Jump to
S2C1
Energy calculated at wB97X-D/TZVP
| | hartrees |
| Energy at 0K | -77.257275 |
| Energy at 298.15K | -77.257018 |
| HF Energy | -77.257275 |
| Nuclear repulsion energy | 23.964080 |
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/TZVP
| 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 |
3148 |
3007 |
49.31 |
|
|
|
| 2 |
A1 |
1738 |
1660 |
91.70 |
|
|
|
| 3 |
A1 |
1230 |
1174 |
27.48 |
|
|
|
| 4 |
B1 |
782 |
746 |
104.64 |
|
|
|
| 5 |
B2 |
3236 |
3090 |
22.60 |
|
|
|
| 6 |
B2 |
376 |
359 |
5.21 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5254.8 cm
-1
Scaled (by 0.955) Zero Point Vibrational Energy (zpe) 5018.3 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 wB97X-D/TZVP
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-0.475 |
| C2 |
0.000 |
0.000 |
0.815 |
| H3 |
0.000 |
0.940 |
-1.022 |
| H4 |
0.000 |
-0.940 |
-1.022 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.2900 | 1.0876 | 1.0876 |
C2 | 1.2900 | | 2.0639 | 2.0639 | H3 | 1.0876 | 2.0639 | | 1.8793 | H4 | 1.0876 | 2.0639 | 1.8793 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C2 |
C1 |
H3 |
120.231 |
|
C2 |
C1 |
H4 |
120.231 |
| H3 |
C1 |
H4 |
119.538 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.350 |
|
|
|
| 2 |
C |
-0.042 |
|
|
|
| 3 |
H |
0.196 |
|
|
|
| 4 |
H |
0.196 |
|
|
|
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 |
-2.497 |
2.497 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.355 |
0.000 |
0.000 |
| y |
0.000 |
-10.278 |
0.000 |
| z |
0.000 |
0.000 |
-14.393 |
|
| Traceless |
| | x | y | z |
| x |
-2.020 |
0.000 |
0.000 |
| y |
0.000 |
4.096 |
0.000 |
| z |
0.000 |
0.000 |
-2.076 |
|
| Polar |
| 3z2-r2 | -4.153 |
| x2-y2 | -4.077 |
| 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 |
2.320 |
0.000 |
0.000 |
| y |
0.000 |
2.807 |
0.000 |
| z |
0.000 |
0.000 |
4.377 |
<r2> (average value of r
2) Å
2
| <r2> |
17.322 |
| (<r2>)1/2 |
4.162 |
Jump to
S1C1
Energy calculated at wB97X-D/TZVP
| | hartrees |
| Energy at 0K | -77.184732 |
| Energy at 298.15K | -77.184814 |
| HF Energy | -77.184732 |
| Nuclear repulsion energy | 23.662423 |
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/TZVP
| 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 |
3067 |
2929 |
3.82 |
|
|
|
| 2 |
A1 |
1599 |
1527 |
2.71 |
|
|
|
| 3 |
A1 |
1409 |
1346 |
3.08 |
|
|
|
| 4 |
B1 |
819 |
783 |
13.61 |
|
|
|
| 5 |
B2 |
3149 |
3008 |
3.20 |
|
|
|
| 6 |
B2 |
1005 |
959 |
4.99 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5524.5 cm
-1
Scaled (by 0.955) Zero Point Vibrational Energy (zpe) 5275.9 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/TZVP
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 |
0.830 |
| H3 |
0.000 |
0.936 |
-1.043 |
| H4 |
0.000 |
-0.936 |
-1.043 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3119 | 1.0910 | 1.0910 |
C2 | 1.3119 | | 2.0934 | 2.0934 | H3 | 1.0910 | 2.0934 | | 1.8721 | H4 | 1.0910 | 2.0934 | 1.8721 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.271 |
|
|
|
| 2 |
C |
-0.018 |
|
|
|
| 3 |
H |
0.145 |
|
|
|
| 4 |
H |
0.145 |
|
|
|
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 |
-0.612 |
0.612 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.977 |
0.000 |
0.000 |
| y |
0.000 |
-11.990 |
0.000 |
| z |
0.000 |
0.000 |
-11.295 |
|
| Traceless |
| | x | y | z |
| x |
-2.335 |
0.000 |
0.000 |
| y |
0.000 |
0.646 |
0.000 |
| z |
0.000 |
0.000 |
1.689 |
|
| Polar |
| 3z2-r2 | 3.377 |
| x2-y2 | -1.987 |
| 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 |
2.550 |
0.000 |
0.000 |
| y |
0.000 |
2.450 |
0.000 |
| z |
0.000 |
0.000 |
4.490 |
<r2> (average value of r
2) Å
2
| <r2> |
17.208 |
| (<r2>)1/2 |
4.148 |