Jump to
S2C1
Energy calculated at B3PW91/3-21G
| | hartrees |
| Energy at 0K | -76.797434 |
| Energy at 298.15K | -76.797290 |
| Nuclear repulsion energy | 23.724331 |
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 B3PW91/3-21G
| 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 |
3147 |
3025 |
47.92 |
|
|
|
| 2 |
A1 |
1688 |
1623 |
82.14 |
|
|
|
| 3 |
A1 |
1282 |
1232 |
32.39 |
|
|
|
| 4 |
B1 |
823 |
791 |
148.02 |
|
|
|
| 5 |
B2 |
3218 |
3093 |
23.27 |
|
|
|
| 6 |
B2 |
485 |
466 |
0.29 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5321.1 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 5114.6 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 B3PW91/3-21G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-0.479 |
| C2 |
0.000 |
0.000 |
0.827 |
| H3 |
0.000 |
0.932 |
-1.045 |
| H4 |
0.000 |
-0.932 |
-1.045 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3067 | 1.0902 | 1.0902 |
C2 | 1.3067 | | 2.0913 | 2.0913 | H3 | 1.0902 | 2.0913 | | 1.8642 | H4 | 1.0902 | 2.0913 | 1.8642 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C2 |
C1 |
H3 |
121.242 |
|
C2 |
C1 |
H4 |
121.242 |
| H3 |
C1 |
H4 |
117.516 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.633 |
|
|
|
| 2 |
C |
0.052 |
|
|
|
| 3 |
H |
0.290 |
|
|
|
| 4 |
H |
0.290 |
|
|
|
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 |
-2.329 |
2.329 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.994 |
0.000 |
0.000 |
| y |
0.000 |
-10.005 |
0.000 |
| z |
0.000 |
0.000 |
-13.839 |
|
| Traceless |
| | x | y | z |
| x |
-2.072 |
0.000 |
0.000 |
| y |
0.000 |
3.911 |
0.000 |
| z |
0.000 |
0.000 |
-1.839 |
|
| Polar |
| 3z2-r2 | -3.678 |
| x2-y2 | -3.988 |
| 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 |
1.177 |
0.000 |
0.000 |
| y |
0.000 |
2.331 |
0.000 |
| z |
0.000 |
0.000 |
3.605 |
<r2> (average value of r
2) Å
2
| <r2> |
17.284 |
| (<r2>)1/2 |
4.157 |
Jump to
S1C1
Energy calculated at B3PW91/3-21G
| | hartrees |
| Energy at 0K | -76.735786 |
| Energy at 298.15K | -76.735888 |
| HF Energy | -76.735786 |
| Nuclear repulsion energy | 23.550352 |
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 B3PW91/3-21G
| 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 |
3056 |
2938 |
1.58 |
|
|
|
| 2 |
A1 |
1591 |
1529 |
2.63 |
|
|
|
| 3 |
A1 |
1459 |
1402 |
4.12 |
|
|
|
| 4 |
B1 |
859 |
826 |
34.99 |
|
|
|
| 5 |
B2 |
3123 |
3002 |
7.11 |
|
|
|
| 6 |
B2 |
1045 |
1004 |
7.65 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5566.4 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 5350.5 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 B3PW91/3-21G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-0.483 |
| C2 |
0.000 |
0.000 |
0.835 |
| H3 |
0.000 |
0.931 |
-1.057 |
| H4 |
0.000 |
-0.931 |
-1.057 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3185 | 1.0937 | 1.0937 |
C2 | 1.3185 | | 2.1087 | 2.1087 | H3 | 1.0937 | 2.1087 | | 1.8627 | H4 | 1.0937 | 2.1087 | 1.8627 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.492 |
|
|
|
| 2 |
C |
0.017 |
|
|
|
| 3 |
H |
0.237 |
|
|
|
| 4 |
H |
0.237 |
|
|
|
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 |
-0.570 |
0.570 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.715 |
0.000 |
0.000 |
| y |
0.000 |
-11.809 |
0.000 |
| z |
0.000 |
0.000 |
-10.962 |
|
| Traceless |
| | x | y | z |
| x |
-2.329 |
0.000 |
0.000 |
| y |
0.000 |
0.529 |
0.000 |
| z |
0.000 |
0.000 |
1.800 |
|
| Polar |
| 3z2-r2 | 3.599 |
| x2-y2 | -1.905 |
| 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 |
1.228 |
0.000 |
0.000 |
| y |
0.000 |
1.906 |
0.000 |
| z |
0.000 |
0.000 |
3.681 |
<r2> (average value of r
2) Å
2
| <r2> |
17.151 |
| (<r2>)1/2 |
4.141 |