Jump to
S1C2
Energy calculated at wB97X-D/cc-pVDZ
| | hartrees |
| Energy at 0K | -154.633086 |
| Energy at 298.15K | -154.636224 |
| HF Energy | -154.633086 |
| Nuclear repulsion energy | 98.915875 |
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-pVDZ
| 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 |
3302 |
3146 |
0.00 |
|
|
|
| 2 |
Ag |
1666 |
1587 |
0.00 |
|
|
|
| 3 |
Ag |
1145 |
1091 |
0.00 |
|
|
|
| 4 |
Ag |
983 |
937 |
0.00 |
|
|
|
| 5 |
Au |
900 |
857 |
0.00 |
|
|
|
| 6 |
Au |
538 |
512 |
0.00 |
|
|
|
| 7 |
B1g |
905 |
862 |
0.00 |
|
|
|
| 8 |
B1u |
3291 |
3135 |
19.16 |
|
|
|
| 9 |
B1u |
1678 |
1598 |
7.68 |
|
|
|
| 10 |
B1u |
1085 |
1033 |
0.99 |
|
|
|
| 11 |
B2g |
617 |
587 |
0.00 |
|
|
|
| 12 |
B2u |
3269 |
3115 |
10.70 |
|
|
|
| 13 |
B2u |
1295 |
1233 |
41.45 |
|
|
|
| 14 |
B2u |
749 |
713 |
9.14 |
|
|
|
| 15 |
B3g |
3255 |
3101 |
0.00 |
|
|
|
| 16 |
B3g |
1216 |
1159 |
0.00 |
|
|
|
| 17 |
B3g |
854 |
814 |
0.00 |
|
|
|
| 18 |
B3u |
609 |
580 |
174.25 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13678.0 cm
-1
Scaled (by 0.9526) Zero Point Vibrational Energy (zpe) 13029.7 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-pVDZ
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.668 |
0.785 |
| C2 |
0.000 |
0.668 |
-0.785 |
| C3 |
0.000 |
-0.668 |
0.785 |
| C4 |
0.000 |
-0.668 |
-0.785 |
| 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 | | 1.5703 | 1.3354 | 2.0614 | 1.0831 | 2.4562 | 2.2387 | 3.1419 |
C2 | 1.5703 | | 2.0614 | 1.3354 | 2.4562 | 1.0831 | 3.1419 | 2.2387 | C3 | 1.3354 | 2.0614 | | 1.5703 | 2.2387 | 3.1419 | 1.0831 | 2.4562 | C4 | 2.0614 | 1.3354 | 1.5703 | | 3.1419 | 2.2387 | 2.4562 | 1.0831 | H5 | 1.0831 | 2.4562 | 2.2387 | 3.1419 | | 3.0947 | 2.8745 | 4.2237 | H6 | 2.4562 | 1.0831 | 3.1419 | 2.2387 | 3.0947 | | 4.2237 | 2.8745 | H7 | 2.2387 | 3.1419 | 1.0831 | 2.4562 | 2.8745 | 4.2237 | | 3.0947 | H8 | 3.1419 | 2.2387 | 2.4562 | 1.0831 | 4.2237 | 2.8745 | 3.0947 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C4 |
90.000 |
|
C1 |
C2 |
H6 |
134.724 |
| C1 |
C3 |
C4 |
90.000 |
|
C1 |
C3 |
H7 |
135.276 |
| C2 |
C1 |
C3 |
90.000 |
|
C2 |
C1 |
H5 |
134.724 |
| C2 |
C4 |
C3 |
90.000 |
|
C3 |
C1 |
H5 |
135.276 |
| C4 |
C2 |
H6 |
135.276 |
|
C4 |
C3 |
H7 |
134.724 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.161 |
|
|
|
| 2 |
C |
-0.161 |
|
|
|
| 3 |
C |
-0.161 |
|
|
|
| 4 |
C |
-0.161 |
|
|
|
| 5 |
H |
0.161 |
|
|
|
| 6 |
H |
0.161 |
|
|
|
| 7 |
H |
0.161 |
|
|
|
| 8 |
H |
0.161 |
|
|
|
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 |
-27.138 |
0.000 |
0.000 |
| y |
0.000 |
-20.675 |
0.000 |
| z |
0.000 |
0.000 |
-22.241 |
|
| Traceless |
| | x | y | z |
| x |
-5.680 |
0.000 |
0.000 |
| y |
0.000 |
4.014 |
0.000 |
| z |
0.000 |
0.000 |
1.666 |
|
| Polar |
| 3z2-r2 | 3.332 |
| x2-y2 | -6.463 |
| 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 |
4.337 |
0.000 |
0.000 |
| y |
0.000 |
7.677 |
0.000 |
| z |
0.000 |
0.000 |
6.105 |
<r2> (average value of r
2) Å
2
| <r2> |
57.866 |
| (<r2>)1/2 |
7.607 |
Jump to
S1C1
Energy calculated at wB97X-D/cc-pVDZ
