Jump to
S1C2
Energy calculated at B3LYP/cc-pVTZ
| | hartrees |
| Energy at 0K | -79.864340 |
| Energy at 298.15K | -79.870247 |
| HF Energy | -79.864340 |
| Nuclear repulsion energy | 42.258512 |
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/cc-pVTZ
| 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 |
3027 |
2926 |
0.00 |
292.27 |
0.01 |
0.01 |
| 2 |
A1g |
1424 |
1376 |
0.00 |
1.01 |
0.74 |
0.85 |
| 3 |
A1g |
996 |
962 |
0.00 |
11.06 |
0.23 |
0.37 |
| 4 |
A1u |
305 |
295 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
3028 |
2927 |
60.59 |
0.00 |
0.00 |
0.00 |
| 6 |
A2u |
1414 |
1367 |
0.98 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3071 |
2968 |
0.00 |
138.50 |
0.75 |
0.86 |
| 7 |
Eg |
3071 |
2968 |
0.00 |
138.50 |
0.75 |
0.86 |
| 8 |
Eg |
1504 |
1454 |
0.00 |
18.00 |
0.75 |
0.86 |
| 8 |
Eg |
1504 |
1454 |
0.00 |
18.00 |
0.75 |
0.86 |
| 9 |
Eg |
1223 |
1182 |
0.00 |
0.30 |
0.75 |
0.86 |
| 9 |
Eg |
1223 |
1182 |
0.00 |
0.30 |
0.75 |
0.86 |
| 10 |
Eu |
3096 |
2993 |
67.73 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3096 |
2993 |
67.73 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1508 |
1457 |
8.57 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1508 |
1457 |
8.57 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
827 |
799 |
3.85 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
827 |
799 |
3.85 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 16325.1 cm
-1
Scaled (by 0.9666) Zero Point Vibrational Energy (zpe) 15779.9 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/cc-pVTZ
Point Group is D3d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.764 |
| C2 |
0.000 |
0.000 |
-0.764 |
| H3 |
0.000 |
1.016 |
1.161 |
| H4 |
-0.880 |
-0.508 |
1.161 |
| H5 |
0.880 |
-0.508 |
1.161 |
| H6 |
0.000 |
-1.016 |
-1.161 |
| H7 |
-0.880 |
0.508 |
-1.161 |
| H8 |
0.880 |
0.508 |
-1.161 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5273 | 1.0910 | 1.0910 | 1.0910 | 2.1763 | 2.1763 | 2.1763 |
C2 | 1.5273 | | 2.1763 | 2.1763 | 2.1763 | 1.0910 | 1.0910 | 1.0910 | H3 | 1.0910 | 2.1763 | | 1.7600 | 1.7600 | 3.0856 | 2.5344 | 2.5344 | H4 | 1.0910 | 2.1763 | 1.7600 | | 1.7600 | 2.5344 | 2.5344 | 3.0856 | H5 | 1.0910 | 2.1763 | 1.7600 | 1.7600 | | 2.5344 | 3.0856 | 2.5344 | H6 | 2.1763 | 1.0910 | 3.0856 | 2.5344 | 2.5344 | | 1.7600 | 1.7600 | H7 | 2.1763 | 1.0910 | 2.5344 | 2.5344 | 3.0856 | 1.7600 | | 1.7600 | H8 | 2.1763 | 1.0910 | 2.5344 | 3.0856 | 2.5344 | 1.7600 | 1.7600 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.352 |
|
C1 |
C2 |
H7 |
111.352 |
| C1 |
C2 |
H8 |
111.352 |
|
C2 |
C1 |
H3 |
111.352 |
| C2 |
C1 |
H4 |
111.352 |
|
C2 |
C1 |
H5 |
111.352 |
| H3 |
C1 |
H4 |
107.527 |
|
H3 |
C1 |
H5 |
107.527 |
| H4 |
C1 |
H5 |
107.527 |
|
H6 |
C2 |
H7 |
107.527 |
| H6 |
C2 |
H8 |
107.527 |
|
H7 |
C2 |
H8 |
107.527 |
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.282 |
|
|
|
| 2 |
C |
-0.282 |
|
|
|
| 3 |
H |
0.094 |
|
|
|
| 4 |
H |
0.094 |
|
|
|
| 5 |
H |
0.094 |
|
|
|
| 6 |
H |
0.094 |
|
|
|
| 7 |
H |
0.094 |
|
|
|
| 8 |
H |
0.094 |
|
|
|
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 |
-0.006 |
0.000 |
0.000 |
0.006 |
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.014 |
0.000 |
0.000 |
| y |
0.000 |
-15.014 |
0.000 |
| z |
0.000 |
0.000 |
-15.692 |
|
| Traceless |
| | x | y | z |
| x |
0.339 |
0.000 |
0.000 |
| y |
0.000 |
0.339 |
0.000 |
| z |
0.000 |
0.000 |
-0.678 |
|
