Jump to
S1C2
Energy calculated at BLYP/6-311G*
| hartrees |
Energy at 0K | -189.122782 |
Energy at 298.15K | -189.123844 |
HF Energy | -189.122782 |
Nuclear repulsion energy | 62.522478 |
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 BLYP/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' |
3310 |
3302 |
13.78 |
|
|
|
2 |
A' |
1784 |
1780 |
268.89 |
|
|
|
3 |
A' |
1264 |
1261 |
7.46 |
|
|
|
4 |
A' |
1003 |
1001 |
113.29 |
|
|
|
5 |
A' |
568 |
567 |
26.85 |
|
|
|
6 |
A" |
608 |
606 |
110.83 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4268.4 cm
-1
Scaled (by 0.9975) Zero Point Vibrational Energy (zpe) 4257.7 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 BLYP/6-311G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.447 |
0.000 |
O2 |
-1.071 |
-0.359 |
0.000 |
O3 |
1.168 |
0.187 |
0.000 |
H4 |
-0.775 |
-1.308 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
O2 |
O3 |
H4 |
C1 | | 1.3402 | 1.1964 | 1.9179 |
O2 | 1.3402 | | 2.3047 | 0.9937 | O3 | 1.1964 | 2.3047 | | 2.4517 | H4 | 1.9179 | 0.9937 | 2.4517 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
O2 |
H4 |
109.630 |
|
O2 |
C1 |
O3 |
130.540 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.250 |
|
|
|
2 |
O |
-0.396 |
|
|
|
3 |
O |
-0.208 |
|
|
|
4 |
H |
0.355 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.785 |
-1.797 |
0.000 |
1.961 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-20.209 |
0.702 |
0.000 |
y |
0.702 |
-14.001 |
0.000 |
z |
0.000 |
0.000 |
-16.198 |
|
Traceless |
| x | y | z |
x |
-5.109 |
0.702 |
0.000 |
y |
0.702 |
4.203 |
0.000 |
z |
0.000 |
0.000 |
0.906 |
|
Polar |
3z2-r2 | 1.813 |
x2-y2 | -6.208 |
xy | 0.702 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.336 |
0.417 |
0.000 |
y |
0.417 |
2.991 |
0.000 |
z |
0.000 |
0.000 |
1.519 |
<r2> (average value of r
2) Å
2
<r2> |
35.404 |
(<r2>)1/2 |
5.950 |
Jump to
S1C1
Energy calculated at BLYP/6-311G*
| hartrees |
Energy at 0K | -189.125136 |
Energy at 298.15K | -189.126175 |
HF Energy | -189.125136 |
Nuclear repulsion energy | 62.161485 |
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 BLYP/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' |
3614 |
3605 |
53.25 |
|
|
|
2 |
A' |
1817 |
1812 |
171.79 |
|
|
|
3 |
A' |
1215 |
1212 |
222.62 |
|
|
|
4 |
A' |
1005 |
1002 |
75.25 |
|
|
|
5 |
A' |
592 |
591 |
6.35 |
|
|
|
6 |
A" |
553 |
552 |
101.91 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4397.7 cm
-1
Scaled (by 0.9975) Zero Point Vibrational Energy (zpe) 4386.7 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 BLYP/6-311G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.423 |
0.000 |
O2 |
-0.950 |
-0.558 |
0.000 |
O3 |
1.179 |
0.257 |
0.000 |
H4 |
-1.829 |
-0.130 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
O2 |
O3 |
H4 |
C1 | | 1.3663 | 1.1909 | 1.9114 |
O2 | 1.3663 | | 2.2801 | 0.9774 | O3 | 1.1909 | 2.2801 | | 3.0333 | H4 | 1.9114 | 0.9774 | 3.0333 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
O2 |
H4 |
108.139 |
|
O2 |
C1 |
O3 |
126.030 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.199 |
|
|
|
2 |
O |
-0.401 |
|
|
|
3 |
O |
-0.192 |
|
|
|
4 |
H |
0.394 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-2.893 |
0.335 |
0.000 |
2.912 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-13.618 |
-0.984 |
0.000 |
y |
-0.984 |
-17.971 |
0.000 |
z |
0.000 |
0.000 |
-16.237 |
|
Traceless |
| x | y | z |
x |
3.486 |
-0.984 |
0.000 |
y |
-0.984 |
-3.043 |
0.000 |
z |
0.000 |
0.000 |
-0.443 |
|
Polar |
3z2-r2 | -0.885 |
x2-y2 | 4.353 |
xy | -0.984 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.954 |
0.277 |
0.000 |
y |
0.277 |
2.092 |
0.000 |
z |
0.000 |
0.000 |
1.554 |
<r2> (average value of r
2) Å
2
<r2> |
35.765 |
(<r2>)1/2 |
5.980 |