Jump to
S1C2
Energy calculated at HF/Def2TZVPP
| | hartrees |
| Energy at 0K | -113.842227 |
| Energy at 298.15K | -113.843660 |
| HF Energy | -113.842227 |
| Nuclear repulsion energy | 31.231320 |
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 HF/Def2TZVPP
| 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' |
4102 |
3718 |
124.78 |
|
|
|
| 2 |
A' |
3058 |
2772 |
129.41 |
|
|
|
| 3 |
A' |
1611 |
1460 |
45.36 |
|
|
|
| 4 |
A' |
1440 |
1305 |
137.90 |
|
|
|
| 5 |
A' |
1318 |
1195 |
143.36 |
|
|
|
| 6 |
A" |
1118 |
1013 |
139.13 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6323.3 cm
-1
Scaled (by 0.9064) Zero Point Vibrational Energy (zpe) 5731.5 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 HF/Def2TZVPP
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.004 |
0.724 |
0.000 |
| O2 |
-0.004 |
-0.574 |
0.000 |
| H3 |
0.964 |
1.117 |
0.000 |
| H4 |
-0.902 |
-0.865 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.2977 | 1.0456 | 1.8249 |
O2 | 1.2977 | | 1.9491 | 0.9436 | H3 | 1.0456 | 1.9491 | | 2.7227 | H4 | 1.8249 | 0.9436 | 2.7227 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
107.981 |
|
O2 |
C1 |
H3 |
112.117 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/Def2TZVPP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.034 |
|
|
|
| 2 |
O |
-0.283 |
|
|
|
| 3 |
H |
0.046 |
|
|
|
| 4 |
H |
0.271 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.089 |
-1.425 |
0.000 |
1.427 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.238 |
3.954 |
0.000 |
| y |
3.954 |
-13.744 |
0.000 |
| z |
0.000 |
0.000 |
-11.960 |
|
| Traceless |
| | x | y | z |
| x |
1.614 |
3.954 |
0.000 |
| y |
3.954 |
-2.145 |
0.000 |
| z |
0.000 |
0.000 |
0.531 |
|
| Polar |
| 3z2-r2 | 1.061 |
| x2-y2 | 2.506 |
| xy | 3.954 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.649 |
0.378 |
0.000 |
| y |
0.378 |
2.692 |
0.000 |
| z |
0.000 |
0.000 |
1.969 |
<r2> (average value of r
2) Å
2
| <r2> |
17.090 |
| (<r2>)1/2 |
4.134 |
Jump to
S1C1
Energy calculated at HF/Def2TZVPP
| | hartrees |
| Energy at 0K | -113.833682 |
| Energy at 298.15K | -113.835104 |
| HF Energy | -113.833682 |
| Nuclear repulsion energy | 31.126773 |
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 HF/Def2TZVPP
| 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' |
4041 |
3663 |
53.29 |
|
|
|
| 2 |
A' |
2966 |
2688 |
189.53 |
|
|
|
| 3 |
A' |
1586 |
1437 |
51.15 |
|
|
|
| 4 |
A' |
1433 |
1299 |
193.14 |
|
|
|
| 5 |
A' |
1348 |
1222 |
19.82 |
|
|
|
| 6 |
A" |
1034 |
938 |
35.87 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6204.4 cm
-1
Scaled (by 0.9064) Zero Point Vibrational Energy (zpe) 5623.7 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 HF/Def2TZVPP
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.115 |
0.731 |
0.000 |
| O2 |
0.115 |
-0.570 |
0.000 |
| H3 |
-0.857 |
1.133 |
0.000 |
| H4 |
-0.754 |
-0.955 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.3007 | 1.0518 | 1.8961 |
O2 | 1.3007 | | 1.9608 | 0.9502 | H3 | 1.0518 | 1.9608 | | 2.0901 | H4 | 1.8961 | 0.9502 | 2.0901 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
113.871 |
|
O2 |
C1 |
H3 |
112.488 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/Def2TZVPP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.036 |
|
|
|
| 2 |
O |
-0.286 |
|
|
|
| 3 |
H |
0.019 |
|
|
|
| 4 |
H |
0.230 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.124 |
-1.472 |
0.000 |
3.454 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.401 |
-0.257 |
0.000 |
| y |
-0.257 |
-13.307 |
0.000 |
| z |
0.000 |
0.000 |
-11.891 |
|
| Traceless |
| | x | y | z |
| x |
0.198 |
-0.257 |
0.000 |
| y |
-0.257 |
-1.161 |
0.000 |
| z |
0.000 |
0.000 |
0.963 |
|
| Polar |
| 3z2-r2 | 1.925 |
| x2-y2 | 0.906 |
| xy | -0.257 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.616 |
-0.068 |
0.000 |
| y |
-0.068 |
2.867 |
0.000 |
| z |
0.000 |
0.000 |
1.945 |
<r2> (average value of r
2) Å
2
| <r2> |
17.235 |
| (<r2>)1/2 |
4.152 |