Jump to
S1C2
Energy calculated at BLYP/3-21G
| | hartrees |
| Energy at 0K | -188.007050 |
| Energy at 298.15K | -188.008037 |
| HF Energy | -188.007050 |
| Nuclear repulsion energy | 60.987625 |
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/3-21G
| 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' |
2964 |
2948 |
40.69 |
|
|
|
| 2 |
A' |
1683 |
1674 |
166.50 |
|
|
|
| 3 |
A' |
1263 |
1256 |
10.88 |
|
|
|
| 4 |
A' |
898 |
893 |
79.85 |
|
|
|
| 5 |
A' |
532 |
529 |
27.20 |
|
|
|
| 6 |
A" |
563 |
559 |
111.54 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3951.5 cm
-1
Scaled (by 0.9945) Zero Point Vibrational Energy (zpe) 3929.8 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 BLYP/3-21G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.448 |
0.000 |
| O2 |
-1.096 |
-0.372 |
0.000 |
| O3 |
1.199 |
0.207 |
0.000 |
| H4 |
-0.826 |
-1.367 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
H4 |
| C1 | | 1.3685 | 1.2230 | 1.9936 |
O2 | 1.3685 | | 2.3670 | 1.0309 | O3 | 1.2230 | 2.3670 | | 2.5648 | H4 | 1.9936 | 1.0309 | 2.5648 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
111.607 |
|
O2 |
C1 |
O3 |
131.867 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.498 |
|
|
|
| 2 |
O |
-0.463 |
|
|
|
| 3 |
O |
-0.366 |
|
|
|
| 4 |
H |
0.332 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.697 |
-2.045 |
0.000 |
2.160 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.105 |
0.783 |
0.000 |
| y |
0.783 |
-13.628 |
0.000 |
| z |
0.000 |
0.000 |
-15.759 |
|
| Traceless |
| | x | y | z |
| x |
-5.412 |
0.783 |
0.000 |
| y |
0.783 |
4.303 |
0.000 |
| z |
0.000 |
0.000 |
1.108 |
|
| Polar |
| 3z2-r2 | 2.216 |
| x2-y2 | -6.477 |
| xy | 0.783 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.908 |
0.493 |
0.000 |
| y |
0.493 |
2.533 |
0.000 |
| z |
0.000 |
0.000 |
1.011 |
<r2> (average value of r
2) Å
2
| <r2> |
36.618 |
| (<r2>)1/2 |
6.051 |
Jump to
S1C1
Energy calculated at BLYP/3-21G
| | hartrees |
| Energy at 0K | -188.009497 |
| Energy at 298.15K | -188.010458 |
| HF Energy | -188.009497 |
| Nuclear repulsion energy | 60.570628 |
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/3-21G
| 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' |
3338 |
3320 |
27.89 |
|
|
|
| 2 |
A' |
1727 |
1717 |
89.45 |
|
|
|
| 3 |
A' |
1159 |
1153 |
164.55 |
|
|
|
| 4 |
A' |
926 |
921 |
85.92 |
|
|
|
| 5 |
A' |
558 |
555 |
9.70 |
|
|
|
| 6 |
A" |
504 |
502 |
109.43 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4106.1 cm
-1
Scaled (by 0.9945) Zero Point Vibrational Energy (zpe) 4083.5 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 BLYP/3-21G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.434 |
0.000 |
| O2 |
-0.972 |
-0.584 |
0.000 |
| O3 |
1.206 |
0.275 |
0.000 |
| H4 |
-1.874 |
-0.135 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
H4 |
| C1 | | 1.4076 | 1.2166 | 1.9588 |
O2 | 1.4076 | | 2.3414 | 1.0083 | O3 | 1.2166 | 2.3414 | | 3.1077 | H4 | 1.9588 | 1.0083 | 3.1077 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
107.193 |
|
O2 |
C1 |
O3 |
126.155 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.451 |
|
|
|
| 2 |
O |
-0.461 |
|
|
|
| 3 |
O |
-0.361 |
|
|
|
| 4 |
H |
0.370 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.861 |
0.274 |
0.000 |
2.874 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.349 |
-1.027 |
0.000 |
| y |
-1.027 |
-17.736 |
0.000 |
| z |
0.000 |
0.000 |
-15.768 |
|
| Traceless |
| | x | y | z |
| x |
3.403 |
-1.027 |
0.000 |
| y |
-1.027 |
-3.178 |
0.000 |
| z |
0.000 |
0.000 |
-0.225 |
|
| Polar |
| 3z2-r2 | -0.450 |
| x2-y2 | 4.387 |
| xy | -1.027 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.599 |
0.316 |
0.000 |
| y |
0.316 |
1.634 |
0.000 |
| z |
0.000 |
0.000 |
1.020 |
<r2> (average value of r
2) Å
2
| <r2> |
36.946 |
| (<r2>)1/2 |
6.078 |