Jump to
S1C2
Energy calculated at B3LYP/Def2TZVPP
| | hartrees |
| Energy at 0K | -270.994230 |
| Energy at 298.15K | |
| HF Energy | -270.994230 |
| Nuclear repulsion energy | 258.633087 |
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 B3LYP/Def2TZVPP
| 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 |
3183 |
3064 |
3.05 |
|
|
|
| 2 |
A1 |
3174 |
3056 |
26.20 |
|
|
|
| 3 |
A1 |
3157 |
3039 |
17.56 |
|
|
|
| 4 |
A1 |
3134 |
3017 |
4.45 |
|
|
|
| 5 |
A1 |
1650 |
1588 |
2.19 |
|
|
|
| 6 |
A1 |
1594 |
1535 |
14.32 |
|
|
|
| 7 |
A1 |
1482 |
1426 |
6.86 |
|
|
|
| 8 |
A1 |
1288 |
1240 |
0.87 |
|
|
|
| 9 |
A1 |
1244 |
1198 |
2.97 |
|
|
|
| 10 |
A1 |
964 |
928 |
2.68 |
|
|
|
| 11 |
A1 |
918 |
883 |
0.83 |
|
|
|
| 12 |
A1 |
847 |
816 |
0.19 |
|
|
|
| 13 |
A1 |
421 |
405 |
0.26 |
|
|
|
| 14 |
A2 |
1013 |
975 |
0.00 |
|
|
|
| 15 |
A2 |
999 |
961 |
0.00 |
|
|
|
| 16 |
A2 |
771 |
743 |
0.00 |
|
|
|
| 17 |
A2 |
568 |
547 |
0.00 |
|
|
|
| 18 |
A2 |
290 |
280 |
0.00 |
|
|
|
| 19 |
B1 |
990 |
953 |
0.35 |
|
|
|
| 20 |
B1 |
850 |
818 |
0.01 |
|
|
|
| 21 |
B1 |
766 |
737 |
1.04 |
|
|
|
| 22 |
B1 |
653 |
629 |
78.17 |
|
|
|
| 23 |
B1 |
519 |
500 |
36.55 |
|
|
|
| 24 |
B1 |
153 |
148 |
0.00 |
|
|
|
| 25 |
B2 |
3173 |
3055 |
40.47 |
|
|
|
| 26 |
B2 |
3141 |
3023 |
2.61 |
|
|
|
| 27 |
B2 |
3134 |
3017 |
7.47 |
|
|
|
| 28 |
B2 |
1553 |
1495 |
7.12 |
|
|
|
| 29 |
B2 |
1486 |
1430 |
1.49 |
|
|
|
| 30 |
B2 |
1422 |
1369 |
0.01 |
|
|
|
| 31 |
B2 |
1309 |
1260 |
0.11 |
|
|
|
| 32 |
B2 |
1189 |
1144 |
2.39 |
|
|
|
| 33 |
B2 |
967 |
931 |
6.63 |
|
|
|
| 34 |
B2 |
909 |
875 |
1.15 |
|
|
|
| 35 |
B2 |
448 |
431 |
0.21 |
|
|
|
| 36 |
B2 |
68i |
66i |
24.72 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 24645.8 cm
-1
Scaled (by 0.9626) Zero Point Vibrational Energy (zpe) 23724.0 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 B3LYP/Def2TZVPP
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 |
0.994 |
| C3 |
0.000 |
-1.264 |
0.994 |
| C4 |
0.000 |
1.586 |
-0.340 |
| C5 |
0.000 |
-1.586 |
-0.340 |
| C6 |
0.000 |
0.677 |
-1.464 |
| C7 |
0.000 |
-0.677 |
-1.464 |
| H8 |
0.000 |
0.000 |
2.700 |
| H9 |
0.000 |
2.110 |
1.673 |
| H10 |
0.000 |
-2.110 |
1.673 |
| H11 |
0.000 |
2.640 |
-0.584 |
| H12 |
0.000 |
-2.640 |
-0.584 |
| H13 |
0.000 |
1.157 |
-2.436 |
