Jump to
S1C2
Energy calculated at M06-2X/6-311G**
| | hartrees |
| Energy at 0K | -114.401019 |
| Energy at 298.15K | -114.402442 |
| HF Energy | -114.401019 |
| Nuclear repulsion energy | 30.862108 |
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/6-311G**
| 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' |
3805 |
3805 |
92.87 |
|
|
|
| 2 |
A' |
2926 |
2926 |
138.92 |
|
|
|
| 3 |
A' |
1531 |
1531 |
28.01 |
|
|
|
| 4 |
A' |
1394 |
1394 |
97.39 |
|
|
|
| 5 |
A' |
1238 |
1238 |
122.49 |
|
|
|
| 6 |
A" |
1114 |
1114 |
126.19 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6004.2 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 6004.2 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/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.011 |
0.739 |
0.000 |
| O2 |
0.011 |
-0.566 |
0.000 |
| H3 |
-1.079 |
0.969 |
0.000 |
| H4 |
0.926 |
-0.876 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.3044 | 1.1137 | 1.8555 |
O2 | 1.3044 | | 1.8824 | 0.9657 | H3 | 1.1137 | 1.8824 | | 2.7241 | H4 | 1.8555 | 0.9657 | 2.7241 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
108.723 |
|
O2 |
C1 |
H3 |
101.949 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.127 |
|
|
|
| 2 |
O |
-0.259 |
|
|
|
| 3 |
H |
0.095 |
|
|
|
| 4 |
H |
0.291 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.256 |
-1.556 |
0.000 |
1.577 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-10.971 |
-3.723 |
0.000 |
| y |
-3.723 |
-13.651 |
0.000 |
| z |
0.000 |
0.000 |
-11.901 |
|
| Traceless |
| | x | y | z |
| x |
1.804 |
-3.723 |
0.000 |
| y |
-3.723 |
-2.214 |
0.000 |
| z |
0.000 |
0.000 |
0.410 |
|
| Polar |
| 3z2-r2 | 0.819 |
| x2-y2 | 2.679 |
| xy | -3.723 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.470 |
-0.519 |
0.000 |
| y |
-0.519 |
2.515 |
0.000 |
| z |
0.000 |
0.000 |
1.581 |
<r2> (average value of r
2) Å
2
| <r2> |
17.166 |
| (<r2>)1/2 |
4.143 |
Jump to
S1C1
Energy calculated at M06-2X/6-311G**
| | hartrees |
| Energy at 0K | -114.391909 |
| Energy at 298.15K | -114.393319 |
| HF Energy | -114.391909 |
| Nuclear repulsion energy | 30.779860 |
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/6-311G**
| 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' |
3652 |
3652 |
21.40 |
|
|
|
| 2 |
A' |
2802 |
2802 |
206.22 |
|
|
|
| 3 |
A' |
1491 |
1491 |
53.09 |
|
|
|
| 4 |
A' |
1392 |
1392 |
102.23 |
|
|
|
| 5 |
A' |
1243 |
1243 |
23.73 |
|
|
|
| 6 |
A" |
1033 |
1033 |
37.75 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5806.7 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 5806.7 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/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.122 |
0.738 |
0.000 |
| O2 |
0.122 |
-0.563 |
0.000 |
| H3 |
-0.952 |
1.059 |
0.000 |
| H4 |
-0.753 |
-0.985 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.3017 | 1.1211 | 1.9329 |
O2 | 1.3017 | | 1.9459 | 0.9714 | H3 | 1.1211 | 1.9459 | | 2.0541 | H4 | 1.9329 | 0.9714 | 2.0541 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
115.735 |
|
O2 |
C1 |
H3 |
106.637 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.083 |
|
|
|
| 2 |
O |
-0.255 |
|
|
|
| 3 |
H |
0.071 |
|
|
|
| 4 |
H |
0.267 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.084 |
-1.631 |
0.000 |
3.489 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.262 |
-0.077 |
0.000 |
| y |
-0.077 |
-13.192 |
0.000 |
| z |
0.000 |
0.000 |
-11.846 |
|
| Traceless |
| | x | y | z |
| x |
0.257 |
-0.077 |
0.000 |
| y |
-0.077 |
-1.138 |
0.000 |
| z |
0.000 |
0.000 |
0.881 |
|
| Polar |
| 3z2-r2 | 1.762 |
| x2-y2 | 0.930 |
| xy | -0.077 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.403 |
-0.042 |
0.000 |
| y |
-0.042 |
2.852 |
0.000 |
| z |
0.000 |
0.000 |
1.575 |
<r2> (average value of r
2) Å
2
| <r2> |
17.350 |
| (<r2>)1/2 |
4.165 |