Jump to
S1C2
Energy calculated at wB97X-D/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -193.459344 |
| Energy at 298.15K | -193.463484 |
| HF Energy | -193.459344 |
| Nuclear repulsion energy | 149.447224 |
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/aug-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 |
A1 |
3268 |
3126 |
0.17 |
|
|
|
| 2 |
A1 |
3239 |
3099 |
18.17 |
|
|
|
| 3 |
A1 |
3230 |
3090 |
2.30 |
|
|
|
| 4 |
A1 |
1515 |
1449 |
15.72 |
|
|
|
| 5 |
A1 |
1392 |
1332 |
30.42 |
|
|
|
| 6 |
A1 |
1149 |
1099 |
0.02 |
|
|
|
| 7 |
A1 |
1059 |
1013 |
0.31 |
|
|
|
| 8 |
A1 |
949 |
908 |
0.97 |
|
|
|
| 9 |
A1 |
847 |
810 |
0.44 |
|
|
|
| 10 |
A2 |
927 |
887 |
0.00 |
|
|
|
| 11 |
A2 |
731 |
699 |
0.00 |
|
|
|
| 12 |
A2 |
523 |
500 |
0.00 |
|
|
|
| 13 |
B1 |
912 |
873 |
3.15 |
|
|
|
| 14 |
B1 |
827 |
791 |
5.36 |
|
|
|
| 15 |
B1 |
686 |
656 |
114.27 |
|
|
|
| 16 |
B1 |
497 |
475 |
11.83 |
|
|
|
| 17 |
B2 |
3260 |
3119 |
6.64 |
|
|
|
| 18 |
B2 |
3227 |
3087 |
1.24 |
|
|
|
| 19 |
B2 |
1549 |
1482 |
1.78 |
|
|
|
| 20 |
B2 |
1289 |
1233 |
0.04 |
|
|
|
| 21 |
B2 |
1216 |
1163 |
0.18 |
|
|
|
| 22 |
B2 |
1070 |
1023 |
17.03 |
|
|
|
| 23 |
B2 |
922 |
882 |
4.39 |
|
|
|
| 24 |
B2 |
109 |
105 |
4.14 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17195.1 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 16448.9 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/aug-cc-pVTZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
1.185 |
| C2 |
0.000 |
1.164 |
0.350 |
| C3 |
0.000 |
0.736 |
-0.942 |
| C4 |
0.000 |
-0.736 |
-0.942 |
| C5 |
0.000 |
-1.164 |
0.350 |
| H6 |
0.000 |
0.000 |
2.265 |
| H7 |
0.000 |
2.183 |
0.697 |
| H8 |
0.000 |
1.350 |
-1.829 |
| H9 |
0.000 |
-1.350 |
-1.829 |
| H10 |
0.000 |
-2.183 |
0.697 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
C5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.4328 | 2.2503 | 2.2503 | 1.4328 | 1.0804 | 2.2371 | 3.3028 | 3.3028 | 2.2371 |
C2 | 1.4328 | | 1.3608 | 2.2974 | 2.3285 | 2.2415 | 1.0768 | 2.1870 | 3.3274 | 3.3656 | C3 | 2.2503 | 1.3608 | | 1.4715 | 2.2974 | 3.2904 | 2.1871 | 1.0795 | 2.2670 | 3.3480 | C4 | 2.2503 | 2.2974 | 1.4715 | | 1.3608 | 3.2904 | 3.3480 | 2.2670 | 1.0795 | 2.1871 | C5 | 1.4328 | 2.3285 | 2.2974 | 1.3608 | | 2.2415 | 3.3656 | 3.3274 | 2.1870 | 1.0768 | H6 | 1.0804 | 2.2415 | 3.2904 | 3.2904 | 2.2415 | | 2.6879 | 4.3114 | 4.3114 | 2.6879 | H7 | 2.2371 | 1.0768 | 2.1871 | 3.3480 | 3.3656 | 2.6879 | | 2.6606 | 4.3442 | 4.3668 | H8 | 3.3028 | 2.1870 | 1.0795 | 2.2670 | 3.3274 | 4.3114 | 2.6606 | | 2.7006 | 4.3442 | H9 | 3.3028 | 3.3274 | 2.2670 | 1.0795 | 2.1870 | 4.3114 | 4.3442 | 2.7006 | | 2.6606 | H10 | 2.2371 | 3.3656 | 3.3480 | 2.1871 | 1.0768 | 2.6879 | 4.3668 | 4.3442 | 2.6606 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
