Jump to
S1C2
Energy calculated at HF/daug-cc-pVTZ
| | hartrees |
| Energy at 0K | -79.260531 |
| Energy at 298.15K | -79.266529 |
| HF Energy | -79.260531 |
| Nuclear repulsion energy | 42.455003 |
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/daug-cc-pVTZ
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1g |
3158 |
2857 |
0.00 |
344.33 |
0.01 |
0.01 |
| 2 |
A1g |
1548 |
1400 |
0.00 |
0.36 |
0.23 |
0.38 |
| 3 |
A1g |
1049 |
949 |
0.00 |
15.80 |
0.20 |
0.33 |
| 4 |
A1u |
328 |
296 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
3152 |
2851 |
73.09 |
0.00 |
0.00 |
0.00 |
| 6 |
A2u |
1521 |
1376 |
0.31 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3194 |
2889 |
0.00 |
125.93 |
0.75 |
0.86 |
| 7 |
Eg |
3194 |
2889 |
0.00 |
125.93 |
0.75 |
0.86 |
| 8 |
Eg |
1614 |
1460 |
0.00 |
8.55 |
0.75 |
0.86 |
| 8 |
Eg |
1614 |
1460 |
0.00 |
8.55 |
0.75 |
0.86 |
| 9 |
Eg |
1323 |
1197 |
0.00 |
0.13 |
0.75 |
0.86 |
| 9 |
Eg |
1323 |
1197 |
0.00 |
0.13 |
0.75 |
0.86 |
| 10 |
Eu |
3221 |
2914 |
97.44 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3221 |
2914 |
97.44 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1618 |
1464 |
7.55 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1618 |
1464 |
7.55 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
881 |
797 |
2.24 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
881 |
797 |
2.24 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 17228.4 cm
-1
Scaled (by 0.9046) Zero Point Vibrational Energy (zpe) 15584.8 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/daug-cc-pVTZ
Point Group is D3d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.762 |
| C2 |
0.000 |
0.000 |
-0.762 |
| H3 |
0.000 |
1.011 |
1.154 |
| H4 |
-0.875 |
-0.505 |
1.154 |
| H5 |
0.875 |
-0.505 |
1.154 |
| H6 |
0.000 |
-1.011 |
-1.154 |
| H7 |
-0.875 |
0.505 |
-1.154 |
| H8 |
0.875 |
0.505 |
-1.154 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5243 | 1.0841 | 1.0841 | 1.0841 | 2.1666 | 2.1666 | 2.1666 |
C2 | 1.5243 | | 2.1666 | 2.1666 | 2.1666 | 1.0841 | 1.0841 | 1.0841 | H3 | 1.0841 | 2.1666 | | 1.7505 | 1.7505 | 3.0684 | 2.5201 | 2.5201 | H4 | 1.0841 | 2.1666 | 1.7505 | | 1.7505 | 2.5201 | 2.5201 | 3.0684 | H5 | 1.0841 | 2.1666 | 1.7505 | 1.7505 | | 2.5201 | 3.0684 | 2.5201 | H6 | 2.1666 | 1.0841 | 3.0684 | 2.5201 | 2.5201 | | 1.7505 | 1.7505 | H7 | 2.1666 | 1.0841 | 2.5201 | 2.5201 | 3.0684 | 1.7505 | | 1.7505 | H8 | 2.1666 | 1.0841 | 2.5201 | 3.0684 | 2.5201 | 1.7505 | 1.7505 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.208 |
|
C1 |
C2 |
H7 |
111.208 |
| C1 |
C2 |
H8 |
111.208 |
|
C2 |
C1 |
H3 |
111.208 |
| C2 |
C1 |
H4 |
111.208 |
|
C2 |
C1 |
H5 |
111.208 |
| H3 |
C1 |
H4 |
107.680 |
|
H3 |
C1 |
H5 |
107.680 |
| H4 |
C1 |
H5 |
107.680 |
|
H6 |
C2 |
H7 |
107.680 |
| H6 |
C2 |
H8 |
107.680 |
|
H7 |
C2 |
H8 |
107.680 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/daug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-1.173 |
|
|
|
| 2 |
C |
-1.173 |
|
|
|
| 3 |
H |
0.391 |
|
|
|
| 4 |
H |
0.391 |
|
|
|
| 5 |
H |
0.391 |
|
|
|
| 6 |
H |
0.391 |
|
|
|
| 7 |
H |
0.391 |
|
|
|
| 8 |
H |
0.391 |
|
|
|
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 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.892 |
0.000 |
0.000 |
| y |
0.000 |
-14.892 |
0.000 |
| z |
0.000 |
0.000 |
-15.647 |
|
| Traceless |
| | x | y | z |
| x |
0.378 |
0.000 |
0.000 |
| y |
0.000 |
0.378 |
0.000 |
| z |
0.000 |
0.000 |
-0.756 |
|
| Polar |
| 3z2-r2 | -1.511 |
| x2-y2 | 0.000 |
