Jump to
S2C1
Energy calculated at LSDA/6-31G
| | hartrees |
| Energy at 0K | -76.757866 |
| Energy at 298.15K | -76.757592 |
| Nuclear repulsion energy | 23.622803 |
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/6-31G
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
3087 |
3024 |
63.71 |
|
|
|
| 2 |
A1 |
1688 |
1654 |
93.78 |
|
|
|
| 3 |
A1 |
1198 |
1173 |
44.80 |
|
|
|
| 4 |
B1 |
769 |
754 |
147.56 |
|
|
|
| 5 |
B2 |
3165 |
3100 |
30.67 |
|
|
|
| 6 |
B2 |
373 |
365 |
0.03 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5139.5 cm
-1
Scaled (by 0.9797) Zero Point Vibrational Energy (zpe) 5035.1 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/6-31G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-0.479 |
| C2 |
0.000 |
0.000 |
0.830 |
| H3 |
0.000 |
0.937 |
-1.055 |
| H4 |
0.000 |
-0.937 |
-1.055 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3093 | 1.0998 | 1.0998 |
C2 | 1.3093 | | 2.1055 | 2.1055 | H3 | 1.0998 | 2.1055 | | 1.8733 | H4 | 1.0998 | 2.1055 | 1.8733 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C2 |
C1 |
H3 |
121.606 |
|
C2 |
C1 |
H4 |
121.606 |
| H3 |
C1 |
H4 |
116.788 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.520 |
|
|
|
| 2 |
C |
0.036 |
|
|
|
| 3 |
H |
0.242 |
|
|
|
| 4 |
H |
0.242 |
|
|
|
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 |
-2.499 |
2.499 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.820 |
0.000 |
0.000 |
| y |
0.000 |
-9.920 |
0.000 |
| z |
0.000 |
0.000 |
-13.791 |
|
| Traceless |
| | x | y | z |
| x |
-1.965 |
0.000 |
0.000 |
| y |
0.000 |
3.886 |
0.000 |
| z |
0.000 |
0.000 |
-1.921 |
|
| Polar |
| 3z2-r2 | -3.842 |
| x2-y2 | -3.900 |
| 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 |
1.382 |
0.000 |
0.000 |
| y |
0.000 |
2.473 |
0.000 |
| z |
0.000 |
0.000 |
3.817 |
<r2> (average value of r
2) Å
2
| <r2> |
0.000 |
| (<r2>)1/2 |
0.000 |
Jump to
S1C1
Energy calculated at LSDA/6-31G
| | hartrees |
| Energy at 0K | -76.688391 |
| Energy at 298.15K | -76.688454 |
| HF Energy | -76.688391 |
| Nuclear repulsion energy | 23.443207 |
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/6-31G
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
2979 |
2919 |
1.30 |
|
|
|
| 2 |
A1 |
1604 |
1572 |
4.16 |
|
|
|
| 3 |
A1 |
1380 |
1352 |
2.64 |
|
|
|
| 4 |
B1 |
785 |
769 |
20.04 |
|
|
|
| 5 |
B2 |
3051 |
2989 |
8.57 |
|
|
|
| 6 |
B2 |
987 |
967 |
11.06 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5393.5 cm
-1
Scaled (by 0.9797) Zero Point Vibrational Energy (zpe) 5284.0 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 LSDA/6-31G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-0.483 |
| C2 |
0.000 |
0.000 |
0.838 |
| H3 |
0.000 |
0.939 |
-1.065 |
| H4 |
0.000 |
-0.939 |
-1.065 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3211 | 1.1046 | 1.1046 |
C2 | 1.3211 | | 2.1219 | 2.1219 | H3 | 1.1046 | 2.1219 | | 1.8782 | H4 | 1.1046 | 2.1219 | 1.8782 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.410 |
|
|
|
| 2 |
C |
0.038 |
|
|
|
| 3 |
H |
0.186 |
|
|
|
| 4 |
H |
0.186 |
|
|
|
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 |
-0.639 |
0.639 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.517 |
0.000 |
0.000 |
| y |
0.000 |
-11.712 |
0.000 |
| z |
0.000 |
0.000 |
-11.076 |
|
| Traceless |
| | x | y | z |
| x |
-2.123 |
0.000 |
0.000 |
| y |
0.000 |
0.584 |
0.000 |
| z |
0.000 |
0.000 |
1.538 |
|
| Polar |
| 3z2-r2 | 3.076 |
| x2-y2 | -1.805 |
| 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 |
1.602 |
0.000 |
0.000 |
| y |
0.000 |
2.143 |
0.000 |
| z |
0.000 |
0.000 |
4.006 |
<r2> (average value of r
2) Å
2
| <r2> |
17.203 |
| (<r2>)1/2 |
4.148 |