Jump to
S1C2
Energy calculated at wB97X-D/6-311G**
| | hartrees |
| Energy at 0K | -270.850916 |
| Energy at 298.15K | |
| HF Energy | -270.850916 |
| Nuclear repulsion energy | 258.582971 |
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 |
A1 |
3207 |
3068 |
3.64 |
|
|
|
| 2 |
A1 |
3198 |
3059 |
40.11 |
|
|
|
| 3 |
A1 |
3182 |
3044 |
9.72 |
|
|
|
| 4 |
A1 |
3158 |
3021 |
4.52 |
|
|
|
| 5 |
A1 |
1688 |
1615 |
1.63 |
|
|
|
| 6 |
A1 |
1623 |
1553 |
13.10 |
|
|
|
| 7 |
A1 |
1483 |
1418 |
8.03 |
|
|
|
| 8 |
A1 |
1305 |
1248 |
0.58 |
|
|
|
| 9 |
A1 |
1256 |
1202 |
2.39 |
|
|
|
| 10 |
A1 |
974 |
932 |
2.65 |
|
|
|
| 11 |
A1 |
918 |
878 |
0.89 |
|
|
|
| 12 |
A1 |
852 |
815 |
0.21 |
|
|
|
| 13 |
A1 |
420 |
402 |
0.29 |
|
|
|
| 14 |
A2 |
1025 |
981 |
0.00 |
|
|
|
| 15 |
A2 |
1006 |
963 |
0.00 |
|
|
|
| 16 |
A2 |
768 |
735 |
0.00 |
|
|
|
| 17 |
A2 |
567 |
543 |
0.00 |
|
|
|
| 18 |
A2 |
290 |
277 |
0.00 |
|
|
|
| 19 |
B1 |
1003 |
959 |
0.09 |
|
|
|
| 20 |
B1 |
848 |
811 |
0.00 |
|
|
|
| 21 |
B1 |
759 |
726 |
1.29 |
|
|
|
| 22 |
B1 |
644 |
616 |
84.30 |
|
|
|
| 23 |
B1 |
518 |
495 |
43.67 |
|
|
|
| 24 |
B1 |
141 |
135 |
0.00 |
|
|
|
| 25 |
B2 |
3193 |
3054 |
49.21 |
|
|
|
| 26 |
B2 |
3168 |
3030 |
2.52 |
|
|
|
| 27 |
B2 |
3159 |
3022 |
5.72 |
|
|
|
| 28 |
B2 |
1569 |
1500 |
6.94 |
|
|
|
| 29 |
B2 |
1492 |
1427 |
3.74 |
|
|
|
| 30 |
B2 |
1418 |
1356 |
0.10 |
|
|
|
| 31 |
B2 |
1316 |
1259 |
0.10 |
|
|
|
| 32 |
B2 |
1199 |
1147 |
1.47 |
|
|
|
| 33 |
B2 |
978 |
935 |
5.67 |
|
|
|
| 34 |
B2 |
905 |
866 |
1.20 |
|
|
|
| 35 |
B2 |
446 |
427 |
0.26 |
|
|
|
| 36 |
B2 |
149i |
142i |
22.35 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 24764.2 cm
-1
Scaled (by 0.9565) Zero Point Vibrational Energy (zpe) 23687.0 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 C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
1.618 |
| C2 |
0.000 |
1.264 |
0.993 |
| C3 |
0.000 |
-1.264 |
0.993 |
| C4 |
0.000 |
1.585 |
-0.339 |
| C5 |
0.000 |
-1.585 |
-0.339 |
| C6 |
0.000 |
0.676 |
-1.464 |
| C7 |
0.000 |
-0.676 |
-1.464 |
| H8 |
0.000 |
0.000 |
2.702 |
| H9 |
0.000 |
2.112 |
1.674 |
| H10 |
0.000 |
-2.112 |
1.674 |
| H11 |
0.000 |
2.642 |
-0.583 |
| H12 |
0.000 |
-2.642 |
-0.583 |
| H13 |
0.000 |
1.158 |
-2.438 |
| H14 |
0.000 |
-1.158 |
