Jump to
S2C1
Energy calculated at BLYP/6-31G
| | hartrees |
| Energy at 0K | -77.208520 |
| Energy at 298.15K | -77.208333 |
| Nuclear repulsion energy | 23.462758 |
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 BLYP/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 |
3068 |
3045 |
36.11 |
|
|
|
| 2 |
A1 |
1632 |
1619 |
86.56 |
|
|
|
| 3 |
A1 |
1240 |
1231 |
25.08 |
|
|
|
| 4 |
B1 |
777 |
771 |
119.59 |
|
|
|
| 5 |
B2 |
3138 |
3115 |
10.00 |
|
|
|
| 6 |
B2 |
459 |
456 |
1.11 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5157.3 cm
-1
Scaled (by 0.9924) Zero Point Vibrational Energy (zpe) 5118.1 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 BLYP/6-31G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-0.485 |
| C2 |
0.000 |
0.000 |
0.838 |
| H3 |
0.000 |
0.935 |
-1.060 |
| H4 |
0.000 |
-0.935 |
-1.060 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3233 | 1.0980 | 1.0980 |
C2 | 1.3233 | | 2.1163 | 2.1163 | H3 | 1.0980 | 2.1163 | | 1.8707 | H4 | 1.0980 | 2.1163 | 1.8707 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C2 |
C1 |
H3 |
121.584 |
|
C2 |
C1 |
H4 |
121.584 |
| H3 |
C1 |
H4 |
116.833 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.420 |
|
|
|
| 2 |
C |
0.035 |
|
|
|
| 3 |
H |
0.192 |
|
|
|
| 4 |
H |
0.192 |
|
|
|
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 |
-2.323 |
2.323 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.703 |
0.000 |
0.000 |
| y |
0.000 |
-10.060 |
0.000 |
| z |
0.000 |
0.000 |
-13.919 |
|
| Traceless |
| | x | y | z |
| x |
-1.713 |
0.000 |
0.000 |
| y |
0.000 |
3.751 |
0.000 |
| z |
0.000 |
0.000 |
-2.038 |
|
| Polar |
| 3z2-r2 | -4.076 |
| x2-y2 | -3.643 |
| 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 |
1.358 |
0.000 |
0.000 |
| y |
0.000 |
2.453 |
0.000 |
| z |
0.000 |
0.000 |
3.838 |
<r2> (average value of r
2) Å
2
| <r2> |
0.000 |
| (<r2>)1/2 |
0.000 |
Jump to
S1C1
Energy calculated at BLYP/6-31G
| | hartrees |
| Energy at 0K | -77.137942 |
| Energy at 298.15K | -77.137942 |
| HF Energy | -77.137942 |
| Nuclear repulsion energy | 23.294996 |
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 BLYP/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 |
2957 |
2934 |
4.54 |
|
|
|
| 2 |
A1 |
1534 |
1523 |
6.62 |
|
|
|
| 3 |
A1 |
1408 |
1397 |
0.78 |
|
|
|
| 4 |
B1 |
636 |
631 |
1.29 |
|
|
|
| 5 |
B2 |
3018 |
2995 |
18.41 |
|
|
|
| 6 |
B2 |
1004 |
997 |
6.95 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5278.5 cm
-1
Scaled (by 0.9924) Zero Point Vibrational Energy (zpe) 5238.4 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 BLYP/6-31G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-0.489 |
| C2 |
0.000 |
0.000 |
0.845 |
| H3 |
0.000 |
0.939 |
-1.068 |
| H4 |
0.000 |
-0.939 |
-1.068 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3342 | 1.1033 | 1.1033 |
C2 | 1.3342 | | 2.1316 | 2.1316 | H3 | 1.1033 | 2.1316 | | 1.8777 | H4 | 1.1033 | 2.1316 | 1.8777 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.303 |
|
|
|
| 2 |
C |
0.014 |
|
|
|
| 3 |
H |
0.144 |
|
|
|
| 4 |
H |
0.144 |
|
|
|
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 |
-0.600 |
0.600 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.414 |
0.000 |
0.000 |
| y |
0.000 |
-11.786 |
0.000 |
| z |
0.000 |
0.000 |
-11.135 |
|
| Traceless |
| | x | y | z |
| x |
-1.953 |
0.000 |
0.000 |
| y |
0.000 |
0.489 |
0.000 |
| z |
0.000 |
0.000 |
1.465 |
|
| Polar |
| 3z2-r2 | 2.930 |
| x2-y2 | -1.628 |
| 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 |
2.012 |
0.000 |
0.000 |
| y |
0.000 |
2.138 |
0.000 |
| z |
0.000 |
0.000 |
4.031 |
<r2> (average value of r
2) Å
2
| <r2> |
17.332 |
| (<r2>)1/2 |
4.163 |