Jump to
S2C1
Energy calculated at wB97X-D/6-311G**
| | hartrees |
| Energy at 0K | -77.249764 |
| Energy at 298.15K | -77.249471 |
| HF Energy | -77.249764 |
| Nuclear repulsion energy | 23.912436 |
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 wB97X-D/6-311G**
| 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 |
3140 |
3004 |
43.51 |
|
|
|
| 2 |
A1 |
1729 |
1654 |
89.28 |
|
|
|
| 3 |
A1 |
1219 |
1166 |
27.80 |
|
|
|
| 4 |
B1 |
767 |
733 |
96.06 |
|
|
|
| 5 |
B2 |
3229 |
3089 |
20.31 |
|
|
|
| 6 |
B2 |
349 |
334 |
4.83 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5216.5 cm
-1
Scaled (by 0.9565) Zero Point Vibrational Energy (zpe) 4989.6 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 wB97X-D/6-311G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-0.476 |
| C2 |
0.000 |
0.000 |
0.817 |
| H3 |
0.000 |
0.941 |
-1.023 |
| H4 |
0.000 |
-0.941 |
-1.023 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.2938 | 1.0882 | 1.0882 |
C2 | 1.2938 | | 2.0673 | 2.0673 | H3 | 1.0882 | 2.0673 | | 1.8812 | H4 | 1.0882 | 2.0673 | 1.8812 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C2 |
C1 |
H3 |
120.185 |
|
C2 |
C1 |
H4 |
120.185 |
| H3 |
C1 |
H4 |
119.629 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.332 |
|
|
|
| 2 |
C |
-0.035 |
|
|
|
| 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 |
-2.404 |
2.404 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.115 |
0.000 |
0.000 |
| y |
0.000 |
-10.177 |
0.000 |
| z |
0.000 |
0.000 |
-14.186 |
|
| Traceless |
| | x | y | z |
| x |
-1.934 |
0.000 |
0.000 |
| y |
0.000 |
3.974 |
0.000 |
| z |
0.000 |
0.000 |
-2.039 |
|
| Polar |
| 3z2-r2 | -4.079 |
| x2-y2 | -3.939 |
| 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 |
1.845 |
0.000 |
0.000 |
| y |
0.000 |
2.663 |
0.000 |
| z |
0.000 |
0.000 |
4.085 |
<r2> (average value of r
2) Å
2
| <r2> |
17.246 |
| (<r2>)1/2 |
4.153 |
Jump to
S1C1
Energy calculated at wB97X-D/6-311G**
| | hartrees |
| Energy at 0K | -77.177518 |
| Energy at 298.15K | -77.177594 |
| HF Energy | -77.177518 |
| Nuclear repulsion energy | 23.618061 |
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 wB97X-D/6-311G**
| 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 |
3058 |
2925 |
4.34 |
|
|
|
| 2 |
A1 |
1592 |
1523 |
3.03 |
|
|
|
| 3 |
A1 |
1402 |
1341 |
3.37 |
|
|
|
| 4 |
B1 |
804 |
769 |
13.94 |
|
|
|
| 5 |
B2 |
3141 |
3004 |
5.23 |
|
|
|
| 6 |
B2 |
998 |
955 |
3.82 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5496.8 cm
-1
Scaled (by 0.9565) Zero Point Vibrational Energy (zpe) 5257.7 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 wB97X-D/6-311G**
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 |
0.831 |
| H3 |
0.000 |
0.937 |
-1.044 |
| H4 |
0.000 |
-0.937 |
-1.044 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3148 | 1.0921 | 1.0921 |
C2 | 1.3148 | | 2.0966 | 2.0966 | H3 | 1.0921 | 2.0966 | | 1.8744 | H4 | 1.0921 | 2.0966 | 1.8744 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.236 |
|
|
|
| 2 |
C |
-0.052 |
|
|
|
| 3 |
H |
0.144 |
|
|
|
| 4 |
H |
0.144 |
|
|
|
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 |
-0.599 |
0.599 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.826 |
0.000 |
0.000 |
| y |
0.000 |
-11.911 |
0.000 |
| z |
0.000 |
0.000 |
-11.144 |
|
| Traceless |
| | x | y | z |
| x |
-2.299 |
0.000 |
0.000 |
| y |
0.000 |
0.574 |
0.000 |
| z |
0.000 |
0.000 |
1.725 |
|
| Polar |
| 3z2-r2 | 3.450 |
| x2-y2 | -1.915 |
| 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 |
2.067 |
0.000 |
0.000 |
| y |
0.000 |
2.289 |
0.000 |
| z |
0.000 |
0.000 |
4.237 |
<r2> (average value of r
2) Å
2
| <r2> |
17.163 |
| (<r2>)1/2 |
4.143 |