Jump to
S2C1
Energy calculated at HF/cc-pVQZ
| | hartrees |
| Energy at 0K | -76.799114 |
| Energy at 298.15K | -76.799033 |
| Nuclear repulsion energy | 24.113391 |
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/cc-pVQZ
| 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 |
3272 |
2972 |
28.41 |
|
|
|
| 2 |
A1 |
1819 |
1653 |
70.74 |
|
|
|
| 3 |
A1 |
1353 |
1229 |
14.49 |
|
|
|
| 4 |
B1 |
914 |
830 |
79.18 |
|
|
|
| 5 |
B2 |
3361 |
3053 |
7.56 |
|
|
|
| 6 |
B2 |
525 |
477 |
16.07 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5622.2 cm
-1
Scaled (by 0.9084) Zero Point Vibrational Energy (zpe) 5107.2 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/cc-pVQZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-0.474 |
| C2 |
0.000 |
0.000 |
0.811 |
| H3 |
0.000 |
0.934 |
-1.009 |
| H4 |
0.000 |
-0.934 |
-1.009 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.2852 | 1.0758 | 1.0758 |
C2 | 1.2852 | | 2.0451 | 2.0451 | H3 | 1.0758 | 2.0451 | | 1.8675 | H4 | 1.0758 | 2.0451 | 1.8675 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C2 |
C1 |
H3 |
119.777 |
|
C2 |
C1 |
H4 |
119.777 |
| H3 |
C1 |
H4 |
120.447 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/cc-pVQZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.299 |
|
|
|
| 2 |
C |
0.028 |
|
|
|
| 3 |
H |
0.135 |
|
|
|
| 4 |
H |
0.135 |
|
|
|
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 |
-2.370 |
2.370 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.506 |
0.000 |
0.000 |
| y |
0.000 |
-10.461 |
0.000 |
| z |
0.000 |
0.000 |
-14.462 |
|
| Traceless |
| | x | y | z |
| x |
-2.044 |
0.000 |
0.000 |
| y |
0.000 |
4.023 |
0.000 |
| z |
0.000 |
0.000 |
-1.979 |
|
| Polar |
| 3z2-r2 | -3.958 |
| x2-y2 | -4.045 |
| 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 |
2.535 |
0.000 |
0.000 |
| y |
0.000 |
2.932 |
0.000 |
| z |
0.000 |
0.000 |
4.277 |
<r2> (average value of r
2) Å
2
| <r2> |
17.283 |
| (<r2>)1/2 |
4.157 |
Jump to
S1C1
Energy calculated at HF/cc-pVQZ
| | hartrees |
| Energy at 0K | -76.765399 |
| Energy at 298.15K | -76.765510 |
| HF Energy | -76.765399 |
| Nuclear repulsion energy | 23.488596 |
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/cc-pVQZ
| 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 |
3212 |
2918 |
9.80 |
|
|
|
| 2 |
A1 |
1584 |
1439 |
0.05 |
|
|
|
| 3 |
A1 |
1401 |
1273 |
9.66 |
|
|
|
| 4 |
B1 |
879 |
798 |
38.81 |
|
|
|
| 5 |
B2 |
3294 |
2992 |
7.48 |
|
|
|
| 6 |
B2 |
1081 |
982 |
0.28 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5725.4 cm
-1
Scaled (by 0.9084) Zero Point Vibrational Energy (zpe) 5201.0 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/cc-pVQZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-0.492 |
| C2 |
0.000 |
0.000 |
0.842 |
| H3 |
0.000 |
0.921 |
-1.050 |
| H4 |
0.000 |
-0.921 |
-1.050 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3333 | 1.0771 | 1.0771 |
C2 | 1.3333 | | 2.1039 | 2.1039 | H3 | 1.0771 | 2.1039 | | 1.8425 | H4 | 1.0771 | 2.1039 | 1.8425 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/cc-pVQZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.185 |
|
|
|
| 2 |
C |
-0.049 |
|
|
|
| 3 |
H |
0.117 |
|
|
|
| 4 |
H |
0.117 |
|
|
|
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 |
-0.522 |
0.522 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.934 |
0.000 |
0.000 |
| y |
0.000 |
-12.058 |
0.000 |
| z |
0.000 |
0.000 |
-11.423 |
|
| Traceless |
| | x | y | z |
| x |
-2.193 |
0.000 |
0.000 |
| y |
0.000 |
0.621 |
0.000 |
| z |
0.000 |
0.000 |
1.573 |
|
| Polar |
| 3z2-r2 | 3.145 |
| x2-y2 | -1.876 |
| 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 |
2.422 |
0.000 |
0.000 |
| y |
0.000 |
2.653 |
0.000 |
| z |
0.000 |
0.000 |
3.935 |
<r2> (average value of r
2) Å
2
| <r2> |
17.392 |
| (<r2>)1/2 |
4.170 |