Jump to
S1C2
Energy calculated at wB97X-D/cc-pVDZ
| | hartrees |
| Energy at 0K | -114.387233 |
| Energy at 298.15K | -114.388652 |
| HF Energy | -114.387233 |
| Nuclear repulsion energy | 30.751662 |
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/cc-pVDZ
| 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' |
3821 |
3640 |
98.45 |
|
|
|
| 2 |
A' |
2898 |
2761 |
139.78 |
|
|
|
| 3 |
A' |
1518 |
1446 |
38.06 |
|
|
|
| 4 |
A' |
1370 |
1305 |
116.84 |
|
|
|
| 5 |
A' |
1231 |
1172 |
121.58 |
|
|
|
| 6 |
A" |
1099 |
1047 |
136.15 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5968.7 cm
-1
Scaled (by 0.9526) Zero Point Vibrational Energy (zpe) 5685.8 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 wB97X-D/cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.004 |
0.727 |
0.000 |
| O2 |
-0.004 |
-0.578 |
0.000 |
| H3 |
0.970 |
1.127 |
0.000 |
| H4 |
-0.915 |
-0.869 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.3048 | 1.0531 | 1.8380 |
O2 | 1.3048 | | 1.9635 | 0.9567 | H3 | 1.0531 | 1.9635 | | 2.7459 | H4 | 1.8380 | 0.9567 | 2.7459 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
107.736 |
|
O2 |
C1 |
H3 |
112.328 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.101 |
|
|
|
| 2 |
O |
-0.409 |
|
|
|
| 3 |
H |
0.103 |
|
|
|
| 4 |
H |
0.407 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.149 |
-1.662 |
0.000 |
1.669 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.281 |
4.092 |
0.000 |
| y |
4.092 |
-14.155 |
0.000 |
| z |
0.000 |
0.000 |
-12.278 |
|
| Traceless |
| | x | y | z |
| x |
1.935 |
4.092 |
0.000 |
| y |
4.092 |
-2.375 |
0.000 |
| z |
0.000 |
0.000 |
0.440 |
|
| Polar |
| 3z2-r2 | 0.881 |
| x2-y2 | 2.874 |
| xy | 4.092 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.786 |
0.321 |
0.000 |
| y |
0.321 |
3.069 |
0.000 |
| z |
0.000 |
0.000 |
2.008 |
<r2> (average value of r
2) Å
2
| <r2> |
17.489 |
| (<r2>)1/2 |
4.182 |
Jump to
S1C1
Energy calculated at wB97X-D/cc-pVDZ
| | hartrees |
| Energy at 0K | -114.377092 |
| Energy at 298.15K | -114.378496 |
| HF Energy | -114.377092 |
| Nuclear repulsion energy | 30.646466 |
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/cc-pVDZ
| 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' |
3679 |
3505 |
16.37 |
|
|
|
| 2 |
A' |
2783 |
2651 |
223.44 |
|
|
|
| 3 |
A' |
1472 |
1402 |
66.38 |
|
|
|
| 4 |
A' |
1365 |
1300 |
112.34 |
|
|
|
| 5 |
A' |
1233 |
1174 |
29.08 |
|
|
|
| 6 |
A" |
1007 |
959 |
38.22 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5769.3 cm
-1
Scaled (by 0.9526) Zero Point Vibrational Energy (zpe) 5495.8 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 wB97X-D/cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.116 |
0.734 |
0.000 |
| O2 |
0.116 |
-0.573 |
0.000 |
| H3 |
-0.860 |
1.147 |
0.000 |
| H4 |
-0.766 |
-0.968 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.3077 | 1.0601 | 1.9177 |
O2 | 1.3077 | | 1.9783 | 0.9669 | H3 | 1.0601 | 1.9783 | | 2.1175 | H4 | 1.9177 | 0.9669 | 2.1175 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
114.104 |
|
O2 |
C1 |
H3 |
112.919 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.087 |
|
|
|
| 2 |
O |
-0.338 |
|
|
|
| 3 |
H |
0.065 |
|
|
|
| 4 |
H |
0.360 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.314 |
-1.743 |
0.000 |
3.744 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.624 |
-0.180 |
0.000 |
| y |
-0.180 |
-13.525 |
0.000 |
| z |
0.000 |
0.000 |
-12.157 |
|
| Traceless |
| | x | y | z |
| x |
0.217 |
-0.180 |
0.000 |
| y |
-0.180 |
-1.134 |
0.000 |
| z |
0.000 |
0.000 |
0.917 |
|
| Polar |
| 3z2-r2 | 1.835 |
| x2-y2 | 0.900 |
| xy | -0.180 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.765 |
0.028 |
0.000 |
| y |
0.028 |
3.311 |
0.000 |
| z |
0.000 |
0.000 |
1.976 |
<r2> (average value of r
2) Å
2
| <r2> |
17.654 |
| (<r2>)1/2 |
4.202 |