H6 |
C2 |
H8 |
107.635 |
|
H7 |
C2 |
H8 |
107.635 |
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 |
-0.367 |
|
|
|
| 2 |
C |
-0.367 |
|
|
|
| 3 |
H |
0.122 |
|
|
|
| 4 |
H |
0.122 |
|
|
|
| 5 |
H |
0.122 |
|
|
|
| 6 |
H |
0.122 |
|
|
|
| 7 |
H |
0.122 |
|
|
|
| 8 |
H |
0.122 |
|
|
|
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 |
-14.745 |
0.000 |
0.000 |
| y |
0.000 |
-14.745 |
0.000 |
| z |
0.000 |
0.000 |
-15.237 |
|
| Traceless |
| | x | y | z |
| x |
0.246 |
0.000 |
0.000 |
| y |
0.000 |
0.246 |
0.000 |
| z |
0.000 |
0.000 |
-0.492 |
|
| Polar |
| 3z2-r2 | -0.984 |
| 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 |
3.415 |
0.000 |
0.000 |
| y |
0.000 |
3.425 |
0.004 |
| z |
0.000 |
0.004 |
3.643 |
<r2> (average value of r
2) Å
2
| <r2> |
30.588 |
| (<r2>)1/2 |
5.531 |
Jump to
S1C1
Energy calculated at M06-2X/6-31G**
| | hartrees |
| Energy at 0K | -79.773913 |
| Energy at 298.15K | |
| HF Energy | -79.773913 |
| Nuclear repulsion energy | 42.069678 |
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' |
3080 |
2928 |
0.00 |
|
|
|
| 2 |
A1' |
1460 |
1388 |
0.00 |
|
|
|
| 3 |
A1' |
1026 |
975 |
0.00 |
|
|
|
| 4 |
A1" |
317i |
301i |
0.00 |
|
|
|
| 5 |
A2" |
3075 |
2923 |
50.04 |
|
|
|
| 6 |
A2" |
1408 |
1338 |
0.68 |
|
|
|
| 7 |
E' |
3160 |
3004 |
45.78 |
|
|
|
| 7 |
E' |
3160 |
3004 |
45.97 |
|
|
|
| 8 |
E' |
1528 |
1452 |
9.33 |
|
|
|
| 8 |
E' |
1528 |
1452 |
9.18 |
|
|
|
| 9 |
E' |
897 |
853 |
4.54 |
|
|
|
| 9 |
E' |
897 |
853 |
4.50 |
|
|
|
| 10 |
E" |
3142 |
2986 |
0.00 |
|
|
|
| 10 |
E" |
3142 |
2986 |
0.00 |
|
|
|
| 11 |
E" |
1518 |
1442 |
0.00 |
|
|
|
| 11 |
E" |
1518 |
1442 |
0.00 |
|
|
|
| 12 |
E" |
1174 |
1115 |
0.00 |
|
|
|
| 12 |
E" |
1174 |
1115 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16285.6 cm
-1
Scaled (by 0.9504) Zero Point Vibrational Energy (zpe) 15477.8 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 |
0.770 |
| C2 |
0.000 |
0.000 |
-0.770 |
| H3 |
0.000 |
1.015 |
1.174 |
| H4 |
-0.879 |
-0.507 |
1.174 |
| H5 |
0.879 |
-0.507 |
1.174 |
| H6 |
0.000 |
1.015 |
-1.174 |
| H7 |
0.879 |
-0.507 |
-1.174 |
| H8 |
-0.879 |
-0.507 |
-1.174 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5397 | 1.0921 | 1.0921 | 1.0921 | 2.1928 | 2.1928 | 2.1928 |
C2 | 1.5397 | | 2.1928 | 2.1928 | 2.1928 | 1.0921 | 1.0921 | 1.0921 | H3 | 1.0921 | 2.1928 | | 1.7573 | 1.7573 | 2.3481 | 2.9329 | 2.9329 | H4 | 1.0921 | 2.1928 | 1.7573 | | 1.7573 | 2.9329 | 2.9329 | 2.3481 | H5 | 1.0921 | 2.1928 | 1.7573 | 1.7573 | | 2.9329 | 2.3481 | 2.9329 | H6 | 2.1928 | 1.0921 | 2.3481 | 2.9329 | 2.9329 | | 1.7573 | 1.7573 | H7 | 2.1928 | 1.0921 | 2.9329 | 2.9329 | 2.3481 | 1.7573 | | 1.7573 | H8 | 2.1928 | 1.0921 | 2.9329 | 2.3481 | 2.9329 | 1.7573 | 1.7573 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.723 |
|
C1 |
C2 |
H7 |
111.723 |
| C1 |
C2 |
H8 |
111.723 |
|
C2 |
C1 |
H3 |
111.723 |
| C2 |
C1 |
H4 |
111.723 |
|
C2 |
C1 |
H5 |
111.723 |
| H3 |
C1 |
H4 |
107.128 |
|
H3 |
C1 |
H5 |
107.128 |
| H4 |
C1 |
H5 |
107.129 |
|
H6 |
C2 |
H7 |
107.128 |
| H6 |
C2 |
H8 |
107.128 |
|
H7 |
C2 |
H8 |
107.129 |
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 |
-0.377 |
|
|
|
| 2 |
C |
-0.377 |
|
|
|
| 3 |
H |
0.126 |
|
|
|
| 4 |
H |
0.126 |
|
|
|
| 5 |
H |
0.126 |
|
|
|
| 6 |
H |
0.126 |
|
|
|
| 7 |
H |
0.126 |
|
|
|
| 8 |
H |
0.126 |
|
|
|
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 |
-14.725 |
0.000 |
0.000 |
| y |
0.000 |
-14.725 |
0.000 |
| z |
0.000 |
0.000 |
-15.171 |
|
| Traceless |
| | x | y | z |
| x |
0.223 |
0.000 |
0.000 |
| y |
0.000 |
0.223 |
0.000 |
| z |
0.000 |
0.000 |
-0.446 |
|
| Polar |
| 3z2-r2 | -0.891 |
| 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 |
3.336 |
0.000 |
0.000 |
| y |
0.000 |
3.323 |
0.000 |
| z |
0.000 |
0.000 |
3.558 |
<r2> (average value of r
2) Å
2
| <r2> |
30.849 |
| (<r2>)1/2 |
5.554 |