| H14 |
0.000 |
-1.157 |
-2.436 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
C5 |
C6 |
C7 |
H8 |
H9 |
H10 |
H11 |
H12 |
H13 |
H14 |
| C1 | | 1.4096 | 1.4096 | 2.5196 | 2.5196 | 3.1553 | 3.1553 | 1.0820 | 2.1106 | 2.1106 | 3.4379 | 3.4379 | 4.2160 | 4.2160 |
C2 | 1.4096 | | 2.5275 | 1.3719 | 3.1460 | 2.5263 | 3.1315 | 2.1235 | 1.0849 | 3.4413 | 2.0937 | 4.2104 | 3.4314 | 4.1979 | C3 | 1.4096 | 2.5275 | | 3.1460 | 1.3719 | 3.1315 | 2.5263 | 2.1235 | 3.4413 | 1.0849 | 4.2104 | 2.0937 | 4.1979 | 3.4314 | C4 | 2.5196 | 1.3719 | 3.1460 | | 3.1713 | 1.4449 | 2.5266 | 3.4288 | 2.0797 | 4.2080 | 1.0821 | 4.2325 | 2.1395 | 3.4519 | C5 | 2.5196 | 3.1460 | 1.3719 | 3.1713 | | 2.5266 | 1.4449 | 3.4288 | 4.2080 | 2.0797 | 4.2325 | 1.0821 | 3.4519 | 2.1395 | C6 | 3.1553 | 2.5263 | 3.1315 | 1.4449 | 2.5266 | | 1.3546 | 4.2186 | 3.4479 | 4.1958 | 2.1505 | 3.4317 | 1.0843 | 2.0761 | C7 | 3.1553 | 3.1315 | 2.5263 | 2.5266 | 1.4449 | 1.3546 | | 4.2186 | 4.1958 | 3.4479 | 3.4317 | 2.1505 | 2.0761 | 1.0843 | H8 | 1.0820 | 2.1235 | 2.1235 | 3.4288 | 3.4288 | 4.2186 | 4.2186 | | 2.3468 | 2.3468 | 4.2138 | 4.2138 | 5.2649 | 5.2649 | H9 | 2.1106 | 1.0849 | 3.4413 | 2.0797 | 4.2080 | 3.4479 | 4.1958 | 2.3468 | | 4.2198 | 2.3182 | 5.2586 | 4.2177 | 5.2491 | H10 | 2.1106 | 3.4413 | 1.0849 | 4.2080 | 2.0797 | 4.1958 | 3.4479 | 2.3468 | 4.2198 | | 5.2586 | 2.3182 | 5.2491 | 4.2177 | H11 | 3.4379 | 2.0937 | 4.2104 | 1.0821 | 4.2325 | 2.1505 | 3.4317 | 4.2138 | 2.3182 | 5.2586 | | 5.2797 | 2.3723 | 4.2243 | H12 | 3.4379 | 4.2104 | 2.0937 | 4.2325 | 1.0821 | 3.4317 | 2.1505 | 4.2138 | 5.2586 | 2.3182 | 5.2797 | | 4.2243 | 2.3723 | H13 | 4.2160 | 3.4314 | 4.1979 | 2.1395 | 3.4519 | 1.0843 | 2.0761 | 5.2649 | 4.2177 | 5.2491 | 2.3723 | 4.2243 | | 2.3139 | H14 | 4.2160 | 4.1979 | 3.4314 | 3.4519 | 2.1395 | 2.0761 | 1.0843 | 5.2649 | 5.2491 | 4.2177 | 4.2243 | 2.3723 | 2.3139 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
26.297 |
|
C1 |
C2 |
H9 |
114.960 |
| C1 |
C7 |
C6 |
77.605 |
|
C1 |
C7 |
H14 |
166.139 |
| C2 |
C1 |
C7 |
76.098 |
|
C2 |
C1 |
H8 |
116.297 |
| C2 |
C3 |
C4 |
25.081 |
|
C2 |
C3 |
H10 |
141.257 |
| C3 |
C2 |
H9 |
141.257 |
|
C3 |
C4 |
C5 |
25.081 |
| C3 |
C4 |
H11 |
167.966 |
|
C4 |
C3 |
H10 |
166.338 |
| C4 |
C5 |
C6 |
26.407 |
|
C4 |
C5 |
H12 |
166.952 |
