Jump to
S1C2
Energy calculated at M06-2X/6-311+G(3df,2p)
| hartrees |
Energy at 0K | -190.641509 |
Energy at 298.15K | |
HF Energy | -190.641509 |
Nuclear repulsion energy | 88.871502 |
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/6-311+G(3df,2p)
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 |
3105 |
3105 |
20.85 |
190.79 |
0.11 |
0.19 |
2 |
A1 |
2354 |
2354 |
1135.73 |
58.78 |
0.48 |
0.65 |
3 |
A1 |
1835 |
1835 |
35.67 |
2.25 |
0.14 |
0.25 |
4 |
A1 |
1486 |
1486 |
2.13 |
10.67 |
0.61 |
0.76 |
5 |
A1 |
943 |
943 |
4.94 |
49.52 |
0.16 |
0.28 |
6 |
B1 |
1043 |
1043 |
24.49 |
2.35 |
0.75 |
0.86 |
7 |
B1 |
668 |
668 |
22.34 |
0.39 |
0.75 |
0.86 |
8 |
B1 |
218 |
218 |
0.47 |
1.91 |
0.75 |
0.86 |
9 |
B2 |
3178 |
3178 |
2.88 |
114.35 |
0.75 |
0.86 |
10 |
B2 |
1069 |
1069 |
2.70 |
0.01 |
0.75 |
0.86 |
11 |
B2 |
487 |
487 |
11.23 |
2.61 |
0.75 |
0.86 |
12 |
B2 |
98i |
98i |
14.23 |
0.09 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 8144.3 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 8144.3 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/6-311+G(3df,2p)
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.000 |
-1.865 |
C2 |
0.000 |
0.000 |
-0.554 |
C3 |
0.000 |
0.000 |
0.720 |
O4 |
0.000 |
0.000 |
1.884 |
H5 |
0.000 |
0.923 |
-2.439 |
H6 |
0.000 |
-0.923 |
-2.439 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
C1 | | 1.3102 | 2.5843 | 3.7487 | 1.0868 | 1.0868 |
C2 | 1.3102 | | 1.2740 | 2.4385 | 2.0980 | 2.0980 | C3 | 2.5843 | 1.2740 | | 1.1645 | 3.2902 | 3.2902 | O4 | 3.7487 | 2.4385 | 1.1645 | | 4.4201 | 4.4201 | H5 | 1.0868 | 2.0980 | 3.2902 | 4.4201 | | 1.8457 | H6 | 1.0868 | 2.0980 | 3.2902 | 4.4201 | 1.8457 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
C3 |
180.000 |
|
C2 |
C1 |
H5 |
121.877 |
C2 |
C1 |
H6 |
121.877 |
|
C2 |
C3 |
O4 |
180.000 |
H5 |
C1 |
H6 |
116.246 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-311+G(3df,2p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.198 |
|
|
|
2 |
C |
0.735 |
|
|
|
3 |
C |
-0.197 |
|
|
|
4 |
O |
-0.756 |
|
|
|
5 |
H |
0.208 |
|
|
|
6 |
H |
0.208 |
|
|
|
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 |
-2.804 |
2.804 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-22.930 |
0.000 |
0.000 |
y |
0.000 |
-22.645 |
0.000 |
z |
0.000 |
0.000 |
-21.930 |
|
Traceless |
| x | y | z |
x |
-0.642 |
0.000 |
0.000 |
y |
0.000 |
-0.215 |
0.000 |
z |
0.000 |
0.000 |
0.858 |
|
Polar |
3z2-r2 | 1.715 |
x2-y2 | -0.285 |
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 |
3.600 |
0.000 |
0.000 |
y |
0.000 |
4.075 |
0.000 |
z |
0.000 |
0.000 |
10.936 |
<r2> (average value of r
2) Å
2
<r2> |
81.861 |
(<r2>)1/2 |
9.048 |
Jump to
S1C1
