Jump to
S2C1
Energy calculated at HF/daug-cc-pVTZ
| | hartrees |
| Energy at 0K | -76.795257 |
| Energy at 298.15K | -76.795175 |
| HF Energy | -76.795257 |
| Nuclear repulsion energy | 24.097545 |
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/daug-cc-pVTZ
| 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 |
2961 |
29.07 |
|
|
|
| 2 |
A1 |
1817 |
1644 |
71.07 |
|
|
|
| 3 |
A1 |
1354 |
1225 |
14.32 |
|
|
|
| 4 |
B1 |
913 |
826 |
80.30 |
|
|
|
| 5 |
B2 |
3361 |
3040 |
7.42 |
|
|
|
| 6 |
B2 |
527 |
477 |
16.70 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5622.6 cm
-1
Scaled (by 0.9046) Zero Point Vibrational Energy (zpe) 5086.2 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/daug-cc-pVTZ
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 |
0.811 |
| H3 |
0.000 |
0.934 |
-1.010 |
| H4 |
0.000 |
-0.934 |
-1.010 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.2862 | 1.0762 | 1.0762 |
C2 | 1.2862 | | 2.0468 | 2.0468 | H3 | 1.0762 | 2.0468 | | 1.8674 | H4 | 1.0762 | 2.0468 | 1.8674 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C2 |
C1 |
H3 |
119.822 |
|
C2 |
C1 |
H4 |
119.822 |
| H3 |
C1 |
H4 |
120.355 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/daug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.734 |
|
|
|
| 2 |
C |
-0.670 |
|
|
|
| 3 |
H |
0.702 |
|
|
|
| 4 |
H |
0.702 |
|
|
|
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 |
-2.379 |
2.379 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.587 |
0.000 |
0.000 |
| y |
0.000 |
-10.534 |
0.000 |
| z |
0.000 |
0.000 |
-14.469 |
|
| Traceless |
| | x | y | z |
| x |
-2.086 |
0.000 |
0.000 |
| y |
0.000 |
3.994 |
0.000 |
| z |
0.000 |
0.000 |
-1.908 |
|
| Polar |
| 3z2-r2 | -3.817 |
| x2-y2 | -4.053 |
| 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 |
2.959 |
0.000 |
0.000 |
| y |
0.000 |
3.157 |
0.000 |
| z |
0.000 |
0.000 |
4.346 |
<r2> (average value of r
2) Å
2
| <r2> |
17.329 |
| (<r2>)1/2 |
4.163 |
Jump to
S1C1
Energy calculated at HF/daug-cc-pVTZ
| | hartrees |
| Energy at 0K | -76.761307 |
| Energy at 298.15K | -76.761415 |
| HF Energy | -76.761307 |
| Nuclear repulsion energy | 23.474472 |
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/daug-cc-pVTZ
| 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 |
3213 |
2906 |
9.69 |
|
|
|
| 2 |
A1 |
1584 |
1433 |
0.05 |
|
|
|
| 3 |
A1 |
1401 |
1267 |
9.42 |
|
|
|
| 4 |
B1 |
878 |
794 |
39.65 |
|
|
|
| 5 |
B2 |
3293 |
2979 |
6.85 |
|
|
|
| 6 |
B2 |
1080 |
977 |
0.26 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5723.9 cm
-1
Scaled (by 0.9046) Zero Point Vibrational Energy (zpe) 5177.8 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/daug-cc-pVTZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-0.492 |
| C2 |
0.000 |
0.000 |
0.842 |
| H3 |
0.000 |
0.921 |
-1.051 |
| H4 |
0.000 |
-0.921 |
-1.051 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3342 | 1.0776 | 1.0776 |
C2 | 1.3342 | | 2.1056 | 2.1056 | H3 | 1.0776 | 2.1056 | | 1.8423 | H4 | 1.0776 | 2.1056 | 1.8423 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/daug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.784 |
|
|
|
| 2 |
C |
-0.315 |
|
|
|
| 3 |
H |
0.550 |
|
|
|
| 4 |
H |
0.550 |
|
|
|
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 |
-0.526 |
0.526 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.980 |
0.000 |
0.000 |
| y |
0.000 |
-12.094 |
0.000 |
| z |
0.000 |
0.000 |
-11.442 |
|
| Traceless |
| | x | y | z |
| x |
-2.212 |
0.000 |
0.000 |
| y |
0.000 |
0.617 |
0.000 |
| z |
0.000 |
0.000 |
1.595 |
|
| Polar |
| 3z2-r2 | 3.190 |
| x2-y2 | -1.885 |
| 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 |
2.873 |
0.000 |
0.000 |
| y |
0.000 |
2.953 |
0.000 |
| z |
0.000 |
0.000 |
4.044 |
<r2> (average value of r
2) Å
2
| <r2> |
17.426 |
| (<r2>)1/2 |
4.174 |