| C5 |
C4 |
H11 |
166.952 |
|
C5 |
C6 |
C7 |
26.407 |
| C5 |
C6 |
H13 |
142.663 |
|
C6 |
C5 |
H12 |
140.545 |
| C6 |
C7 |
H14 |
116.256 |
|
C7 |
C1 |
H8 |
167.605 |
| C7 |
C6 |
H13 |
116.256 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/Def2TZVPP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.148 |
|
|
|
| 2 |
C |
-0.082 |
|
|
|
| 3 |
C |
-0.082 |
|
|
|
| 4 |
C |
-0.134 |
|
|
|
| 5 |
C |
-0.134 |
|
|
|
| 6 |
C |
-0.103 |
|
|
|
| 7 |
C |
-0.103 |
|
|
|
| 8 |
H |
0.111 |
|
|
|
| 9 |
H |
0.113 |
|
|
|
| 10 |
H |
0.113 |
|
|
|
| 11 |
H |
0.112 |
|
|
|
| 12 |
H |
0.112 |
|
|
|
| 13 |
H |
0.113 |
|
|
|
| 14 |
H |
0.113 |
|
|
|
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 |
-0.066 |
0.066 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-46.520 |
0.000 |
0.000 |
| y |
0.000 |
-37.774 |
0.000 |
| z |
0.000 |
0.000 |
-37.776 |
|
| Traceless |
| | x | y | z |
| x |
-8.745 |
0.000 |
0.000 |
| y |
0.000 |
4.374 |
0.000 |
| z |
0.000 |
0.000 |
4.371 |
|
| Polar |
| 3z2-r2 | 8.743 |
| x2-y2 | -8.746 |
| 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 |
6.787 |
0.000 |
0.000 |
| y |
0.000 |
14.691 |
0.000 |
| z |
0.000 |
0.000 |
14.672 |
<r2> (average value of r
2) Å
2
| <r2> |
185.865 |
| (<r2>)1/2 |
13.633 |
Jump to
S1C1
Energy calculated at B3LYP/Def2TZVPP
| | hartrees |
| Energy at 0K | -270.994212 |
| Energy at 298.15K | |
| HF Energy | -270.994212 |
| Nuclear repulsion energy | 258.633222 |
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 B3LYP/Def2TZVPP
| 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' |
3183 |
3064 |
2.93 |
|
|
|
| 2 |
A' |
3175 |
3057 |
30.30 |
|
|
|
| 3 |
A' |
3172 |
3054 |
38.56 |
|
|
|
| 4 |
A' |
3158 |
3040 |
15.39 |
|
|
|
| 5 |
A' |
3141 |
3024 |
3.48 |
|
|
|
| 6 |
A' |
3136 |
3018 |
5.34 |
|
|
|
| 7 |
A' |
3134 |
3017 |
5.71 |
|
|
|
| 8 |
A' |
1638 |
1577 |
9.06 |
|
|
|
| 9 |
A' |
1612 |
1552 |
3.02 |
|
|
|
| 10 |
A' |
1543 |
1485 |
12.26 |
|
|
|
| 11 |
A' |
1490 |
1434 |
2.54 |
|
|
|
| 12 |
A' |
1479 |
1424 |
5.10 |
|
|
|
| 13 |
A' |
1422 |
1368 |
0.01 |
|
|
|
| 14 |
A' |
1308 |
1259 |
0.11 |
|
|
|
| 15 |
A' |
1288 |
1239 |
0.98 |
|
|
|
| 16 |
A' |
1245 |
1198 |
2.20 |
|
|
|
| 17 |
A' |
1188 |
1143 |
3.40 |
|
|
|
| 18 |
A' |
972 |
936 |
5.96 |
|
|
|
| 19 |
A' |
960 |
924 |
3.17 |
