Jump to
S1C2
Energy calculated at wB97X-D/6-31G*
| | hartrees |
| Energy at 0K | -154.619747 |
| Energy at 298.15K | -154.622856 |
| HF Energy | -154.619747 |
| Nuclear repulsion energy | |
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 wB97X-D/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 |
Ag |
3306 |
3136 |
0.00 |
|
|
|
| 2 |
Ag |
1682 |
1596 |
0.00 |
|
|
|
| 3 |
Ag |
1150 |
1091 |
0.00 |
|
|
|
| 4 |
Ag |
986 |
936 |
0.00 |
|
|
|
| 5 |
Au |
900 |
854 |
0.00 |
|
|
|
| 6 |
Au |
547 |
519 |
0.00 |
|
|
|
| 7 |
B1g |
882 |
837 |
0.00 |
|
|
|
| 8 |
B1u |
3295 |
3125 |
25.88 |
|
|
|
| 9 |
B1u |
1695 |
1608 |
2.64 |
|
|
|
| 10 |
B1u |
1090 |
1034 |
0.31 |
|
|
|
| 11 |
B2g |
613 |
581 |
0.00 |
|
|
|
| 12 |
B2u |
3273 |
3105 |
14.35 |
|
|
|
| 13 |
B2u |
1300 |
1233 |
37.11 |
|
|
|
| 14 |
B2u |
750 |
712 |
8.06 |
|
|
|
| 15 |
B3g |
3258 |
3090 |
0.00 |
|
|
|
| 16 |
B3g |
1214 |
1151 |
0.00 |
|
|
|
| 17 |
B3g |
853 |
809 |
0.00 |
|
|
|
| 18 |
B3u |
608 |
577 |
131.83 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13701.0 cm
-1
Scaled (by 0.9485) Zero Point Vibrational Energy (zpe) 12995.4 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 wB97X-D/6-31G*
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.666 |
0.786 |
| C2 |
0.000 |
0.666 |
-0.786 |
| C3 |
0.000 |
-0.666 |
0.786 |
| C4 |
0.000 |
-0.666 |
-0.786 |
| H5 |
0.000 |
1.437 |
1.547 |
| H6 |
0.000 |
1.437 |
-1.547 |
| H7 |
0.000 |
-1.437 |
1.547 |
| H8 |
0.000 |
-1.437 |
-1.547 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5714 | 1.3327 | 2.0604 | 1.0837 | 2.4570 | 2.2373 | 3.1414 |
C2 | 1.5714 | | 2.0604 | 1.3327 | 2.4570 | 1.0837 | 3.1414 | 2.2373 | C3 | 1.3327 | 2.0604 | | 1.5714 | 2.2373 | 3.1414 | 1.0837 | 2.4570 | C4 | 2.0604 | 1.3327 | 1.5714 | | 3.1414 | 2.2373 | 2.4570 | 1.0837 | H5 | 1.0837 | 2.4570 | 2.2373 | 3.1414 | | 3.0945 | 2.8747 | 4.2237 | H6 | 2.4570 | 1.0837 | 3.1414 | 2.2373 | 3.0945 | | 4.2237 | 2.8747 | H7 | 2.2373 | 3.1414 | 1.0837 | 2.4570 | 2.8747 | 4.2237 | | 3.0945 | H8 | 3.1414 | 2.2373 | 2.4570 | 1.0837 | 4.2237 | 2.8747 | 3.0945 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C4 |
90.000 |
|
C1 |
C2 |
H6 |
134.645 |
| C1 |
C3 |
C4 |
90.000 |
|
C1 |
C3 |
H7 |
135.355 |
| C2 |
C1 |
C3 |
90.000 |
|
C2 |
C1 |
H5 |
134.645 |
| C2 |
C4 |
C3 |
90.000 |
|
C3 |
C1 |
H5 |
135.355 |
| C4 |
C2 |
H6 |
135.355 |
|
C4 |
C3 |
H7 |
134.645 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.172 |
|
|
|
| 2 |
C |
-0.172 |
|
|
|
| 3 |
C |
-0.172 |
|
|
|
| 4 |
C |
-0.172 |
|
|
|
| 5 |
H |
0.172 |
|
|
|
| 6 |
H |
0.172 |
|
|
|
| 7 |
H |
0.172 |
|
|
|
| 8 |
H |
0.172 |
|
|
|
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 |
-26.005 |
0.000 |
0.000 |
| y |
0.000 |
-20.269 |
0.000 |
| z |
0.000 |
0.000 |
-21.357 |
|
| Traceless |
| | x | y | z |
| x |
-5.193 |
0.000 |
0.000 |
| y |
0.000 |
3.412 |
0.000 |
| z |
0.000 |
0.000 |
1.781 |
|
| Polar |
| 3z2-r2 | 3.561 |
| x2-y2 | -5.736 |
| 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 |
2.304 |
0.000 |
0.000 |
| y |
0.000 |
6.924 |
0.000 |
| z |
0.000 |
0.000 |
5.478 |
<r2> (average value of r
2) Å
2
| <r2> |
57.339 |
| (<r2>)1/2 |
7.572 |
