Jump to
S1C2
Energy calculated at B3LYP/3-21G
| | hartrees |
| Energy at 0K | -79.400644 |
| Energy at 298.15K | -79.406580 |
| HF Energy | -79.400644 |
| Nuclear repulsion energy | 41.980673 |
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/3-21G
| 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 |
3051 |
2944 |
0.00 |
183.84 |
0.01 |
0.02 |
| 2 |
A1g |
1461 |
1410 |
0.00 |
9.72 |
0.71 |
0.83 |
| 3 |
A1g |
974 |
940 |
0.00 |
7.89 |
0.29 |
0.45 |
| 4 |
A1u |
307 |
296 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
3052 |
2945 |
46.98 |
0.00 |
0.00 |
0.00 |
| 6 |
A2u |
1472 |
1420 |
5.61 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3097 |
2989 |
0.00 |
119.08 |
0.75 |
0.86 |
| 7 |
Eg |
3097 |
2989 |
0.00 |
119.08 |
0.75 |
0.86 |
| 8 |
Eg |
1573 |
1518 |
0.00 |
46.34 |
0.75 |
0.86 |
| 8 |
Eg |
1573 |
1518 |
0.00 |
46.34 |
0.75 |
0.86 |
| 9 |
Eg |
1258 |
1214 |
0.00 |
3.87 |
0.75 |
0.86 |
| 9 |
Eg |
1258 |
1214 |
0.00 |
3.87 |
0.75 |
0.86 |
| 10 |
Eu |
3125 |
3015 |
60.10 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3125 |
3015 |
60.10 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1575 |
1519 |
11.17 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1575 |
1519 |
11.17 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
863 |
833 |
8.21 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
863 |
833 |
8.21 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 16649.2 cm
-1
Scaled (by 0.9649) Zero Point Vibrational Energy (zpe) 16064.8 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 B3LYP/3-21G
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 |
1.162 |
| H4 |
-0.887 |
-0.512 |
1.162 |
| H5 |
0.887 |
-0.512 |
1.162 |
| H6 |
0.000 |
-1.024 |
-1.162 |
| H7 |
-0.887 |
0.512 |
-1.162 |
| H8 |
0.887 |
0.512 |
-1.162 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5444 | 1.0955 | 1.0955 | 1.0955 | 2.1888 | 2.1888 | 2.1888 |
C2 | 1.5444 | | 2.1888 | 2.1888 | 2.1888 | 1.0955 | 1.0955 | 1.0955 | H3 | 1.0955 | 2.1888 | | 1.7731 | 1.7731 | 3.0978 | 2.5402 | 2.5402 | H4 | 1.0955 | 2.1888 | 1.7731 | | 1.7731 | 2.5402 | 2.5402 | 3.0978 | H5 | 1.0955 | 2.1888 | 1.7731 | 1.7731 | | 2.5402 | 3.0978 | 2.5402 | H6 | 2.1888 | 1.0955 | 3.0978 | 2.5402 | 2.5402 | | 1.7731 | 1.7731 | H7 | 2.1888 | 1.0955 | 2.5402 | 2.5402 | 3.0978 | 1.7731 | | 1.7731 | H8 | 2.1888 | 1.0955 | 2.5402 | 3.0978 | 2.5402 | 1.7731 | 1.7731 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
110.864 |
|
C1 |
C2 |
H7 |
110.864 |
| C1 |
C2 |
H8 |
110.864 |
|
C2 |
C1 |
H3 |
110.864 |
| C2 |
C1 |
H4 |
110.864 |
|
C2 |
C1 |
H5 |
110.864 |
| H3 |
C1 |
H4 |
108.044 |
|
H3 |
C1 |
H5 |
108.044 |
| H4 |
C1 |
H5 |
108.044 |
|
H6 |
C2 |
H7 |
108.044 |
| H6 |
C2 |
H8 |
108.044 |
|
H7 |
C2 |
H8 |
108.044 |
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.563 |
|
|
|
| 2 |
C |
-0.563 |
|
|
|
| 3 |
H |
0.188 |
|
|
|
| 4 |
H |
0.188 |
|
|
|
| 5 |
H |
0.188 |
|
|
|
| 6 |
H |
0.188 |
|
|
|
| 7 |
H |
0.188 |
|
|
|
| 8 |
H |
0.188 |
|
|
|
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 |
-0.003 |
0.000 |
0.001 |
0.003 |
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.775 |
0.000 |
0.000 |
| y |
0.000 |
-14.775 |
0.000 |
| z |
0.000 |
0.000 |
-15.170 |
|
| Traceless |
| | x | y | z |
| x |
0.197 |
0.000 |
0.000 |
| y |
0.000 |
0.197 |
0.000 |
| z |
0.000 |
0.000 |
-0.394 |
|
| Polar |
| 3z2-r2 | -0.789 |