-2.438 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
C5 |
C6 |
C7 |
H8 |
H9 |
H10 |
H11 |
H12 |
H13 |
H14 |
| C1 | | 1.4100 | 1.4100 | 2.5178 | 2.5178 | 3.1548 | 3.1548 | 1.0846 | 2.1127 | 2.1127 | 3.4383 | 3.4383 | 4.2176 | 4.2176 |
C2 | 1.4100 | | 2.5282 | 1.3696 | 3.1452 | 2.5261 | 3.1306 | 2.1259 | 1.0873 | 3.4440 | 2.0932 | 4.2120 | 3.4326 | 4.1995 | C3 | 1.4100 | 2.5282 | | 3.1452 | 1.3696 | 3.1306 | 2.5261 | 2.1259 | 3.4440 | 1.0873 | 4.2120 | 2.0932 | 4.1995 | 3.4326 | C4 | 2.5178 | 1.3696 | 3.1452 | | 3.1707 | 1.4467 | 2.5261 | 3.4291 | 2.0799 | 4.2094 | 1.0846 | 4.2345 | 2.1427 | 3.4542 | C5 | 2.5178 | 3.1452 | 1.3696 | 3.1707 | | 2.5261 | 1.4467 | 3.4291 | 4.2094 | 2.0799 | 4.2345 | 1.0846 | 3.4542 | 2.1427 | C6 | 3.1548 | 2.5261 | 3.1306 | 1.4467 | 2.5261 | | 1.3525 | 4.2205 | 3.4504 | 4.1974 | 2.1543 | 3.4334 | 1.0866 | 2.0765 | C7 | 3.1548 | 3.1306 | 2.5261 | 2.5261 | 1.4467 | 1.3525 | | 4.2205 | 4.1974 | 3.4504 | 3.4334 | 2.1543 | 2.0765 | 1.0866 | H8 | 1.0846 | 2.1259 | 2.1259 | 3.4291 | 3.4291 | 4.2205 | 4.2205 | | 2.3491 | 2.3491 | 4.2156 | 4.2156 | 5.2689 | 5.2689 | H9 | 2.1127 | 1.0873 | 3.4440 | 2.0799 | 4.2094 | 3.4504 | 4.1974 | 2.3491 | | 4.2239 | 2.3178 | 5.2624 | 4.2210 | 5.2532 | H10 | 2.1127 | 3.4440 | 1.0873 | 4.2094 | 2.0799 | 4.1974 | 3.4504 | 2.3491 | 4.2239 | | 5.2624 | 2.3178 | 5.2532 | 4.2210 | H11 | 3.4383 | 2.0932 | 4.2120 | 1.0846 | 4.2345 | 2.1543 | 3.4334 | 4.2156 | 2.3178 | 5.2624 | | 5.2843 | 2.3762 | 4.2285 | H12 | 3.4383 | 4.2120 | 2.0932 | 4.2345 | 1.0846 | 3.4334 | 2.1543 | 4.2156 | 5.2624 | 2.3178 | 5.2843 | | 4.2285 | 2.3762 | H13 | 4.2176 | 3.4326 | 4.1995 | 2.1427 | 3.4542 | 1.0866 | 2.0765 | 5.2689 | 4.2210 | 5.2532 | 2.3762 | 4.2285 | | 2.3151 | H14 | 4.2176 | 4.1995 | 3.4326 | 3.4542 | 2.1427 | 2.0765 | 1.0866 | 5.2689 | 5.2532 | 4.2210 | 4.2285 | 2.3762 | 2.3151 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
26.296 |
|
C1 |
C2 |
H9 |
114.944 |
| C1 |
C7 |
C6 |
77.622 |
|
C1 |
C7 |
H14 |
166.085 |
| C2 |
C1 |
C7 |
76.082 |
|
C2 |
C1 |
H8 |
116.296 |
| C2 |
C3 |
C4 |
25.045 |
|
C2 |
C3 |
H10 |
141.240 |
| C3 |
C2 |
H9 |
141.240 |
|
C3 |
C4 |
C5 |
25.045 |
| C3 |
C4 |
H11 |
167.968 |
|
C4 |
C3 |
H10 |
166.284 |
| C4 |
C5 |
C6 |
26.455 |
|
C4 |
C5 |
H12 |
166.987 |
| C5 |
C4 |
H11 |
166.987 |
|
C5 |
C6 |
C7 |
26.455 |
