Jump to
S1C2
Energy calculated at HF/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -79.241729 |
| Energy at 298.15K | -79.247731 |
| HF Energy | -79.241729 |
| Nuclear repulsion energy | 42.381552 |
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/6-31G(2df,p)
| 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 |
3169 |
2870 |
0.00 |
216.66 |
0.02 |
0.03 |
| 2 |
A1g |
1551 |
1404 |
0.00 |
2.38 |
0.69 |
0.82 |
| 3 |
A1g |
1051 |
952 |
0.00 |
13.67 |
0.27 |
0.42 |
| 4 |
A1u |
330 |
299 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
3163 |
2864 |
68.29 |
0.00 |
0.00 |
0.00 |
| 6 |
A2u |
1521 |
1377 |
0.04 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3215 |
2912 |
0.00 |
137.24 |
0.75 |
0.86 |
| 7 |
Eg |
3215 |
2912 |
0.00 |
137.24 |
0.75 |
0.86 |
| 8 |
Eg |
1616 |
1464 |
0.00 |
28.76 |
0.75 |
0.86 |
| 8 |
Eg |
1616 |
1464 |
0.00 |
28.76 |
0.75 |
0.86 |
| 9 |
Eg |
1324 |
1199 |
0.00 |
1.99 |
0.75 |
0.86 |
| 9 |
Eg |
1324 |
1199 |
0.00 |
1.99 |
0.75 |
0.86 |
| 10 |
Eu |
3242 |
2936 |
91.06 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3242 |
2936 |
91.06 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1622 |
1469 |
5.24 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1622 |
1469 |
5.24 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
878 |
795 |
2.58 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
878 |
795 |
2.58 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 17290.8 cm
-1
Scaled (by 0.9055) Zero Point Vibrational Energy (zpe) 15656.8 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/6-31G(2df,p)
Point Group is D3d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.763 |
| C2 |
0.000 |
0.000 |
-0.763 |
| H3 |
0.000 |
1.013 |
1.156 |
| H4 |
-0.877 |
-0.506 |
1.156 |
| H5 |
0.877 |
-0.506 |
1.156 |
| H6 |
0.000 |
-1.013 |
-1.156 |
| H7 |
-0.877 |
0.506 |
-1.156 |
| H8 |
0.877 |
0.506 |
-1.156 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5268 | 1.0861 | 1.0861 | 1.0861 | 2.1700 | 2.1700 | 2.1700 |
C2 | 1.5268 | | 2.1700 | 2.1700 | 2.1700 | 1.0861 | 1.0861 | 1.0861 | H3 | 1.0861 | 2.1700 | | 1.7540 | 1.7540 | 3.0735 | 2.5238 | 2.5238 | H4 | 1.0861 | 2.1700 | 1.7540 | | 1.7540 | 2.5238 | 2.5238 | 3.0735 | H5 | 1.0861 | 2.1700 | 1.7540 | 1.7540 | | 2.5238 | 3.0735 | 2.5238 | H6 | 2.1700 | 1.0861 | 3.0735 | 2.5238 | 2.5238 | | 1.7540 | 1.7540 | H7 | 2.1700 | 1.0861 | 2.5238 | 2.5238 | 3.0735 | 1.7540 | | 1.7540 | H8 | 2.1700 | 1.0861 | 2.5238 | 3.0735 | 2.5238 | 1.7540 | 1.7540 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.185 |
|
C1 |
C2 |
H7 |
111.185 |
| C1 |
C2 |
H8 |
111.185 |
|
C2 |
C1 |
H3 |
111.185 |
| C2 |
C1 |
H4 |
111.185 |
|
C2 |
C1 |
H5 |
111.185 |
| H3 |
C1 |
H4 |
107.705 |
|
H3 |
C1 |
H5 |
107.705 |
| H4 |
C1 |
H5 |
107.705 |
|
H6 |
C2 |
H7 |
107.705 |
| H6 |
C2 |
H8 |
107.705 |
|
H7 |
C2 |
H8 |
107.705 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.393 |
|
|
|
| 2 |
C |
-0.393 |
|
|
|
| 3 |
H |
0.131 |
|
|
|
| 4 |
H |
0.131 |
|
|
|
| 5 |
H |
0.131 |
|
|
|
| 6 |
H |
0.131 |
|
|
|
| 7 |
H |
0.131 |
|
|
|
| 8 |
H |
0.131 |
|
|
|
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 |
-14.770 |
0.000 |
0.000 |
| y |
0.000 |
-14.770 |
0.000 |
| z |
0.000 |
0.000 |
-15.428 |
|
| Traceless |
