Jump to
S1C2
Energy calculated at PBEPBE/6-31G
| | hartrees |
| Energy at 0K | -79.684336 |
| Energy at 298.15K | -79.690230 |
| HF Energy | -79.684336 |
| Nuclear repulsion energy | 41.863867 |
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 PBEPBE/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 |
2982 |
2941 |
0.00 |
223.46 |
0.01 |
0.02 |
| 2 |
A1g |
1417 |
1398 |
0.00 |
11.36 |
0.69 |
0.82 |
| 3 |
A1g |
1007 |
994 |
0.00 |
7.16 |
0.28 |
0.44 |
| 4 |
A1u |
302 |
298 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
2981 |
2940 |
62.59 |
0.00 |
0.00 |
0.00 |
| 6 |
A2u |
1417 |
1397 |
4.69 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3047 |
3005 |
0.00 |
134.43 |
0.75 |
0.86 |
| 7 |
Eg |
3047 |
3005 |
0.00 |
134.43 |
0.75 |
0.86 |
| 8 |
Eg |
1505 |
1484 |
0.00 |
46.76 |
0.75 |
0.86 |
| 8 |
Eg |
1505 |
1484 |
0.00 |
46.76 |
0.75 |
0.86 |
| 9 |
Eg |
1214 |
1197 |
0.00 |
3.82 |
0.75 |
0.86 |
| 9 |
Eg |
1214 |
1197 |
0.00 |
3.82 |
0.75 |
0.86 |
| 10 |
Eu |
3075 |
3033 |
72.74 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3075 |
3033 |
72.74 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1508 |
1487 |
12.96 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1508 |
1487 |
12.96 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
833 |
822 |
8.87 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
833 |
822 |
8.87 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 16234.7 cm
-1
Scaled (by 0.9862) Zero Point Vibrational Energy (zpe) 16010.6 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 PBEPBE/6-31G
Point Group is D3d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.768 |
| C2 |
0.000 |
0.000 |
-0.768 |
| H3 |
0.000 |
1.029 |
1.170 |
| H4 |
-0.891 |
-0.514 |
1.170 |
| H5 |
0.891 |
-0.514 |
1.170 |
| H6 |
0.000 |
-1.029 |
-1.170 |
| H7 |
-0.891 |
0.514 |
-1.170 |
| H8 |
0.891 |
0.514 |
-1.170 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5366 | 1.1043 | 1.1043 | 1.1043 | 2.1945 | 2.1945 | 2.1945 |
C2 | 1.5366 | | 2.1945 | 2.1945 | 2.1945 | 1.1043 | 1.1043 | 1.1043 | H3 | 1.1043 | 2.1945 | | 1.7814 | 1.7814 | 3.1160 | 2.5565 | 2.5565 | H4 | 1.1043 | 2.1945 | 1.7814 | | 1.7814 | 2.5565 | 2.5565 | 3.1160 | H5 | 1.1043 | 2.1945 | 1.7814 | 1.7814 | | 2.5565 | 3.1160 | 2.5565 | H6 | 2.1945 | 1.1043 | 3.1160 | 2.5565 | 2.5565 | | 1.7814 | 1.7814 | H7 | 2.1945 | 1.1043 | 2.5565 | 2.5565 | 3.1160 | 1.7814 | | 1.7814 | H8 | 2.1945 | 1.1043 | 2.5565 | 3.1160 | 2.5565 | 1.7814 | 1.7814 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.346 |
|
C1 |
C2 |
H7 |
111.346 |
| C1 |
C2 |
H8 |
111.346 |
|
C2 |
C1 |
H3 |
111.346 |
| C2 |
C1 |
H4 |
111.346 |
|
C2 |
C1 |
H5 |
111.346 |
| H3 |
C1 |
H4 |
107.533 |
|
H3 |
C1 |
H5 |
107.533 |
| H4 |
C1 |
H5 |
107.533 |
|
H6 |
C2 |
H7 |
107.533 |
| H6 |
C2 |
H8 |
107.533 |
|
H7 |
C2 |
H8 |
107.533 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.454 |
|
|
|
| 2 |
C |
-0.454 |
|
|
|
| 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 |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.769 |
0.000 |
0.000 |
| y |
0.000 |
-14.769 |
0.000 |
| z |
0.000 |
0.000 |
-15.135 |
|
| Traceless |
| | x | y | z |
| x |
0.183 |
0.000 |
0.000 |
| y |
0.000 |
0.183 |
0.000 |
| z |
0.000 |
0.000 |
-0.366 |
|
| Polar |
| 3z2-r2 | -0.733 |
| 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 |