| C5 |
C6 |
H13 |
142.748 |
|
C6 |
C5 |
H12 |
140.532 |
| C6 |
C7 |
H14 |
116.293 |
|
C7 |
C1 |
H8 |
167.622 |
| C7 |
C6 |
H13 |
116.293 |
|
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 |
-0.169 |
|
|
|
| 2 |
C |
-0.070 |
|
|
|
| 3 |
C |
-0.070 |
|
|
|
| 4 |
C |
-0.148 |
|
|
|
| 5 |
C |
-0.148 |
|
|
|
| 6 |
C |
-0.103 |
|
|
|
| 7 |
C |
-0.103 |
|
|
|
| 8 |
H |
0.114 |
|
|
|
| 9 |
H |
0.117 |
|
|
|
| 10 |
H |
0.117 |
|
|
|
| 11 |
H |
0.115 |
|
|
|
| 12 |
H |
0.115 |
|
|
|
| 13 |
H |
0.117 |
|
|
|
| 14 |
H |
0.117 |
|
|
|
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 |
-0.067 |
0.067 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-46.313 |
0.000 |
0.000 |
| y |
0.000 |
-36.621 |
0.000 |
| z |
0.000 |
0.000 |
-36.626 |
|
| Traceless |
| | x | y | z |
| x |
-9.689 |
0.000 |
0.000 |
| y |
0.000 |
4.849 |
0.000 |
| z |
0.000 |
0.000 |
4.840 |
|
| Polar |
| 3z2-r2 | 9.681 |
| x2-y2 | -9.692 |
| 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 |
4.883 |
0.000 |
0.000 |
| y |
0.000 |
13.770 |
0.000 |
| z |
0.000 |
0.000 |
13.756 |
<r2> (average value of r
2) Å
2
| <r2> |
185.399 |
| (<r2>)1/2 |
13.616 |
Jump to
S1C1
Energy calculated at wB97X-D/6-311G**
| | hartrees |
| Energy at 0K | -270.850905 |
| Energy at 298.15K | |
| HF Energy | -270.850905 |
| Nuclear repulsion energy | 258.581792 |
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 |
A' |
3208 |
3068 |
0.00 |
|
|
|
| 2 |
A' |
3199 |
3060 |
48.22 |
|
|
|
| 3 |
A' |
3197 |
3058 |
39.03 |
|
|
|
| 4 |
A' |
3185 |
3047 |
10.39 |
|
|
|
| 5 |
A' |
3165 |
3028 |
7.49 |
|
|
|
| 6 |
A' |
3160 |
3022 |
1.85 |
|
|
|
| 7 |
A' |
3159 |
3021 |
8.28 |
|
|
|
| 8 |
A' |
1668 |
1596 |
9.29 |
|
|
|
| 9 |
A' |
1653 |
1581 |
1.86 |
|
|
|
| 10 |
A' |
1558 |
1490 |
10.34 |
|
|
|
| 11 |
A' |
1490 |
1426 |
4.05 |
|
|
|
| 12 |
A' |
1484 |
1420 |
7.49 |
|
|
|
| 13 |
A' |
1418 |
1356 |
0.10 |
|
|
|
| 14 |
A' |
1316 |
1259 |
0.13 |
|
|
|
| 15 |
A' |
1303 |
1247 |
0.90 |
|
|
|
| 16 |
A' |
1258 |
1203 |
1.33 |
|
|
|
| 17 |
A' |
1198 |
1146 |
2.38 |
|
|
|
| 18 |
A' |
981 |
938 |
5.51 |
|
|
|
| 19 |
A' |
971 |
929 |
2.96 |
|
|
|
| 20 |
A' |
918 |
878 |
0.84 |
|
|
|
| 21 |
A' |
905 |
865 |
1.15 |
|
|
|
| 22 |
A' |
852 |
815 |
0.21 |
|
|
|
| 23 |
A' |
446 |
427 |
0.24 |
|
|
|
| 24 |
A' |
420 |
401 |
