Jump to
S2C1
Energy calculated at M06-2X/3-21G*
| | hartrees |
| Energy at 0K | -76.788979 |
| Energy at 298.15K | -76.788877 |
| HF Energy | -76.788979 |
| Nuclear repulsion energy | 23.754896 |
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 M06-2X/3-21G*
| 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 |
3167 |
2999 |
51.05 |
|
|
|
| 2 |
A1 |
1705 |
1615 |
83.40 |
|
|
|
| 3 |
A1 |
1297 |
1228 |
27.62 |
|
|
|
| 4 |
B1 |
874 |
827 |
145.17 |
|
|
|
| 5 |
B2 |
3240 |
3069 |
26.94 |
|
|
|
| 6 |
B2 |
522 |
495 |
0.24 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5401.7 cm
-1
Scaled (by 0.9472) Zero Point Vibrational Energy (zpe) 5116.5 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 M06-2X/3-21G*
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 |
0.826 |
| H3 |
0.000 |
0.932 |
-1.041 |
| H4 |
0.000 |
-0.932 |
-1.041 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3053 | 1.0884 | 1.0884 |
C2 | 1.3053 | | 2.0870 | 2.0870 | H3 | 1.0884 | 2.0870 | | 1.8643 | H4 | 1.0884 | 2.0870 | 1.8643 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C2 |
C1 |
H3 |
121.083 |
|
C2 |
C1 |
H4 |
121.083 |
| H3 |
C1 |
H4 |
117.834 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.625 |
|
|
|
| 2 |
C |
0.067 |
|
|
|
| 3 |
H |
0.279 |
|
|
|
| 4 |
H |
0.279 |
|
|
|
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 |
-2.219 |
2.219 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.062 |
0.000 |
0.000 |
| y |
0.000 |
-10.087 |
0.000 |
| z |
0.000 |
0.000 |
-13.942 |
|
| Traceless |
| | x | y | z |
| x |
-2.048 |
0.000 |
0.000 |
| y |
0.000 |
3.915 |
0.000 |
| z |
0.000 |
0.000 |
-1.867 |
|
| Polar |
| 3z2-r2 | -3.734 |
| x2-y2 | -3.975 |
| 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 |
1.161 |
0.000 |
0.000 |
| y |
0.000 |
2.312 |
0.000 |
| z |
0.000 |
0.000 |
3.651 |
<r2> (average value of r
2) Å
2
| <r2> |
17.309 |
| (<r2>)1/2 |
4.160 |
Jump to
S1C1
Energy calculated at M06-2X/3-21G*
| | hartrees |
| Energy at 0K | -76.724080 |
| Energy at 298.15K | -76.724081 |
| HF Energy | -76.724080 |
| Nuclear repulsion energy | 23.585068 |
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 M06-2X/3-21G*
| 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 |
3076 |
2914 |
0.29 |
|
|
|
| 2 |
A1 |
1623 |
1537 |
0.81 |
|
|
|
| 3 |
A1 |
1469 |
1391 |
4.78 |
|
|
|
| 4 |
B1 |
612 |
580 |
45.81 |
|
|
|
| 5 |
B2 |
3148 |
2982 |
3.08 |
|
|
|
| 6 |
B2 |
1058 |
1002 |
5.87 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5492.9 cm
-1
Scaled (by 0.9472) Zero Point Vibrational Energy (zpe) 5202.9 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 M06-2X/3-21G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-0.483 |
| C2 |
0.000 |
0.000 |
0.834 |
| H3 |
0.000 |
0.931 |
-1.053 |
| H4 |
0.000 |
-0.931 |
-1.053 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3173 | 1.0910 | 1.0910 |
C2 | 1.3173 | | 2.1038 | 2.1038 | H3 | 1.0910 | 2.1038 | | 1.8610 | H4 | 1.0910 | 2.1038 | 1.8610 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.488 |
|
|
|
| 2 |
C |
0.033 |
|
|
|
| 3 |
H |
0.228 |
|
|
|
| 4 |
H |
0.228 |
|
|
|
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 |
-0.597 |
0.597 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.787 |
0.000 |
0.000 |
| y |
0.000 |
-11.897 |
0.000 |
| z |
0.000 |
0.000 |
-11.135 |
|
| Traceless |
| | x | y | z |
| x |
-2.271 |
0.000 |
0.000 |
| y |
0.000 |
0.564 |
0.000 |
| z |
0.000 |
0.000 |
1.707 |
|
| Polar |
| 3z2-r2 | 3.413 |
| x2-y2 | -1.890 |
| 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 |
2.706 |
0.000 |
0.000 |
| y |
0.000 |
1.858 |
0.000 |
| z |
0.000 |
0.000 |
3.627 |
<r2> (average value of r
2) Å
2
| <r2> |
17.189 |
| (<r2>)1/2 |
4.146 |