Jump to
S1C2
Energy calculated at B3PW91/6-311G**
| | hartrees |
| Energy at 0K | -189.074698 |
| Energy at 298.15K | -189.075808 |
| HF Energy | -189.074698 |
| Nuclear repulsion energy | 63.393471 |
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 B3PW91/6-311G**
| 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' |
3624 |
3490 |
17.52 |
|
|
|
| 2 |
A' |
1901 |
1831 |
325.43 |
|
|
|
| 3 |
A' |
1305 |
1257 |
0.51 |
|
|
|
| 4 |
A' |
1101 |
1060 |
157.41 |
|
|
|
| 5 |
A' |
606 |
584 |
35.67 |
|
|
|
| 6 |
A" |
612 |
589 |
117.60 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4574.4 cm
-1
Scaled (by 0.9631) Zero Point Vibrational Energy (zpe) 4405.6 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 B3PW91/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.440 |
0.000 |
| O2 |
-1.058 |
-0.351 |
0.000 |
| O3 |
1.153 |
0.181 |
0.000 |
| H4 |
-0.759 |
-1.279 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
H4 |
| C1 | | 1.3213 | 1.1820 | 1.8795 |
O2 | 1.3213 | | 2.2744 | 0.9752 | O3 | 1.1820 | 2.2744 | | 2.4057 | H4 | 1.8795 | 0.9752 | 2.4057 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
108.920 |
|
O2 |
C1 |
O3 |
130.522 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.277 |
|
|
|
| 2 |
O |
-0.269 |
|
|
|
| 3 |
O |
-0.255 |
|
|
|
| 4 |
H |
0.247 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.977 |
-1.763 |
0.000 |
2.016 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.092 |
0.654 |
0.000 |
| y |
0.654 |
-13.743 |
0.000 |
| z |
0.000 |
0.000 |
-15.950 |
|
| Traceless |
| | x | y | z |
| x |
-5.246 |
0.654 |
0.000 |
| y |
0.654 |
4.279 |
0.000 |
| z |
0.000 |
0.000 |
0.967 |
|
| Polar |
| 3z2-r2 | 1.935 |
| x2-y2 | -6.350 |
| xy | 0.654 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.190 |
0.248 |
0.000 |
| y |
0.248 |
2.653 |
0.000 |
| z |
0.000 |
0.000 |
1.529 |
<r2> (average value of r
2) Å
2
| <r2> |
34.583 |
| (<r2>)1/2 |
5.881 |
Jump to
S1C1
Energy calculated at B3PW91/6-311G**
| | hartrees |
| Energy at 0K | -189.076823 |
| Energy at 298.15K | -189.077905 |
| HF Energy | -189.076823 |
| Nuclear repulsion energy | 63.100658 |
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 B3PW91/6-311G**
| 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' |
3840 |
3698 |
120.28 |
|
|
|
| 2 |
A' |
1932 |
1861 |
229.34 |
|
|
|
| 3 |
A' |
1248 |
1202 |
266.47 |
|
|
|
| 4 |
A' |
1109 |
1068 |
51.21 |
|
|
|
| 5 |
A' |
626 |
603 |
4.71 |
|
|
|
| 6 |
A" |
553 |
533 |
95.24 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4653.8 cm
-1
Scaled (by 0.9631) Zero Point Vibrational Energy (zpe) 4482.1 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 B3PW91/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.409 |
0.000 |
| O2 |
-0.941 |
-0.543 |
0.000 |
| O3 |
1.166 |
0.250 |
0.000 |
| H4 |
-1.803 |
-0.111 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
H4 |
| C1 | | 1.3382 | 1.1771 | 1.8760 |
O2 | 1.3382 | | 2.2517 | 0.9638 | O3 | 1.1771 | 2.2517 | | 2.9909 | H4 | 1.8760 | 0.9638 | 2.9909 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
108.059 |
|
O2 |
C1 |
O3 |
126.944 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.221 |
|
|
|
| 2 |
O |
-0.262 |
|
|
|
| 3 |
O |
-0.235 |
|
|
|
| 4 |
H |
0.275 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.018 |
0.358 |
0.000 |
3.039 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.709 |
-1.082 |
0.000 |
| y |
-1.082 |
-17.699 |
0.000 |
| z |
0.000 |
0.000 |
-15.992 |
|
| Traceless |
| | x | y | z |
| x |
3.136 |
-1.082 |
0.000 |
| y |
-1.082 |
-2.849 |
0.000 |
| z |
0.000 |
0.000 |
-0.288 |
|
| Polar |
| 3z2-r2 | -0.576 |
| x2-y2 | 3.990 |
| xy | -1.082 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.690 |
0.179 |
0.000 |
| y |
0.179 |
2.028 |
0.000 |
| z |
0.000 |
0.000 |
1.558 |
<r2> (average value of r
2) Å
2
| <r2> |
34.958 |
| (<r2>)1/2 |
5.913 |