| | hartrees |
| Energy at 0K | -154.575727 |
| Energy at 298.15K | |
| HF Energy | -154.575727 |
| Nuclear repulsion energy | 99.639396 |
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-pVDZ
| 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 |
3374 |
3214 |
0.00 |
|
|
|
| 2 |
Ag |
3182 |
3031 |
0.00 |
|
|
|
| 3 |
Ag |
1323 |
1261 |
0.00 |
|
|
|
| 4 |
Ag |
958 |
912 |
0.00 |
|
|
|
| 5 |
B1g |
1112 |
1059 |
0.00 |
|
|
|
| 6 |
B1u |
3366 |
3206 |
18.99 |
|
|
|
| 7 |
B1u |
1488 |
1417 |
124.90 |
|
|
|
| 8 |
B1u |
989 |
942 |
186.33 |
|
|
|
| 9 |
B2g |
436i |
415i |
0.00 |
|
|
|
| 10 |
B2u |
3188 |
3037 |
59.71 |
|
|
|
| 11 |
B2u |
1330 |
1267 |
164.68 |
|
|
|
| 12 |
B2u |
971 |
925 |
1.58 |
|
|
|
| 13 |
B3g |
2563 |
2442 |
0.00 |
|
|
|
| 14 |
B3g |
1214 |
1156 |
0.00 |
|
|
|
| 15 |
B3g |
1039 |
989 |
0.00 |
|
|
|
| 16 |
B3u |
939 |
894 |
0.21 |
|
|
|
| 17 |
B3u |
525 |
500 |
149.46 |
|
|
|
| 18 |
B3u |
449i |
428i |
181.54 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13336.4 cm
-1
Scaled (by 0.9526) Zero Point Vibrational Energy (zpe) 12704.3 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/cc-pVDZ
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
1.069 |
| C2 |
0.000 |
0.957 |
0.000 |
| C3 |
0.000 |
-0.957 |
0.000 |
| C4 |
0.000 |
0.000 |
-1.069 |
| H5 |
0.000 |
0.000 |
2.147 |
| H6 |
0.000 |
2.042 |
0.000 |
| H7 |
0.000 |
-2.042 |
0.000 |
| H8 |
0.000 |
0.000 |
-2.147 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.4342 | 1.4342 | 2.1371 | 1.0780 | 2.3047 | 2.3047 | 3.2150 |
C2 | 1.4342 | | 1.9133 | 1.4342 | 2.3500 | 1.0854 | 2.9987 | 2.3500 | C3 | 1.4342 | 1.9133 | | 1.4342 | 2.3500 | 2.9987 | 1.0854 | 2.3500 | C4 | 2.1371 | 1.4342 | 1.4342 | | 3.2150 | 2.3047 | 2.3047 | 1.0780 | H5 | 1.0780 | 2.3500 | 2.3500 | 3.2150 | | 2.9627 | 2.9627 | 4.2930 | H6 | 2.3047 | 1.0854 | 2.9987 | 2.3047 | 2.9627 | | 4.0841 | 2.9627 | H7 | 2.3047 | 2.9987 | 1.0854 | 2.3047 | 2.9627 | 4.0841 | | 2.9627 | H8 | 3.2150 | 2.3500 | 2.3500 | 1.0780 | 4.2930 | 2.9627 | 2.9627 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C4 |
96.325 |
|
C1 |
C2 |
H6 |
131.838 |
| C1 |
C3 |
C4 |
96.325 |
|
C1 |
C3 |
H7 |
131.838 |
| C2 |
C1 |
C3 |
83.675 |
|
C2 |
C1 |
H5 |
138.162 |
| C2 |
C4 |
C3 |
83.675 |
|
C3 |
C1 |
H5 |
138.162 |
| C4 |
C2 |
H6 |
131.838 |
|
C4 |
C3 |
H7 |
131.838 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.553 |
|
|
|
| 2 |
C |
0.219 |
|
|
|
| 3 |
C |
0.219 |
|
|
|
| 4 |
C |
-0.553 |
|
|
|
| 5 |
H |
0.165 |
|
|
|
| 6 |
H |
0.169 |
|
|
|
| 7 |
H |
0.169 |
|
|
|
| 8 |
H |
0.165 |
|
|
|
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 |
-28.086 |
0.000 |
0.000 |
| y |
0.000 |
-18.347 |
0.000 |
| z |
0.000 |
0.000 |
-25.809 |
|
| Traceless |
| | x | y | z |
| x |
-6.008 |
0.000 |
0.000 |
| y |
0.000 |
8.601 |
0.000 |
| z |
0.000 |
0.000 |
-2.593 |
|
| Polar |
| 3z2-r2 | -5.185 |
| x2-y2 | -9.739 |
| 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 |
5.232 |
0.000 |
0.000 |
| y |
0.000 |
6.881 |
0.000 |
| z |
0.000 |
0.000 |
9.457 |
<r2> (average value of r
2) Å
2
| <r2> |
57.335 |
| (<r2>)1/2 |
7.572 |