0.30 |
|
|
|
| 25 |
A' |
148i |
142i |
22.77 |
|
|
|
| 26 |
A" |
1013 |
969 |
0.01 |
|
|
|
| 27 |
A" |
1000 |
957 |
0.00 |
|
|
|
| 28 |
A" |
991 |
948 |
0.60 |
|
|
|
| 29 |
A" |
852 |
815 |
0.00 |
|
|
|
| 30 |
A" |
774 |
740 |
0.20 |
|
|
|
| 31 |
A" |
771 |
738 |
0.00 |
|
|
|
| 32 |
A" |
654 |
626 |
82.53 |
|
|
|
| 33 |
A" |
568 |
543 |
0.00 |
|
|
|
| 34 |
A" |
512 |
490 |
45.98 |
|
|
|
| 35 |
A" |
286 |
274 |
0.00 |
|
|
|
| 36 |
A" |
141 |
135 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 24763.0 cm
-1
Scaled (by 0.9565) Zero Point Vibrational Energy (zpe) 23685.8 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 Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.787 |
-1.392 |
0.000 |
| C2 |
-0.814 |
-1.116 |
0.000 |
| C3 |
1.644 |
-0.505 |
0.000 |
| C4 |
-1.451 |
-0.205 |
0.000 |
| C5 |
1.156 |
1.127 |
0.000 |
| C6 |
-1.239 |
0.724 |
0.000 |
| C7 |
0.000 |
1.363 |
0.000 |
| H8 |
1.057 |
-2.439 |
0.000 |
| H9 |
-1.314 |
-2.093 |
0.000 |
| H10 |
2.713 |
-0.626 |
0.000 |
| H11 |
-2.533 |
-0.155 |
0.000 |
| H12 |
2.082 |
1.727 |
0.000 |
| H13 |
-2.181 |
1.144 |
0.000 |
| H14 |
-0.323 |
2.467 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
C5 |
C6 |
C7 |
H8 |
H9 |
H10 |
H11 |
H12 |
H13 |
H14 |
| C1 | | 1.6245 | 1.2335 | 2.5325 | 2.5460 | 2.9284 | 2.8645 | 1.0818 | 2.2148 | 2.0727 | 3.5427 | 3.3771 | 3.9032 | 4.0147 |
C2 | 1.6245 | | 2.5332 | 1.1113 | 2.9861 | 1.8880 | 2.6092 | 2.2919 | 1.0977 | 3.5610 | 1.9693 | 4.0588 | 2.6410 | 3.6164 | C3 | 1.2335 | 2.5332 | | 3.1092 | 1.7035 | 3.1333 | 2.4880 | 2.0213 | 3.3577 | 1.0757 | 4.1917 | 2.2745 | 4.1650 | 3.5634 | C4 | 2.5325 | 1.1113 | 3.1092 | | 2.9278 | 0.9527 | 2.1361 | 3.3586 | 1.8933 | 4.1848 | 1.0835 | 4.0268 | 1.5339 | 2.9002 | C5 | 2.5460 | 2.9861 | 1.7035 | 2.9278 | | 2.4286 | 1.1800 | 3.5678 | 4.0592 | 2.3448 | 3.9059 | 1.1032 | 3.3371 | 1.9953 | C6 | 2.9284 | 1.8880 | 3.1333 | 0.9527 | 2.4286 | | 1.3937 | 3.9080 | 2.8181 | 4.1755 | 1.5645 | 3.4690 | 1.0318 | 1.9690 | C7 | 2.8645 | 2.6092 | 2.4880 | 2.1361 | 1.1800 | 1.3937 | | 3.9460 | 3.6976 | 3.3638 | 2.9529 | 2.1139 | 2.1918 | 1.1502 | H8 | 1.0818 | 2.2919 | 2.0213 | 3.3586 | 3.5678 | 3.9080 | 3.9460 | | 2.3963 | 2.4551 | 4.2553 | 4.2904 | 4.8293 | 5.0961 | H9 | 2.2148 | 1.0977 | 3.3577 | 1.8933 | 4.0592 | 2.8181 | 3.6976 | 