Jump to
S2C1
Energy calculated at B1B95/6-31G*
| | hartrees |
| Energy at 0K | -77.215759 |
| Energy at 298.15K | -77.215419 |
| Nuclear repulsion energy | 23.806975 |
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 B1B95/6-31G*
| 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 |
3165 |
3005 |
42.03 |
|
|
|
| 2 |
A1 |
1733 |
1645 |
84.45 |
|
|
|
| 3 |
A1 |
1233 |
1170 |
24.17 |
|
|
|
| 4 |
B1 |
749 |
711 |
98.88 |
|
|
|
| 5 |
B2 |
3244 |
3079 |
16.98 |
|
|
|
| 6 |
B2 |
319 |
303 |
1.91 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5221.1 cm
-1
Scaled (by 0.9493) Zero Point Vibrational Energy (zpe) 4956.4 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 B1B95/6-31G*
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 |
0.823 |
| H3 |
0.000 |
0.935 |
-1.036 |
| H4 |
0.000 |
-0.935 |
-1.036 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3010 | 1.0893 | 1.0893 |
C2 | 1.3010 | | 2.0811 | 2.0811 | H3 | 1.0893 | 2.0811 | | 1.8708 | H4 | 1.0893 | 2.0811 | 1.8708 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C2 |
C1 |
H3 |
120.822 |
|
C2 |
C1 |
H4 |
120.822 |
| H3 |
C1 |
H4 |
118.357 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.485 |
|
|
|
| 2 |
C |
0.024 |
|
|
|
| 3 |
H |
0.231 |
|
|
|
| 4 |
H |
0.231 |
|
|
|
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 |
-2.260 |
2.260 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.663 |
0.000 |
0.000 |
| y |
0.000 |
-9.939 |
0.000 |
| z |
0.000 |
0.000 |
-13.631 |
|
| Traceless |
| | x | y | z |
| x |
-1.878 |
0.000 |
0.000 |
| y |
0.000 |
3.708 |
0.000 |
| z |
0.000 |
0.000 |
-1.831 |
|
| Polar |
| 3z2-r2 | -3.661 |
| x2-y2 | -3.724 |
| 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 |
1.433 |
0.000 |
0.000 |
| y |
0.000 |
2.445 |
0.000 |
| z |
0.000 |
0.000 |
3.746 |
<r2> (average value of r
2) Å
2
| <r2> |
17.083 |
| (<r2>)1/2 |
4.133 |
Jump to
S1C1
Energy calculated at B1B95/6-31G*
| | hartrees |
| Energy at 0K | -77.144569 |
| Energy at 298.15K | -77.144627 |
| HF Energy | -77.144569 |
| Nuclear repulsion energy | 23.610336 |
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 B1B95/6-31G*
| 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 |
3086 |
2930 |
3.57 |
|
|
|
| 2 |
A1 |
1622 |
1540 |
5.07 |
|
|
|
| 3 |
A1 |
1420 |
1348 |
1.20 |
|
|
|
| 4 |
B1 |
763 |
724 |
10.29 |
|
|
|
| 5 |
B2 |
3161 |
3001 |
7.75 |
|
|
|
| 6 |
B2 |
1005 |
954 |
4.09 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5528.3 cm
-1
Scaled (by 0.9493) Zero Point Vibrational Energy (zpe) 5248.0 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 B1B95/6-31G*
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 |
0.832 |
| H3 |
0.000 |
0.933 |
-1.050 |
| H4 |
0.000 |
-0.933 |
-1.050 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3147 | 1.0922 | 1.0922 |
C2 | 1.3147 | | 2.1008 | 2.1008 | H3 | 1.0922 | 2.1008 | | 1.8665 | H4 | 1.0922 | 2.1008 | 1.8665 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.373 |
|
|
|
| 2 |
C |
0.002 |
|
|
|
| 3 |
H |
0.185 |
|
|
|
| 4 |
H |
0.185 |
|
|
|
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 |
-0.552 |
0.552 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.392 |
0.000 |
0.000 |
| y |
0.000 |
-11.637 |
0.000 |
| z |
0.000 |
0.000 |
-10.864 |
|
| Traceless |
| | x | y | z |
| x |
-2.142 |
0.000 |
0.000 |
| y |
0.000 |
0.492 |
0.000 |
| z |
0.000 |
0.000 |
1.650 |
|
| Polar |
| 3z2-r2 | 3.300 |
| x2-y2 | -1.755 |
| 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 |
1.598 |
0.000 |
0.000 |
| y |
0.000 |
2.133 |
0.000 |
| z |
0.000 |
0.000 |
3.893 |
<r2> (average value of r
2) Å
2
| <r2> |
16.972 |
| (<r2>)1/2 |
4.120 |