|
|
|
| 20 |
A' |
917 |
883 |
0.78 |
|
|
|
| 21 |
A' |
909 |
875 |
1.18 |
|
|
|
| 22 |
A' |
847 |
816 |
0.19 |
|
|
|
| 23 |
A' |
448 |
431 |
0.22 |
|
|
|
| 24 |
A' |
420 |
405 |
0.27 |
|
|
|
| 25 |
A' |
121i |
117i |
24.47 |
|
|
|
| 26 |
A" |
1014 |
976 |
0.00 |
|
|
|
| 27 |
A" |
999 |
962 |
0.00 |
|
|
|
| 28 |
A" |
991 |
953 |
0.27 |
|
|
|
| 29 |
A" |
849 |
818 |
0.00 |
|
|
|
| 30 |
A" |
772 |
743 |
1.11 |
|
|
|
| 31 |
A" |
761 |
733 |
0.01 |
|
|
|
| 32 |
A" |
651 |
627 |
78.22 |
|
|
|
| 33 |
A" |
567 |
546 |
0.00 |
|
|
|
| 34 |
A" |
519 |
500 |
36.60 |
|
|
|
| 35 |
A" |
290 |
279 |
0.00 |
|
|
|
| 36 |
A" |
152 |
147 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 24614.9 cm
-1
Scaled (by 0.9626) Zero Point Vibrational Energy (zpe) 23694.3 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 B3LYP/Def2TZVPP
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 |
1.128 |
0.000 |
| C6 |
-1.239 |
0.724 |
0.000 |
| C7 |
0.000 |
1.363 |
0.000 |
| H8 |
1.058 |
-2.439 |
0.000 |
| H9 |
-1.314 |
-2.094 |
0.000 |
| H10 |
2.713 |
-0.626 |
0.000 |
| H11 |
-2.534 |
-0.156 |
0.000 |
| H12 |
2.082 |
1.728 |
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 | | 1.6252 | 1.2329 | 2.5333 | 2.5464 | 2.9290 | 2.8649 | 1.0816 | 2.2152 | 2.0721 | 3.5441 | 3.3771 | 3.9038 | 4.0153 |
C2 | 1.6252 | | 2.5334 | 1.1113 | 2.9863 | 1.8881 | 2.6095 | 2.2921 | 1.0976 | 3.5611 | 1.9699 | 4.0589 | 2.6412 | 3.6168 | C3 | 1.2329 | 2.5334 | | 3.1098 | 1.7045 | 3.1338 | 2.4886 | 2.0207 | 3.3575 | 1.0755 | 4.1930 | 2.2751 | 4.1654 | 3.5644 | C4 | 2.5333 | 1.1113 | 3.1098 | | 2.9282 | 0.9530 | 2.1367 | 3.3589 | 1.8932 | 4.1851 | 1.0843 | 4.0271 | 1.5341 | 2.9007 | C5 | 2.5464 | 2.9863 | 1.7045 | 2.9282 | | 2.4285 | 1.1795 | 3.5681 | 4.0592 | 2.3453 | 3.9069 | 1.1030 | 3.3368 | 1.9953 | C6 | 2.9290 | 1.8881 | 3.1338 | 0.9530 | 2.4285 | | 1.3940 | 3.9082 | 2.8182 | 4.1757 | 1.5656 | 3.4689 | 1.0317 | 1.9692 | C7 | 2.8649 | 2.6095 | 2.4886 | 2.1367 | 1.1795 | 1.3940 | | 3.9462 | 3.6978 | 3.3639 | 2.9544 | 2.1134 | 2.1918 | 1.1504 | H8 | 1.0816 | 2.2921 | 2.0207 | 3.3589 | 3.5681 | 3.9082 | 3.9462 | | 2.3964 | 2.4548 | 4.2562 | 4.2904 | 4.8296 | 5.0965 | H9 | 2.2152 | 1.0976 | 3.3575 | 1.8932 | 4.0592 | 2.8182 | 3.6978 | 2.3964 | | 4.2857 | 2.2903 | 5.1118 | 3.3517 | 4.6670 | H10 | 2.0721 | 3.5611 | 1.0755 | 4.1851 | 2.3453 | 4.1757 | 3.3639 | 2.4548 | 4.2857 | | 5.2681 | 2.4367 | 5.2039 | 4.3342 | H11 | 3.5441 | 1.9699 | 4.1930 | 1.0843 | 3.9069 | 1.5656 | 2.9544 | 4.2562 | 2.2903 | 5.2681 | | 4.9853 | 1.3468 | 3.4302 | H12 | 3.3771 | 4.0589 | 2.2751 | 4.0271 | 1.1030 | 3.4689 | 2.1134 | 4.2904 | 5.1118 | 2.4367 | 4.9853 | | 4.3023 | 2.5161 | H13 | 3.9038 | 2.6412 | 4.1654 | 1.5341 | 3.3368 | 1.0317 | 2.1918 | 4.8296 | 3.3517 | 5.2039 | 1.3468 | 4.3023 | | 2.2806 | H14 | 4.0153 | 3.6168 | 3.5644 | 2.9007 | 1.9953 | 1.9692 | 1.1504 | 5.0965 | 4.6670 | 4.3342 | 3.4302 | 2.5161 | 2.2806 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
23.714 |
|
C1 |
C2 |
H9 |
107.306 |
| C1 |
C7 |
C6 |
78.650 |
|
C1 |
C7 |
H14 |
179.630 |
| C2 |
C1 |
C7 |
64.293 |
|
C2 |
C1 |
H8 |
114.230 |
| C2 |
C3 |
C4 |
19.489 |
|
C2 |
C3 |
H10 |
159.586 |
| C3 |
C2 |
H9 |
131.020 |
|
C3 |
C4 |
C5 |
32.618 |
| C3 |
C4 |
H11 |
177.106 |
|
C4 |
C3 |
H10 |
179.075 |
| C4 |
C5 |
C6 |
17.503 |
|
C4 |
C5 |
H12 |
174.160 |
| C5 |
C4 |
H11 |
150.275 |
|
C5 |
C6 |
C7 |
17.716 |
| C5 |
C6 |
H13 |
146.365 |
|
C6 |
C5 |
H12 |
156.657 |
| C6 |
C7 |
H14 |
100.980 |
|
C7 |
C1 |
H8 |
178.523 |
| C7 |
C6 |
H13 |
128.649 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/Def2TZVPP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.079 |
|
|
|
| 2 |
C |
-0.144 |
|
|
|
| 3 |
C |
-0.144 |
|
|
|
| 4 |
C |
-0.091 |
|
|
|
| 5 |
C |
-0.090 |
|
|
|
| 6 |
C |
-0.118 |
|
|
|
| 7 |
C |
-0.120 |
|
|
|
| 8 |
H |
0.113 |
|
|
|
| 9 |
H |
0.111 |
|
|
|
| 10 |
H |
0.111 |
|
|
|
| 11 |
H |
0.113 |
|
|
|
| 12 |
H |
0.113 |
|
|
|
| 13 |
H |
0.112 |
|
|
|
| 14 |
H |
0.112 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.003 |
-0.068 |
0.000 |
0.068 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-37.772 |
-0.001 |
0.000 |
| y |
-0.001 |
-37.777 |
0.000 |
| z |
0.000 |
0.000 |
-46.520 |
|
| Traceless |
| | x | y | z |
| x |
4.376 |
-0.001 |
0.000 |
| y |
-0.001 |
4.369 |
0.000 |
| z |
0.000 |
0.000 |
-8.745 |
|
| Polar |
| 3z2-r2 | -17.491 |
| x2-y2 | 0.005 |
| 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 |
14.682 |
0.000 |
0.000 |
| y |
0.000 |
14.680 |
0.000 |
| z |
0.000 |
0.000 |
6.786 |
<r2> (average value of r
2) Å
2
| <r2> |
185.865 |
| (<r2>)1/2 |
13.633 |