Jump to
S2C1
Energy calculated at HF/Def2TZVPP
| | hartrees |
| Energy at 0K | -76.796701 |
| Energy at 298.15K | -76.796621 |
| HF Energy | -76.796701 |
| Nuclear repulsion energy | 24.104436 |
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 HF/Def2TZVPP
| 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 |
3274 |
2968 |
28.79 |
|
|
|
| 2 |
A1 |
1822 |
1652 |
70.61 |
|
|
|
| 3 |
A1 |
1354 |
1228 |
15.00 |
|
|
|
| 4 |
B1 |
914 |
828 |
82.36 |
|
|
|
| 5 |
B2 |
3363 |
3049 |
7.67 |
|
|
|
| 6 |
B2 |
529 |
479 |
15.58 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5628.6 cm
-1
Scaled (by 0.9064) Zero Point Vibrational Energy (zpe) 5101.8 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 HF/Def2TZVPP
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-0.474 |
| C2 |
0.000 |
0.000 |
0.811 |
| H3 |
0.000 |
0.933 |
-1.011 |
| H4 |
0.000 |
-0.933 |
-1.011 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.2853 | 1.0762 | 1.0762 |
C2 | 1.2853 | | 2.0471 | 2.0471 | H3 | 1.0762 | 2.0471 | | 1.8650 | H4 | 1.0762 | 2.0471 | 1.8650 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C2 |
C1 |
H3 |
119.942 |
|
C2 |
C1 |
H4 |
119.942 |
| H3 |
C1 |
H4 |
120.116 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/Def2TZVPP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.119 |
|
|
|
| 2 |
C |
-0.071 |
|
|
|
| 3 |
H |
0.095 |
|
|
|
| 4 |
H |
0.095 |
|
|
|
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 |
-2.373 |
2.373 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.547 |
0.000 |
0.000 |
| y |
0.000 |
-10.465 |
0.000 |
| z |
0.000 |
0.000 |
-14.487 |
|
| Traceless |
| | x | y | z |
| x |
-2.071 |
0.000 |
0.000 |
| y |
0.000 |
4.052 |
0.000 |
| z |
0.000 |
0.000 |
-1.981 |
|
| Polar |
| 3z2-r2 | -3.962 |
| x2-y2 | -4.082 |
| 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 |
2.480 |
0.000 |
0.000 |
| y |
0.000 |
2.834 |
0.000 |
| z |
0.000 |
0.000 |
4.273 |
<r2> (average value of r
2) Å
2
| <r2> |
17.305 |
| (<r2>)1/2 |
4.160 |
Jump to
S1C1
Energy calculated at HF/Def2TZVPP
| | hartrees |
| Energy at 0K | -76.763050 |
| Energy at 298.15K | -76.763160 |
| HF Energy | -76.763050 |
| Nuclear repulsion energy | 23.478419 |
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 HF/Def2TZVPP
| 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 |
3214 |
2913 |
9.71 |
|
|
|
| 2 |
A1 |
1585 |
1436 |
0.05 |
|
|
|
| 3 |
A1 |
1403 |
1271 |
9.61 |
|
|
|
| 4 |
B1 |
879 |
797 |
39.30 |
|
|
|
| 5 |
B2 |
3295 |
2987 |
7.60 |
|
|
|
| 6 |
B2 |
1081 |
979 |
0.36 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5728.1 cm
-1
Scaled (by 0.9064) Zero Point Vibrational Energy (zpe) 5192.0 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 HF/Def2TZVPP
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 |
0.839 |
| H3 |
0.000 |
0.921 |
-1.050 |
| H4 |
0.000 |
-0.921 |
-1.050 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3274 | 1.0789 | 1.0789 |
C2 | 1.3274 | | 2.1014 | 2.1014 | H3 | 1.0789 | 2.1014 | | 1.8428 | H4 | 1.0789 | 2.1014 | 1.8428 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/Def2TZVPP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.110 |
|
|
|
| 2 |
C |
-0.036 |
|
|
|
| 3 |
H |
0.073 |
|
|
|
| 4 |
H |
0.073 |
|
|
|
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 |
-0.522 |
0.522 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.953 |
0.000 |
0.000 |
| y |
0.000 |
-12.069 |
0.000 |
| z |
0.000 |
0.000 |
-11.421 |
|
| Traceless |
| | x | y | z |
| x |
-2.208 |
0.000 |
0.000 |
| y |
0.000 |
0.618 |
0.000 |
| z |
0.000 |
0.000 |
1.590 |
|
| Polar |
| 3z2-r2 | 3.180 |
| x2-y2 | -1.884 |
| 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 |
2.327 |
0.000 |
0.000 |
| y |
0.000 |
2.536 |
0.000 |
| z |
0.000 |
0.000 |
3.911 |
<r2> (average value of r
2) Å
2
| <r2> |
17.408 |
| (<r2>)1/2 |
4.172 |