Jump to
S2C1
Energy calculated at BLYP/6-31G**
| | hartrees |
| Energy at 0K | -77.228552 |
| Energy at 298.15K | -77.228182 |
| Nuclear repulsion energy | 23.600864 |
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 |
3059 |
3036 |
36.36 |
|
|
|
| 2 |
A1 |
1658 |
1645 |
81.07 |
|
|
|
| 3 |
A1 |
1191 |
1181 |
22.64 |
|
|
|
| 4 |
B1 |
705 |
699 |
82.76 |
|
|
|
| 5 |
B2 |
3130 |
3106 |
13.42 |
|
|
|
| 6 |
B2 |
311 |
308 |
2.02 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5026.4 cm
-1
Scaled (by 0.9923) Zero Point Vibrational Energy (zpe) 4987.7 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 |
-0.482 |
| C2 |
0.000 |
0.000 |
0.831 |
| H3 |
0.000 |
0.940 |
-1.048 |
| H4 |
0.000 |
-0.940 |
-1.048 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3128 | 1.0974 | 1.0974 |
C2 | 1.3128 | | 2.1013 | 2.1013 | H3 | 1.0974 | 2.1013 | | 1.8797 | H4 | 1.0974 | 2.1013 | 1.8797 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C2 |
C1 |
H3 |
121.083 |
|
C2 |
C1 |
H4 |
121.083 |
| H3 |
C1 |
H4 |
117.834 |
|
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 |
-0.294 |
|
|
|
| 2 |
C |
-0.019 |
|
|
|
| 3 |
H |
0.157 |
|
|
|
| 4 |
H |
0.157 |
|
|
|
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 |
-2.279 |
2.279 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.603 |
0.000 |
0.000 |
| y |
0.000 |
-10.065 |
0.000 |
| z |
0.000 |
0.000 |
-13.720 |
|
| Traceless |
| | x | y | z |
| x |
-1.710 |
0.000 |
0.000 |
| y |
0.000 |
3.596 |
0.000 |
| z |
0.000 |
0.000 |
-1.886 |
|
| Polar |
| 3z2-r2 | -3.773 |
| x2-y2 | -3.538 |
| 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 |
1.471 |
0.000 |
0.000 |
| y |
0.000 |
2.511 |
0.000 |
| z |
0.000 |
0.000 |
3.821 |
<r2> (average value of r
2) Å
2
| <r2> |
17.285 |
| (<r2>)1/2 |
4.158 |
Jump to
S1C1
Energy calculated at BLYP/6-31G**
| | hartrees |
| Energy at 0K | -77.154642 |
| Energy at 298.15K | -77.154495 |
| HF Energy | -77.154642 |
| Nuclear repulsion energy | 23.391062 |
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 |
2945 |
2923 |
4.59 |
|
|
|
| 2 |
A1 |
1545 |
1533 |
8.21 |
|
|
|
| 3 |
A1 |
1369 |
1358 |
0.32 |
|
|
|
| 4 |
B1 |
438 |
435 |
17.06 |
|
|
|
| 5 |
B2 |
3006 |
2983 |
12.07 |
|
|
|
| 6 |
B2 |
969 |
962 |
4.12 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5136.2 cm
-1
Scaled (by 0.9923) Zero Point Vibrational Energy (zpe) 5096.6 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/6-31G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-0.487 |
| C2 |
0.000 |
0.000 |
0.840 |
| H3 |
0.000 |
0.942 |
-1.060 |
| H4 |
0.000 |
-0.942 |
-1.060 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3267 | 1.1031 | 1.1031 |
C2 | 1.3267 | | 2.1209 | 2.1209 | H3 | 1.1031 | 2.1209 | | 1.8847 | H4 | 1.1031 | 2.1209 | 1.8847 | |
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 |
-0.210 |
|
|
|
| 2 |
C |
-0.023 |
|
|
|
| 3 |
H |
0.116 |
|
|
|
| 4 |
H |
0.116 |
|
|
|
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 |
-0.594 |
0.594 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.336 |
0.000 |
0.000 |
| y |
0.000 |
-11.732 |
0.000 |
| z |
0.000 |
0.000 |
-11.030 |
|
| Traceless |
| | x | y | z |
| x |
-1.955 |
0.000 |
0.000 |
| y |
0.000 |
0.451 |
0.000 |
| z |
0.000 |
0.000 |
1.504 |
|
| Polar |
| 3z2-r2 | 3.008 |
| x2-y2 | -1.604 |
| 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 |
2.218 |
0.000 |
0.000 |
| y |
0.000 |
2.257 |
0.000 |
| z |
0.000 |
0.000 |
4.044 |
<r2> (average value of r
2) Å
2
| <r2> |
17.193 |
| (<r2>)1/2 |
4.147 |