Jump to
S1C2
Energy calculated at wB97X-D/TZVP
| | hartrees |
| Energy at 0K | -114.422365 |
| Energy at 298.15K | -114.423785 |
| HF Energy | -114.422365 |
| Nuclear repulsion energy | 30.874339 |
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 wB97X-D/TZVP
| 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' |
3788 |
3618 |
76.11 |
|
|
|
| 2 |
A' |
2885 |
2755 |
138.70 |
|
|
|
| 3 |
A' |
1518 |
1450 |
31.20 |
|
|
|
| 4 |
A' |
1371 |
1310 |
97.92 |
|
|
|
| 5 |
A' |
1230 |
1174 |
116.92 |
|
|
|
| 6 |
A" |
1109 |
1059 |
126.92 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5950.8 cm
-1
Scaled (by 0.955) Zero Point Vibrational Energy (zpe) 5683.0 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 wB97X-D/TZVP
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.004 |
0.726 |
0.000 |
| O2 |
-0.004 |
-0.577 |
0.000 |
| H3 |
0.969 |
1.125 |
0.000 |
| H4 |
-0.914 |
-0.866 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.3026 | 1.0516 | 1.8339 |
O2 | 1.3026 | | 1.9602 | 0.9554 | H3 | 1.0516 | 1.9602 | | 2.7407 | H4 | 1.8339 | 0.9554 | 2.7407 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
107.624 |
|
O2 |
C1 |
H3 |
112.312 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.146 |
|
|
|
| 2 |
O |
-0.252 |
|
|
|
| 3 |
H |
0.069 |
|
|
|
| 4 |
H |
0.329 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.185 |
-1.689 |
0.000 |
1.699 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.197 |
3.959 |
0.000 |
| y |
3.959 |
-13.986 |
0.000 |
| z |
0.000 |
0.000 |
-12.072 |
|
| Traceless |
| | x | y | z |
| x |
1.832 |
3.959 |
0.000 |
| y |
3.959 |
-2.351 |
0.000 |
| z |
0.000 |
0.000 |
0.519 |
|
| Polar |
| 3z2-r2 | 1.038 |
| x2-y2 | 2.789 |
| xy | 3.959 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.791 |
0.463 |
0.000 |
| y |
0.463 |
2.841 |
0.000 |
| z |
0.000 |
0.000 |
1.876 |
<r2> (average value of r
2) Å
2
| <r2> |
17.322 |
| (<r2>)1/2 |
4.162 |
Jump to
S1C1
Energy calculated at wB97X-D/TZVP
| | hartrees |
| Energy at 0K | -114.412449 |
| Energy at 298.15K | -114.413854 |
| HF Energy | -114.412449 |
| Nuclear repulsion energy | 30.777106 |
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 wB97X-D/TZVP
| 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' |
3646 |
3482 |
15.99 |
|
|
|
| 2 |
A' |
2770 |
2646 |
214.95 |
|
|
|
| 3 |
A' |
1480 |
1414 |
53.44 |
|
|
|
| 4 |
A' |
1367 |
1306 |
101.64 |
|
|
|
| 5 |
A' |
1229 |
1173 |
27.85 |
|
|
|
| 6 |
A" |
1020 |
974 |
39.03 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5756.2 cm
-1
Scaled (by 0.955) Zero Point Vibrational Energy (zpe) 5497.1 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 wB97X-D/TZVP
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.116 |
0.733 |
0.000 |
| O2 |
0.116 |
-0.572 |
0.000 |
| H3 |
-0.860 |
1.144 |
0.000 |
| H4 |
-0.766 |
-0.965 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.3048 | 1.0592 | 1.9129 |
O2 | 1.3048 | | 1.9744 | 0.9654 | H3 | 1.0592 | 1.9744 | | 2.1112 | H4 | 1.9129 | 0.9654 | 2.1112 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
114.004 |
|
O2 |
C1 |
H3 |
112.868 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.070 |
|
|
|
| 2 |
O |
-0.246 |
|
|
|
| 3 |
H |
0.032 |
|
|
|
| 4 |
H |
0.284 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.210 |
-1.763 |
0.000 |
3.662 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.515 |
-0.132 |
0.000 |
| y |
-0.132 |
-13.495 |
0.000 |
| z |
0.000 |
0.000 |
-11.971 |
|
| Traceless |
| | x | y | z |
| x |
0.218 |
-0.132 |
0.000 |
| y |
-0.132 |
-1.252 |
0.000 |
| z |
0.000 |
0.000 |
1.034 |
|
| Polar |
| 3z2-r2 | 2.068 |
| x2-y2 | 0.980 |
| xy | -0.132 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.771 |
-0.041 |
0.000 |
| y |
-0.041 |
3.174 |
0.000 |
| z |
0.000 |
0.000 |
1.849 |
<r2> (average value of r
2) Å
2
| <r2> |
17.503 |
| (<r2>)1/2 |
4.184 |