Jump to
S1C2
Energy calculated at B3LYP/LANL2DZ
| | hartrees |
| Energy at 0K | -79.818877 |
| Energy at 298.15K | -79.824771 |
| HF Energy | -79.818877 |
| Nuclear repulsion energy | 41.928900 |
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 B3LYP/LANL2DZ
| 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 |
3040 |
2922 |
0.00 |
257.08 |
0.01 |
0.02 |
| 2 |
A1g |
1440 |
1384 |
0.00 |
2.64 |
0.68 |
0.81 |
| 3 |
A1g |
1015 |
975 |
0.00 |
16.87 |
0.27 |
0.42 |
| 4 |
A1u |
295 |
284 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
3035 |
2917 |
74.42 |
0.00 |
0.00 |
0.00 |
| 6 |
A2u |
1438 |
1382 |
16.40 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3110 |
2989 |
0.00 |
112.58 |
0.75 |
0.86 |
| 7 |
Eg |
3110 |
2989 |
0.00 |
112.58 |
0.75 |
0.86 |
| 8 |
Eg |
1528 |
1469 |
0.00 |
32.04 |
0.75 |
0.86 |
| 8 |
Eg |
1528 |
1469 |
0.00 |
32.04 |
0.75 |
0.86 |
| 9 |
Eg |
1231 |
1183 |
0.00 |
5.38 |
0.75 |
0.86 |
| 9 |
Eg |
1231 |
1183 |
0.00 |
5.38 |
0.75 |
0.86 |
| 10 |
Eu |
3138 |
3016 |
107.23 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3138 |
3016 |
107.23 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1529 |
1470 |
18.96 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1529 |
1470 |
18.97 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
840 |
807 |
12.09 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
840 |
807 |
12.09 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 16505.4 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 15865.0 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 B3LYP/LANL2DZ
Point Group is D3d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.772 |
| C2 |
0.000 |
0.000 |
-0.772 |
| H3 |
0.000 |
1.024 |
1.168 |
| H4 |
-0.887 |
-0.512 |
1.168 |
| H5 |
0.887 |
-0.512 |
1.168 |
| H6 |
0.000 |
-1.024 |
-1.168 |
| H7 |
-0.887 |
0.512 |
-1.168 |
| H8 |
0.887 |
0.512 |
-1.168 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5431 | 1.0980 | 1.0980 | 1.0980 | 2.1930 | 2.1930 | 2.1930 |
C2 | 1.5431 | | 2.1930 | 2.1930 | 2.1930 | 1.0980 | 1.0980 | 1.0980 | H3 | 1.0980 | 2.1930 | | 1.7737 | 1.7737 | 3.1062 | 2.5500 | 2.5500 | H4 | 1.0980 | 2.1930 | 1.7737 | | 1.7737 | 2.5500 | 2.5500 | 3.1062 | H5 | 1.0980 | 2.1930 | 1.7737 | 1.7737 | | 2.5500 | 3.1062 | 2.5500 | H6 | 2.1930 | 1.0980 | 3.1062 | 2.5500 | 2.5500 | | 1.7737 | 1.7737 | H7 | 2.1930 | 1.0980 | 2.5500 | 2.5500 | 3.1062 | 1.7737 | | 1.7737 | H8 | 2.1930 | 1.0980 | 2.5500 | 3.1062 | 2.5500 | 1.7737 | 1.7737 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.148 |
|
C1 |
C2 |
H7 |
111.148 |
| C1 |
C2 |
H8 |
111.148 |
|
C2 |
C1 |
H3 |
111.148 |
| C2 |
C1 |
H4 |
111.148 |
|
C2 |
C1 |
H5 |
111.148 |
| H3 |
C1 |
H4 |
107.744 |
|
H3 |
C1 |
H5 |
107.744 |
| H4 |
C1 |
H5 |
107.744 |
|
H6 |
C2 |
H7 |
107.744 |
| H6 |
C2 |
H8 |
107.744 |
|
H7 |
C2 |
H8 |
107.744 |
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.590 |
|
|
|
| 2 |
C |
-0.590 |
|
|
|
| 3 |
H |
0.197 |
|
|
|
| 4 |
H |
0.197 |
|
|
|
| 5 |
H |
0.197 |
|
|
|
| 6 |
H |
0.197 |
|
|
|
| 7 |
H |
0.197 |
|
|
|
| 8 |
H |
0.197 |
|
|
|
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 |
-14.563 |
0.000 |
0.000 |
| y |
0.000 |
-14.563 |
0.000 |
| z |
0.000 |
0.000 |
-15.054 |
|
| Traceless |
| | x | y | z |
| x |
0.246 |
0.000 |
0.000 |
| y |
0.000 |
0.246 |
0.000 |
| z |
0.000 |
0.000 |
-0.491 |
|
| Polar |
| 3z2-r2 | -0.983 |
