Jump to
S1C2
Energy calculated at HF/6-31G
| | hartrees |
| Energy at 0K | -79.197572 |
| Energy at 298.15K | -79.203584 |
| HF Energy | -79.197572 |
| Nuclear repulsion energy | 42.381887 |
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
| 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 |
3191 |
2881 |
0.00 |
239.14 |
0.02 |
0.04 |
| 2 |
A1g |
1582 |
1428 |
0.00 |
5.00 |
0.75 |
0.86 |
| 3 |
A1g |
1064 |
961 |
0.00 |
16.12 |
0.29 |
0.45 |
| 4 |
A1u |
314 |
283 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
3183 |
2874 |
72.15 |
0.00 |
0.00 |
0.00 |
| 6 |
A2u |
1582 |
1429 |
4.56 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3239 |
2924 |
0.00 |
154.30 |
0.75 |
0.86 |
| 7 |
Eg |
3239 |
2924 |
0.00 |
154.30 |
0.75 |
0.86 |
| 8 |
Eg |
1660 |
1498 |
0.00 |
46.78 |
0.75 |
0.86 |
| 8 |
Eg |
1660 |
1498 |
0.00 |
46.78 |
0.75 |
0.86 |
| 9 |
Eg |
1357 |
1225 |
0.00 |
4.31 |
0.75 |
0.86 |
| 9 |
Eg |
1357 |
1225 |
0.00 |
4.31 |
0.75 |
0.86 |
| 10 |
Eu |
3266 |
2949 |
96.60 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3266 |
2949 |
96.60 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1663 |
1502 |
10.62 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1663 |
1502 |
10.62 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
920 |
831 |
5.13 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
920 |
831 |
5.13 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 17561.7 cm
-1
Scaled (by 0.9029) Zero Point Vibrational Energy (zpe) 15856.5 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
Point Group is D3d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.765 |
| C2 |
0.000 |
0.000 |
-0.765 |
| H3 |
0.000 |
1.011 |
1.157 |
| H4 |
-0.876 |
-0.506 |
1.157 |
| H5 |
0.876 |
-0.506 |
1.157 |
| H6 |
0.000 |
-1.011 |
-1.157 |
| H7 |
-0.876 |
0.506 |
-1.157 |
| H8 |
0.876 |
0.506 |
-1.157 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5295 | 1.0845 | 1.0845 | 1.0845 | 2.1714 | 2.1714 | 2.1714 |
C2 | 1.5295 | | 2.1714 | 2.1714 | 2.1714 | 1.0845 | 1.0845 | 1.0845 | H3 | 1.0845 | 2.1714 | | 1.7513 | 1.7513 | 3.0729 | 2.5251 | 2.5251 | H4 | 1.0845 | 2.1714 | 1.7513 | | 1.7513 | 2.5251 | 2.5251 | 3.0729 | H5 | 1.0845 | 2.1714 | 1.7513 | 1.7513 | | 2.5251 | 3.0729 | 2.5251 | H6 | 2.1714 | 1.0845 | 3.0729 | 2.5251 | 2.5251 | | 1.7513 | 1.7513 | H7 | 2.1714 | 1.0845 | 2.5251 | 2.5251 | 3.0729 | 1.7513 | | 1.7513 | H8 | 2.1714 | 1.0845 | 2.5251 | 3.0729 | 2.5251 | 1.7513 | 1.7513 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.198 |
|
C1 |
C2 |
H7 |
111.198 |
| C1 |
C2 |
H8 |
111.198 |
|
C2 |
C1 |
H3 |
111.198 |
| C2 |
C1 |
H4 |
111.198 |
|
C2 |
C1 |
H5 |
111.198 |
| H3 |
C1 |
H4 |
107.691 |
|
H3 |
C1 |
H5 |
107.691 |
| H4 |
C1 |
H5 |
107.691 |
|
H6 |
C2 |
H7 |
107.691 |
| H6 |
C2 |
H8 |
107.691 |
|
H7 |
C2 |
H8 |
107.691 |
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.453 |
|
|
|
| 2 |
C |
-0.453 |
|
|
|
| 3 |
H |
0.151 |
|
|
|
| 4 |
H |
0.151 |
|
|
|
| 5 |
H |
0.151 |
|
|
|
| 6 |
H |
0.151 |
|
|
|
| 7 |
H |
0.151 |
|
|
|
| 8 |
H |
0.151 |
|
|
|
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 |
0.000 |
0.000 |
0.000 |
0.000 |
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.040 |
0.000 |
0.000 |
| y |
0.000 |
-15.040 |
0.000 |
| z |
0.000 |
0.000 |
-15.528 |
|
| Traceless |
| | x | y | z |
| x |
0.244 |
0.000 |
0.000 |
| y |
0.000 |
0.244 |
0.000 |
| z |
