Jump to
S1C2
Energy calculated at M06-2X/6-311G*
| | hartrees |
| Energy at 0K | -114.393989 |
| Energy at 298.15K | -114.395415 |
| HF Energy | -114.393989 |
| Nuclear repulsion energy | 30.867306 |
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' |
3772 |
3772 |
63.33 |
|
|
|
| 2 |
A' |
2951 |
2951 |
144.44 |
|
|
|
| 3 |
A' |
1554 |
1554 |
36.87 |
|
|
|
| 4 |
A' |
1393 |
1393 |
99.51 |
|
|
|
| 5 |
A' |
1258 |
1258 |
121.46 |
|
|
|
| 6 |
A" |
1133 |
1133 |
136.60 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6030.3 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 6030.3 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/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.011 |
0.739 |
0.000 |
| O2 |
0.011 |
-0.564 |
0.000 |
| H3 |
-1.079 |
0.966 |
0.000 |
| H4 |
0.922 |
-0.887 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.3038 | 1.1130 | 1.8639 |
O2 | 1.3038 | | 1.8784 | 0.9662 | H3 | 1.1130 | 1.8784 | | 2.7264 | H4 | 1.8639 | 0.9662 | 2.7264 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
109.488 |
|
O2 |
C1 |
H3 |
101.723 |
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 |
-0.175 |
|
|
|
| 2 |
O |
-0.425 |
|
|
|
| 3 |
H |
0.172 |
|
|
|
| 4 |
H |
0.428 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.325 |
-1.584 |
0.000 |
1.617 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-10.986 |
-3.836 |
0.000 |
| y |
-3.836 |
-13.668 |
0.000 |
| z |
0.000 |
0.000 |
-11.964 |
|
| Traceless |
| | x | y | z |
| x |
1.830 |
-3.836 |
0.000 |
| y |
-3.836 |
-2.193 |
0.000 |
| z |
0.000 |
0.000 |
0.363 |
|
| Polar |
| 3z2-r2 | 0.726 |
| x2-y2 | 2.682 |
| xy | -3.836 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.430 |
-0.536 |
0.000 |
| y |
-0.536 |
2.462 |
0.000 |
| z |
0.000 |
0.000 |
1.509 |
<r2> (average value of r
2) Å
2
| <r2> |
17.186 |
| (<r2>)1/2 |
4.146 |
Jump to
S1C1
Energy calculated at M06-2X/6-311G*
| | hartrees |
| Energy at 0K | -114.384547 |
| Energy at 298.15K | -114.385962 |
| HF Energy | -114.384547 |
| Nuclear repulsion energy | 30.775942 |
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' |
3592 |
3592 |
12.29 |
|
|
|
| 2 |
A' |
2815 |
2815 |
217.32 |
|
|
|
| 3 |
A' |
1510 |
1510 |
68.13 |
|
|
|
| 4 |
A' |
1393 |
1393 |
98.26 |
|
|
|
| 5 |
A' |
1293 |
1293 |
20.29 |
|
|
|
| 6 |
A" |
1048 |
1048 |
47.20 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5825.0 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 5825.0 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 |
0.121 |
0.739 |
0.000 |
| O2 |
0.121 |
-0.562 |
0.000 |
| H3 |
-0.953 |
1.060 |
0.000 |
| H4 |
-0.747 |
-1.002 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.3006 | 1.1209 | 1.9453 |
O2 | 1.3006 | | 1.9450 | 0.9735 | H3 | 1.1209 | 1.9450 | | 2.0721 | H4 | 1.9453 | 0.9735 | 2.0721 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
116.887 |
|
O2 |
C1 |
H3 |
106.644 |
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 |
-0.124 |
|
|
|
| 2 |
O |
-0.423 |
|
|
|
| 3 |
H |
0.142 |
|
|
|
| 4 |
H |
0.406 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.182 |
-1.669 |
0.000 |
3.593 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.319 |
0.012 |
0.000 |
| y |
0.012 |
-13.181 |
0.000 |
| z |
0.000 |
0.000 |
-11.914 |
|
| Traceless |
| | x | y | z |
| x |
0.228 |
0.012 |
0.000 |
| y |
0.012 |
-1.064 |
0.000 |
| z |
0.000 |
0.000 |
0.836 |
|
| Polar |
| 3z2-r2 | 1.672 |
| x2-y2 | 0.861 |
| xy | 0.012 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.364 |
-0.032 |
0.000 |
| y |
-0.032 |
2.842 |
0.000 |
| z |
0.000 |
0.000 |
1.508 |
<r2> (average value of r
2) Å
2
| <r2> |
17.388 |
| (<r2>)1/2 |
4.170 |