| 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 |
3.129 |
0.000 |
0.000 |
| y |
0.000 |
3.129 |
0.000 |
| z |
0.000 |
0.000 |
3.340 |
<r2> (average value of r
2) Å
2
| <r2> |
30.861 |
| (<r2>)1/2 |
5.555 |
Jump to
S1C1
Energy calculated at B3LYP/3-21G
| | hartrees |
| Energy at 0K | -79.396324 |
| Energy at 298.15K | |
| HF Energy | -79.396324 |
| Nuclear repulsion energy | 41.810349 |
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/3-21G
| 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' |
3067 |
2959 |
0.00 |
|
|
|
| 2 |
A1' |
1484 |
1432 |
0.00 |
|
|
|
| 3 |
A1' |
965 |
931 |
0.00 |
|
|
|
| 4 |
A1" |
299i |
288i |
0.00 |
|
|
|
| 5 |
A2" |
3060 |
2952 |
49.29 |
|
|
|
| 6 |
A2" |
1468 |
1417 |
5.56 |
|
|
|
| 7 |
E' |
3132 |
3022 |
50.96 |
|
|
|
| 7 |
E' |
3132 |
3022 |
50.96 |
|
|
|
| 8 |
E' |
1584 |
1528 |
13.10 |
|
|
|
| 8 |
E' |
1584 |
1528 |
13.10 |
|
|
|
| 9 |
E' |
937 |
904 |
8.15 |
|
|
|
| 9 |
E' |
937 |
904 |
8.15 |
|
|
|
| 10 |
E" |
3108 |
2999 |
0.00 |
|
|
|
| 10 |
E" |
3108 |
2999 |
0.00 |
|
|
|
| 11 |
E" |
1572 |
1517 |
0.00 |
|
|
|
| 11 |
E" |
1572 |
1517 |
0.00 |
|
|
|
| 12 |
E" |
1210 |
1168 |
0.00 |
|
|
|
| 12 |
E" |
1210 |
1168 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16415.4 cm
-1
Scaled (by 0.9649) Zero Point Vibrational Energy (zpe) 15839.2 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/3-21G
Point Group is D3h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.780 |
| C2 |
0.000 |
0.000 |
-0.780 |
| H3 |
0.000 |
1.020 |
1.177 |
| H4 |
-0.883 |
-0.510 |
1.177 |
| H5 |
0.883 |
-0.510 |
1.177 |
| H6 |
0.000 |
1.020 |
-1.177 |
| H7 |
0.883 |
-0.510 |
-1.177 |
| H8 |
-0.883 |
-0.510 |
-1.177 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5592 | 1.0944 | 1.0944 | 1.0944 | 2.2062 | 2.2062 | 2.2062 |
C2 | 1.5592 | | 2.2062 | 2.2062 | 2.2062 | 1.0944 | 1.0944 | 1.0944 | H3 | 1.0944 | 2.2062 | | 1.7665 | 1.7665 | 2.3533 | 2.9425 | 2.9425 | H4 | 1.0944 | 2.2062 | 1.7665 | | 1.7665 | 2.9425 | 2.9425 | 2.3533 | H5 | 1.0944 | 2.2062 | 1.7665 | 1.7665 | | 2.9425 | 2.3533 | 2.9425 | H6 | 2.2062 | 1.0944 | 2.3533 | 2.9425 | 2.9425 | | 1.7665 | 1.7665 | H7 | 2.2062 | 1.0944 | 2.9425 | 2.9425 | 2.3533 | 1.7665 | | 1.7665 | H8 | 2.2062 | 1.0944 | 2.9425 | 2.3533 | 2.9425 | 1.7665 | 1.7665 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.271 |
|
C1 |
C2 |
H7 |
111.271 |
| C1 |
C2 |
H8 |
111.271 |
|
C2 |
C1 |
H3 |
111.271 |
| C2 |
C1 |
H4 |
111.271 |
|
C2 |
C1 |
H5 |
111.271 |
| H3 |
C1 |
H4 |
107.613 |
|
H3 |
C1 |
H5 |
107.613 |
| H4 |
C1 |
H5 |
107.613 |
|
H6 |
C2 |
H7 |
107.613 |
| H6 |
C2 |
H8 |
107.613 |
|
H7 |
C2 |
H8 |
107.613 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.572 |
|
|
|
| 2 |
C |
-0.572 |
|
|
|
| 3 |
H |
0.191 |
|
|
|
| 4 |
H |
0.191 |
|
|
|
| 5 |
H |
0.191 |
|
|
|
| 6 |
H |
0.191 |
|
|
|
| 7 |
H |
0.191 |
|
|
|
| 8 |
H |
0.191 |
|
|
|
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 |
-14.757 |
0.000 |
0.000 |
| y |
0.000 |
-14.757 |
0.000 |
| z |
0.000 |
0.000 |
-15.078 |
|
| Traceless |
| | x | y | z |
| x |
0.160 |
0.000 |
0.000 |
| y |
0.000 |
0.160 |
0.000 |
| z |
0.000 |
0.000 |
-0.321 |
|
| Polar |
| 3z2-r2 | -0.641 |
| 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 |
3.060 |
0.000 |
0.000 |
| y |
0.000 |
3.060 |
0.000 |
| z |
0.000 |
0.000 |
3.292 |
<r2> (average value of r
2) Å
2
| <r2> |
31.125 |
| (<r2>)1/2 |
5.579 |