Jump to
S2C1
Energy calculated at PBEPBE/cc-pVDZ
| | hartrees |
| Energy at 0K | -77.153482 |
| Energy at 298.15K | -77.152841 |
| Nuclear repulsion energy | 23.547965 |
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 PBEPBE/cc-pVDZ
| 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 |
3056 |
3039 |
49.35 |
|
|
|
| 2 |
A1 |
1669 |
1659 |
89.64 |
|
|
|
| 3 |
A1 |
1119 |
1112 |
31.73 |
|
|
|
| 4 |
B1 |
670 |
666 |
77.49 |
|
|
|
| 5 |
B2 |
3144 |
3126 |
30.51 |
|
|
|
| 6 |
B2 |
134 |
133 |
2.08 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4895.8 cm
-1
Scaled (by 0.9942) Zero Point Vibrational Energy (zpe) 4867.4 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 PBEPBE/cc-pVDZ
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 |
0.831 |
| H3 |
0.000 |
0.951 |
-1.046 |
| H4 |
0.000 |
-0.951 |
-1.046 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3131 | 1.1056 | 1.1056 |
C2 | 1.3131 | | 2.1040 | 2.1040 | H3 | 1.1056 | 2.1040 | | 1.9023 | H4 | 1.1056 | 2.1040 | 1.9023 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C2 |
C1 |
H3 |
120.651 |
|
C2 |
C1 |
H4 |
120.651 |
| H3 |
C1 |
H4 |
118.699 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.091 |
|
|
|
| 2 |
C |
-0.106 |
|
|
|
| 3 |
H |
0.099 |
|
|
|
| 4 |
H |
0.099 |
|
|
|
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 |
-2.403 |
2.403 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.900 |
0.000 |
0.000 |
| y |
0.000 |
-10.224 |
0.000 |
| z |
0.000 |
0.000 |
-13.979 |
|
| Traceless |
| | x | y | z |
| x |
-1.798 |
0.000 |
0.000 |
| y |
0.000 |
3.716 |
0.000 |
| z |
0.000 |
0.000 |
-1.917 |
|
| Polar |
| 3z2-r2 | -3.835 |
| x2-y2 | -3.676 |
| 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 |
1.688 |
0.000 |
0.000 |
| y |
0.000 |
2.670 |
0.000 |
| z |
0.000 |
0.000 |
4.102 |
<r2> (average value of r
2) Å
2
| <r2> |
17.467 |
| (<r2>)1/2 |
4.179 |
Jump to
S1C1
Energy calculated at PBEPBE/cc-pVDZ
| | hartrees |
| Energy at 0K | -77.085851 |
| Energy at 298.15K | -77.085845 |
| HF Energy | -77.085851 |
| Nuclear repulsion energy | 23.338584 |
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 PBEPBE/cc-pVDZ
| 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 |
2952 |
2935 |
2.99 |
|
|
|
| 2 |
A1 |
1569 |
1559 |
6.65 |
|
|
|
| 3 |
A1 |
1313 |
1306 |
1.37 |
|
|
|
| 4 |
B1 |
650 |
646 |
0.78 |
|
|
|
| 5 |
B2 |
3030 |
3013 |
4.95 |
|
|
|
| 6 |
B2 |
939 |
933 |
3.95 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5226.0 cm
-1
Scaled (by 0.9942) Zero Point Vibrational Energy (zpe) 5195.7 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 PBEPBE/cc-pVDZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-0.487 |
| C2 |
0.000 |
0.000 |
0.840 |
| H3 |
0.000 |
0.952 |
-1.060 |
| H4 |
0.000 |
-0.952 |
-1.060 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3271 | 1.1107 | 1.1107 |
C2 | 1.3271 | | 2.1248 | 2.1248 | H3 | 1.1107 | 2.1248 | | 1.9033 | H4 | 1.1107 | 2.1248 | 1.9033 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.034 |
|
|
|
| 2 |
C |
-0.103 |
|
|
|
| 3 |
H |
0.068 |
|
|
|
| 4 |
H |
0.068 |
|
|
|
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 |
-0.629 |
0.629 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.634 |
0.000 |
0.000 |
| y |
0.000 |
-11.932 |
0.000 |
| z |
0.000 |
0.000 |
-11.193 |
|
| Traceless |
| | x | y | z |
| x |
-2.072 |
0.000 |
0.000 |
| y |
0.000 |
0.482 |
0.000 |
| z |
0.000 |
0.000 |
1.590 |
|
| Polar |
| 3z2-r2 | 3.181 |
| x2-y2 | -1.702 |
| 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 |
2.047 |
0.000 |
0.000 |
| y |
0.000 |
2.396 |
0.000 |
| z |
0.000 |
0.000 |
4.238 |
<r2> (average value of r
2) Å
2
| <r2> |
17.368 |
| (<r2>)1/2 |
4.167 |