Jump to
S2C1
Energy calculated at HF/6-311G**
| | hartrees |
| Energy at 0K | -76.784910 |
| Energy at 298.15K | -76.784829 |
| Nuclear repulsion energy | 24.040055 |
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 HF/6-311G**
| 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 |
3274 |
2974 |
26.66 |
|
|
|
| 2 |
A1 |
1825 |
1658 |
69.29 |
|
|
|
| 3 |
A1 |
1348 |
1225 |
17.29 |
|
|
|
| 4 |
B1 |
908 |
825 |
91.48 |
|
|
|
| 5 |
B2 |
3365 |
3057 |
7.70 |
|
|
|
| 6 |
B2 |
527 |
479 |
12.22 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5623.6 cm
-1
Scaled (by 0.9085) Zero Point Vibrational Energy (zpe) 5109.0 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 HF/6-311G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-0.476 |
| C2 |
0.000 |
0.000 |
0.813 |
| H3 |
0.000 |
0.936 |
-1.012 |
| H4 |
0.000 |
-0.936 |
-1.012 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.2896 | 1.0783 | 1.0783 |
C2 | 1.2896 | | 2.0514 | 2.0514 | H3 | 1.0783 | 2.0514 | | 1.8712 | H4 | 1.0783 | 2.0514 | 1.8712 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C2 |
C1 |
H3 |
119.810 |
|
C2 |
C1 |
H4 |
119.810 |
| H3 |
C1 |
H4 |
120.380 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.330 |
|
|
|
| 2 |
C |
0.001 |
|
|
|
| 3 |
H |
0.165 |
|
|
|
| 4 |
H |
0.165 |
|
|
|
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 |
-2.296 |
2.296 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.356 |
0.000 |
0.000 |
| y |
0.000 |
-10.292 |
0.000 |
| z |
0.000 |
0.000 |
-14.486 |
|
| Traceless |
| | x | y | z |
| x |
-1.968 |
0.000 |
0.000 |
| y |
0.000 |
4.129 |
0.000 |
| z |
0.000 |
0.000 |
-2.162 |
|
| Polar |
| 3z2-r2 | -4.323 |
| x2-y2 | -4.065 |
| 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 |
1.789 |
0.000 |
0.000 |
| y |
0.000 |
2.561 |
0.000 |
| z |
0.000 |
0.000 |
4.049 |
<r2> (average value of r
2) Å
2
| <r2> |
17.277 |
| (<r2>)1/2 |
4.157 |
Jump to
S1C1
Energy calculated at HF/6-311G**
| | hartrees |
| Energy at 0K | -76.752965 |
| Energy at 298.15K | -76.753070 |
| HF Energy | -76.752965 |
| Nuclear repulsion energy | 23.391428 |
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 HF/6-311G**
| 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 |
3213 |
2919 |
9.79 |
|
|
|
| 2 |
A1 |
1578 |
1434 |
0.05 |
|
|
|
| 3 |
A1 |
1396 |
1269 |
10.40 |
|
|
|
| 4 |
B1 |
859 |
781 |
39.21 |
|
|
|
| 5 |
B2 |
3297 |
2995 |
10.87 |
|
|
|
| 6 |
B2 |
1077 |
979 |
0.73 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5710.1 cm
-1
Scaled (by 0.9085) Zero Point Vibrational Energy (zpe) 5187.6 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 HF/6-311G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-0.494 |
| C2 |
0.000 |
0.000 |
0.846 |
| H3 |
0.000 |
0.924 |
-1.054 |
| H4 |
0.000 |
-0.924 |
-1.054 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3398 | 1.0800 | 1.0800 |
C2 | 1.3398 | | 2.1122 | 2.1122 | H3 | 1.0800 | 2.1122 | | 1.8471 | H4 | 1.0800 | 2.1122 | 1.8471 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.188 |
|
|
|
| 2 |
C |
-0.061 |
|
|
|
| 3 |
H |
0.124 |
|
|
|
| 4 |
H |
0.124 |
|
|
|
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 |
-0.507 |
0.507 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.858 |
0.000 |
0.000 |
| y |
0.000 |
-12.015 |
0.000 |
| z |
0.000 |
0.000 |
-11.375 |
|
| Traceless |
| | x | y | z |
| x |
-2.162 |
0.000 |
0.000 |
| y |
0.000 |
0.602 |
0.000 |
| z |
0.000 |
0.000 |
1.561 |
|
| Polar |
| 3z2-r2 | 3.121 |
| x2-y2 | -1.843 |
| 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 |
1.595 |
0.000 |
0.000 |
| y |
0.000 |
2.116 |
0.000 |
| z |
0.000 |
0.000 |
3.604 |
<r2> (average value of r
2) Å
2
| <r2> |
17.438 |
| (<r2>)1/2 |
4.176 |