Jump to
S2C1
Energy calculated at B3PW91/6-31G
| | hartrees |
| Energy at 0K | -77.205325 |
| Energy at 298.15K | -77.205183 |
| Nuclear repulsion energy | 23.652642 |
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 B3PW91/6-31G
| 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 |
3166 |
3032 |
42.57 |
|
|
|
| 2 |
A1 |
1697 |
1625 |
88.22 |
|
|
|
| 3 |
A1 |
1277 |
1223 |
28.38 |
|
|
|
| 4 |
B1 |
836 |
801 |
141.57 |
|
|
|
| 5 |
B2 |
3248 |
3111 |
14.69 |
|
|
|
| 6 |
B2 |
486 |
465 |
1.07 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5354.9 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 5128.4 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 B3PW91/6-31G
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 |
0.931 |
-1.048 |
| H4 |
0.000 |
-0.931 |
-1.048 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3127 | 1.0896 | 1.0896 |
C2 | 1.3127 | | 2.0971 | 2.0971 | H3 | 1.0896 | 2.0971 | | 1.8614 | H4 | 1.0896 | 2.0971 | 1.8614 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C2 |
C1 |
H3 |
121.332 |
|
C2 |
C1 |
H4 |
121.332 |
| H3 |
C1 |
H4 |
117.335 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.536 |
|
|
|
| 2 |
C |
0.062 |
|
|
|
| 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 |
-2.348 |
2.348 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.794 |
0.000 |
0.000 |
| y |
0.000 |
-9.941 |
0.000 |
| z |
0.000 |
0.000 |
-13.891 |
|
| Traceless |
| | x | y | z |
| x |
-1.879 |
0.000 |
0.000 |
| y |
0.000 |
3.902 |
0.000 |
| z |
0.000 |
0.000 |
-2.023 |
|
| Polar |
| 3z2-r2 | -4.046 |
| x2-y2 | -3.854 |
| 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 |
1.351 |
0.000 |
0.000 |
| y |
0.000 |
2.420 |
0.000 |
| z |
0.000 |
0.000 |
3.808 |
<r2> (average value of r
2) Å
2
| <r2> |
0.000 |
| (<r2>)1/2 |
0.000 |
Jump to
S1C1
Energy calculated at B3PW91/6-31G
| | hartrees |
| Energy at 0K | -77.144156 |
| Energy at 298.15K | -77.144253 |
| HF Energy | -77.144156 |
| Nuclear repulsion energy | 23.469135 |
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 B3PW91/6-31G
| 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 |
3079 |
2949 |
3.53 |
|
|
|
| 2 |
A1 |
1598 |
1530 |
2.70 |
|
|
|
| 3 |
A1 |
1449 |
1387 |
2.92 |
|
|
|
| 4 |
B1 |
854 |
818 |
26.79 |
|
|
|
| 5 |
B2 |
3157 |
3023 |
12.66 |
|
|
|
| 6 |
B2 |
1036 |
992 |
7.03 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5586.1 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 5349.8 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 B3PW91/6-31G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-0.486 |
| C2 |
0.000 |
0.000 |
0.839 |
| H3 |
0.000 |
0.931 |
-1.060 |
| H4 |
0.000 |
-0.931 |
-1.060 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3254 | 1.0931 | 1.0931 |
C2 | 1.3254 | | 2.1147 | 2.1147 | H3 | 1.0931 | 2.1147 | | 1.8613 | H4 | 1.0931 | 2.1147 | 1.8613 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.392 |
|
|
|
| 2 |
C |
0.026 |
|
|
|
| 3 |
H |
0.183 |
|
|
|
| 4 |
H |
0.183 |
|
|
|
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 |
-0.553 |
0.553 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.487 |
0.000 |
0.000 |
| y |
0.000 |
-11.701 |
0.000 |
| z |
0.000 |
0.000 |
-10.992 |
|
| Traceless |
| | x | y | z |
| x |
-2.140 |
0.000 |
0.000 |
| y |
0.000 |
0.538 |
0.000 |
| z |
0.000 |
0.000 |
1.602 |
|
| Polar |
| 3z2-r2 | 3.204 |
| x2-y2 | -1.786 |
| 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 |
1.460 |
0.000 |
0.000 |
| y |
0.000 |
2.030 |
0.000 |
| z |
0.000 |
0.000 |
3.900 |
<r2> (average value of r
2) Å
2
| <r2> |
17.155 |
| (<r2>)1/2 |
4.142 |