Jump to
S1C2
Energy calculated at wB97X-D/6-311G**
| | hartrees |
| Energy at 0K | -154.659056 |
| Energy at 298.15K | -154.662199 |
| HF Energy | -154.659056 |
| Nuclear repulsion energy | 99.067159 |
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/6-311G**
| 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 |
3277 |
3134 |
0.00 |
|
|
|
| 2 |
Ag |
1663 |
1591 |
0.00 |
|
|
|
| 3 |
Ag |
1137 |
1087 |
0.00 |
|
|
|
| 4 |
Ag |
977 |
934 |
0.00 |
|
|
|
| 5 |
Au |
913 |
873 |
0.00 |
|
|
|
| 6 |
Au |
544 |
520 |
0.00 |
|
|
|
| 7 |
B1g |
914 |
874 |
0.00 |
|
|
|
| 8 |
B1u |
3265 |
3123 |
20.33 |
|
|
|
| 9 |
B1u |
1671 |
1598 |
3.27 |
|
|
|
| 10 |
B1u |
1074 |
1028 |
0.55 |
|
|
|
| 11 |
B2g |
622 |
595 |
0.00 |
|
|
|
| 12 |
B2u |
3242 |
3101 |
11.39 |
|
|
|
| 13 |
B2u |
1283 |
1227 |
40.96 |
|
|
|
| 14 |
B2u |
740 |
707 |
9.97 |
|
|
|
| 15 |
B3g |
3227 |
3087 |
0.00 |
|
|
|
| 16 |
B3g |
1206 |
1153 |
0.00 |
|
|
|
| 17 |
B3g |
856 |
819 |
0.00 |
|
|
|
| 18 |
B3u |
608 |
582 |
146.76 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13608.1 cm
-1
Scaled (by 0.9565) Zero Point Vibrational Energy (zpe) 13016.1 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/6-311G**
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.665 |
0.786 |
| C2 |
0.000 |
0.665 |
-0.786 |
| C3 |
0.000 |
-0.665 |
0.786 |
| C4 |
0.000 |
-0.665 |
-0.786 |
| H5 |
0.000 |
1.433 |
1.547 |
| H6 |
0.000 |
1.433 |
-1.547 |
| H7 |
0.000 |
-1.433 |
1.547 |
| H8 |
0.000 |
-1.433 |
-1.547 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5715 | 1.3295 | 2.0584 | 1.0814 | 2.4561 | 2.2314 | 3.1372 |
C2 | 1.5715 | | 2.0584 | 1.3295 | 2.4561 | 1.0814 | 3.1372 | 2.2314 | C3 | 1.3295 | 2.0584 | | 1.5715 | 2.2314 | 3.1372 | 1.0814 | 2.4561 | C4 | 2.0584 | 1.3295 | 1.5715 | | 3.1372 | 2.2314 | 2.4561 | 1.0814 | H5 | 1.0814 | 2.4561 | 2.2314 | 3.1372 | | 3.0943 | 2.8654 | 4.2173 | H6 | 2.4561 | 1.0814 | 3.1372 | 2.2314 | 3.0943 | | 4.2173 | 2.8654 | H7 | 2.2314 | 3.1372 | 1.0814 | 2.4561 | 2.8654 | 4.2173 | | 3.0943 | H8 | 3.1372 | 2.2314 | 2.4561 | 1.0814 | 4.2173 | 2.8654 | 3.0943 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C4 |
90.000 |
|
C1 |
C2 |
H6 |
134.755 |
| C1 |
C3 |
C4 |
90.000 |
|
C1 |
C3 |
H7 |
135.245 |
| C2 |
C1 |
C3 |
90.000 |
|
C2 |
C1 |
H5 |
134.755 |
| C2 |
C4 |
C3 |
90.000 |
|
C3 |
C1 |
H5 |
135.245 |
| C4 |
C2 |
H6 |
135.245 |
|
C4 |
C3 |
H7 |
134.755 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.109 |
|
|
|
| 2 |
C |
-0.109 |
|
|
|
| 3 |
C |
-0.109 |
|
|
|
| 4 |
C |
-0.109 |
|
|
|
| 5 |
H |
0.109 |
|
|
|
| 6 |
H |
0.109 |
|
|
|
| 7 |
H |
0.109 |
|
|
|
| 8 |
H |
0.109 |
|
|
|
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 |
-26.625 |
0.000 |
0.000 |
| y |
0.000 |
-20.635 |
0.000 |
| z |
0.000 |
0.000 |
-21.788 |
|
| Traceless |
| | x | y | z |
| x |
-5.413 |
0.000 |
0.000 |
| y |
0.000 |
3.572 |
0.000 |
| z |
0.000 |
0.000 |
1.842 |
|
| Polar |
| 3z2-r2 | 3.684 |
| x2-y2 | -5.990 |
| 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 |
3.022 |
0.000 |
0.000 |
| y |
0.000 |
7.295 |
0.000 |
| z |
0.000 |
0.000 |
5.782 |
<r2> (average value of r
2) Å
2
| <r2> |
57.554 |
| (<r2>)1/2 |
7.586 |
