Jump to
S1C2
Energy calculated at B3LYPultrafine/6-311+G(3df,2p)
| hartrees |
Energy at 0K | -189.172385 |
Energy at 298.15K | -189.173470 |
HF Energy | -189.172385 |
Nuclear repulsion energy | 63.349403 |
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 B3LYPultrafine/6-311+G(3df,2p)
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' |
3592 |
3592 |
17.00 |
|
|
|
2 |
A' |
1871 |
1871 |
340.75 |
|
|
|
3 |
A' |
1290 |
1290 |
0.44 |
|
|
|
4 |
A' |
1071 |
1071 |
165.06 |
|
|
|
5 |
A' |
598 |
598 |
31.76 |
|
|
|
6 |
A" |
586 |
586 |
107.18 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4503.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4503.8 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 B3LYPultrafine/6-311+G(3df,2p)
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.438 |
0.000 |
O2 |
-1.057 |
-0.357 |
0.000 |
O3 |
1.154 |
0.189 |
0.000 |
H4 |
-0.772 |
-1.290 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
O2 |
O3 |
H4 |
C1 | | 1.3227 | 1.1804 | 1.8927 |
O2 | 1.3227 | | 2.2775 | 0.9765 | O3 | 1.1804 | 2.2775 | | 2.4281 | H4 | 1.8927 | 0.9765 | 2.4281 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
O2 |
H4 |
109.904 |
|
O2 |
C1 |
O3 |
130.901 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYPultrafine/6-311+G(3df,2p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.602 |
|
|
|
2 |
O |
-0.377 |
|
|
|
3 |
O |
-0.462 |
|
|
|
4 |
H |
0.237 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-1.056 |
-1.662 |
0.000 |
1.969 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-20.405 |
0.779 |
0.000 |
y |
0.779 |
-14.197 |
0.000 |
z |
0.000 |
0.000 |
-16.484 |
|
Traceless |
| x | y | z |
x |
-5.065 |
0.779 |
0.000 |
y |
0.779 |
4.248 |
0.000 |
z |
0.000 |
0.000 |
0.817 |
|
Polar |
3z2-r2 | 1.634 |
x2-y2 | -6.208 |
xy | 0.779 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.971 |
0.212 |
0.000 |
y |
0.212 |
3.487 |
0.000 |
z |
0.000 |
0.000 |
2.385 |
<r2> (average value of r
2) Å
2
<r2> |
34.945 |
(<r2>)1/2 |
5.911 |
Jump to
S1C1
Energy calculated at B3LYPultrafine/6-311+G(3df,2p)
| hartrees |
Energy at 0K | -189.175472 |
Energy at 298.15K | -189.176545 |
HF Energy | -189.175472 |
Nuclear repulsion energy | 63.094965 |
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 B3LYPultrafine/6-311+G(3df,2p)
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' |
3811 |
3811 |
126.33 |
|
|
|
2 |
A' |
1907 |
1907 |
245.98 |
|
|
|
3 |
A' |
1239 |
1239 |
241.01 |
|
|
|
4 |
A' |
1081 |
1081 |
75.39 |
|
|
|
5 |
A' |
622 |
622 |
4.45 |
|
|
|
6 |
A" |
548 |
548 |
85.76 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4604.2 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4604.2 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 B3LYPultrafine/6-311+G(3df,2p)
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.409 |
0.000 |
O2 |
-0.939 |
-0.546 |
0.000 |
O3 |
1.165 |
0.256 |
0.000 |
H4 |
-1.810 |
-0.130 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
O2 |
O3 |
H4 |
C1 | | 1.3392 | 1.1754 | 1.8880 |
O2 | 1.3392 | | 2.2522 | 0.9648 | O3 | 1.1754 | 2.2522 | | 2.9999 | H4 | 1.8880 | 0.9648 | 2.9999 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
O2 |
H4 |
108.969 |
|
O2 |
C1 |
O3 |
127.065 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYPultrafine/6-311+G(3df,2p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.559 |
|
|
|
2 |
O |
-0.385 |
|
|
|
3 |
O |
-0.442 |
|
|
|
4 |
H |
0.268 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-2.985 |
0.303 |
0.000 |
3.001 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-14.225 |
-0.919 |
0.000 |
y |
-0.919 |
-18.256 |
0.000 |
z |
0.000 |
0.000 |
-16.538 |
|
Traceless |
| x | y | z |
x |
3.173 |
-0.919 |
0.000 |
y |
-0.919 |
-2.875 |
0.000 |
z |
0.000 |
0.000 |
-0.298 |
|
Polar |
3z2-r2 | -0.595 |
x2-y2 | 4.032 |
xy | -0.919 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
4.367 |
0.154 |
0.000 |
y |
0.154 |
3.021 |
0.000 |
z |
0.000 |
0.000 |
2.438 |
<r2> (average value of r
2) Å
2
<r2> |
35.330 |
(<r2>)1/2 |
5.944 |