Energy calculated at M06-2X/6-311+G(3df,2p)
| hartrees |
Energy at 0K | -190.641843 |
Energy at 298.15K | |
HF Energy | -190.641843 |
Nuclear repulsion energy | 89.055749 |
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/6-311+G(3df,2p)
Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
1 |
A' |
3186 |
3186 |
3.38 |
104.69 |
0.71 |
0.83 |
2 |
A' |
3109 |
3109 |
21.37 |
162.82 |
0.11 |
0.19 |
3 |
A' |
2295 |
2295 |
1173.68 |
60.67 |
0.50 |
0.67 |
4 |
A' |
1817 |
1817 |
13.61 |
5.61 |
0.14 |
0.24 |
5 |
A' |
1490 |
1490 |
1.17 |
10.78 |
0.64 |
0.78 |
6 |
A' |
1076 |
1076 |
17.39 |
2.93 |
0.05 |
0.09 |
7 |
A' |
960 |
960 |
2.91 |
44.25 |
0.13 |
0.22 |
8 |
A' |
512 |
512 |
15.27 |
3.99 |
0.75 |
0.86 |
9 |
A' |
119 |
119 |
23.39 |
4.01 |
0.75 |
0.85 |
10 |
A" |
1049 |
1049 |
23.88 |
2.28 |
0.75 |
0.86 |
11 |
A" |
702 |
702 |
17.99 |
0.57 |
0.75 |
0.86 |
12 |
A" |
258 |
258 |
0.55 |
2.57 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 8286.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 8286.8 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/6-311+G(3df,2p)
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.838 |
-1.629 |
0.000 |
C2 |
0.000 |
-0.615 |
0.000 |
C3 |
-0.291 |
0.640 |
0.000 |
O4 |
-0.711 |
1.721 |
0.000 |
H5 |
1.916 |
-1.489 |
0.000 |
H6 |
0.487 |
-2.656 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
C1 | | 1.3150 | 2.5339 | 3.6904 | 1.0870 | 1.0856 |
C2 | 1.3150 | | 1.2884 | 2.4421 | 2.1059 | 2.0981 | C3 | 2.5339 | 1.2884 | | 1.1599 | 3.0665 | 3.3864 | O4 | 3.6904 | 2.4421 | 1.1599 | | 4.1478 | 4.5381 | H5 | 1.0870 | 2.1059 | 3.0665 | 4.1478 | | 1.8446 | H6 | 1.0856 | 2.0981 | 3.3864 | 4.5381 | 1.8446 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
C3 |
153.468 |
|
C2 |
C1 |
H5 |
122.217 |
C2 |
C1 |
H6 |
121.560 |
|
C2 |
C3 |
O4 |
171.866 |
H5 |
C1 |
H6 |
116.222 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-311+G(3df,2p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.308 |
|
|
|
2 |
C |
0.092 |
|
|
|
3 |
C |
0.536 |
|
|
|
4 |
O |
-0.724 |
|
|
|
5 |
H |
0.206 |
|
|
|
6 |
H |
0.198 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
1.615 |
-2.022 |
0.000 |
2.588 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-22.219 |
-0.813 |
0.000 |
y |
-0.813 |
-22.570 |
0.000 |
z |
0.000 |
0.000 |
-23.039 |
|
Traceless |
| x | y | z |
x |
0.586 |
-0.813 |
0.000 |
y |
-0.813 |
0.059 |
0.000 |
z |
0.000 |
0.000 |
-0.645 |
|
Polar |
3z2-r2 | -1.290 |
x2-y2 | 0.351 |
xy | -0.813 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.335 |
-2.346 |
0.000 |
y |
-2.346 |
9.618 |
0.000 |
z |
0.000 |
0.000 |
3.665 |
<r2> (average value of r
2) Å
2
<r2> |
80.403 |
(<r2>)1/2 |
8.967 |