Jump to
S2C1
Energy calculated at CCD/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -77.066135 |
| Energy at 298.15K | -77.065873 |
| HF Energy | -76.772728 |
| Nuclear repulsion energy | 23.782629 |
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 CCD/6-31G(2df,p)
| 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 |
3197 |
3028 |
36.99 |
|
|
|
| 2 |
A1 |
1701 |
1612 |
70.78 |
|
|
|
| 3 |
A1 |
1253 |
1187 |
15.73 |
|
|
|
| 4 |
B1 |
790 |
749 |
69.61 |
|
|
|
| 5 |
B2 |
3292 |
3118 |
14.25 |
|
|
|
| 6 |
B2 |
371 |
351 |
6.13 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5302.3 cm
-1
Scaled (by 0.9472) Zero Point Vibrational Energy (zpe) 5022.3 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 CCD/6-31G(2df,p)
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-0.481 |
| C2 |
0.000 |
0.000 |
0.824 |
| H3 |
0.000 |
0.937 |
-1.029 |
| H4 |
0.000 |
-0.937 |
-1.029 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3057 | 1.0852 | 1.0852 |
C2 | 1.3057 | | 2.0765 | 2.0765 | H3 | 1.0852 | 2.0765 | | 1.8739 | H4 | 1.0852 | 2.0765 | 1.8739 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C2 |
C1 |
H3 |
120.298 |
|
C2 |
C1 |
H4 |
120.298 |
| H3 |
C1 |
H4 |
119.404 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at CCD/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -76.986570 |
| Energy at 298.15K | -76.986692 |
| HF Energy | -76.740666 |
| Nuclear repulsion energy | 23.773237 |
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 CCD/6-31G(2df,p)
| 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 |
3146 |
2980 |
2.17 |
|
|
|
| 2 |
A1 |
1626 |
1540 |
3.56 |
|
|
|
| 3 |
A1 |
1441 |
1365 |
4.68 |
|
|
|
| 4 |
B1 |
956 |
906 |
27.85 |
|
|
|
| 5 |
B2 |
3230 |
3059 |
3.27 |
|
|
|
| 6 |
B2 |
1029 |
974 |
1.23 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5713.2 cm
-1
Scaled (by 0.9472) Zero Point Vibrational Energy (zpe) 5411.5 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 CCD/6-31G(2df,p)
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-0.478 |
| C2 |
0.000 |
0.000 |
0.826 |
| H3 |
0.000 |
0.929 |
-1.044 |
| H4 |
0.000 |
-0.929 |
-1.044 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3040 | 1.0877 | 1.0877 |
C2 | 1.3040 | | 2.0879 | 2.0879 | H3 | 1.0877 | 2.0879 | | 1.8579 | H4 | 1.0877 | 2.0879 | 1.8579 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability