Jump to
S1C2
Energy calculated at LSDA/3-21G
| | hartrees |
| Energy at 0K | -150.258170 |
| Energy at 298.15K | -150.257654 |
| HF Energy | -150.258170 |
| Nuclear repulsion energy | 51.915448 |
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/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' |
3426 |
3370 |
106.69 |
|
|
|
| 2 |
A' |
2110 |
2075 |
71.92 |
|
|
|
| 3 |
A' |
1280 |
1259 |
17.28 |
|
|
|
| 4 |
A' |
606 |
597 |
16.28 |
|
|
|
| 5 |
A' |
402 |
396 |
144.90 |
|
|
|
| 6 |
A" |
517 |
509 |
2.09 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4170.5 cm
-1
Scaled (by 0.9836) Zero Point Vibrational Energy (zpe) 4102.1 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/3-21G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.008 |
0.000 |
| C2 |
0.040 |
-1.248 |
0.000 |
| O3 |
-0.039 |
1.220 |
0.000 |
| H4 |
0.076 |
-2.318 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2575 | 1.2121 | 2.3280 |
C2 | 1.2575 | | 2.4696 | 1.0706 | O3 | 1.2121 | 2.4696 | | 3.5402 | H4 | 2.3280 | 1.0706 | 3.5402 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H4 |
179.886 |
|
C2 |
C1 |
O3 |
179.955 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.161 |
|
|
|
| 2 |
C |
-0.071 |
|
|
|
| 3 |
O |
-0.377 |
|
|
|
| 4 |
H |
0.288 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.066 |
-1.924 |
0.000 |
1.925 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.595 |
-0.106 |
0.000 |
| y |
-0.106 |
-14.527 |
0.000 |
| z |
0.000 |
0.000 |
-16.000 |
|
| Traceless |
| | x | y | z |
| x |
-2.332 |
-0.106 |
0.000 |
| y |
-0.106 |
2.270 |
0.000 |
| z |
0.000 |
0.000 |
0.061 |
|
| Polar |
| 3z2-r2 | 0.123 |
| x2-y2 | -3.068 |
| xy | -0.106 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.981 |
-0.128 |
0.000 |
| y |
-0.128 |
4.994 |
0.000 |
| z |
0.000 |
0.000 |
1.098 |
<r2> (average value of r
2) Å
2
| <r2> |
36.679 |
| (<r2>)1/2 |
6.056 |
Jump to
S1C1
Energy calculated at LSDA/3-21G
| | hartrees |
| Energy at 0K | -150.258170 |
| Energy at 298.15K | -150.257654 |
| Nuclear repulsion energy | 51.915448 |
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/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' |
3426 |
3370 |
106.69 |
|
|
|
| 2 |
A' |
2110 |
2075 |
71.92 |
|
|
|
| 3 |
A' |
1280 |
1259 |
17.28 |
|
|
|
| 4 |
A' |
606 |
597 |
16.28 |
|
|
|
| 5 |
A' |
402 |
396 |
144.90 |
|
|
|
| 6 |
A" |
517 |
509 |
2.09 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4170.5 cm
-1
Scaled (by 0.9836) Zero Point Vibrational Energy (zpe) 4102.1 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/3-21G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.008 |
0.000 |
| C2 |
0.040 |
-1.248 |
0.000 |
| O3 |
-0.039 |
1.220 |
0.000 |
| H4 |
0.076 |
-2.318 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2575 | 1.2121 | 2.3280 |
C2 | 1.2575 | | 2.4696 | 1.0706 | O3 | 1.2121 | 2.4696 | | 3.5402 | H4 | 2.3280 | 1.0706 | 3.5402 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H4 |
179.886 |
|
C2 |
C1 |
O3 |
179.955 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.161 |
|
|
|
| 2 |
C |
-0.071 |
|
|
|
| 3 |
O |
-0.377 |
|
|
|
| 4 |
H |
0.288 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.066 |
-1.924 |
0.000 |
1.925 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.595 |
-0.106 |
0.000 |
| y |
-0.106 |
-14.527 |
0.000 |
| z |
0.000 |
0.000 |
-16.000 |
|
| Traceless |
| | x | y | z |
| x |
-2.332 |
-0.106 |
0.000 |
| y |
-0.106 |
2.270 |
0.000 |
| z |
0.000 |
0.000 |
0.061 |
|
| Polar |
| 3z2-r2 | 0.123 |
| x2-y2 | -3.068 |
| xy | -0.106 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.981 |
-0.128 |
0.000 |
| y |
-0.128 |
4.994 |
0.000 |
| z |
0.000 |
0.000 |
1.098 |
<r2> (average value of r
2) Å
2
| <r2> |
36.679 |
| (<r2>)1/2 |
6.056 |