Jump to
S1C1
Energy calculated at wB97X-D/6-31G*
| | hartrees |
| Energy at 0K | -154.559059 |
| Energy at 298.15K | |
| HF Energy | -154.559059 |
| Nuclear repulsion energy | |
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 wB97X-D/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 |
Ag |
3383 |
3208 |
0.00 |
|
|
|
| 2 |
Ag |
3181 |
3017 |
0.00 |
|
|
|
| 3 |
Ag |
1331 |
1262 |
0.00 |
|
|
|
| 4 |
Ag |
961 |
911 |
0.00 |
|
|
|
| 5 |
B1g |
1128 |
1070 |
0.00 |
|
|
|
| 6 |
B1u |
3374 |
3201 |
11.09 |
|
|
|
| 7 |
B1u |
1516 |
1438 |
68.84 |
|
|
|
| 8 |
B1u |
1000 |
949 |
132.48 |
|
|
|
| 9 |
B2g |
531i |
504i |
0.00 |
|
|
|
| 10 |
B2u |
3185 |
3021 |
81.00 |
|
|
|
| 11 |
B2u |
1333 |
1264 |
146.38 |
|
|
|
| 12 |
B2u |
974 |
924 |
1.57 |
|
|
|
| 13 |
B3g |
2582 |
2449 |
0.00 |
|
|
|
| 14 |
B3g |
1217 |
1155 |
0.00 |
|
|
|
| 15 |
B3g |
1042 |
988 |
0.00 |
|
|
|
| 16 |
B3u |
952 |
903 |
4.02 |
|
|
|
| 17 |
B3u |
523 |
496 |
79.65 |
|
|
|
| 18 |
B3u |
470i |
445i |
190.62 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13340.3 cm
-1
Scaled (by 0.9485) Zero Point Vibrational Energy (zpe) 12653.3 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 wB97X-D/6-31G*
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
1.068 |
| C2 |
0.000 |
0.954 |
0.000 |
| C3 |
0.000 |
-0.954 |
0.000 |
| C4 |
0.000 |
0.000 |
-1.068 |
| H5 |
0.000 |
0.000 |
2.146 |
| H6 |
0.000 |
2.040 |
0.000 |
| H7 |
0.000 |
-2.040 |
0.000 |
| H8 |
0.000 |
0.000 |
-2.146 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.4320 | 1.4320 | 2.1353 | 1.0781 | 2.3027 | 2.3027 | 3.2134 |
C2 | 1.4320 | | 1.9088 | 1.4320 | 2.3484 | 1.0859 | 2.9947 | 2.3484 | C3 | 1.4320 | 1.9088 | | 1.4320 | 2.3484 | 2.9947 | 1.0859 | 2.3484 | C4 | 2.1353 | 1.4320 | 1.4320 | | 3.2134 | 2.3027 | 2.3027 | 1.0781 | H5 | 1.0781 | 2.3484 | 2.3484 | 3.2134 | | 2.9609 | 2.9609 | 4.2914 | H6 | 2.3027 | 1.0859 | 2.9947 | 2.3027 | 2.9609 | | 4.0806 | 2.9609 | H7 | 2.3027 | 2.9947 | 1.0859 | 2.3027 | 2.9609 | 4.0806 | | 2.9609 | H8 | 3.2134 | 2.3484 | 2.3484 | 1.0781 | 4.2914 | 2.9609 | 2.9609 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C4 |
96.411 |
|
C1 |
C2 |
H6 |
131.794 |
| C1 |
C3 |
C4 |
96.411 |
|
C1 |
C3 |
H7 |
131.794 |
| C2 |
C1 |
C3 |
83.589 |
|
C2 |
C1 |
H5 |
138.206 |
| C2 |
C4 |
C3 |
83.589 |
|
C3 |
C1 |
H5 |
138.206 |
| C4 |
C2 |
H6 |
131.794 |
|
C4 |
C3 |
H7 |
131.794 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.330 |
|
|
|
| 2 |
C |
-0.018 |
|
|
|
| 3 |
C |
-0.018 |
|
|
|
| 4 |
C |
-0.330 |
|
|
|
| 5 |
H |
0.158 |
|
|
|
| 6 |
H |
0.190 |
|
|
|
| 7 |
H |
0.190 |
|
|
|
| 8 |
H |
0.158 |
|
|
|
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 |
-26.347 |
0.000 |
0.000 |
| y |
0.000 |
-18.075 |
0.000 |
| z |
0.000 |
0.000 |
-24.235 |
|
| Traceless |
| | x | y | z |
| x |
-5.192 |
0.000 |
0.000 |
| y |
0.000 |
7.216 |
0.000 |
| z |
0.000 |
0.000 |
-2.024 |
|
| Polar |
| 3z2-r2 | -4.048 |
| x2-y2 | -8.272 |
| 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 |
2.336 |
0.000 |
0.000 |
| y |
0.000 |
6.548 |
0.000 |
| z |
0.000 |
0.000 |
7.178 |
<r2> (average value of r
2) Å
2
| <r2> |
56.524 |
| (<r2>)1/2 |
7.518 |