Jump to
S2C1
Energy calculated at B3LYP/STO-3G
| | hartrees |
| Energy at 0K | -76.278245 |
| Energy at 298.15K | -76.278050 |
| Nuclear repulsion energy | 23.341945 |
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 B3LYP/STO-3G
| 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 |
3363 |
3001 |
86.06 |
|
|
|
| 2 |
A1 |
1738 |
1551 |
85.18 |
|
|
|
| 3 |
A1 |
1360 |
1214 |
6.45 |
|
|
|
| 4 |
B1 |
845 |
754 |
60.99 |
|
|
|
| 5 |
B2 |
3492 |
3117 |
28.41 |
|
|
|
| 6 |
B2 |
507 |
452 |
0.02 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5652.5 cm
-1
Scaled (by 0.8924) Zero Point Vibrational Energy (zpe) 5044.3 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 B3LYP/STO-3G
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 |
0.844 |
| H3 |
0.000 |
0.936 |
-1.064 |
| H4 |
0.000 |
-0.936 |
-1.064 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3333 | 1.0981 | 1.0981 |
C2 | 1.3333 | | 2.1250 | 2.1250 | H3 | 1.0981 | 2.1250 | | 1.8716 | H4 | 1.0981 | 2.1250 | 1.8716 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C2 |
C1 |
H3 |
121.547 |
|
C2 |
C1 |
H4 |
121.547 |
| H3 |
C1 |
H4 |
116.905 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.275 |
|
|
|
| 2 |
C |
0.045 |
|
|
|
| 3 |
H |
0.115 |
|
|
|
| 4 |
H |
0.115 |
|
|
|
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 |
-1.637 |
1.637 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.000 |
0.000 |
0.000 |
| y |
0.000 |
-9.385 |
0.000 |
| z |
0.000 |
0.000 |
-12.783 |
|
| Traceless |
| | x | y | z |
| x |
-0.915 |
0.000 |
0.000 |
| y |
0.000 |
3.006 |
0.000 |
| z |
0.000 |
0.000 |
-2.091 |
|
| Polar |
| 3z2-r2 | -4.182 |
| x2-y2 | -2.615 |
| 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 |
0.577 |
0.000 |
0.000 |
| y |
0.000 |
1.427 |
0.000 |
| z |
0.000 |
0.000 |
2.077 |
<r2> (average value of r
2) Å
2
| <r2> |
16.839 |
| (<r2>)1/2 |
4.104 |
Jump to
S1C1
Energy calculated at B3LYP/STO-3G
| | hartrees |
| Energy at 0K | -76.215276 |
| Energy at 298.15K | -76.215327 |
| HF Energy | -76.215276 |
| Nuclear repulsion energy | 23.367569 |
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 B3LYP/STO-3G
| 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 |
3273 |
2921 |
11.86 |
|
|
|
| 2 |
A1 |
1692 |
1510 |
0.02 |
|
|
|
| 3 |
A1 |
1545 |
1378 |
1.18 |
|
|
|
| 4 |
B1 |
836 |
746 |
10.18 |
|
|
|
| 5 |
B2 |
3400 |
3034 |
0.00 |
|
|
|
| 6 |
B2 |
1087 |
970 |
2.37 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5916.6 cm
-1
Scaled (by 0.8924) Zero Point Vibrational Energy (zpe) 5280.0 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 B3LYP/STO-3G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-0.484 |
| C2 |
0.000 |
0.000 |
0.842 |
| H3 |
0.000 |
0.935 |
-1.075 |
| H4 |
0.000 |
-0.935 |
-1.075 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3263 | 1.1057 | 1.1057 |
C2 | 1.3263 | | 2.1326 | 2.1326 | H3 | 1.1057 | 2.1326 | | 1.8696 | H4 | 1.1057 | 2.1326 | 1.8696 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.191 |
|
|
|
| 2 |
C |
0.027 |
|
|
|
| 3 |
H |
0.082 |
|
|
|
| 4 |
H |
0.082 |
|
|
|
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 |
0.044 |
0.044 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.767 |
0.000 |
0.000 |
| y |
0.000 |
-10.711 |
0.000 |
| z |
0.000 |
0.000 |
-9.835 |
|
| Traceless |
| | x | y | z |
| x |
-1.494 |
0.000 |
0.000 |
| y |
0.000 |
0.090 |
0.000 |
| z |
0.000 |
0.000 |
1.404 |
|
| Polar |
| 3z2-r2 | 2.807 |
| x2-y2 | -1.056 |
| 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 |
0.548 |
0.000 |
0.000 |
| y |
0.000 |
1.074 |
0.000 |
| z |
0.000 |
0.000 |
2.127 |
<r2> (average value of r
2) Å
2
| <r2> |
16.446 |
| (<r2>)1/2 |
4.055 |