Jump to
S1C2
Energy calculated at B3LYP/CEP-121G*
| | hartrees |
| Energy at 0K | -14.922648 |
| Energy at 298.15K | -14.928530 |
| HF Energy | -14.922648 |
| Nuclear repulsion energy | 26.381777 |
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/CEP-121G*
| 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 |
3014 |
2922 |
0.00 |
273.50 |
0.01 |
0.02 |
| 2 |
A1g |
1433 |
1389 |
0.00 |
2.75 |
0.71 |
0.83 |
| 3 |
A1g |
985 |
955 |
0.00 |
14.25 |
0.27 |
0.43 |
| 4 |
A1u |
303 |
293 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
3012 |
2920 |
79.87 |
0.00 |
0.00 |
0.00 |
| 6 |
A2u |
1408 |
1365 |
0.67 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3064 |
2970 |
0.00 |
162.01 |
0.75 |
0.86 |
| 7 |
Eg |
3064 |
2970 |
0.00 |
162.02 |
0.75 |
0.86 |
| 8 |
Eg |
1513 |
1467 |
0.00 |
30.87 |
0.75 |
0.86 |
| 8 |
Eg |
1513 |
1467 |
0.00 |
30.87 |
0.75 |
0.86 |
| 9 |
Eg |
1214 |
1177 |
0.00 |
1.28 |
0.75 |
0.86 |
| 9 |
Eg |
1214 |
1177 |
0.00 |
1.27 |
0.75 |
0.86 |
| 10 |
Eu |
3090 |
2995 |
104.54 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3090 |
2995 |
104.60 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1519 |
1472 |
10.53 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1519 |
1472 |
10.53 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
815 |
790 |
3.45 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
815 |
790 |
3.45 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 16291.6 cm
-1
Scaled (by 0.9694) Zero Point Vibrational Energy (zpe) 15793.1 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 B3LYP/CEP-121G*
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 |
1.023 |
1.171 |
| H4 |
-0.886 |
-0.511 |
1.171 |
| H5 |
0.886 |
-0.511 |
1.171 |
| H6 |
0.000 |
-1.023 |
-1.171 |
| H7 |
-0.886 |
0.511 |
-1.171 |
| H8 |
0.886 |
0.511 |
-1.171 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5433 | 1.0981 | 1.0981 | 1.0981 | 2.1954 | 2.1954 | 2.1954 |
C2 | 1.5433 | | 2.1954 | 2.1954 | 2.1954 | 1.0981 | 1.0981 | 1.0981 | H3 | 1.0981 | 2.1954 | | 1.7719 | 1.7719 | 3.1095 | 2.5553 | 2.5553 | H4 | 1.0981 | 2.1954 | 1.7719 | | 1.7719 | 2.5553 | 2.5553 | 3.1095 | H5 | 1.0981 | 2.1954 | 1.7719 | 1.7719 | | 2.5553 | 3.1095 | 2.5553 | H6 | 2.1954 | 1.0981 | 3.1095 | 2.5553 | 2.5553 | | 1.7719 | 1.7719 | H7 | 2.1954 | 1.0981 | 2.5553 | 2.5553 | 3.1095 | 1.7719 | | 1.7719 | H8 | 2.1954 | 1.0981 | 2.5553 | 3.1095 | 2.5553 | 1.7719 | 1.7719 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.315 |
|
C1 |
C2 |
H7 |
111.315 |
| C1 |
C2 |
H8 |
111.315 |
|
C2 |
C1 |
H3 |
111.315 |
| C2 |
C1 |
H4 |
111.315 |
|
C2 |
C1 |
H5 |
111.315 |
| H3 |
C1 |
H4 |
107.566 |
|
H3 |
C1 |
H5 |
107.566 |
| H4 |
C1 |
H5 |
107.566 |
|
H6 |
C2 |
H7 |
107.566 |
| H6 |
C2 |
H8 |
107.566 |
|
H7 |
C2 |
H8 |
107.566 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/CEP-121G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.477 |
|
|
|
| 2 |
C |
-0.477 |
|
|
|
| 3 |
H |
0.159 |
|
|
|
| 4 |
H |
0.159 |
|
|
|
| 5 |
H |
0.159 |
|
|
|
| 6 |
H |
0.159 |
|
|
|
| 7 |
H |
0.159 |
|
|
|
| 8 |
H |
0.159 |
|
|
|
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 |
-14.992 |
0.000 |
0.000 |
| y |
0.000 |
-14.992 |
0.000 |
| z |
0.000 |
0.000 |
-15.710 |
|
| Traceless |
| | x | y | z |
| x |
0.359 |
0.000 |
0.000 |
| y |
0.000 |
0.359 |
0.000 |
| z |
0.000 |
0.000 |
-0.718 |
|
| Polar |
| 3z2-r2 | -1.436 |
| 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 |
