Jump to
S2C1
Energy calculated at PBEPBE/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -77.151640 |
| Energy at 298.15K | -77.151022 |
| Nuclear repulsion energy | 23.658350 |
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/6-31G(2df,p)
| 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 |
3071 |
3040 |
47.13 |
|
|
|
| 2 |
A1 |
1661 |
1643 |
84.41 |
|
|
|
| 3 |
A1 |
1152 |
1140 |
29.22 |
|
|
|
| 4 |
B1 |
695 |
688 |
72.63 |
|
|
|
| 5 |
B2 |
3149 |
3116 |
23.09 |
|
|
|
| 6 |
B2 |
139 |
138 |
2.05 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4933.7 cm
-1
Scaled (by 0.9897) Zero Point Vibrational Energy (zpe) 4882.9 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 PBEPBE/6-31G(2df,p)
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-0.480 |
| C2 |
0.000 |
0.000 |
0.829 |
| H3 |
0.000 |
0.939 |
-1.047 |
| H4 |
0.000 |
-0.939 |
-1.047 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3083 | 1.0971 | 1.0971 |
C2 | 1.3083 | | 2.0978 | 2.0978 | H3 | 1.0971 | 2.0978 | | 1.8775 | H4 | 1.0971 | 2.0978 | 1.8775 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C2 |
C1 |
H3 |
121.168 |
|
C2 |
C1 |
H4 |
121.168 |
| H3 |
C1 |
H4 |
117.664 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.329 |
|
|
|
| 2 |
C |
-0.057 |
|
|
|
| 3 |
H |
0.193 |
|
|
|
| 4 |
H |
0.193 |
|
|
|
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 |
-2.387 |
2.387 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.622 |
0.000 |
0.000 |
| y |
0.000 |
-10.100 |
0.000 |
| z |
0.000 |
0.000 |
-13.653 |
|
| Traceless |
| | x | y | z |
| x |
-1.746 |
0.000 |
0.000 |
| y |
0.000 |
3.538 |
0.000 |
| z |
0.000 |
0.000 |
-1.792 |
|
| Polar |
| 3z2-r2 | -3.584 |
| x2-y2 | -3.522 |
| 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 |
1.809 |
0.000 |
0.000 |
| y |
0.000 |
2.639 |
0.000 |
| z |
0.000 |
0.000 |
3.875 |
<r2> (average value of r
2) Å
2
| <r2> |
17.238 |
| (<r2>)1/2 |
4.152 |
Jump to
S1C1
Energy calculated at PBEPBE/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -77.083743 |
| Energy at 298.15K | -77.083747 |
| HF Energy | -77.083743 |
| Nuclear repulsion energy | 23.459931 |
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/6-31G(2df,p)
| 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 |
2966 |
2935 |
3.18 |
|
|
|
| 2 |
A1 |
1566 |
1550 |
5.53 |
|
|
|
| 3 |
A1 |
1346 |
1332 |
0.88 |
|
|
|
| 4 |
B1 |
663 |
656 |
1.17 |
|
|
|
| 5 |
B2 |
3032 |
3001 |
6.48 |
|
|
|
| 6 |
B2 |
952 |
943 |
3.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5262.3 cm
-1
Scaled (by 0.9897) Zero Point Vibrational Energy (zpe) 5208.1 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/6-31G(2df,p)
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-0.484 |
| C2 |
0.000 |
0.000 |
0.837 |
| H3 |
0.000 |
0.941 |
-1.058 |
| H4 |
0.000 |
-0.941 |
-1.058 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3213 | 1.1024 | 1.1024 |
C2 | 1.3213 | | 2.1161 | 2.1161 | H3 | 1.1024 | 2.1161 | | 1.8826 | H4 | 1.1024 | 2.1161 | 1.8826 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.252 |
|
|
|
| 2 |
C |
-0.050 |
|
|
|
| 3 |
H |
0.151 |
|
|
|
| 4 |
H |
0.151 |
|
|
|
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 |
-0.598 |
0.598 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.333 |
0.000 |
0.000 |
| y |
0.000 |
-11.687 |
0.000 |
| z |
0.000 |
0.000 |
-10.980 |
|
| Traceless |
| | x | y | z |
| x |
-1.999 |
0.000 |
0.000 |
| y |
0.000 |
0.469 |
0.000 |
| z |
0.000 |
0.000 |
1.530 |
|
| Polar |
| 3z2-r2 | 3.060 |
| x2-y2 | -1.645 |
| 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 |
2.113 |
0.000 |
0.000 |
| y |
0.000 |
2.461 |
0.000 |
| z |
0.000 |
0.000 |
4.042 |
<r2> (average value of r
2) Å
2
| <r2> |
17.117 |
| (<r2>)1/2 |
4.137 |