Jump to
S2C1
Energy calculated at LSDA/6-31+G**
| | hartrees |
| Energy at 0K | -76.790413 |
| Energy at 298.15K | -76.789770 |
| Nuclear repulsion energy | 23.772774 |
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 LSDA/6-31+G**
| 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 |
3065 |
3019 |
73.05 |
|
|
|
| 2 |
A1 |
1715 |
1689 |
101.60 |
|
|
|
| 3 |
A1 |
1125 |
1108 |
42.97 |
|
|
|
| 4 |
B1 |
683 |
672 |
120.90 |
|
|
|
| 5 |
B2 |
3145 |
3098 |
44.48 |
|
|
|
| 6 |
B2 |
130 |
128 |
1.68 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4931.1 cm
-1
Scaled (by 0.985) Zero Point Vibrational Energy (zpe) 4857.1 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 LSDA/6-31+G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-0.476 |
| C2 |
0.000 |
0.000 |
0.822 |
| H3 |
0.000 |
0.946 |
-1.039 |
| H4 |
0.000 |
-0.946 |
-1.039 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.2975 | 1.1009 | 1.1009 |
C2 | 1.2975 | | 2.0874 | 2.0874 | H3 | 1.1009 | 2.0874 | | 1.8918 | H4 | 1.1009 | 2.0874 | 1.8918 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C2 |
C1 |
H3 |
120.776 |
|
C2 |
C1 |
H4 |
120.776 |
| H3 |
C1 |
H4 |
118.449 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.018 |
|
|
|
| 2 |
C |
-0.494 |
|
|
|
| 3 |
H |
0.238 |
|
|
|
| 4 |
H |
0.238 |
|
|
|
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 |
-2.671 |
2.671 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.719 |
0.000 |
0.000 |
| y |
0.000 |
-10.482 |
0.000 |
| z |
0.000 |
0.000 |
-14.422 |
|
| Traceless |
| | x | y | z |
| x |
-2.267 |
0.000 |
0.000 |
| y |
0.000 |
4.088 |
0.000 |
| z |
0.000 |
0.000 |
-1.821 |
|
| Polar |
| 3z2-r2 | -3.642 |
| x2-y2 | -4.237 |
| 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 |
2.665 |
0.000 |
0.000 |
| y |
0.000 |
2.986 |
0.000 |
| z |
0.000 |
0.000 |
4.711 |
<r2> (average value of r
2) Å
2
| <r2> |
0.000 |
| (<r2>)1/2 |
0.000 |
Jump to
S1C1
Energy calculated at LSDA/6-31+G**
| | hartrees |
| Energy at 0K | -76.714432 |
| Energy at 298.15K | -76.714445 |
| HF Energy | -76.714432 |
| Nuclear repulsion energy | 23.509804 |
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 LSDA/6-31+G**
| 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 |
2964 |
2920 |
1.47 |
|
|
|
| 2 |
A1 |
1600 |
1576 |
4.76 |
|
|
|
| 3 |
A1 |
1322 |
1302 |
1.56 |
|
|
|
| 4 |
B1 |
690 |
680 |
4.11 |
|
|
|
| 5 |
B2 |
3038 |
2992 |
1.08 |
|
|
|
| 6 |
B2 |
939 |
925 |
10.58 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5276.9 cm
-1
Scaled (by 0.985) Zero Point Vibrational Energy (zpe) 5197.7 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 LSDA/6-31+G**
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 |
0.946 |
-1.054 |
| H4 |
0.000 |
-0.946 |
-1.054 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3160 | 1.1051 | 1.1051 |
C2 | 1.3160 | | 2.1113 | 2.1113 | H3 | 1.1051 | 2.1113 | | 1.8916 | H4 | 1.1051 | 2.1113 | 1.8916 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.321 |
|
|
|
| 2 |
C |
-0.063 |
|
|
|
| 3 |
H |
0.192 |
|
|
|
| 4 |
H |
0.192 |
|
|
|
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 |
-0.770 |
0.770 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.273 |
0.000 |
0.000 |
| y |
0.000 |
-12.226 |
0.000 |
| z |
0.000 |
0.000 |
-11.574 |
|
| Traceless |
| | x | y | z |
| x |
-2.373 |
0.000 |
0.000 |
| y |
0.000 |
0.697 |
0.000 |
| z |
0.000 |
0.000 |
1.676 |
|
| Polar |
| 3z2-r2 | 3.351 |
| x2-y2 | -2.047 |
| 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 |
3.029 |
0.000 |
0.000 |
| y |
0.000 |
2.714 |
0.000 |
| z |
0.000 |
0.000 |
4.731 |
<r2> (average value of r
2) Å
2
| <r2> |
17.503 |
| (<r2>)1/2 |
4.184 |