| | x | y | z |
| x |
0.329 |
0.000 |
0.000 |
| y |
0.000 |
0.329 |
0.000 |
| z |
0.000 |
0.000 |
-0.657 |
|
| Polar |
| 3z2-r2 | -1.315 |
| 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 |
3.360 |
0.000 |
0.000 |
| y |
0.000 |
3.360 |
0.000 |
| z |
0.000 |
0.000 |
3.621 |
<r2> (average value of r
2) Å
2
| <r2> |
30.525 |
| (<r2>)1/2 |
5.525 |
Jump to
S1C1
Energy calculated at HF/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -79.236822 |
| Energy at 298.15K | |
| HF Energy | -79.236822 |
| Nuclear repulsion energy | 42.211974 |
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/6-31G(2df,p)
| 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' |
3184 |
2883 |
0.00 |
|
|
|
| 2 |
A1' |
1567 |
1419 |
0.00 |
|
|
|
| 3 |
A1' |
1050 |
951 |
0.00 |
|
|
|
| 4 |
A1" |
320i |
290i |
0.00 |
|
|
|
| 5 |
A2" |
3170 |
2871 |
71.43 |
|
|
|
| 6 |
A2" |
1519 |
1375 |
0.02 |
|
|
|
| 7 |
E' |
3249 |
2942 |
79.18 |
|
|
|
| 7 |
E' |
3249 |
2942 |
79.18 |
|
|
|
| 8 |
E' |
1627 |
1474 |
6.48 |
|
|
|
| 8 |
E' |
1627 |
1474 |
6.48 |
|
|
|
| 9 |
E' |
958 |
868 |
2.11 |
|
|
|
| 9 |
E' |
958 |
868 |
2.11 |
|
|
|
| 10 |
E" |
3224 |
2919 |
0.00 |
|
|
|
| 10 |
E" |
3224 |
2919 |
0.00 |
|
|
|
| 11 |
E" |
1616 |
1463 |
0.00 |
|
|
|
| 11 |
E" |
1616 |
1463 |
0.00 |
|
|
|
| 12 |
E" |
1278 |
1157 |
0.00 |
|
|
|
| 12 |
E" |
1278 |
1157 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17037.1 cm
-1
Scaled (by 0.9055) Zero Point Vibrational Energy (zpe) 15427.1 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 HF/6-31G(2df,p)
Point Group is D3h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.771 |
| C2 |
0.000 |
0.000 |
-0.771 |
| H3 |
0.000 |
1.009 |
1.170 |
| H4 |
-0.874 |
-0.504 |
1.170 |
| H5 |
0.874 |
-0.504 |
1.170 |
| H6 |
0.000 |
1.009 |
-1.170 |
| H7 |
0.874 |
-0.504 |
-1.170 |
| H8 |
-0.874 |
-0.504 |
-1.170 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5411 | 1.0850 | 1.0850 | 1.0850 | 2.1873 | 2.1873 | 2.1873 |
C2 | 1.5411 | | 2.1873 | 2.1873 | 2.1873 | 1.0850 | 1.0850 | 1.0850 | H3 | 1.0850 | 2.1873 | | 1.7471 | 1.7471 | 2.3405 | 2.9206 | 2.9206 | H4 | 1.0850 | 2.1873 | 1.7471 | | 1.7471 | 2.9206 | 2.9206 | 2.3405 | H5 | 1.0850 | 2.1873 | 1.7471 | 1.7471 | | 2.9206 | 2.3405 | 2.9206 | H6 | 2.1873 | 1.0850 | 2.3405 | 2.9206 | 2.9206 | | 1.7471 | 1.7471 | H7 | 2.1873 | 1.0850 | 2.9206 | 2.9206 | 2.3405 | 1.7471 | | 1.7471 | H8 | 2.1873 | 1.0850 | 2.9206 | 2.3405 | 2.9206 | 1.7471 | 1.7471 | |
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/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.405 |
|
|
|
| 2 |
C |
-0.405 |
|
|
|
| 3 |
H |
0.135 |
|
|
|
| 4 |
H |
0.135 |
|
|
|
| 5 |
H |
0.135 |
|
|
|
| 6 |
H |
0.135 |
|
|
|
| 7 |
H |
0.135 |
|
|
|
| 8 |
H |
0.135 |
|
|
|
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 |
-14.751 |
0.000 |
0.000 |
| y |
0.000 |
-14.751 |
0.000 |
| z |
0.000 |
0.000 |
-15.384 |
|
| Traceless |
| | x | y | z |
| x |
0.317 |
0.000 |
0.000 |
| y |
0.000 |
0.317 |
0.000 |
| z |
0.000 |
0.000 |
-0.634 |
|
| Polar |
| 3z2-r2 | -1.267 |
| 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 |
3.312 |
0.000 |
0.000 |
| y |
0.000 |
3.312 |
0.000 |
| z |
0.000 |
0.000 |
3.610 |
<r2> (average value of r
2) Å
2
| <r2> |
30.791 |
| (<r2>)1/2 |
5.549 |