Jump to
S1C2
Energy calculated at PBEPBE/6-31G*
| | hartrees |
| Energy at 0K | -114.273778 |
| Energy at 298.15K | -114.275181 |
| HF Energy | -114.273778 |
| Nuclear repulsion energy | 30.291486 |
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 PBEPBE/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 |
A' |
3496 |
3446 |
26.42 |
|
|
|
| 2 |
A' |
2710 |
2672 |
183.86 |
|
|
|
| 3 |
A' |
1498 |
1477 |
27.76 |
|
|
|
| 4 |
A' |
1289 |
1271 |
39.85 |
|
|
|
| 5 |
A' |
1177 |
1161 |
121.47 |
|
|
|
| 6 |
A" |
1089 |
1073 |
110.51 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5629.9 cm
-1
Scaled (by 0.9857) Zero Point Vibrational Energy (zpe) 5549.4 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 PBEPBE/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.011 |
0.754 |
0.000 |
| O2 |
0.011 |
-0.577 |
0.000 |
| H3 |
-1.108 |
0.958 |
0.000 |
| H4 |
0.953 |
-0.868 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.3304 | 1.1369 | 1.8755 |
O2 | 1.3304 | | 1.8987 | 0.9863 | H3 | 1.1369 | 1.8987 | | 2.7530 | H4 | 1.8755 | 0.9863 | 2.7530 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
107.165 |
|
O2 |
C1 |
H3 |
100.325 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.122 |
|
|
|
| 2 |
O |
-0.422 |
|
|
|
| 3 |
H |
0.117 |
|
|
|
| 4 |
H |
0.427 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.437 |
-1.722 |
0.000 |
1.776 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-10.825 |
-3.386 |
0.000 |
| y |
-3.386 |
-13.569 |
0.000 |
| z |
0.000 |
0.000 |
-11.735 |
|
| Traceless |
| | x | y | z |
| x |
1.827 |
-3.386 |
0.000 |
| y |
-3.386 |
-2.289 |
0.000 |
| z |
0.000 |
0.000 |
0.462 |
|
| Polar |
| 3z2-r2 | 0.924 |
| x2-y2 | 2.745 |
| xy | -3.386 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.549 |
-0.636 |
0.000 |
| y |
-0.636 |
2.450 |
0.000 |
| z |
0.000 |
0.000 |
1.353 |
<r2> (average value of r
2) Å
2
| <r2> |
17.398 |
| (<r2>)1/2 |
4.171 |
Jump to
S1C1
Energy calculated at PBEPBE/6-31G*
| | hartrees |
| Energy at 0K | -114.266331 |
| Energy at 298.15K | -114.267720 |
| HF Energy | -114.266331 |
| Nuclear repulsion energy | 30.278917 |
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 PBEPBE/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 |
A' |
3173 |
3128 |
107.98 |
|
|
|
| 2 |
A' |
2617 |
2579 |
273.29 |
|
|
|
| 3 |
A' |
1447 |
1426 |
52.03 |
|
|
|
| 4 |
A' |
1316 |
1297 |
27.28 |
|
|
|
| 5 |
A' |
1166 |
1149 |
18.22 |
|
|
|
| 6 |
A" |
1011 |
997 |
34.50 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5364.3 cm
-1
Scaled (by 0.9857) Zero Point Vibrational Energy (zpe) 5287.6 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 PBEPBE/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.124 |
0.749 |
0.000 |
| O2 |
0.124 |
-0.568 |
0.000 |
| H3 |
-0.970 |
1.078 |
0.000 |
| H4 |
-0.766 |
-1.026 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.3176 | 1.1420 | 1.9860 |
O2 | 1.3176 | | 1.9764 | 1.0010 | H3 | 1.1420 | 1.9764 | | 2.1137 | H4 | 1.9860 | 1.0010 | 2.1137 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
117.209 |
|
O2 |
C1 |
H3 |
106.722 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.066 |
|
|
|
| 2 |
O |
-0.407 |
|
|
|
| 3 |
H |
0.086 |
|
|
|
| 4 |
H |
0.387 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.797 |
-1.742 |
0.000 |
3.295 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.164 |
0.054 |
0.000 |
| y |
0.054 |
-12.911 |
0.000 |
| z |
0.000 |
0.000 |
-11.710 |
|
| Traceless |
| | x | y | z |
| x |
0.147 |
0.054 |
0.000 |
| y |
0.054 |
-0.974 |
0.000 |
| z |
0.000 |
0.000 |
0.827 |
|
| Polar |
| 3z2-r2 | 1.654 |
| x2-y2 | 0.747 |
| xy | 0.054 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.419 |
0.045 |
0.000 |
| y |
0.045 |
3.171 |
0.000 |
| z |
0.000 |
0.000 |
1.369 |
<r2> (average value of r
2) Å
2
| <r2> |
17.568 |
| (<r2>)1/2 |
4.191 |