Jump to
S1C2
Energy calculated at BLYP/3-21G
| | hartrees |
| Energy at 0K | -79.333451 |
| Energy at 298.15K | -79.339349 |
| HF Energy | -79.333451 |
| Nuclear repulsion energy | 41.687367 |
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 BLYP/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 |
2973 |
2957 |
0.00 |
184.44 |
0.01 |
0.02 |
| 2 |
A1g |
1422 |
1414 |
0.00 |
11.56 |
0.69 |
0.81 |
| 3 |
A1g |
941 |
936 |
0.00 |
6.71 |
0.29 |
0.45 |
| 4 |
A1u |
303 |
301 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
2974 |
2958 |
51.08 |
0.00 |
0.00 |
0.00 |
| 6 |
A2u |
1434 |
1426 |
2.83 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3015 |
2999 |
0.00 |
118.40 |
0.75 |
0.86 |
| 7 |
Eg |
3015 |
2999 |
0.00 |
118.39 |
0.75 |
0.86 |
| 8 |
Eg |
1537 |
1528 |
0.00 |
47.07 |
0.75 |
0.86 |
| 8 |
Eg |
1537 |
1528 |
0.00 |
47.07 |
0.75 |
0.86 |
| 9 |
Eg |
1225 |
1218 |
0.00 |
4.13 |
0.75 |
0.86 |
| 9 |
Eg |
1225 |
1218 |
0.00 |
4.13 |
0.75 |
0.86 |
| 10 |
Eu |
3044 |
3027 |
67.37 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3044 |
3027 |
67.36 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1540 |
1531 |
9.25 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1540 |
1531 |
9.25 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
841 |
836 |
7.63 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
841 |
836 |
7.63 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 16224.7 cm
-1
Scaled (by 0.9945) Zero Point Vibrational Energy (zpe) 16135.5 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 BLYP/3-21G
Point Group is D3d
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 |
1.031 |
1.170 |
| H4 |
-0.893 |
-0.515 |
1.170 |
| H5 |
0.893 |
-0.515 |
1.170 |
| H6 |
0.000 |
-1.031 |
-1.170 |
| H7 |
-0.893 |
0.515 |
-1.170 |
| H8 |
0.893 |
0.515 |
-1.170 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5560 | 1.1029 | 1.1029 | 1.1029 | 2.2042 | 2.2042 | 2.2042 |
C2 | 1.5560 | | 2.2042 | 2.2042 | 2.2042 | 1.1029 | 1.1029 | 1.1029 | H3 | 1.1029 | 2.2042 | | 1.7853 | 1.7853 | 3.1192 | 2.5577 | 2.5577 | H4 | 1.1029 | 2.2042 | 1.7853 | | 1.7853 | 2.5577 | 2.5577 | 3.1192 | H5 | 1.1029 | 2.2042 | 1.7853 | 1.7853 | | 2.5577 | 3.1192 | 2.5577 | H6 | 2.2042 | 1.1029 | 3.1192 | 2.5577 | 2.5577 | | 1.7853 | 1.7853 | H7 | 2.2042 | 1.1029 | 2.5577 | 2.5577 | 3.1192 | 1.7853 | | 1.7853 | H8 | 2.2042 | 1.1029 | 2.5577 | 3.1192 | 2.5577 | 1.7853 | 1.7853 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
110.843 |
|
C1 |
C2 |
H7 |
110.843 |
| C1 |
C2 |
H8 |
110.843 |
|
C2 |
C1 |
H3 |
110.843 |
| C2 |
C1 |
H4 |
110.843 |
|
C2 |
C1 |
H5 |
110.843 |
| H3 |
C1 |
H4 |
108.065 |
|
H3 |
C1 |
H5 |
108.065 |
| H4 |
C1 |
H5 |
108.065 |
|
H6 |
C2 |
H7 |
108.065 |
| H6 |
C2 |
H8 |
108.065 |
|
H7 |
C2 |
H8 |
108.065 |
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.525 |
|
|
|
| 2 |
C |
-0.525 |
|
|
|
| 3 |
H |
0.175 |
|
|
|
| 4 |
H |
0.175 |
|
|
|
| 5 |
H |
0.175 |
|
|
|
| 6 |
H |
0.175 |
|
|
|
| 7 |
H |
0.175 |
|
|
|
| 8 |
H |
0.175 |
|
|
|
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 |
-14.812 |
0.000 |
0.000 |
| y |
0.000 |
-14.812 |
0.000 |
| z |
0.000 |
0.000 |
-15.182 |
|
| Traceless |
| | x | y | z |
| x |
0.185 |
0.000 |
0.000 |
| y |
0.000 |
0.185 |
0.000 |
| z |
0.000 |
0.000 |
-0.370 |
|
| Polar |
| 3z2-r2 | -0.741 |
| 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 |
