Jump to
S2C1
Energy calculated at BLYP/3-21G*
| | hartrees |
| Energy at 0K | -76.799351 |
| Energy at 298.15K | -76.799162 |
| Nuclear repulsion energy | 23.550101 |
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 BLYP/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 |
3055 |
3035 |
40.77 |
|
|
|
| 2 |
A1 |
1626 |
1615 |
81.68 |
|
|
|
| 3 |
A1 |
1253 |
1245 |
27.57 |
|
|
|
| 4 |
B1 |
765 |
760 |
125.03 |
|
|
|
| 5 |
B2 |
3115 |
3095 |
16.85 |
|
|
|
| 6 |
B2 |
462 |
459 |
0.37 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5137.7 cm
-1
Scaled (by 0.9935) Zero Point Vibrational Energy (zpe) 5104.3 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 BLYP/3-21G*
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 |
0.834 |
| H3 |
0.000 |
0.935 |
-1.056 |
| H4 |
0.000 |
-0.935 |
-1.056 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3167 | 1.0972 | 1.0972 |
C2 | 1.3167 | | 2.1090 | 2.1090 | H3 | 1.0972 | 2.1090 | | 1.8706 | H4 | 1.0972 | 2.1090 | 1.8706 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C2 |
C1 |
H3 |
121.519 |
|
C2 |
C1 |
H4 |
121.519 |
| H3 |
C1 |
H4 |
116.961 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.527 |
|
|
|
| 2 |
C |
0.027 |
|
|
|
| 3 |
H |
0.250 |
|
|
|
| 4 |
H |
0.250 |
|
|
|
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 |
-2.302 |
2.302 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.878 |
0.000 |
0.000 |
| y |
0.000 |
-10.103 |
0.000 |
| z |
0.000 |
0.000 |
-13.825 |
|
| Traceless |
| | x | y | z |
| x |
-1.914 |
0.000 |
0.000 |
| y |
0.000 |
3.748 |
0.000 |
| z |
0.000 |
0.000 |
-1.834 |
|
| Polar |
| 3z2-r2 | -3.669 |
| x2-y2 | -3.775 |
| 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 |
1.187 |
0.000 |
0.000 |
| y |
0.000 |
2.349 |
0.000 |
| z |
0.000 |
0.000 |
3.628 |
<r2> (average value of r
2) Å
2
| <r2> |
0.000 |
| (<r2>)1/2 |
0.000 |
Jump to
S1C1
Energy calculated at BLYP/3-21G*
| | hartrees |
| Energy at 0K | -76.728060 |
| Energy at 298.15K | -76.728086 |
| HF Energy | -76.728060 |
| Nuclear repulsion energy | 23.395578 |
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 BLYP/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 |
2937 |
2918 |
2.32 |
|
|
|
| 2 |
A1 |
1531 |
1521 |
6.28 |
|
|
|
| 3 |
A1 |
1425 |
1416 |
1.45 |
|
|
|
| 4 |
B1 |
683 |
678 |
0.83 |
|
|
|
| 5 |
B2 |
2988 |
2969 |
11.58 |
|
|
|
| 6 |
B2 |
1016 |
1009 |
7.32 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5290.1 cm
-1
Scaled (by 0.9935) Zero Point Vibrational Energy (zpe) 5255.7 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 BLYP/3-21G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-0.486 |
| C2 |
0.000 |
0.000 |
0.841 |
| H3 |
0.000 |
0.938 |
-1.065 |
| H4 |
0.000 |
-0.938 |
-1.065 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3261 | 1.1028 | 1.1028 |
C2 | 1.3261 | | 2.1241 | 2.1241 | H3 | 1.1028 | 2.1241 | | 1.8764 | H4 | 1.1028 | 2.1241 | 1.8764 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.410 |
|
|
|
| 2 |
C |
0.006 |
|
|
|
| 3 |
H |
0.202 |
|
|
|
| 4 |
H |
0.202 |
|
|
|
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 |
-0.611 |
0.611 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.615 |
0.000 |
0.000 |
| y |
0.000 |
-11.868 |
0.000 |
| z |
0.000 |
0.000 |
-11.056 |
|
| Traceless |
| | x | y | z |
| x |
-2.153 |
0.000 |
0.000 |
| y |
0.000 |
0.467 |
0.000 |
| z |
0.000 |
0.000 |
1.686 |
|
| Polar |
| 3z2-r2 | 3.371 |
| x2-y2 | -1.747 |
| 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 |
1.647 |
0.000 |
0.000 |
| y |
0.000 |
1.998 |
0.000 |
| z |
0.000 |
0.000 |
3.788 |
<r2> (average value of r
2) Å
2
| <r2> |
17.290 |
| (<r2>)1/2 |
4.158 |