Jump to
S1C2
Energy calculated at HF/aug-cc-pVQZ
| | hartrees |
| Energy at 0K | -79.265431 |
| Energy at 298.15K | -79.271435 |
| HF Energy | -79.265431 |
| Nuclear repulsion energy | 42.471338 |
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 HF/aug-cc-pVQZ
| 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 |
3158 |
2869 |
0.00 |
343.47 |
0.01 |
0.01 |
| 2 |
A1g |
1549 |
1407 |
0.00 |
0.35 |
0.24 |
0.38 |
| 3 |
A1g |
1049 |
953 |
0.00 |
15.78 |
0.20 |
0.33 |
| 4 |
A1u |
328 |
298 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
3152 |
2863 |
72.97 |
0.00 |
0.00 |
0.00 |
| 6 |
A2u |
1522 |
1383 |
0.31 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3194 |
2902 |
0.00 |
125.60 |
0.75 |
0.86 |
| 7 |
Eg |
3194 |
2902 |
0.00 |
125.60 |
0.75 |
0.86 |
| 8 |
Eg |
1614 |
1467 |
0.00 |
8.51 |
0.75 |
0.86 |
| 8 |
Eg |
1614 |
1467 |
0.00 |
8.51 |
0.75 |
0.86 |
| 9 |
Eg |
1324 |
1202 |
0.00 |
0.13 |
0.75 |
0.86 |
| 9 |
Eg |
1324 |
1202 |
0.00 |
0.13 |
0.75 |
0.86 |
| 10 |
Eu |
3221 |
2927 |
97.43 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3221 |
2927 |
97.43 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1619 |
1471 |
7.57 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1619 |
1471 |
7.57 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
881 |
800 |
2.26 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
881 |
800 |
2.26 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 17231.2 cm
-1
Scaled (by 0.9085) Zero Point Vibrational Energy (zpe) 15654.5 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 HF/aug-cc-pVQZ
Point Group is D3d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.762 |
| C2 |
0.000 |
0.000 |
-0.762 |
| H3 |
0.000 |
1.010 |
1.154 |
| H4 |
-0.875 |
-0.505 |
1.154 |
| H5 |
0.875 |
-0.505 |
1.154 |
| H6 |
0.000 |
-1.010 |
-1.154 |
| H7 |
-0.875 |
0.505 |
-1.154 |
| H8 |
0.875 |
0.505 |
-1.154 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5238 | 1.0836 | 1.0836 | 1.0836 | 2.1659 | 2.1659 | 2.1659 |
C2 | 1.5238 | | 2.1659 | 2.1659 | 2.1659 | 1.0836 | 1.0836 | 1.0836 | H3 | 1.0836 | 2.1659 | | 1.7496 | 1.7496 | 3.0673 | 2.5194 | 2.5194 | H4 | 1.0836 | 2.1659 | 1.7496 | | 1.7496 | 2.5194 | 2.5194 | 3.0673 | H5 | 1.0836 | 2.1659 | 1.7496 | 1.7496 | | 2.5194 | 3.0673 | 2.5194 | H6 | 2.1659 | 1.0836 | 3.0673 | 2.5194 | 2.5194 | | 1.7496 | 1.7496 | H7 | 2.1659 | 1.0836 | 2.5194 | 2.5194 | 3.0673 | 1.7496 | | 1.7496 | H8 | 2.1659 | 1.0836 | 2.5194 | 3.0673 | 2.5194 | 1.7496 | 1.7496 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.214 |
|
C1 |
C2 |
H7 |
111.214 |
| C1 |
C2 |
H8 |
111.214 |
|
C2 |
C1 |
H3 |
111.214 |
| C2 |
C1 |
H4 |
111.214 |
|
C2 |
C1 |
H5 |
111.214 |
| H3 |
C1 |
H4 |
107.673 |
|
H3 |
C1 |
H5 |
107.673 |
| H4 |
C1 |
H5 |
107.673 |
|
H6 |
C2 |
H7 |
107.673 |
| H6 |
C2 |
H8 |
107.673 |
|
H7 |
C2 |
H8 |
107.673 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/aug-cc-pVQZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.747 |
|
|
|
| 2 |
C |
-0.747 |
|
|
|
| 3 |
H |
0.249 |
|
|
|
| 4 |
H |
0.249 |
|
|
|
| 5 |
H |
0.249 |
|
|
|
| 6 |
H |
0.249 |
|
|
|
| 7 |
H |
0.249 |
|
|
|
| 8 |
H |
0.249 |
|
|
|
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 |
-14.884 |
0.000 |
0.000 |
| y |
0.000 |
-14.884 |
0.000 |
| z |
0.000 |
0.000 |
-15.638 |
|
| Traceless |
| | x | y | z |
| x |
0.377 |
0.000 |
0.000 |
| y |
0.000 |
0.377 |
0.000 |
| z |
0.000 |
0.000 |
-0.754 |
|
| Polar |
| 3z2-r2 | -1.509 |