| Polar |
| 3z2-r2 | -1.355 |
| 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 |
3.874 |
0.000 |
0.000 |
| y |
0.000 |
3.874 |
0.000 |
| z |
0.000 |
0.000 |
4.358 |
<r2> (average value of r
2) Å
2
| <r2> |
30.798 |
| (<r2>)1/2 |
5.550 |
Jump to
S1C1
Energy calculated at B3LYP/cc-pVTZ
| | hartrees |
| Energy at 0K | -79.860126 |
| Energy at 298.15K | |
| HF Energy | -79.860126 |
| Nuclear repulsion energy | 42.095686 |
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/cc-pVTZ
| 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' |
3043 |
2941 |
0.00 |
|
|
|
| 2 |
A1' |
1440 |
1392 |
0.00 |
|
|
|
| 3 |
A1' |
992 |
958 |
0.00 |
|
|
|
| 4 |
A1" |
297i |
288i |
0.00 |
|
|
|
| 5 |
A2" |
3036 |
2935 |
61.80 |
|
|
|
| 6 |
A2" |
1411 |
1363 |
0.67 |
|
|
|
| 7 |
E' |
3104 |
3000 |
57.09 |
|
|
|
| 7 |
E' |
3104 |
3000 |
57.08 |
|
|
|
| 8 |
E' |
1512 |
1461 |
9.98 |
|
|
|
| 8 |
E' |
1512 |
1461 |
9.98 |
|
|
|
| 9 |
E' |
899 |
869 |
2.88 |
|
|
|
| 9 |
E' |
899 |
869 |
2.88 |
|
|
|
| 10 |
E" |
3081 |
2978 |
0.00 |
|
|
|
| 10 |
E" |
3081 |
2978 |
0.00 |
|
|
|
| 11 |
E" |
1504 |
1453 |
0.00 |
|
|
|
| 11 |
E" |
1504 |
1453 |
0.00 |
|
|
|
| 12 |
E" |
1174 |
1135 |
0.00 |
|
|
|
| 12 |
E" |
1174 |
1135 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16085.6 cm
-1
Scaled (by 0.9666) Zero Point Vibrational Energy (zpe) 15548.4 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 B3LYP/cc-pVTZ
Point Group is D3h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.771 |
| C2 |
0.000 |
0.000 |
-0.771 |
| H3 |
0.000 |
1.012 |
1.175 |
| H4 |
-0.877 |
-0.506 |
1.175 |
| H5 |
0.877 |
-0.506 |
1.175 |
| H6 |
0.000 |
1.012 |
-1.175 |
| H7 |
0.877 |
-0.506 |
-1.175 |
| H8 |
-0.877 |
-0.506 |
-1.175 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5412 | 1.0899 | 1.0899 | 1.0899 | 2.1931 | 2.1931 | 2.1931 |
C2 | 1.5412 | | 2.1931 | 2.1931 | 2.1931 | 1.0899 | 1.0899 | 1.0899 | H3 | 1.0899 | 2.1931 | | 1.7531 | 1.7531 | 2.3499 | 2.9318 | 2.9318 | H4 | 1.0899 | 2.1931 | 1.7531 | | 1.7531 | 2.9318 | 2.9318 | 2.3499 | H5 | 1.0899 | 2.1931 | 1.7531 | 1.7531 | | 2.9318 | 2.3499 | 2.9318 | H6 | 2.1931 | 1.0899 | 2.3499 | 2.9318 | 2.9318 | | 1.7531 | 1.7531 | H7 | 2.1931 | 1.0899 | 2.9318 | 2.9318 | 2.3499 | 1.7531 | | 1.7531 | H8 | 2.1931 | 1.0899 | 2.9318 | 2.3499 | 2.9318 | 1.7531 | 1.7531 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.776 |
|
C1 |
C2 |
H7 |
111.776 |
| C1 |
C2 |
H8 |
111.776 |
|
C2 |
C1 |
H3 |
111.776 |
| C2 |
C1 |
H4 |
111.776 |
|
C2 |
C1 |
H5 |
111.776 |
| H3 |
C1 |
H4 |
107.071 |
|
H3 |
C1 |
H5 |
107.071 |
| H4 |
C1 |
H5 |
107.071 |
|
H6 |
C2 |
H7 |
107.071 |
| H6 |
C2 |
H8 |
107.071 |
|
H7 |
C2 |
H8 |
107.071 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.290 |
|
|
|
| 2 |
C |
-0.290 |
|
|
|
| 3 |
H |
0.097 |
|
|
|
| 4 |
H |
0.097 |
|
|
|
| 5 |
H |
0.097 |
|
|
|
| 6 |
H |
0.097 |
|
|
|
| 7 |
H |
0.097 |
|
|
|
| 8 |
H |
0.097 |
|
|
|
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 |
-15.000 |
0.000 |
0.000 |
| y |
0.000 |
-15.000 |
0.000 |
| z |
0.000 |
0.000 |
-15.673 |
|
| Traceless |
| | x | y | z |
| x |
0.337 |
0.000 |
0.000 |
| y |
0.000 |
0.337 |
0.000 |
| z |
0.000 |
0.000 |
-0.673 |
|
| Polar |
| 3z2-r2 | -1.346 |
| 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 |
3.832 |
0.000 |
0.000 |
| y |
0.000 |
3.832 |
0.000 |
| z |
0.000 |
0.000 |
4.317 |
<r2> (average value of r
2) Å
2
| <r2> |
31.065 |
| (<r2>)1/2 |
5.574 |