Jump to
S2C1
Energy calculated at B1B95/cc-pVDZ
| | hartrees |
| Energy at 0K | -77.224701 |
| Energy at 298.15K | -77.224197 |
| Nuclear repulsion energy | 23.756925 |
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 B1B95/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 |
3143 |
3021 |
50.00 |
|
|
|
| 2 |
A1 |
1730 |
1663 |
88.08 |
|
|
|
| 3 |
A1 |
1166 |
1121 |
28.75 |
|
|
|
| 4 |
B1 |
716 |
689 |
79.20 |
|
|
|
| 5 |
B2 |
3238 |
3113 |
28.36 |
|
|
|
| 6 |
B2 |
204 |
196 |
3.25 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5098.5 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 4900.7 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 B1B95/cc-pVDZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-0.479 |
| C2 |
0.000 |
0.000 |
0.823 |
| H3 |
0.000 |
0.947 |
-1.031 |
| H4 |
0.000 |
-0.947 |
-1.031 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3021 | 1.0956 | 1.0956 |
C2 | 1.3021 | | 2.0815 | 2.0815 | H3 | 1.0956 | 2.0815 | | 1.8931 | H4 | 1.0956 | 2.0815 | 1.8931 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C2 |
C1 |
H3 |
120.235 |
|
C2 |
C1 |
H4 |
120.235 |
| H3 |
C1 |
H4 |
119.529 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.107 |
|
|
|
| 2 |
C |
-0.091 |
|
|
|
| 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 |
-2.341 |
2.341 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.866 |
0.000 |
0.000 |
| y |
0.000 |
-10.149 |
0.000 |
| z |
0.000 |
0.000 |
-13.956 |
|
| Traceless |
| | x | y | z |
| x |
-1.813 |
0.000 |
0.000 |
| y |
0.000 |
3.761 |
0.000 |
| z |
0.000 |
0.000 |
-1.949 |
|
| Polar |
| 3z2-r2 | -3.897 |
| x2-y2 | -3.716 |
| 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 |
1.660 |
0.000 |
0.000 |
| y |
0.000 |
2.605 |
0.000 |
| z |
0.000 |
0.000 |
3.991 |
<r2> (average value of r
2) Å
2
| <r2> |
17.263 |
| (<r2>)1/2 |
4.155 |
Jump to
S1C1
Energy calculated at B1B95/cc-pVDZ
| | hartrees |
| Energy at 0K | -77.151973 |
| Energy at 298.15K | -77.152021 |
| HF Energy | -77.151973 |
| Nuclear repulsion energy | 23.531798 |
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 B1B95/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 |
3063 |
2944 |
2.12 |
|
|
|
| 2 |
A1 |
1613 |
1550 |
5.47 |
|
|
|
| 3 |
A1 |
1363 |
1310 |
2.07 |
|
|
|
| 4 |
B1 |
745 |
716 |
6.09 |
|
|
|
| 5 |
B2 |
3153 |
3031 |
2.93 |
|
|
|
| 6 |
B2 |
972 |
934 |
3.27 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5453.7 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 5242.1 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 B1B95/cc-pVDZ
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 |
0.834 |
| H3 |
0.000 |
0.943 |
-1.049 |
| H4 |
0.000 |
-0.943 |
-1.049 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3179 | 1.0987 | 1.0987 |
C2 | 1.3179 | | 2.1052 | 2.1052 | H3 | 1.0987 | 2.1052 | | 1.8850 | H4 | 1.0987 | 2.1052 | 1.8850 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.027 |
|
|
|
| 2 |
C |
-0.110 |
|
|
|
| 3 |
H |
0.069 |
|
|
|
| 4 |
H |
0.069 |
|
|
|
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 |
-0.601 |
0.601 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.613 |
0.000 |
0.000 |
| y |
0.000 |
-11.859 |
0.000 |
| z |
0.000 |
0.000 |
-11.090 |
|
| Traceless |
| | x | y | z |
| x |
-2.138 |
0.000 |
0.000 |
| y |
0.000 |
0.493 |
0.000 |
| z |
0.000 |
0.000 |
1.646 |
|
| Polar |
| 3z2-r2 | 3.292 |
| x2-y2 | -1.754 |
| 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 |
1.895 |
0.000 |
0.000 |
| y |
0.000 |
2.290 |
0.000 |
| z |
0.000 |
0.000 |
4.117 |
<r2> (average value of r
2) Å
2
| <r2> |
17.166 |
| (<r2>)1/2 |
4.143 |