Jump to
S1C2
Energy calculated at B97D3/6-31G*
| | hartrees |
| Energy at 0K | -114.342391 |
| Energy at 298.15K | -114.343793 |
| HF Energy | -114.342391 |
| 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 B97D3/6-31G*
| 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' |
3530 |
3461 |
27.74 |
|
|
|
| 2 |
A' |
2729 |
2676 |
201.11 |
|
|
|
| 3 |
A' |
1513 |
1483 |
29.30 |
|
|
|
| 4 |
A' |
1271 |
1246 |
28.63 |
|
|
|
| 5 |
A' |
1191 |
1167 |
141.65 |
|
|
|
| 6 |
A" |
1085 |
1064 |
112.52 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5659.1 cm
-1
Scaled (by 0.9804) Zero Point Vibrational Energy (zpe) 5548.2 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 B97D3/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.011 |
0.755 |
0.000 |
| O2 |
-0.011 |
-0.578 |
0.000 |
| H3 |
1.103 |
0.959 |
0.000 |
| H4 |
-0.948 |
-0.870 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.3329 | 1.1321 | 1.8760 |
O2 | 1.3329 | | 1.8978 | 0.9812 | H3 | 1.1321 | 1.8978 | | 2.7476 | H4 | 1.8760 | 0.9812 | 2.7476 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
107.235 |
|
O2 |
C1 |
H3 |
112.431 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.097 |
|
|
|
| 2 |
O |
-0.442 |
|
|
|
| 3 |
H |
0.113 |
|
|
|
| 4 |
H |
0.426 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.435 |
-1.625 |
0.000 |
1.683 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-10.792 |
3.386 |
0.000 |
| y |
3.386 |
-13.495 |
0.000 |
| z |
0.000 |
0.000 |
-11.660 |
|
| Traceless |
| | x | y | z |
| x |
1.785 |
3.386 |
0.000 |
| y |
3.386 |
-2.268 |
0.000 |
| z |
0.000 |
0.000 |
0.483 |
|
| Polar |
| 3z2-r2 | 0.966 |
| x2-y2 | 2.702 |
| 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 |
2.522 |
0.626 |
0.000 |
| y |
0.626 |
2.445 |
0.000 |
| z |
0.000 |
0.000 |
1.354 |
<r2> (average value of r
2) Å
2
| <r2> |
17.368 |
| (<r2>)1/2 |
4.168 |
Jump to
S1C1
Energy calculated at B97D3/6-31G*
| | hartrees |
| Energy at 0K | -114.335043 |
| Energy at 298.15K | -114.336433 |
| HF Energy | -114.335043 |
| 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 B97D3/6-31G*
| 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' |
3228 |
3165 |
82.37 |
|
|
|
| 2 |
A' |
2617 |
2566 |
293.79 |
|
|
|
| 3 |
A' |
1462 |
1433 |
50.05 |
|
|
|
| 4 |
A' |
1300 |
1275 |
30.17 |
|
|
|
| 5 |
A' |
1179 |
1156 |
26.95 |
|
|
|
| 6 |
A" |
1008 |
988 |
36.84 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5396.7 cm
-1
Scaled (by 0.9804) Zero Point Vibrational Energy (zpe) 5291.0 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 B97D3/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.124 |
0.751 |
0.000 |
| O2 |
0.124 |
-0.570 |
0.000 |
| H3 |
-0.968 |
1.075 |
0.000 |
| H4 |
-0.762 |
-1.022 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.3204 | 1.1389 | 1.9814 |
O2 | 1.3204 | | 1.9739 | 0.9944 | H3 | 1.1389 | 1.9739 | | 2.1065 | H4 | 1.9814 | 0.9944 | 2.1065 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
114.760 |
|
O2 |
C1 |
H3 |
113.347 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.042 |
|
|
|
| 2 |
O |
-0.428 |
|
|
|
| 3 |
H |
0.080 |
|
|
|
| 4 |
H |
0.391 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.797 |
-1.673 |
0.000 |
3.259 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.111 |
0.095 |
0.000 |
| y |
0.095 |
-12.866 |
0.000 |
| z |
0.000 |
0.000 |
-11.638 |
|
| Traceless |
| | x | y | z |
| x |
0.141 |
0.095 |
0.000 |
| y |
0.095 |
-0.991 |
0.000 |
| z |
0.000 |
0.000 |
0.850 |
|
| Polar |
| 3z2-r2 | 1.700 |
| x2-y2 | 0.755 |
| xy | 0.095 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.399 |
-0.003 |
0.000 |
| y |
-0.003 |
3.085 |
0.000 |
| z |
0.000 |
0.000 |
1.371 |
<r2> (average value of r
2) Å
2
| <r2> |
17.532 |
| (<r2>)1/2 |
4.187 |