107.296 |
|
C1 |
C2 |
H7 |
125.506 |
| C1 |
C5 |
C4 |
107.296 |
|
C1 |
C5 |
H10 |
125.506 |
| C2 |
C1 |
C5 |
108.699 |
|
C2 |
C1 |
H6 |
125.650 |
| C2 |
C3 |
C4 |
108.354 |
|
C2 |
C3 |
H8 |
126.943 |
| C3 |
C2 |
H7 |
127.198 |
|
C3 |
C4 |
C5 |
108.354 |
| C3 |
C4 |
H9 |
124.702 |
|
C4 |
C3 |
H8 |
124.702 |
| C4 |
C5 |
H10 |
127.198 |
|
C5 |
C1 |
H6 |
125.650 |
| C5 |
C4 |
H9 |
126.943 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.352 |
|
|
|
| 2 |
C |
-0.585 |
|
|
|
| 3 |
C |
-0.401 |
|
|
|
| 4 |
C |
-0.401 |
|
|
|
| 5 |
C |
-0.585 |
|
|
|
| 6 |
H |
0.447 |
|
|
|
| 7 |
H |
0.474 |
|
|
|
| 8 |
H |
0.464 |
|
|
|
| 9 |
H |
0.464 |
|
|
|
| 10 |
H |
0.474 |
|
|
|
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 |
0.071 |
0.071 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-33.279 |
0.000 |
0.000 |
| y |
0.000 |
-27.740 |
0.000 |
| z |
0.000 |
0.000 |
-25.524 |
|
| Traceless |
| | x | y | z |
| x |
-6.647 |
0.000 |
0.000 |
| y |
0.000 |
1.662 |
0.000 |
| z |
0.000 |
0.000 |
4.985 |
|
| Polar |
| 3z2-r2 | 9.971 |
| x2-y2 | -5.539 |
| 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 |
5.821 |
0.000 |
0.000 |
| y |
0.000 |
9.234 |
0.000 |
| z |
0.000 |
0.000 |
9.876 |
<r2> (average value of r
2) Å
2
| <r2> |
87.227 |
| (<r2>)1/2 |
9.340 |
Jump to
S1C1
Energy calculated at wB97X-D/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -193.459355 |
| Energy at 298.15K | |
| HF Energy | -193.459355 |
| Nuclear repulsion energy | 149.446709 |
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/aug-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 |
A1 |
3271 |
3129 |
0.66 |
|
|
|
| 2 |
A1 |
3261 |
3119 |
6.14 |
|
|
|
| 3 |
A1 |
3227 |
3087 |
1.06 |
|
|
|
| 4 |
A1 |
1593 |
1524 |
0.34 |
|
|
|
| 5 |
A1 |
1466 |
1402 |
2.73 |
|
|
|
| 6 |
A1 |
1149 |
1099 |
0.06 |
|
|
|
| 7 |
A1 |
1080 |
1034 |
8.80 |
|
|
|
| 8 |
A1 |
1038 |
993 |
12.65 |
|
|
|
| 9 |
A1 |
848 |
811 |
0.27 |
|
|
|
| 10 |
A2 |
942 |
901 |
0.00 |
|
|
|
| 11 |
A2 |
823 |
787 |
0.00 |
|
|
|
| 12 |
A2 |
527 |
504 |
0.00 |
|
|
|
| 13 |
B1 |
896 |
857 |
8.31 |
|
|
|
| 14 |
B1 |
739 |
707 |
5.54 |
|
|
|
| 15 |
B1 |
686 |
656 |
107.21 |
|
|
|
| 16 |
B1 |
489 |
468 |
13.35 |
|
|
|
| 17 |
B2 |
3242 |
3102 |
13.55 |
|
|
|
| 18 |
B2 |
3228 |
3088 |
7.40 |
|
|
|
| 19 |
B2 |
1401 |
1340 |
42.41 |
|
|
|
| 20 |
B2 |
1289 |
1233 |
0.01 |
|
|
|
| 21 |
B2 |
1213 |
1160 |
3.04 |
|
|
|
| 22 |
B2 |
964 |
923 |
0.05 |
|
|
|
| 23 |
B2 |
919 |
879 |
4.91 |
|
|
|
| 24 |
B2 |
54i |
52i |
12.25 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17117.1 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 16374.2 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/aug-cc-pVTZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
