Jump to
S1C2
Energy calculated at wB97X-D/6-31G*
| | hartrees |
| Energy at 0K | -114.370643 |
| Energy at 298.15K | -114.372061 |
| HF Energy | -114.370643 |
| Nuclear repulsion energy | |
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/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' |
3744 |
3551 |
60.66 |
|
|
|
| 2 |
A' |
2860 |
2713 |
171.12 |
|
|
|
| 3 |
A' |
1549 |
1469 |
34.55 |
|
|
|
| 4 |
A' |
1373 |
1303 |
80.68 |
|
|
|
| 5 |
A' |
1244 |
1180 |
128.84 |
|
|
|
| 6 |
A" |
1105 |
1048 |
125.99 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5938.2 cm
-1
Scaled (by 0.9485) Zero Point Vibrational Energy (zpe) 5632.4 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 wB97X-D/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.004 |
0.728 |
0.000 |
| O2 |
-0.004 |
-0.579 |
0.000 |
| H3 |
0.969 |
1.128 |
0.000 |
| H4 |
-0.919 |
-0.863 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.3073 | 1.0521 | 1.8353 |
O2 | 1.3073 | | 1.9653 | 0.9579 | H3 | 1.0521 | 1.9653 | | 2.7440 | H4 | 1.8353 | 0.9579 | 2.7440 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
107.231 |
|
O2 |
C1 |
H3 |
112.362 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.093 |
|
|
|
| 2 |
O |
-0.480 |
|
|
|
| 3 |
H |
0.124 |
|
|
|
| 4 |
H |
0.449 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.380 |
-1.586 |
0.000 |
1.630 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-10.731 |
3.578 |
0.000 |
| y |
3.578 |
-13.460 |
0.000 |
| z |
0.000 |
0.000 |
-11.634 |
|
| Traceless |
| | x | y | z |
| x |
1.816 |
3.578 |
0.000 |
| y |
3.578 |
-2.278 |
0.000 |
| z |
0.000 |
0.000 |
0.462 |
|
| Polar |
| 3z2-r2 | 0.924 |
| x2-y2 | 2.729 |
| xy | 3.578 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.382 |
0.604 |
0.000 |
| y |
0.604 |
2.336 |
0.000 |
| z |
0.000 |
0.000 |
1.354 |
<r2> (average value of r
2) Å
2
| <r2> |
17.123 |
| (<r2>)1/2 |
4.138 |
Jump to
S1C1
Energy calculated at wB97X-D/6-31G*
| | hartrees |
| Energy at 0K | -114.361930 |
| Energy at 298.15K | -114.363337 |
| HF Energy | -114.361930 |
| Nuclear repulsion energy | |
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/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' |
3595 |
3410 |
14.78 |
|
|
|
| 2 |
A' |
2755 |
2613 |
249.01 |
|
|
|
| 3 |
A' |
1502 |
1424 |
55.42 |
|
|
|
| 4 |
A' |
1380 |
1308 |
81.63 |
|
|
|
| 5 |
A' |
1272 |
1207 |
33.93 |
|
|
|
| 6 |
A" |
1024 |
971 |
42.34 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5763.6 cm
-1
Scaled (by 0.9485) Zero Point Vibrational Energy (zpe) 5466.8 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/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.116 |
0.735 |
0.000 |
| O2 |
0.116 |
-0.574 |
0.000 |
| H3 |
-0.860 |
1.148 |
0.000 |
| H4 |
-0.767 |
-0.970 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.3086 | 1.0599 | 1.9206 |
O2 | 1.3086 | | 1.9791 | 0.9684 | H3 | 1.0599 | 1.9791 | | 2.1205 | H4 | 1.9206 | 0.9684 | 2.1205 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
114.186 |
|
O2 |
C1 |
H3 |
112.941 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.040 |
|
|
|
| 2 |
O |
-0.473 |
|
|
|
| 3 |
H |
0.087 |
|
|
|
| 4 |
H |
0.425 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.997 |
-1.692 |
0.000 |
3.442 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.022 |
0.082 |
0.000 |
| y |
0.082 |
-12.906 |
0.000 |
| z |
0.000 |
0.000 |
-11.614 |
|
| Traceless |
| | x | y | z |
| x |
0.238 |
0.082 |
0.000 |
| y |
0.082 |
-1.088 |
0.000 |
| z |
0.000 |
0.000 |
0.850 |
|
| Polar |
| 3z2-r2 | 1.701 |
| x2-y2 | 0.884 |
| xy | 0.082 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.264 |
-0.132 |
0.000 |
| y |
-0.132 |
2.715 |
0.000 |
| z |
0.000 |
0.000 |
1.380 |
<r2> (average value of r
2) Å
2
| <r2> |
17.299 |
| (<r2>)1/2 |
4.159 |