Jump to
S2C1
Energy calculated at BLYP/6-31+G**
| | hartrees |
| Energy at 0K | -77.239209 |
| Energy at 298.15K | -77.238871 |
| Nuclear repulsion energy | 23.611426 |
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/6-31+G**
| 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 |
3049 |
3033 |
42.57 |
|
|
|
| 2 |
A1 |
1655 |
1646 |
93.46 |
|
|
|
| 3 |
A1 |
1183 |
1177 |
25.14 |
|
|
|
| 4 |
B1 |
714 |
710 |
106.16 |
|
|
|
| 5 |
B2 |
3122 |
3105 |
17.96 |
|
|
|
| 6 |
B2 |
335 |
333 |
4.28 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5028.3 cm
-1
Scaled (by 0.9947) Zero Point Vibrational Energy (zpe) 5001.6 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 BLYP/6-31+G**
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 |
0.830 |
| H3 |
0.000 |
0.943 |
-1.046 |
| H4 |
0.000 |
-0.943 |
-1.046 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3115 | 1.0986 | 1.0986 |
C2 | 1.3115 | | 2.0993 | 2.0993 | H3 | 1.0986 | 2.0993 | | 1.8853 | H4 | 1.0986 | 2.0993 | 1.8853 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C2 |
C1 |
H3 |
120.908 |
|
C2 |
C1 |
H4 |
120.908 |
| H3 |
C1 |
H4 |
118.184 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.045 |
|
|
|
| 2 |
C |
-0.437 |
|
|
|
| 3 |
H |
0.196 |
|
|
|
| 4 |
H |
0.196 |
|
|
|
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 |
-2.511 |
2.511 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.780 |
0.000 |
0.000 |
| y |
0.000 |
-10.690 |
0.000 |
| z |
0.000 |
0.000 |
-14.630 |
|
| Traceless |
| | x | y | z |
| x |
-2.119 |
0.000 |
0.000 |
| y |
0.000 |
4.015 |
0.000 |
| z |
0.000 |
0.000 |
-1.896 |
|
| Polar |
| 3z2-r2 | -3.791 |
| x2-y2 | -4.090 |
| 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 |
2.742 |
0.000 |
0.000 |
| y |
0.000 |
2.975 |
0.000 |
| z |
0.000 |
0.000 |
4.837 |
<r2> (average value of r
2) Å
2
| <r2> |
0.000 |
| (<r2>)1/2 |
0.000 |
Jump to
S1C1
Energy calculated at BLYP/6-31+G**
| | hartrees |
| Energy at 0K | -77.162610 |
| Energy at 298.15K | -77.162419 |
| HF Energy | -77.162610 |
| Nuclear repulsion energy | 23.358231 |
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/6-31+G**
| 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 |
2948 |
2932 |
4.81 |
|
|
|
| 2 |
A1 |
1527 |
1519 |
7.50 |
|
|
|
| 3 |
A1 |
1359 |
1352 |
0.30 |
|
|
|
| 4 |
B1 |
393 |
391 |
56.19 |
|
|
|
| 5 |
B2 |
3013 |
2997 |
5.84 |
|
|
|
| 6 |
B2 |
965 |
959 |
7.74 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5101.8 cm
-1
Scaled (by 0.9947) Zero Point Vibrational Energy (zpe) 5074.8 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/6-31+G**
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 |
0.841 |
| H3 |
0.000 |
0.944 |
-1.058 |
| H4 |
0.000 |
-0.944 |
-1.058 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3297 | 1.1028 | 1.1028 |
C2 | 1.3297 | | 2.1212 | 2.1212 | H3 | 1.1028 | 2.1212 | | 1.8887 | H4 | 1.1028 | 2.1212 | 1.8887 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.260 |
|
|
|
| 2 |
C |
-0.056 |
|
|
|
| 3 |
H |
0.158 |
|
|
|
| 4 |
H |
0.158 |
|
|
|
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 |
-0.757 |
0.757 |
| 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 |
-12.403 |
0.000 |
| z |
0.000 |
0.000 |
-11.724 |
|
| Traceless |
| | x | y | z |
| x |
-2.293 |
0.000 |
0.000 |
| y |
0.000 |
0.637 |
0.000 |
| z |
0.000 |
0.000 |
1.656 |
|
| Polar |
| 3z2-r2 | 3.311 |
| x2-y2 | -1.953 |
| 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 |
4.106 |
0.000 |
0.000 |
| y |
0.000 |
2.740 |
0.000 |
| z |
0.000 |
0.000 |
4.848 |
<r2> (average value of r
2) Å
2
| <r2> |
17.713 |
| (<r2>)1/2 |
4.209 |