| 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 |
3.836 |
0.000 |
0.000 |
| y |
0.000 |
3.836 |
0.000 |
| z |
0.000 |
0.000 |
4.339 |
<r2> (average value of r
2) Å
2
| <r2> |
30.532 |
| (<r2>)1/2 |
5.526 |
Jump to
S1C1
Energy calculated at HF/aug-cc-pVQZ
| | hartrees |
| Energy at 0K | -79.260591 |
| Energy at 298.15K | |
| HF Energy | -79.260591 |
| Nuclear repulsion energy | 42.300455 |
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 HF/aug-cc-pVQZ
| 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' |
3173 |
2883 |
0.00 |
|
|
|
| 2 |
A1' |
1562 |
1419 |
0.00 |
|
|
|
| 3 |
A1' |
1047 |
951 |
0.00 |
|
|
|
| 4 |
A1" |
321i |
291i |
0.00 |
|
|
|
| 5 |
A2" |
3160 |
2871 |
77.15 |
|
|
|
| 6 |
A2" |
1519 |
1380 |
0.06 |
|
|
|
| 7 |
E' |
3230 |
2935 |
85.03 |
|
|
|
| 7 |
E' |
3230 |
2935 |
85.03 |
|
|
|
| 8 |
E' |
1624 |
1476 |
9.15 |
|
|
|
| 8 |
E' |
1624 |
1476 |
9.15 |
|
|
|
| 9 |
E' |
958 |
870 |
1.78 |
|
|
|
| 9 |
E' |
958 |
870 |
1.78 |
|
|
|
| 10 |
E" |
3203 |
2910 |
0.00 |
|
|
|
| 10 |
E" |
3203 |
2910 |
0.00 |
|
|
|
| 11 |
E" |
1613 |
1465 |
0.00 |
|
|
|
| 11 |
E" |
1613 |
1465 |
0.00 |
|
|
|
| 12 |
E" |
1277 |
1160 |
0.00 |
|
|
|
| 12 |
E" |
1277 |
1160 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16974.8 cm
-1
Scaled (by 0.9085) Zero Point Vibrational Energy (zpe) 15421.6 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 HF/aug-cc-pVQZ
Point Group is D3h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.769 |
| C2 |
0.000 |
0.000 |
-0.769 |
| H3 |
0.000 |
1.006 |
1.168 |
| H4 |
-0.871 |
-0.503 |
1.168 |
| H5 |
0.871 |
-0.503 |
1.168 |
| H6 |
0.000 |
1.006 |
-1.168 |
| H7 |
0.871 |
-0.503 |
-1.168 |
| H8 |
-0.871 |
-0.503 |
-1.168 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5385 | 1.0824 | 1.0824 | 1.0824 | 2.1831 | 2.1831 | 2.1831 |
C2 | 1.5385 | | 2.1831 | 2.1831 | 2.1831 | 1.0824 | 1.0824 | 1.0824 | H3 | 1.0824 | 2.1831 | | 1.7428 | 1.7428 | 2.3362 | 2.9146 | 2.9146 | H4 | 1.0824 | 2.1831 | 1.7428 | | 1.7428 | 2.9146 | 2.9146 | 2.3362 | H5 | 1.0824 | 2.1831 | 1.7428 | 1.7428 | | 2.9146 | 2.3362 | 2.9146 | H6 | 2.1831 | 1.0824 | 2.3362 | 2.9146 | 2.9146 | | 1.7428 | 1.7428 | H7 | 2.1831 | 1.0824 | 2.9146 | 2.9146 | 2.3362 | 1.7428 | | 1.7428 | H8 | 2.1831 | 1.0824 | 2.9146 | 2.3362 | 2.9146 | 1.7428 | 1.7428 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.623 |
|
C1 |
C2 |
H7 |
111.623 |
| C1 |
C2 |
H8 |
111.623 |
|
C2 |
C1 |
H3 |
111.623 |
| C2 |
C1 |
H4 |
111.623 |
|
C2 |
C1 |
H5 |
111.623 |
| H3 |
C1 |
H4 |
107.237 |
|
H3 |
C1 |
H5 |
107.237 |
| H4 |
C1 |
H5 |
107.237 |
|
H6 |
C2 |
H7 |
107.237 |
| H6 |
C2 |
H8 |
107.237 |
|
H7 |
C2 |
H8 |
107.237 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/aug-cc-pVQZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.739 |
|
|
|
| 2 |
C |
-0.739 |
|
|
|
| 3 |
H |
0.246 |
|
|
|
| 4 |
H |
0.246 |
|
|
|
| 5 |
H |
0.246 |
|
|
|
| 6 |
H |
0.246 |
|
|
|
| 7 |
H |
0.246 |
|
|
|
| 8 |
H |
0.246 |
|
|
|
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 |
-14.864 |
0.000 |
0.000 |
| y |
0.000 |
-14.864 |
0.000 |
| z |
0.000 |
0.000 |
-15.637 |
|
| Traceless |
| | x | y | z |
| x |
0.386 |
0.000 |
0.000 |
| y |
0.000 |
0.386 |
0.000 |
| z |
0.000 |
0.000 |
-0.773 |
|
| Polar |
| 3z2-r2 | -1.546 |
| 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 |
3.802 |
0.000 |
0.000 |
| y |
0.000 |
3.802 |
0.000 |
| z |
0.000 |
0.000 |
4.371 |
<r2> (average value of r
2) Å
2
| <r2> |
30.807 |
| (<r2>)1/2 |
5.550 |