3.177 |
0.000 |
0.000 |
| y |
0.000 |
3.177 |
0.000 |
| z |
0.000 |
0.000 |
3.416 |
<r2> (average value of r
2) Å
2
| <r2> |
31.185 |
| (<r2>)1/2 |
5.584 |
Jump to
S1C1
Energy calculated at BLYP/3-21G
| | hartrees |
| Energy at 0K | -79.329196 |
| Energy at 298.15K | |
| HF Energy | -79.329196 |
| Nuclear repulsion energy | 41.516179 |
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 BLYP/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' |
2989 |
2973 |
0.00 |
|
|
|
| 2 |
A1' |
1445 |
1437 |
0.00 |
|
|
|
| 3 |
A1' |
932 |
927 |
0.00 |
|
|
|
| 4 |
A1" |
294i |
293i |
0.00 |
|
|
|
| 5 |
A2" |
2983 |
2966 |
53.33 |
|
|
|
| 6 |
A2" |
1430 |
1422 |
2.88 |
|
|
|
| 7 |
E' |
3051 |
3034 |
57.55 |
|
|
|
| 7 |
E' |
3051 |
3034 |
57.55 |
|
|
|
| 8 |
E' |
1547 |
1539 |
11.05 |
|
|
|
| 8 |
E' |
1547 |
1539 |
11.05 |
|
|
|
| 9 |
E' |
913 |
908 |
7.59 |
|
|
|
| 9 |
E' |
913 |
908 |
7.59 |
|
|
|
| 10 |
E" |
3027 |
3010 |
0.00 |
|
|
|
| 10 |
E" |
3027 |
3010 |
0.00 |
|
|
|
| 11 |
E" |
1538 |
1529 |
0.00 |
|
|
|
| 11 |
E" |
1538 |
1529 |
0.00 |
|
|
|
| 12 |
E" |
1176 |
1169 |
0.00 |
|
|
|
| 12 |
E" |
1176 |
1169 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15992.4 cm
-1
Scaled (by 0.9945) Zero Point Vibrational Energy (zpe) 15904.4 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 BLYP/3-21G
Point Group is D3h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.786 |
| C2 |
0.000 |
0.000 |
-0.786 |
| H3 |
0.000 |
1.027 |
1.185 |
| H4 |
-0.889 |
-0.513 |
1.185 |
| H5 |
0.889 |
-0.513 |
1.185 |
| H6 |
0.000 |
1.027 |
-1.185 |
| H7 |
0.889 |
-0.513 |
-1.185 |
| H8 |
-0.889 |
-0.513 |
-1.185 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5711 | 1.1018 | 1.1018 | 1.1018 | 2.2219 | 2.2219 | 2.2219 |
C2 | 1.5711 | | 2.2219 | 2.2219 | 2.2219 | 1.1018 | 1.1018 | 1.1018 | H3 | 1.1018 | 2.2219 | | 1.7788 | 1.7788 | 2.3694 | 2.9628 | 2.9628 | H4 | 1.1018 | 2.2219 | 1.7788 | | 1.7788 | 2.9628 | 2.9628 | 2.3694 | H5 | 1.1018 | 2.2219 | 1.7788 | 1.7788 | | 2.9628 | 2.3694 | 2.9628 | H6 | 2.2219 | 1.1018 | 2.3694 | 2.9628 | 2.9628 | | 1.7788 | 1.7788 | H7 | 2.2219 | 1.1018 | 2.9628 | 2.9628 | 2.3694 | 1.7788 | | 1.7788 | H8 | 2.2219 | 1.1018 | 2.9628 | 2.3694 | 2.9628 | 1.7788 | 1.7788 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.239 |
|
C1 |
C2 |
H7 |
111.239 |
| C1 |
C2 |
H8 |
111.239 |
|
C2 |
C1 |
H3 |
111.239 |
| C2 |
C1 |
H4 |
111.239 |
|
C2 |
C1 |
H5 |
111.239 |
| H3 |
C1 |
H4 |
107.647 |
|
H3 |
C1 |
H5 |
107.647 |
| H4 |
C1 |
H5 |
107.647 |
|
H6 |
C2 |
H7 |
107.647 |
| H6 |
C2 |
H8 |
107.647 |
|
H7 |
C2 |
H8 |
107.647 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.534 |
|
|
|
| 2 |
C |
-0.534 |
|
|
|
| 3 |
H |
0.178 |
|
|
|
| 4 |
H |
0.178 |
|
|
|
| 5 |
H |
0.178 |
|
|
|
| 6 |
H |
0.178 |
|
|
|
| 7 |
H |
0.178 |
|
|
|
| 8 |
H |
0.178 |
|
|
|
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 |
-14.791 |
0.000 |
0.000 |
| y |
0.000 |
-14.791 |
0.000 |
| z |
0.000 |
0.000 |
-15.099 |
|
| Traceless |
| | x | y | z |
| x |
0.154 |
0.000 |
0.000 |
| y |
0.000 |
0.154 |
0.000 |
| z |
0.000 |
0.000 |
-0.308 |
|
| Polar |
| 3z2-r2 | -0.615 |
| 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 |
3.106 |
0.000 |
0.000 |
| y |
0.000 |
3.106 |
0.000 |
| z |
0.000 |
0.000 |
3.364 |
<r2> (average value of r
2) Å
2
| <r2> |
31.457 |
| (<r2>)1/2 |
5.609 |