Jump to
S1C2
Energy calculated at wB97X-D/cc-pVTZ
| | hartrees |
| Energy at 0K | -154.675062 |
| Energy at 298.15K | -154.678230 |
| HF Energy | -154.675062 |
| Nuclear repulsion energy | 99.271368 |
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/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 |
Ag |
3282 |
3137 |
0.00 |
|
|
|
| 2 |
Ag |
1663 |
1590 |
0.00 |
|
|
|
| 3 |
Ag |
1143 |
1093 |
0.00 |
|
|
|
| 4 |
Ag |
979 |
936 |
0.00 |
|
|
|
| 5 |
Au |
921 |
881 |
0.00 |
|
|
|
| 6 |
Au |
546 |
522 |
0.00 |
|
|
|
| 7 |
B1g |
923 |
883 |
0.00 |
|
|
|
| 8 |
B1u |
3270 |
3126 |
17.26 |
|
|
|
| 9 |
B1u |
1671 |
1598 |
4.08 |
|
|
|
| 10 |
B1u |
1087 |
1039 |
0.25 |
|
|
|
| 11 |
B2g |
632 |
604 |
0.00 |
|
|
|
| 12 |
B2u |
3248 |
3105 |
10.23 |
|
|
|
| 13 |
B2u |
1296 |
1239 |
41.20 |
|
|
|
| 14 |
B2u |
740 |
707 |
10.05 |
|
|
|
| 15 |
B3g |
3234 |
3091 |
0.00 |
|
|
|
| 16 |
B3g |
1222 |
1168 |
0.00 |
|
|
|
| 17 |
B3g |
858 |
820 |
0.00 |
|
|
|
| 18 |
B3u |
615 |
588 |
134.11 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13663.9 cm
-1
Scaled (by 0.956) Zero Point Vibrational Energy (zpe) 13062.7 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/cc-pVTZ
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.663 |
0.784 |
| C2 |
0.000 |
0.663 |
-0.784 |
| C3 |
0.000 |
-0.663 |
0.784 |
| C4 |
0.000 |
-0.663 |
-0.784 |
| H5 |
0.000 |
1.429 |
1.544 |
| H6 |
0.000 |
1.429 |
-1.544 |
| H7 |
0.000 |
-1.429 |
1.544 |
| H8 |
0.000 |
-1.429 |
-1.544 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5686 | 1.3262 | 2.0541 | 1.0788 | 2.4512 | 2.2257 | 3.1302 |
C2 | 1.5686 | | 2.0541 | 1.3262 | 2.4512 | 1.0788 | 3.1302 | 2.2257 | C3 | 1.3262 | 2.0541 | | 1.5686 | 2.2257 | 3.1302 | 1.0788 | 2.4512 | C4 | 2.0541 | 1.3262 | 1.5686 | | 3.1302 | 2.2257 | 2.4512 | 1.0788 | H5 | 1.0788 | 2.4512 | 2.2257 | 3.1302 | | 3.0885 | 2.8576 | 4.2077 | H6 | 2.4512 | 1.0788 | 3.1302 | 2.2257 | 3.0885 | | 4.2077 | 2.8576 | H7 | 2.2257 | 3.1302 | 1.0788 | 2.4512 | 2.8576 | 4.2077 | | 3.0885 | H8 | 3.1302 | 2.2257 | 2.4512 | 1.0788 | 4.2077 | 2.8576 | 3.0885 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C4 |
90.000 |
|
C1 |
C2 |
H6 |
134.784 |
| C1 |
C3 |
C4 |
90.000 |
|
C1 |
C3 |
H7 |
135.216 |
| C2 |
C1 |
C3 |
90.000 |
|
C2 |
C1 |
H5 |
134.784 |
| C2 |
C4 |
C3 |
90.000 |
|
C3 |
C1 |
H5 |
135.216 |
| C4 |
C2 |
H6 |
135.216 |
|
C4 |
C3 |
H7 |
134.784 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.116 |
|
|
|
| 2 |
C |
-0.116 |
|
|
|
| 3 |
C |
-0.116 |
|
|
|
| 4 |
C |
-0.116 |
|
|
|
| 5 |
H |
0.116 |
|
|
|
| 6 |
H |
0.116 |
|
|
|
| 7 |
H |
0.116 |
|
|
|
| 8 |
H |
0.116 |
|
|
|
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 |
-26.556 |
0.000 |
0.000 |
| y |
0.000 |
-20.620 |
0.000 |
| z |
0.000 |
0.000 |
-21.976 |
|
| Traceless |
| | x | y | z |
| x |
-5.258 |
0.000 |
0.000 |
| y |
0.000 |
3.646 |
0.000 |
| z |
0.000 |
0.000 |
1.612 |
|
| Polar |
| 3z2-r2 | 3.225 |
| x2-y2 | -5.936 |
| 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 |
3.736 |
0.000 |
0.000 |
| y |
0.000 |
7.448 |
0.000 |
| z |
0.000 |
0.000 |
6.224 |
<r2> (average value of r
2) Å
2
| <r2> |
57.400 |
| (<r2>)1/2 |
