Jump to
S2C1
Energy calculated at HF/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -76.777531 |
| Energy at 298.15K | -76.777458 |
| Nuclear repulsion energy | 23.898011 |
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 HF/aug-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 |
3285 |
2992 |
27.96 |
|
|
|
| 2 |
A1 |
1819 |
1657 |
69.21 |
|
|
|
| 3 |
A1 |
1343 |
1223 |
15.48 |
|
|
|
| 4 |
B1 |
908 |
827 |
82.06 |
|
|
|
| 5 |
B2 |
3384 |
3081 |
6.77 |
|
|
|
| 6 |
B2 |
537 |
489 |
17.40 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5638.5 cm
-1
Scaled (by 0.9106) Zero Point Vibrational Energy (zpe) 5134.4 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 HF/aug-cc-pVDZ
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 |
0.818 |
| H3 |
0.000 |
0.941 |
-1.016 |
| H4 |
0.000 |
-0.941 |
-1.016 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.2979 | 1.0837 | 1.0837 |
C2 | 1.2979 | | 2.0621 | 2.0621 | H3 | 1.0837 | 2.0621 | | 1.8828 | H4 | 1.0837 | 2.0621 | 1.8828 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C2 |
C1 |
H3 |
119.689 |
|
C2 |
C1 |
H4 |
119.689 |
| H3 |
C1 |
H4 |
120.622 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.545 |
|
|
|
| 2 |
C |
-0.307 |
|
|
|
| 3 |
H |
-0.119 |
|
|
|
| 4 |
H |
-0.119 |
|
|
|
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 |
-2.374 |
2.374 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.762 |
0.000 |
0.000 |
| y |
0.000 |
-10.528 |
0.000 |
| z |
0.000 |
0.000 |
-14.539 |
|
| Traceless |
| | x | y | z |
| x |
-2.228 |
0.000 |
0.000 |
| y |
0.000 |
4.123 |
0.000 |
| z |
0.000 |
0.000 |
-1.894 |
|
| Polar |
| 3z2-r2 | -3.789 |
| x2-y2 | -4.234 |
| 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 |
2.948 |
0.000 |
0.000 |
| y |
0.000 |
3.116 |
0.000 |
| z |
0.000 |
0.000 |
4.415 |
<r2> (average value of r
2) Å
2
| <r2> |
0.000 |
| (<r2>)1/2 |
0.000 |
Jump to
S1C1
Energy calculated at HF/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -76.744191 |
| Energy at 298.15K | -76.744297 |
| HF Energy | -76.744191 |
| Nuclear repulsion energy | 23.296804 |
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 HF/aug-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 |
3225 |
2937 |
9.61 |
|
|
|
| 2 |
A1 |
1571 |
1431 |
0.00 |
|
|
|
| 3 |
A1 |
1405 |
1279 |
10.11 |
|
|
|
| 4 |
B1 |
863 |
785 |
39.98 |
|
|
|
| 5 |
B2 |
3315 |
3019 |
6.93 |
|
|
|
| 6 |
B2 |
1071 |
976 |
0.25 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5725.3 cm
-1
Scaled (by 0.9106) Zero Point Vibrational Energy (zpe) 5213.4 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 HF/aug-cc-pVDZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-0.496 |
| C2 |
0.000 |
0.000 |
0.849 |
| H3 |
0.000 |
0.929 |
-1.057 |
| H4 |
0.000 |
-0.929 |
-1.057 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3448 | 1.0853 | 1.0853 |
C2 | 1.3448 | | 2.1202 | 2.1202 | H3 | 1.0853 | 2.1202 | | 1.8582 | H4 | 1.0853 | 2.1202 | 1.8582 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.537 |
|
|
|
| 2 |
C |
-0.260 |
|
|
|
| 3 |
H |
-0.138 |
|
|
|
| 4 |
H |
-0.138 |
|
|
|
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 |
-0.533 |
0.533 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.140 |
0.000 |
0.000 |
| y |
0.000 |
-12.137 |
0.000 |
| z |
0.000 |
0.000 |
-11.478 |
|
| Traceless |
| | x | y | z |
| x |
-2.332 |
0.000 |
0.000 |
| y |
0.000 |
0.672 |
0.000 |
| z |
0.000 |
0.000 |
1.661 |
|
| Polar |
| 3z2-r2 | 3.322 |
| x2-y2 | -2.003 |
| 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 |
2.846 |
0.000 |
0.000 |
| y |
0.000 |
2.915 |
0.000 |
| z |
0.000 |
0.000 |
4.057 |
<r2> (average value of r
2) Å
2
| <r2> |
17.620 |
| (<r2>)1/2 |
4.198 |