Jump to
S1C2
Energy calculated at B3LYP/daug-cc-pVDZ
| hartrees |
Energy at 0K | -151.946103 |
Energy at 298.15K | |
HF Energy | -151.946103 |
Nuclear repulsion energy | 52.258202 |
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 B3LYP/daug-cc-pVDZ
Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
1 |
Σ |
3460 |
3460 |
125.37 |
51.38 |
0.23 |
0.38 |
2 |
Σ |
2092 |
2092 |
250.74 |
14.14 |
0.30 |
0.46 |
3 |
Σ |
1300 |
1300 |
25.73 |
47.46 |
0.14 |
0.24 |
4 |
Π |
552 |
552 |
0.84 |
0.24 |
0.75 |
0.86 |
4 |
Π |
501 |
501 |
3.76 |
0.57 |
0.75 |
0.86 |
5 |
Π |
370 |
370 |
25.78 |
0.31 |
0.75 |
0.86 |
5 |
Π |
448i |
448i |
116.77 |
6.43 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 3913.0 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 3913.0 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 B3LYP/daug-cc-pVDZ
Point Group is C∞v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.000 |
0.020 |
C2 |
0.000 |
0.000 |
-1.247 |
O3 |
0.000 |
0.000 |
1.210 |
H4 |
0.000 |
0.000 |
-2.315 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
O3 |
H4 |
C1 | | 1.2670 | 1.1897 | 2.3353 |
C2 | 1.2670 | | 2.4567 | 1.0683 | O3 | 1.1897 | 2.4567 | | 3.5250 | H4 | 2.3353 | 1.0683 | 3.5250 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
H4 |
180.000 |
|
C2 |
C1 |
O3 |
180.000 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/daug-cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.466 |
|
|
|
2 |
C |
0.317 |
|
|
|
3 |
O |
-0.181 |
|
|
|
4 |
H |
-0.602 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.000 |
0.000 |
-2.181 |
2.181 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-16.377 |
0.000 |
0.000 |
y |
0.000 |
-18.205 |
0.000 |
z |
0.000 |
0.000 |
-15.113 |
|
Traceless |
| x | y | z |
x |
0.282 |
0.000 |
0.000 |
y |
0.000 |
-2.460 |
0.000 |
z |
0.000 |
0.000 |
2.178 |
|
Polar |
3z2-r2 | 4.357 |
x2-y2 | 1.828 |
xy | 0.000 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.818 |
0.000 |
0.000 |
y |
0.000 |
3.167 |
0.000 |
z |
0.000 |
0.000 |
6.441 |
<r2> (average value of r
2) Å
2
<r2> |
36.747 |
(<r2>)1/2 |
6.062 |
Jump to
S1C1
Energy calculated at B3LYP/daug-cc-pVDZ
| hartrees |
Energy at 0K | -151.949352 |
Energy at 298.15K | |
HF Energy | -151.949352 |
Nuclear repulsion energy | 52.104363 |
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 B3LYP/daug-cc-pVDZ
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' |
3320 |
3320 |
36.32 |
86.16 |
0.30 |
0.46 |
2 |
A' |
2072 |
2072 |
338.47 |
9.28 |
0.65 |
0.79 |
3 |
A' |
1244 |
1244 |
6.04 |
40.86 |
0.14 |
0.25 |
4 |
A' |
570 |
570 |
68.84 |
2.53 |
0.74 |
0.85 |
5 |
A' |
506 |
506 |
170.93 |
0.87 |
0.27 |
0.43 |
6 |
A" |
486 |
486 |
1.43 |
0.41 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4098.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4098.9 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 B3LYP/daug-cc-pVDZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.053 |
0.000 |
C2 |
1.093 |
-0.658 |
0.000 |
O3 |
-1.088 |
0.504 |
0.000 |
H4 |
2.143 |
-0.400 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
O3 |
H4 |
C1 | | 1.3045 | 1.1773 | 2.1907 |
C2 | 1.3045 | | 2.4712 | 1.0815 | O3 | 1.1773 | 2.4712 | | 3.3551 | H4 | 2.1907 | 1.0815 | 3.3551 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
H4 |
133.104 |
|
C2 |
C1 |
O3 |
169.420 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/daug-cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.819 |
|
|
|
2 |
C |
0.197 |
|
|
|
3 |
O |
-0.230 |
|
|
|
4 |
H |
-0.786 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
1.588 |
0.461 |
0.000 |
1.654 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-15.645 |
1.181 |
0.000 |
y |
1.181 |
-19.372 |
0.000 |
z |
0.000 |
0.000 |
-16.538 |
|
Traceless |
| x | y | z |
x |
2.310 |
1.181 |
0.000 |
y |
1.181 |
-3.281 |
0.000 |
z |
0.000 |
0.000 |
0.971 |
|
Polar |
3z2-r2 | 1.941 |
x2-y2 | 3.727 |
xy | 1.181 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.657 |
-1.448 |
0.000 |
y |
-1.448 |
4.125 |
0.000 |
z |
0.000 |
0.000 |
3.178 |
<r2> (average value of r
2) Å
2
<r2> |
36.771 |
(<r2>)1/2 |
6.064 |