| 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 |
3.199 |
0.000 |
0.000 |
| y |
0.000 |
3.199 |
0.000 |
| z |
0.000 |
0.000 |
3.440 |
<r2> (average value of r
2) Å
2
| <r2> |
30.815 |
| (<r2>)1/2 |
5.551 |
Jump to
S1C1
Energy calculated at B3LYP/LANL2DZ
| | hartrees |
| Energy at 0K | -79.814932 |
| Energy at 298.15K | |
| HF Energy | -79.814932 |
| Nuclear repulsion energy | 41.787133 |
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 B3LYP/LANL2DZ
| 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' |
3054 |
2936 |
0.00 |
|
|
|
| 2 |
A1' |
1467 |
1410 |
0.00 |
|
|
|
| 3 |
A1' |
1009 |
970 |
0.00 |
|
|
|
| 4 |
A1" |
283i |
272i |
0.00 |
|
|
|
| 5 |
A2" |
3042 |
2924 |
79.31 |
|
|
|
| 6 |
A2" |
1439 |
1383 |
18.42 |
|
|
|
| 7 |
E' |
3143 |
3022 |
94.15 |
|
|
|
| 7 |
E' |
3143 |
3022 |
94.14 |
|
|
|
| 8 |
E' |
1537 |
1477 |
21.07 |
|
|
|
| 8 |
E' |
1537 |
1477 |
21.07 |
|
|
|
| 9 |
E' |
915 |
880 |
13.39 |
|
|
|
| 9 |
E' |
915 |
880 |
13.39 |
|
|
|
| 10 |
E" |
3118 |
2997 |
0.00 |
|
|
|
| 10 |
E" |
3118 |
2997 |
0.00 |
|
|
|
| 11 |
E" |
1527 |
1467 |
0.00 |
|
|
|
| 11 |
E" |
1527 |
1467 |
0.00 |
|
|
|
| 12 |
E" |
1191 |
1145 |
0.00 |
|
|
|
| 12 |
E" |
1191 |
1145 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16295.0 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 15662.7 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 B3LYP/LANL2DZ
Point Group is D3h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.778 |
| C2 |
0.000 |
0.000 |
-0.778 |
| H3 |
0.000 |
1.020 |
1.182 |
| H4 |
-0.883 |
-0.510 |
1.182 |
| H5 |
0.883 |
-0.510 |
1.182 |
| H6 |
0.000 |
1.020 |
-1.182 |
| H7 |
0.883 |
-0.510 |
-1.182 |
| H8 |
-0.883 |
-0.510 |
-1.182 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5551 | 1.0970 | 1.0970 | 1.0970 | 2.2087 | 2.2087 | 2.2087 |
C2 | 1.5551 | | 2.2087 | 2.2087 | 2.2087 | 1.0970 | 1.0970 | 1.0970 | H3 | 1.0970 | 2.2087 | | 1.7664 | 1.7664 | 2.3633 | 2.9505 | 2.9505 | H4 | 1.0970 | 2.2087 | 1.7664 | | 1.7664 | 2.9505 | 2.9505 | 2.3633 | H5 | 1.0970 | 2.2087 | 1.7664 | 1.7664 | | 2.9505 | 2.3633 | 2.9505 | H6 | 2.2087 | 1.0970 | 2.3633 | 2.9505 | 2.9505 | | 1.7664 | 1.7664 | H7 | 2.2087 | 1.0970 | 2.9505 | 2.9505 | 2.3633 | 1.7664 | | 1.7664 | H8 | 2.2087 | 1.0970 | 2.9505 | 2.3633 | 2.9505 | 1.7664 | 1.7664 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.616 |
|
C1 |
C2 |
H7 |
111.616 |
| C1 |
C2 |
H8 |
111.616 |
|
C2 |
C1 |
H3 |
111.616 |
| C2 |
C1 |
H4 |
111.616 |
|
C2 |
C1 |
H5 |
111.616 |
| H3 |
C1 |
H4 |
107.244 |
|
H3 |
C1 |
H5 |
107.244 |
| H4 |
C1 |
H5 |
107.244 |
|
H6 |
C2 |
H7 |
107.244 |
| H6 |
C2 |
H8 |
107.244 |
|
H7 |
C2 |
H8 |
107.244 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.612 |
|
|
|
| 2 |
C |
-0.612 |
|
|
|
| 3 |
H |
0.204 |
|
|
|
| 4 |
H |
0.204 |
|
|
|
| 5 |
H |
0.204 |
|
|
|
| 6 |
H |
0.204 |
|
|
|
| 7 |
H |
0.204 |
|
|
|
| 8 |
H |
0.204 |
|
|
|
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 |
-14.563 |
0.000 |
0.000 |
| y |
0.000 |
-14.563 |
0.000 |
| z |
0.000 |
0.000 |
-15.028 |
|
| Traceless |
| | x | y | z |
| x |
0.233 |
0.000 |
0.000 |
| y |
0.000 |
0.233 |
0.000 |
| z |
0.000 |
0.000 |
-0.465 |
|
| Polar |
| 3z2-r2 | -0.930 |
| 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 |
3.158 |
0.000 |
0.000 |
| y |
0.000 |
3.158 |
0.000 |
| z |
0.000 |
0.000 |
3.314 |
<r2> (average value of r
2) Å
2
| <r2> |
31.065 |
| (<r2>)1/2 |
5.574 |