| 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 |
3.842 |
0.000 |
0.000 |
| y |
0.000 |
3.842 |
0.000 |
| z |
0.000 |
0.000 |
4.344 |
<r2> (average value of r
2) Å
2
| <r2> |
30.551 |
| (<r2>)1/2 |
5.527 |
Jump to
S1C1
Energy calculated at HF/daug-cc-pVTZ
| | hartrees |
| Energy at 0K | -79.255691 |
| Energy at 298.15K | |
| HF Energy | -79.255691 |
| Nuclear repulsion energy | 42.284241 |
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/daug-cc-pVTZ
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A' |
3230 |
2922 |
85.03 |
|
|
|
| 2 |
A' |
3230 |
2922 |
85.03 |
|
|
|
| 3 |
A' |
3173 |
2871 |
0.00 |
|
|
|
| 4 |
A' |
1624 |
1469 |
9.13 |
|
|
|
| 5 |
A' |
1624 |
1469 |
9.13 |
|
|
|
| 6 |
A' |
1561 |
1413 |
0.00 |
|
|
|
| 7 |
A' |
1046 |
947 |
0.00 |
|
|
|
| 8 |
A' |
958 |
866 |
1.77 |
|
|
|
| 9 |
A' |
958 |
866 |
1.77 |
|
|
|
| 10 |
A" |
3203 |
2898 |
0.00 |
|
|
|
| 11 |
A" |
3203 |
2898 |
0.00 |
|
|
|
| 12 |
A" |
3160 |
2858 |
77.25 |
|
|
|
| 13 |
A" |
1613 |
1459 |
0.00 |
|
|
|
| 14 |
A" |
1613 |
1459 |
0.00 |
|
|
|
| 15 |
A" |
1517 |
1373 |
0.06 |
|
|
|
| 16 |
A" |
1277 |
1155 |
0.00 |
|
|
|
| 17 |
A" |
1277 |
1155 |
0.00 |
|
|
|
| 18 |
A" |
320i |
290i |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16973.1 cm
-1
Scaled (by 0.9046) Zero Point Vibrational Energy (zpe) 15353.8 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/daug-cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.770 |
| C2 |
0.000 |
0.000 |
-0.770 |
| H3 |
1.007 |
-0.001 |
1.168 |
| H4 |
-0.503 |
0.872 |
1.168 |
| H5 |
-0.504 |
-0.872 |
1.168 |
| H6 |
1.007 |
-0.001 |
-1.168 |
| H7 |
-0.504 |
-0.872 |
-1.168 |
| H8 |
-0.503 |
0.872 |
-1.168 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5390 | 1.0828 | 1.0828 | 1.0828 | 2.1838 | 2.1838 | 2.1838 |
C2 | 1.5390 | | 2.1838 | 2.1838 | 2.1838 | 1.0828 | 1.0828 | 1.0828 | H3 | 1.0828 | 2.1838 | | 1.7437 | 1.7437 | 2.3367 | 2.9156 | 2.9156 | H4 | 1.0828 | 2.1838 | 1.7437 | | 1.7437 | 2.9156 | 2.9156 | 2.3367 | H5 | 1.0828 | 2.1838 | 1.7437 | 1.7437 | | 2.9156 | 2.3367 | 2.9156 | H6 | 2.1838 | 1.0828 | 2.3367 | 2.9156 | 2.9156 | | 1.7437 | 1.7437 | H7 | 2.1838 | 1.0828 | 2.9156 | 2.9156 | 2.3367 | 1.7437 | | 1.7437 | H8 | 2.1838 | 1.0828 | 2.9156 | 2.3367 | 2.9156 | 1.7437 | 1.7437 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.614 |
|
C1 |
C2 |
H7 |
111.614 |
| C1 |
C2 |
H8 |
111.614 |
|
C2 |
C1 |
H3 |
111.614 |
| C2 |
C1 |
H4 |
111.614 |
|
C2 |
C1 |
H5 |
111.614 |
| H3 |
C1 |
H4 |
107.246 |
|
H3 |
C1 |
H5 |
107.246 |
| H4 |
C1 |
H5 |
107.246 |
|
H6 |
C2 |
H7 |
107.246 |
| H6 |
C2 |
H8 |
107.246 |
|
H7 |
C2 |
H8 |
107.246 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/daug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-1.191 |
|
|
|
| 2 |
C |
-1.191 |
|
|
|
| 3 |
H |
0.397 |
|
|
|
| 4 |
H |
0.397 |
|
|
|
| 5 |
H |
0.397 |
|
|
|
| 6 |
H |
0.397 |
|
|
|
| 7 |
H |
0.397 |
|
|
|
| 8 |
H |
0.397 |
|
|
|
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 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.871 |
0.000 |
0.000 |
| y |
0.000 |
-14.871 |
0.000 |
| z |
0.000 |
0.000 |
-15.646 |
|
| Traceless |
| | x | y | z |
| x |
0.387 |
0.000 |
0.000 |
| y |
0.000 |
0.387 |
0.000 |
| z |
0.000 |
0.000 |
-0.774 |
|
| Polar |
| 3z2-r2 | -1.548 |
| x2-y2 | 0.000 |
| 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 |
3.808 |
0.000 |
0.000 |
| y |
0.000 |
3.808 |
0.000 |
| z |
0.000 |
0.000 |
4.376 |
<r2> (average value of r
2) Å
2
| <r2> |
30.826 |
| (<r2>)1/2 |
5.552 |