0.000 |
0.000 |
-0.487 |
|
| Polar |
| 3z2-r2 | -0.975 |
| 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 |
3.246 |
0.000 |
0.000 |
| y |
0.000 |
3.246 |
0.000 |
| z |
0.000 |
0.000 |
3.386 |
<r2> (average value of r
2) Å
2
| <r2> |
30.678 |
| (<r2>)1/2 |
5.539 |
Jump to
S1C1
Energy calculated at HF/6-31G
| | hartrees |
| Energy at 0K | -79.193177 |
| Energy at 298.15K | |
| HF Energy | -79.193177 |
| Nuclear repulsion energy | 42.240393 |
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
| 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' |
3204 |
2893 |
0.00 |
|
|
|
| 2 |
A1' |
1606 |
1450 |
0.00 |
|
|
|
| 3 |
A1' |
1057 |
955 |
0.00 |
|
|
|
| 4 |
A1" |
305i |
275i |
0.00 |
|
|
|
| 5 |
A2" |
3189 |
2879 |
76.34 |
|
|
|
| 6 |
A2" |
1581 |
1428 |
4.22 |
|
|
|
| 7 |
E' |
3272 |
2954 |
82.78 |
|
|
|
| 7 |
E' |
3272 |
2954 |
82.78 |
|
|
|
| 8 |
E' |
1671 |
1509 |
12.30 |
|
|
|
| 8 |
E' |
1671 |
1509 |
12.30 |
|
|
|
| 9 |
E' |
997 |
900 |
5.18 |
|
|
|
| 9 |
E' |
997 |
900 |
5.18 |
|
|
|
| 10 |
E" |
3247 |
2932 |
0.00 |
|
|
|
| 10 |
E" |
3247 |
2932 |
0.00 |
|
|
|
| 11 |
E" |
1658 |
1497 |
0.00 |
|
|
|
| 11 |
E" |
1658 |
1497 |
0.00 |
|
|
|
| 12 |
E" |
1319 |
1191 |
0.00 |
|
|
|
| 12 |
E" |
1319 |
1191 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17329.4 cm
-1
Scaled (by 0.9029) Zero Point Vibrational Energy (zpe) 15646.7 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 HF/6-31G
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 |
1.007 |
1.170 |
| H4 |
-0.872 |
-0.504 |
1.170 |
| H5 |
0.872 |
-0.504 |
1.170 |
| H6 |
0.000 |
1.007 |
-1.170 |
| H7 |
0.872 |
-0.504 |
-1.170 |
| H8 |
-0.872 |
-0.504 |
-1.170 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5412 | 1.0836 | 1.0836 | 1.0836 | 2.1865 | 2.1865 | 2.1865 |
C2 | 1.5412 | | 2.1865 | 2.1865 | 2.1865 | 1.0836 | 1.0836 | 1.0836 | H3 | 1.0836 | 2.1865 | | 1.7447 | 1.7447 | 2.3400 | 2.9188 | 2.9188 | H4 | 1.0836 | 2.1865 | 1.7447 | | 1.7447 | 2.9188 | 2.9188 | 2.3400 | H5 | 1.0836 | 2.1865 | 1.7447 | 1.7447 | | 2.9188 | 2.3400 | 2.9188 | H6 | 2.1865 | 1.0836 | 2.3400 | 2.9188 | 2.9188 | | 1.7447 | 1.7447 | H7 | 2.1865 | 1.0836 | 2.9188 | 2.9188 | 2.3400 | 1.7447 | | 1.7447 | H8 | 2.1865 | 1.0836 | 2.9188 | 2.3400 | 2.9188 | 1.7447 | 1.7447 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.629 |
|
C1 |
C2 |
H7 |
111.629 |
| C1 |
C2 |
H8 |
111.629 |
|
C2 |
C1 |
H3 |
111.629 |
| C2 |
C1 |
H4 |
111.629 |
|
C2 |
C1 |
H5 |
111.629 |
| H3 |
C1 |
H4 |
107.230 |
|
H3 |
C1 |
H5 |
107.230 |
| H4 |
C1 |
H5 |
107.230 |
|
H6 |
C2 |
H7 |
107.230 |
| H6 |
C2 |
H8 |
107.230 |
|
H7 |
C2 |
H8 |
107.230 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.466 |
|
|
|
| 2 |
C |
-0.466 |
|
|
|
| 3 |
H |
0.155 |
|
|
|
| 4 |
H |
0.155 |
|
|
|
| 5 |
H |
0.155 |
|
|
|
| 6 |
H |
0.155 |
|
|
|
| 7 |
H |
0.155 |
|
|
|
| 8 |
H |
0.155 |
|
|
|
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 |
-15.012 |
0.000 |
0.000 |
| y |
0.000 |
-15.012 |
0.000 |
| z |
0.000 |
0.000 |
-15.436 |
|
| Traceless |
| | x | y | z |
| x |
0.212 |
0.000 |
0.000 |
| y |
0.000 |
0.212 |
0.000 |
| z |
0.000 |
0.000 |
-0.423 |
|
| Polar |
| 3z2-r2 | -0.847 |
| 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 |
3.175 |
0.000 |
0.000 |
| y |
0.000 |
3.175 |
0.000 |
| z |
0.000 |
0.000 |
3.326 |
<r2> (average value of r
2) Å
2
| <r2> |
30.892 |
| (<r2>)1/2 |
5.558 |