Jump to
S1C2
Energy calculated at LSDA/cc-pVTZ
| | hartrees |
| Energy at 0K | -151.151684 |
| Energy at 298.15K | -151.151149 |
| HF Energy | -151.151684 |
| Nuclear repulsion energy | 52.450726 |
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 LSDA/cc-pVTZ
| 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' |
3289 |
3253 |
62.66 |
|
|
|
| 2 |
A' |
2108 |
2085 |
244.00 |
|
|
|
| 3 |
A' |
1267 |
1253 |
8.33 |
|
|
|
| 4 |
A' |
546 |
540 |
2.99 |
|
|
|
| 5 |
A' |
443 |
438 |
192.87 |
|
|
|
| 6 |
A" |
487 |
482 |
2.54 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4069.8 cm
-1
Scaled (by 0.9891) Zero Point Vibrational Energy (zpe) 4025.4 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 LSDA/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.041 |
0.000 |
| C2 |
1.048 |
-0.697 |
0.000 |
| O3 |
-1.051 |
0.568 |
0.000 |
| H4 |
2.124 |
-0.615 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2814 | 1.1760 | 2.2228 |
C2 | 1.2814 | | 2.4506 | 1.0793 | O3 | 1.1760 | 2.4506 | | 3.3883 | H4 | 2.2228 | 1.0793 | 3.3883 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H4 |
140.493 |
|
C2 |
C1 |
O3 |
171.473 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.208 |
|
|
|
| 2 |
C |
-0.307 |
|
|
|
| 3 |
O |
-0.097 |
|
|
|
| 4 |
H |
0.195 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.667 |
0.191 |
0.000 |
1.677 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.825 |
0.453 |
0.000 |
| y |
0.453 |
-18.966 |
0.000 |
| z |
0.000 |
0.000 |
-16.366 |
|
| Traceless |
| | x | y | z |
| x |
2.841 |
0.453 |
0.000 |
| y |
0.453 |
-3.371 |
0.000 |
| z |
0.000 |
0.000 |
0.530 |
|
| Polar |
| 3z2-r2 | 1.059 |
| x2-y2 | 4.141 |
| xy | 0.453 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.978 |
-1.608 |
0.000 |
| y |
-1.608 |
3.483 |
0.000 |
| z |
0.000 |
0.000 |
2.465 |
<r2> (average value of r
2) Å
2
| <r2> |
36.263 |
| (<r2>)1/2 |
6.022 |
Jump to
S1C1
Energy calculated at LSDA/cc-pVTZ
| | hartrees |
| Energy at 0K | -151.151684 |
| Energy at 298.15K | -151.151149 |
| Nuclear repulsion energy | 52.450726 |
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 LSDA/cc-pVTZ
| 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' |
3289 |
3253 |
62.66 |
|
|
|
| 2 |
A' |
2108 |
2085 |
244.00 |
|
|
|
| 3 |
A' |
1267 |
1253 |
8.33 |
|
|
|
| 4 |
A' |
546 |
540 |
2.99 |
|
|
|
| 5 |
A' |
443 |
438 |
192.87 |
|
|
|
| 6 |
A" |
487 |
482 |
2.54 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4069.8 cm
-1
Scaled (by 0.9891) Zero Point Vibrational Energy (zpe) 4025.4 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 LSDA/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.041 |
0.000 |
| C2 |
1.048 |
-0.697 |
0.000 |
| O3 |
-1.051 |
0.568 |
0.000 |
| H4 |
2.124 |
-0.615 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2814 | 1.1760 | 2.2228 |
C2 | 1.2814 | | 2.4506 | 1.0793 | O3 | 1.1760 | 2.4506 | | 3.3883 | H4 | 2.2228 | 1.0793 | 3.3883 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H4 |
140.493 |
|
C2 |
C1 |
O3 |
171.473 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.208 |
|
|
|
| 2 |
C |
-0.307 |
|
|
|
| 3 |
O |
-0.097 |
|
|
|
| 4 |
H |
0.195 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.667 |
0.191 |
0.000 |
1.677 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.825 |
0.453 |
0.000 |
| y |
0.453 |
-18.966 |
0.000 |
| z |
0.000 |
0.000 |
-16.366 |
|
| Traceless |
| | x | y | z |
| x |
2.841 |
0.453 |
0.000 |
| y |
0.453 |
-3.371 |
0.000 |
| z |
0.000 |
0.000 |
0.530 |
|
| Polar |
| 3z2-r2 | 1.059 |
| x2-y2 | 4.141 |
| xy | 0.453 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.978 |
-1.608 |
0.000 |
| y |
-1.608 |
3.483 |
0.000 |
| z |
0.000 |
0.000 |
2.465 |
<r2> (average value of r
2) Å
2
| <r2> |
36.263 |
| (<r2>)1/2 |
6.022 |