2.3963 | | 4.2859 | 2.2901 | 5.1119 | 3.3514 | 4.6667 | H10 | 2.0727 | 3.5610 | 1.0757 | 4.1848 | 2.3448 | 4.1755 | 3.3638 | 2.4551 | 4.2859 | | 5.2670 | 2.4363 | 5.2039 | 4.3336 | H11 | 3.5427 | 1.9693 | 4.1917 | 1.0835 | 3.9059 | 1.5645 | 2.9529 | 4.2553 | 2.2901 | 5.2670 | | 4.9843 | 1.3456 | 3.4290 | H12 | 3.3771 | 4.0588 | 2.2745 | 4.0268 | 1.1032 | 3.4690 | 2.1139 | 4.2904 | 5.1119 | 2.4363 | 4.9843 | | 4.3028 | 2.5161 | H13 | 3.9032 | 2.6410 | 4.1650 | 1.5339 | 3.3371 | 1.0318 | 2.1918 | 4.8293 | 3.3514 | 5.2039 | 1.3456 | 4.3028 | | 2.2809 | H14 | 4.0147 | 3.6164 | 3.5634 | 2.9002 | 1.9953 | 1.9690 | 1.1502 | 5.0961 | 4.6667 | 4.3336 | 3.4290 | 2.5161 | 2.2809 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
23.730 |
|
C1 |
C2 |
H9 |
107.316 |
| C1 |
C7 |
C6 |
78.644 |
|
C1 |
C7 |
H14 |
179.643 |
| C2 |
C1 |
C7 |
64.296 |
|
C2 |
C1 |
H8 |
114.246 |
| C2 |
C3 |
C4 |
19.496 |
|
C2 |
C3 |
H10 |
159.555 |
| C3 |
C2 |
H9 |
131.046 |
|
C3 |
C4 |
C5 |
32.604 |
| C3 |
C4 |
H11 |
177.130 |
|
C4 |
C3 |
H10 |
179.051 |
| C4 |
C5 |
C6 |
17.502 |
|
C4 |
C5 |
H12 |
174.145 |
| C5 |
C4 |
H11 |
150.266 |
|
C5 |
C6 |
C7 |
17.725 |
| C5 |
C6 |
H13 |
146.394 |
|
C6 |
C5 |
H12 |
156.643 |
| C6 |
C7 |
H14 |
101.000 |
|
C7 |
C1 |
H8 |
178.542 |
| C7 |
C6 |
H13 |
128.669 |
|
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 |
-0.065 |
|
|
|
| 2 |
C |
-0.163 |
|
|
|
| 3 |
C |
-0.163 |
|
|
|
| 4 |
C |
-0.084 |
|
|
|
| 5 |
C |
-0.084 |
|
|
|
| 6 |
C |
-0.126 |
|
|
|
| 7 |
C |
-0.126 |
|
|
|
| 8 |
H |
0.117 |
|
|
|
| 9 |
H |
0.114 |
|
|
|
| 10 |
H |
0.114 |
|
|
|
| 11 |
H |
0.117 |
|
|
|
| 12 |
H |
0.117 |
|
|
|
| 13 |
H |
0.116 |
|
|
|
| 14 |
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 |
0.069 |
0.000 |
0.069 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-36.624 |
-0.001 |
0.000 |
| y |
-0.001 |
-36.622 |
0.000 |
| z |
0.000 |
0.000 |
-46.312 |
|
| Traceless |
| | x | y | z |
| x |
4.843 |
-0.001 |
0.000 |
| y |
-0.001 |
4.846 |
0.000 |
| z |
0.000 |
0.000 |
-9.689 |
|
| Polar |
| 3z2-r2 | -19.379 |
| x2-y2 | -0.002 |
| xy | -0.001 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
13.768 |
-0.000 |
0.000 |
| y |
-0.000 |
13.755 |
0.000 |
| z |
0.000 |
0.000 |
4.883 |
<r2> (average value of r
2) Å
2
| <r2> |
185.401 |
| (<r2>)1/2 |
13.616 |