3.768 |
0.000 |
0.000 |
| y |
0.000 |
3.768 |
0.000 |
| z |
0.000 |
0.000 |
4.088 |
<r2> (average value of r
2) Å
2
| <r2> |
28.781 |
| (<r2>)1/2 |
5.365 |
Jump to
S1C1
Energy calculated at B3LYP/CEP-121G*
| | hartrees |
| Energy at 0K | -14.918481 |
| Energy at 298.15K | |
| HF Energy | -14.918481 |
| Nuclear repulsion energy | 26.297489 |
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/CEP-121G*
| 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' |
3029 |
2937 |
0.00 |
|
|
|
| 2 |
A1' |
1455 |
1410 |
0.00 |
|
|
|
| 3 |
A1' |
983 |
953 |
0.00 |
|
|
|
| 4 |
A1" |
292i |
283i |
0.00 |
|
|
|
| 5 |
A2" |
3019 |
2927 |
88.31 |
|
|
|
| 6 |
A2" |
1407 |
1364 |
0.65 |
|
|
|
| 7 |
E' |
3096 |
3002 |
90.03 |
|
|
|
| 7 |
E' |
3096 |
3002 |
90.05 |
|
|
|
| 8 |
E' |
1524 |
1478 |
11.72 |
|
|
|
| 8 |
E' |
1524 |
1478 |
11.71 |
|
|
|
| 9 |
E' |
892 |
864 |
3.38 |
|
|
|
| 9 |
E' |
892 |
864 |
3.38 |
|
|
|
| 10 |
E" |
3073 |
2979 |
0.00 |
|
|
|
| 10 |
E" |
3073 |
2979 |
0.00 |
|
|
|
| 11 |
E" |
1514 |
1467 |
0.00 |
|
|
|
| 11 |
E" |
1514 |
1467 |
0.00 |
|
|
|
| 12 |
E" |
1168 |
1132 |
0.00 |
|
|
|
| 12 |
E" |
1168 |
1132 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16066.9 cm
-1
Scaled (by 0.9694) Zero Point Vibrational Energy (zpe) 15575.3 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/CEP-121G*
Point Group is D3h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.779 |
| C2 |
0.000 |
0.000 |
-0.779 |
| H3 |
0.000 |
1.019 |
1.185 |
| H4 |
-0.882 |
-0.509 |
1.185 |
| H5 |
0.882 |
-0.509 |
1.185 |
| H6 |
0.000 |
1.019 |
-1.185 |
| H7 |
0.882 |
-0.509 |
-1.185 |
| H8 |
-0.882 |
-0.509 |
-1.185 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5574 | 1.0970 | 1.0970 | 1.0970 | 2.2125 | 2.2125 | 2.2125 |
C2 | 1.5574 | | 2.2125 | 2.2125 | 2.2125 | 1.0970 | 1.0970 | 1.0970 | H3 | 1.0970 | 2.2125 | | 1.7647 | 1.7647 | 2.3706 | 2.9553 | 2.9553 | H4 | 1.0970 | 2.2125 | 1.7647 | | 1.7647 | 2.9553 | 2.9553 | 2.3706 | H5 | 1.0970 | 2.2125 | 1.7647 | 1.7647 | | 2.9553 | 2.3706 | 2.9553 | H6 | 2.2125 | 1.0970 | 2.3706 | 2.9553 | 2.9553 | | 1.7647 | 1.7647 | H7 | 2.2125 | 1.0970 | 2.9553 | 2.9553 | 2.3706 | 1.7647 | | 1.7647 | H8 | 2.2125 | 1.0970 | 2.9553 | 2.3706 | 2.9553 | 1.7647 | 1.7647 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.755 |
|
C1 |
C2 |
H7 |
111.755 |
| C1 |
C2 |
H8 |
111.755 |
|
C2 |
C1 |
H3 |
111.755 |
| C2 |
C1 |
H4 |
111.755 |
|
C2 |
C1 |
H5 |
111.755 |
| H3 |
C1 |
H4 |
107.094 |
|
H3 |
C1 |
H5 |
107.094 |
| H4 |
C1 |
H5 |
107.094 |
|
H6 |
C2 |
H7 |
107.094 |
| H6 |
C2 |
H8 |
107.094 |
|
H7 |
C2 |
H8 |
107.094 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/CEP-121G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.491 |
|
|
|
| 2 |
C |
-0.491 |
|
|
|
| 3 |
H |
0.164 |
|
|
|
| 4 |
H |
0.164 |
|
|
|
| 5 |
H |
0.164 |
|
|
|
| 6 |
H |
0.164 |
|
|
|
| 7 |
H |
0.164 |
|
|
|
| 8 |
H |
0.164 |
|
|
|
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 |
-14.978 |
0.000 |
0.000 |
| y |
0.000 |
-14.978 |
0.000 |
| z |
0.000 |
0.000 |
-15.676 |
|
| Traceless |
| | x | y | z |
| x |
0.349 |
0.000 |
0.000 |
| y |
0.000 |
0.349 |
0.000 |
| z |
0.000 |
0.000 |
-0.698 |
|
| Polar |
| 3z2-r2 | -1.396 |
| 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 |
3.712 |
0.000 |
0.000 |
| y |
0.000 |
3.712 |
0.000 |
| z |
0.000 |
0.000 |
3.917 |
<r2> (average value of r
2) Å
2
| <r2> |
29.009 |
| (<r2>)1/2 |
5.386 |