Jump to
S1C1
Energy calculated at wB97X-D/6-311G**
| | hartrees |
| Energy at 0K | -154.599414 |
| Energy at 298.15K | |
| HF Energy | -154.599414 |
| Nuclear repulsion energy | 99.777137 |
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/6-311G**
| 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 |
3354 |
3208 |
0.00 |
|
|
|
| 2 |
Ag |
3152 |
3015 |
0.00 |
|
|
|
| 3 |
Ag |
1318 |
1261 |
0.00 |
|
|
|
| 4 |
Ag |
959 |
918 |
0.00 |
|
|
|
| 5 |
B1g |
1120 |
1072 |
0.00 |
|
|
|
| 6 |
B1u |
3344 |
3199 |
14.69 |
|
|
|
| 7 |
B1u |
1485 |
1420 |
79.24 |
|
|
|
| 8 |
B1u |
982 |
939 |
156.12 |
|
|
|
| 9 |
B2g |
461i |
441i |
0.00 |
|
|
|
| 10 |
B2u |
3157 |
3020 |
66.73 |
|
|
|
| 11 |
B2u |
1316 |
1259 |
153.89 |
|
|
|
| 12 |
B2u |
962 |
920 |
1.90 |
|
|
|
| 13 |
B3g |
2605 |
2492 |
0.00 |
|
|
|
| 14 |
B3g |
1204 |
1152 |
0.00 |
|
|
|
| 15 |
B3g |
1028 |
984 |
0.00 |
|
|
|
| 16 |
B3u |
951 |
910 |
1.83 |
|
|
|
| 17 |
B3u |
528 |
505 |
97.04 |
|
|
|
| 18 |
B3u |
459i |
439i |
171.85 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13273.3 cm
-1
Scaled (by 0.9565) Zero Point Vibrational Energy (zpe) 12695.9 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 wB97X-D/6-311G**
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
1.067 |
| C2 |
0.000 |
0.954 |
0.000 |
| C3 |
0.000 |
-0.954 |
0.000 |
| C4 |
0.000 |
0.000 |
-1.067 |
| H5 |
0.000 |
0.000 |
2.143 |
| H6 |
0.000 |
2.038 |
0.000 |
| H7 |
0.000 |
-2.038 |
0.000 |
| H8 |
0.000 |
0.000 |
-2.143 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.4316 | 1.4316 | 2.1349 | 1.0759 | 2.3009 | 2.3009 | 3.2108 |
C2 | 1.4316 | | 1.9078 | 1.4316 | 2.3460 | 1.0844 | 2.9923 | 2.3460 | C3 | 1.4316 | 1.9078 | | 1.4316 | 2.3460 | 2.9923 | 1.0844 | 2.3460 | C4 | 2.1349 | 1.4316 | 1.4316 | | 3.2108 | 2.3009 | 2.3009 | 1.0759 | H5 | 1.0759 | 2.3460 | 2.3460 | 3.2108 | | 2.9578 | 2.9578 | 4.2867 | H6 | 2.3009 | 1.0844 | 2.9923 | 2.3009 | 2.9578 | | 4.0767 | 2.9578 | H7 | 2.3009 | 2.9923 | 1.0844 | 2.3009 | 2.9578 | 4.0767 | | 2.9578 | H8 | 3.2108 | 2.3460 | 2.3460 | 1.0759 | 4.2867 | 2.9578 | 2.9578 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C4 |
96.430 |
|
C1 |
C2 |
H6 |
131.785 |
| C1 |
C3 |
C4 |
96.430 |
|
C1 |
C3 |
H7 |
131.785 |
| C2 |
C1 |
C3 |
83.570 |
|
C2 |
C1 |
H5 |
138.215 |
| C2 |
C4 |
C3 |
83.570 |
|
C3 |
C1 |
H5 |
138.215 |
| C4 |
C2 |
H6 |
131.785 |
|
C4 |
C3 |
H7 |
131.785 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.331 |
|
|
|
| 2 |
C |
0.108 |
|
|
|
| 3 |
C |
0.108 |
|
|
|
| 4 |
C |
-0.331 |
|
|
|
| 5 |
H |
0.098 |
|
|
|
| 6 |
H |
0.125 |
|
|
|
| 7 |
H |
0.125 |
|
|
|
| 8 |
H |
0.098 |
|
|
|
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 |
-27.053 |
0.000 |
0.000 |
| y |
0.000 |
-18.253 |
0.000 |
| z |
0.000 |
0.000 |
-24.878 |
|
| Traceless |
| | x | y | z |
| x |
-5.488 |
0.000 |
0.000 |
| y |
0.000 |
7.713 |
0.000 |
| z |
0.000 |
0.000 |
-2.225 |
|
| Polar |
| 3z2-r2 | -4.450 |
| x2-y2 | -8.800 |
| 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 |
3.156 |
0.000 |
0.000 |
| y |
0.000 |
6.780 |
0.000 |
| z |
0.000 |
0.000 |
7.713 |
<r2> (average value of r
2) Å
2
| <r2> |
56.791 |
| (<r2>)1/2 |
7.536 |