Jump to
S1C2
Energy calculated at ROHF/cc-pVTZ
| | hartrees |
| Energy at 0K | -188.203334 |
| Energy at 298.15K | -188.204508 |
| HF Energy | -188.203334 |
| Nuclear repulsion energy | 64.405780 |
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 ROHF/cc-pVTZ
| 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' |
4022 |
3623 |
103.24 |
|
|
|
| 2 |
A' |
2072 |
1867 |
509.30 |
|
|
|
| 3 |
A' |
1420 |
1279 |
5.74 |
|
|
|
| 4 |
A' |
1230 |
1108 |
237.44 |
|
|
|
| 5 |
A' |
675 |
608 |
49.25 |
|
|
|
| 6 |
A" |
622 |
561 |
151.65 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5020.4 cm
-1
Scaled (by 0.901) Zero Point Vibrational Energy (zpe) 4523.4 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 ROHF/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.430 |
0.000 |
| O2 |
-1.040 |
-0.359 |
0.000 |
| O3 |
1.135 |
0.194 |
0.000 |
| H4 |
-0.759 |
-1.267 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
H4 |
| C1 | | 1.3053 | 1.1589 | 1.8586 |
O2 | 1.3053 | | 2.2437 | 0.9502 | O3 | 1.1589 | 2.2437 | | 2.3914 | H4 | 1.8586 | 0.9502 | 2.3914 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
109.982 |
|
O2 |
C1 |
O3 |
131.065 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at ROHF/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.318 |
|
|
|
| 2 |
O |
-0.271 |
|
|
|
| 3 |
O |
-0.290 |
|
|
|
| 4 |
H |
0.243 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.393 |
-1.495 |
0.000 |
2.043 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.650 |
0.527 |
-0.001 |
| y |
0.527 |
-13.382 |
-0.003 |
| z |
-0.001 |
-0.003 |
-15.917 |
|
| Traceless |
| | x | y | z |
| x |
-6.001 |
0.527 |
-0.001 |
| y |
0.527 |
4.901 |
-0.003 |
| z |
-0.001 |
-0.003 |
1.100 |
|
| Polar |
| 3z2-r2 | 2.199 |
| x2-y2 | -7.268 |
| xy | 0.527 |
| xz | -0.001 |
| yz | -0.003 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.000 |
0.000 |
0.000 |
| y |
0.000 |
0.000 |
0.000 |
| z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
| <r2> |
33.971 |
| (<r2>)1/2 |
5.828 |
Jump to
S1C1
Energy calculated at ROHF/cc-pVTZ
| | hartrees |
| Energy at 0K | -188.203434 |
| Energy at 298.15K | -188.204567 |
| HF Energy | -188.203434 |
| Nuclear repulsion energy | 64.195944 |
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 ROHF/cc-pVTZ
| 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' |
4142 |
3732 |
171.46 |
|
|
|
| 2 |
A' |
2122 |
1912 |
420.10 |
|
|
|
| 3 |
A' |
1384 |
1247 |
357.10 |
|
|
|
| 4 |
A' |
1220 |
1099 |
32.41 |
|
|
|
| 5 |
A' |
699 |
629 |
6.83 |
|
|
|
| 6 |
A" |
541 |
487 |
90.64 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5053.5 cm
-1
Scaled (by 0.901) Zero Point Vibrational Energy (zpe) 4553.2 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 ROHF/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.389 |
0.000 |
| O2 |
-0.924 |
-0.544 |
0.000 |
| O3 |
1.147 |
0.271 |
0.000 |
| H4 |
-1.785 |
-0.157 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
H4 |
| C1 | | 1.3132 | 1.1534 | 1.8663 |
O2 | 1.3132 | | 2.2262 | 0.9431 | O3 | 1.1534 | 2.2262 | | 2.9630 | H4 | 1.8663 | 0.9431 | 2.9630 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
110.537 |
|
O2 |
C1 |
O3 |
128.865 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at ROHF/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.252 |
|
|
|
| 2 |
O |
-0.229 |
|
|
|
| 3 |
O |
-0.263 |
|
|
|
| 4 |
H |
0.240 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.450 |
0.576 |
0.000 |
3.498 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.249 |
-1.201 |
-0.004 |
| y |
-1.201 |
-17.641 |
-0.000 |
| z |
-0.004 |
-0.000 |
-15.948 |
|
| Traceless |
| | x | y | z |
| x |
2.545 |
-1.201 |
-0.004 |
| y |
-1.201 |
-2.543 |
-0.000 |
| z |
-0.004 |
-0.000 |
-0.002 |
|
| Polar |
| 3z2-r2 | -0.005 |
| x2-y2 | 3.392 |
| xy | -1.201 |
| xz | -0.004 |
| yz | -0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.000 |
0.000 |
0.000 |
| y |
0.000 |
0.000 |
0.000 |
| z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
| <r2> |
34.397 |
| (<r2>)1/2 |
5.865 |