3.356 |
0.000 |
0.000 |
| y |
0.000 |
3.356 |
0.000 |
| z |
0.000 |
0.000 |
3.564 |
<r2> (average value of r
2) Å
2
| <r2> |
30.948 |
| (<r2>)1/2 |
5.563 |
Jump to
S1C1
Energy calculated at PBEPBE/6-31G
| | hartrees |
| Energy at 0K | -79.680100 |
| Energy at 298.15K | |
| HF Energy | -79.680100 |
| Nuclear repulsion energy | 41.711240 |
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 PBEPBE/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' |
2997 |
2955 |
0.00 |
|
|
|
| 2 |
A1' |
1441 |
1421 |
0.00 |
|
|
|
| 3 |
A1' |
1000 |
986 |
0.00 |
|
|
|
| 4 |
A1" |
295i |
291i |
0.00 |
|
|
|
| 5 |
A2" |
2988 |
2947 |
65.50 |
|
|
|
| 6 |
A2" |
1414 |
1395 |
5.09 |
|
|
|
| 7 |
E' |
3080 |
3038 |
60.14 |
|
|
|
| 7 |
E' |
3080 |
3038 |
60.14 |
|
|
|
| 8 |
E' |
1515 |
1494 |
14.79 |
|
|
|
| 8 |
E' |
1515 |
1494 |
14.79 |
|
|
|
| 9 |
E' |
910 |
897 |
9.11 |
|
|
|
| 9 |
E' |
910 |
897 |
9.11 |
|
|
|
| 10 |
E" |
3057 |
3015 |
0.00 |
|
|
|
| 10 |
E" |
3057 |
3015 |
0.00 |
|
|
|
| 11 |
E" |
1505 |
1484 |
0.00 |
|
|
|
| 11 |
E" |
1505 |
1484 |
0.00 |
|
|
|
| 12 |
E" |
1166 |
1150 |
0.00 |
|
|
|
| 12 |
E" |
1166 |
1150 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16004.4 cm
-1
Scaled (by 0.9862) Zero Point Vibrational Energy (zpe) 15783.5 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 PBEPBE/6-31G
Point Group is D3h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.775 |
| C2 |
0.000 |
0.000 |
-0.775 |
| H3 |
0.000 |
1.024 |
1.184 |
| H4 |
-0.887 |
-0.512 |
1.184 |
| H5 |
0.887 |
-0.512 |
1.184 |
| H6 |
0.000 |
1.024 |
-1.184 |
| H7 |
0.887 |
-0.512 |
-1.184 |
| H8 |
-0.887 |
-0.512 |
-1.184 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5496 | 1.1033 | 1.1033 | 1.1033 | 2.2107 | 2.2107 | 2.2107 |
C2 | 1.5496 | | 2.2107 | 2.2107 | 2.2107 | 1.1033 | 1.1033 | 1.1033 | H3 | 1.1033 | 2.2107 | | 1.7744 | 1.7744 | 2.3686 | 2.9595 | 2.9595 | H4 | 1.1033 | 2.2107 | 1.7744 | | 1.7744 | 2.9595 | 2.9595 | 2.3686 | H5 | 1.1033 | 2.2107 | 1.7744 | 1.7744 | | 2.9595 | 2.3686 | 2.9595 | H6 | 2.2107 | 1.1033 | 2.3686 | 2.9595 | 2.9595 | | 1.7744 | 1.7744 | H7 | 2.2107 | 1.1033 | 2.9595 | 2.9595 | 2.3686 | 1.7744 | | 1.7744 | H8 | 2.2107 | 1.1033 | 2.9595 | 2.3686 | 2.9595 | 1.7744 | 1.7744 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.789 |
|
C1 |
C2 |
H7 |
111.789 |
| C1 |
C2 |
H8 |
111.789 |
|
C2 |
C1 |
H3 |
111.789 |
| C2 |
C1 |
H4 |
111.789 |
|
C2 |
C1 |
H5 |
111.789 |
| H3 |
C1 |
H4 |
107.057 |
|
H3 |
C1 |
H5 |
107.057 |
| H4 |
C1 |
H5 |
107.057 |
|
H6 |
C2 |
H7 |
107.057 |
| H6 |
C2 |
H8 |
107.057 |
|
H7 |
C2 |
H8 |
107.057 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.462 |
|
|
|
| 2 |
C |
-0.462 |
|
|
|
| 3 |
H |
0.154 |
|
|
|
| 4 |
H |
0.154 |
|
|
|
| 5 |
H |
0.154 |
|
|
|
| 6 |
H |
0.154 |
|
|
|
| 7 |
H |
0.154 |
|
|
|
| 8 |
H |
0.154 |
|
|
|
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 |
-14.749 |
0.000 |
0.000 |
| y |
0.000 |
-14.749 |
0.000 |
| z |
0.000 |
0.000 |
-15.063 |
|
| Traceless |
| | x | y | z |
| x |
0.157 |
0.000 |
0.000 |
| y |
0.000 |
0.157 |
0.000 |
| z |
0.000 |
0.000 |
-0.314 |
|
| Polar |
| 3z2-r2 | -0.629 |
| 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 |
3.276 |
0.000 |
0.000 |
| y |
0.000 |
3.276 |
0.000 |
| z |
0.000 |
0.000 |
3.466 |
<r2> (average value of r
2) Å
2
| <r2> |
31.193 |
| (<r2>)1/2 |
5.585 |