Jump to
S1C2
Energy calculated at B97D3/6-31G
| | hartrees |
| Energy at 0K | -188.913506 |
| Energy at 298.15K | -188.914511 |
| HF Energy | -188.913506 |
| Nuclear repulsion energy | 61.235138 |
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' |
3272 |
3272 |
1.40 |
|
|
|
| 2 |
A' |
1687 |
1687 |
233.74 |
|
|
|
| 3 |
A' |
1251 |
1251 |
3.45 |
|
|
|
| 4 |
A' |
940 |
940 |
146.33 |
|
|
|
| 5 |
A' |
547 |
547 |
33.71 |
|
|
|
| 6 |
A" |
567 |
567 |
155.93 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4131.5 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4131.5 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 B97D3/6-31G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.453 |
0.000 |
| O2 |
-1.089 |
-0.367 |
0.000 |
| O3 |
1.197 |
0.195 |
0.000 |
| H4 |
-0.861 |
-1.341 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
H4 |
| C1 | | 1.3637 | 1.2244 | 1.9899 |
O2 | 1.3637 | | 2.3542 | 0.9999 | O3 | 1.2244 | 2.3542 | | 2.5676 | H4 | 1.9899 | 0.9999 | 2.5676 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
113.793 |
|
O2 |
C1 |
O3 |
130.827 |
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 |
0.445 |
|
|
|
| 2 |
O |
-0.501 |
|
|
|
| 3 |
O |
-0.321 |
|
|
|
| 4 |
H |
0.376 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.884 |
-2.055 |
0.000 |
2.237 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-21.013 |
0.968 |
0.000 |
| y |
0.968 |
-13.490 |
0.000 |
| z |
0.000 |
0.000 |
-15.995 |
|
| Traceless |
| | x | y | z |
| x |
-6.271 |
0.968 |
0.000 |
| y |
0.968 |
5.014 |
0.000 |
| z |
0.000 |
0.000 |
1.257 |
|
| Polar |
| 3z2-r2 | 2.513 |
| x2-y2 | -7.523 |
| xy | 0.968 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.299 |
0.398 |
0.000 |
| y |
0.398 |
2.536 |
0.000 |
| z |
0.000 |
0.000 |
1.191 |
<r2> (average value of r
2) Å
2
| <r2> |
36.619 |
| (<r2>)1/2 |
6.051 |
Jump to
S1C1
Energy calculated at B97D3/6-31G
| | hartrees |
| Energy at 0K | -188.918005 |
| Energy at 298.15K | -188.919002 |
| HF Energy | -188.918005 |
| Nuclear repulsion energy | 61.010242 |
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' |
3558 |
3558 |
54.67 |
|
|
|
| 2 |
A' |
1742 |
1742 |
137.77 |
|
|
|
| 3 |
A' |
1158 |
1158 |
193.45 |
|
|
|
| 4 |
A' |
968 |
968 |
104.36 |
|
|
|
| 5 |
A' |
572 |
572 |
9.51 |
|
|
|
| 6 |
A" |
534 |
534 |
132.76 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4265.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4265.8 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 B97D3/6-31G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.433 |
0.000 |
| O2 |
-0.970 |
-0.563 |
0.000 |
| O3 |
1.204 |
0.258 |
0.000 |
| H4 |
-1.868 |
-0.159 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
H4 |
| C1 | | 1.3906 | 1.2164 | 1.9595 |
O2 | 1.3906 | | 2.3236 | 0.9844 | O3 | 1.2164 | 2.3236 | | 3.0996 | H4 | 1.9595 | 0.9844 | 3.0996 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
110.012 |
|
O2 |
C1 |
O3 |
125.944 |
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 |
0.404 |
|
|
|
| 2 |
O |
-0.496 |
|
|
|
| 3 |
O |
-0.310 |
|
|
|
| 4 |
H |
0.402 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.192 |
0.486 |
0.000 |
3.229 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.637 |
-1.123 |
0.000 |
| y |
-1.123 |
-18.098 |
0.000 |
| z |
0.000 |
0.000 |
-16.012 |
|
| Traceless |
| | x | y | z |
| x |
3.418 |
-1.123 |
0.000 |
| y |
-1.123 |
-3.274 |
0.000 |
| z |
0.000 |
0.000 |
-0.145 |
|
| Polar |
| 3z2-r2 | -0.289 |
| x2-y2 | 4.461 |
| xy | -1.123 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.877 |
0.297 |
0.000 |
| y |
0.297 |
1.889 |
0.000 |
| z |
0.000 |
0.000 |
1.209 |
<r2> (average value of r
2) Å
2
| <r2> |
36.768 |
| (<r2>)1/2 |
6.064 |