1.219 |
| C2 |
0.000 |
1.117 |
0.391 |
| C3 |
0.000 |
0.676 |
-1.001 |
| C4 |
0.000 |
-0.676 |
-1.001 |
| C5 |
0.000 |
-1.117 |
0.391 |
| H6 |
0.000 |
0.000 |
2.296 |
| H7 |
0.000 |
2.148 |
0.712 |
| H8 |
0.000 |
1.327 |
-1.859 |
| H9 |
0.000 |
-1.327 |
-1.859 |
| H10 |
0.000 |
-2.148 |
0.712 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
C5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.3900 | 2.3202 | 2.3202 | 1.3900 | 1.0767 | 2.2066 | 3.3520 | 3.3520 | 2.2066 |
C2 | 1.3900 | | 1.4600 | 2.2694 | 2.2333 | 2.2076 | 1.0800 | 2.2603 | 3.3219 | 3.2801 | C3 | 2.3202 | 1.4600 | | 1.3517 | 2.2694 | 3.3648 | 2.2587 | 1.0775 | 2.1789 | 3.3027 | C4 | 2.3202 | 2.2694 | 1.3517 | | 1.4600 | 3.3648 | 3.3027 | 2.1789 | 1.0775 | 2.2587 | C5 | 1.3900 | 2.2333 | 2.2694 | 1.4600 | | 2.2076 | 3.2801 | 3.3219 | 2.2603 | 1.0800 | H6 | 1.0767 | 2.2076 | 3.3648 | 3.3648 | 2.2076 | | 2.6681 | 4.3615 | 4.3615 | 2.6681 | H7 | 2.2066 | 1.0800 | 2.2587 | 3.3027 | 3.2801 | 2.6681 | | 2.6996 | 4.3228 | 4.2954 | H8 | 3.3520 | 2.2603 | 1.0775 | 2.1789 | 3.3219 | 4.3615 | 2.6996 | | 2.6537 | 4.3228 | H9 | 3.3520 | 3.3219 | 2.1789 | 1.0775 | 2.2603 | 4.3615 | 4.3228 | 2.6537 | | 2.6996 | H10 | 2.2066 | 3.2801 | 3.3027 | 2.2587 | 1.0800 | 2.6681 | 4.2954 | 4.3228 | 2.6996 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
108.974 |
|
C1 |
C2 |
H7 |
126.144 |
| C1 |
C5 |
C4 |
108.974 |
|
C1 |
C5 |
H10 |
126.144 |
| C2 |
C1 |
C5 |
106.906 |
|
C2 |
C1 |
H6 |
126.547 |
| C2 |
C3 |
C4 |
107.573 |
|
C2 |
C3 |
H8 |
125.255 |
| C3 |
C2 |
H7 |
124.882 |
|
C3 |
C4 |
C5 |
107.573 |
| C3 |
C4 |
H9 |
127.172 |
|
C4 |
C3 |
H8 |
127.172 |
| C4 |
C5 |
H10 |
124.882 |
|
C5 |
C1 |
H6 |
126.547 |
| C5 |
C4 |
H9 |
125.255 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.631 |
|
|
|
| 2 |
C |
-0.363 |
|
|
|
| 3 |
C |
-0.483 |
|
|
|
| 4 |
C |
-0.483 |
|
|
|
| 5 |
C |
-0.363 |
|
|
|
| 6 |
H |
0.472 |
|
|
|
| 7 |
H |
0.453 |
|
|
|
| 8 |
H |
0.472 |
|
|
|
| 9 |
H |
0.472 |
|
|
|
| 10 |
H |
0.453 |
|
|
|
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 |
0.048 |
0.048 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-33.280 |
0.000 |
0.000 |
| y |
0.000 |
-25.524 |
0.000 |
| z |
0.000 |
0.000 |
-27.739 |
|
| Traceless |
| | x | y | z |
| x |
-6.648 |
0.000 |
0.000 |
| y |
0.000 |
4.985 |
0.000 |
| z |
0.000 |
0.000 |
1.663 |
|
| Polar |
| 3z2-r2 | 3.326 |
| x2-y2 | -7.755 |
| 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 |
5.824 |
0.000 |
0.000 |
| y |
0.000 |
9.889 |
0.000 |
| z |
0.000 |
0.000 |
9.236 |
<r2> (average value of r
2) Å
2
| <r2> |
87.226 |
| (<r2>)1/2 |
9.339 |