7.576 |
Jump to
S1C1
Energy calculated at wB97X-D/cc-pVTZ
| | hartrees |
| Energy at 0K | -154.616319 |
| Energy at 298.15K | |
| HF Energy | -154.616319 |
| Nuclear repulsion energy | 99.997826 |
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/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 |
Ag |
3357 |
3210 |
0.00 |
|
|
|
| 2 |
Ag |
3157 |
3018 |
0.00 |
|
|
|
| 3 |
Ag |
1315 |
1257 |
0.00 |
|
|
|
| 4 |
Ag |
959 |
916 |
0.00 |
|
|
|
| 5 |
B1g |
1118 |
1069 |
0.00 |
|
|
|
| 6 |
B1u |
3348 |
3201 |
15.56 |
|
|
|
| 7 |
B1u |
1478 |
1413 |
87.75 |
|
|
|
| 8 |
B1u |
980 |
937 |
162.30 |
|
|
|
| 9 |
B2g |
474i |
453i |
0.00 |
|
|
|
| 10 |
B2u |
3162 |
3023 |
58.47 |
|
|
|
| 11 |
B2u |
1318 |
1260 |
149.25 |
|
|
|
| 12 |
B2u |
959 |
917 |
2.42 |
|
|
|
| 13 |
B3g |
2638 |
2522 |
0.00 |
|
|
|
| 14 |
B3g |
1207 |
1154 |
0.00 |
|
|
|
| 15 |
B3g |
1028 |
983 |
0.00 |
|
|
|
| 16 |
B3u |
953 |
911 |
1.14 |
|
|
|
| 17 |
B3u |
521 |
498 |
99.21 |
|
|
|
| 18 |
B3u |
470i |
449i |
146.74 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13276.9 cm
-1
Scaled (by 0.956) Zero Point Vibrational Energy (zpe) 12692.7 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/cc-pVTZ
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.951 |
0.000 |
| C2 |
0.000 |
0.000 |
1.066 |
| C3 |
0.000 |
0.000 |
-1.066 |
| C4 |
0.000 |
-0.951 |
0.000 |
| H5 |
0.000 |
2.034 |
0.000 |
| H6 |
0.000 |
0.000 |
2.140 |
| H7 |
0.000 |
0.000 |
-2.140 |
| H8 |
0.000 |
-2.034 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.4290 | 1.4290 | 1.9028 | 1.0822 | 2.3419 | 2.3419 | 2.9850 |
C2 | 1.4290 | | 2.1326 | 1.4290 | 2.2962 | 1.0736 | 3.2062 | 2.2962 | C3 | 1.4290 | 2.1326 | | 1.4290 | 2.2962 | 3.2062 | 1.0736 | 2.2962 | C4 | 1.9028 | 1.4290 | 1.4290 | | 2.9850 | 2.3419 | 2.3419 | 1.0822 | H5 | 1.0822 | 2.2962 | 2.2962 | 2.9850 | | 2.9521 | 2.9521 | 4.0672 | H6 | 2.3419 | 1.0736 | 3.2062 | 2.3419 | 2.9521 | | 4.2798 | 2.9521 | H7 | 2.3419 | 3.2062 | 1.0736 | 2.3419 | 2.9521 | 4.2798 | | 2.9521 | H8 | 2.9850 | 2.2962 | 2.2962 | 1.0822 | 4.0672 | 2.9521 | 2.9521 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C4 |
83.480 |
|
C1 |
C2 |
H6 |
138.260 |
| C1 |
C3 |
C4 |
83.480 |
|
C1 |
C3 |
H7 |
138.260 |
| C2 |
C1 |
C3 |
96.520 |
|
C2 |
C1 |
H5 |
131.740 |
| C2 |
C4 |
C3 |
96.520 |
|
C3 |
C1 |
H5 |
131.740 |
| C4 |
C2 |
H6 |
138.260 |
|
C4 |
C3 |
H7 |
138.260 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.177 |
|
|
|
| 2 |
C |
-0.425 |
|
|
|
| 3 |
C |
-0.425 |
|
|
|
| 4 |
C |
0.177 |
|
|
|
| 5 |
H |
0.116 |
|
|
|
| 6 |
H |
0.133 |
|
|
|
| 7 |
H |
0.133 |
|
|
|
| 8 |
H |
0.116 |
|
|
|
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 |
-27.104 |
0.000 |
0.000 |
| y |
0.000 |
-18.281 |
0.000 |
| z |
0.000 |
0.000 |
-25.027 |
|
| Traceless |
| | x | y | z |
| x |
-5.450 |
0.000 |
0.000 |
| y |
0.000 |
7.784 |
0.000 |
| z |
0.000 |
0.000 |
-2.335 |
|
| Polar |
| 3z2-r2 | -4.670 |
| x2-y2 | -8.823 |
| 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 |
3.964 |
0.000 |
0.000 |
| y |
0.000 |
6.927 |
0.000 |
| z |
0.000 |
0.000 |
8.198 |
<r2> (average value of r
2) Å
2
| <r2> |
56.652 |
| (<r2>)1/2 |
7.527 |