Jump to
S1C2
Energy calculated at B3PW91/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -217.133983 |
| Energy at 298.15K | |
| HF Energy | -217.133983 |
| Nuclear repulsion energy | 116.654308 |
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 B3PW91/6-311+G(3df,2p)
| 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' |
3241 |
3103 |
4.05 |
51.98 |
0.71 |
0.83 |
| 2 |
A' |
3156 |
3021 |
3.19 |
160.01 |
0.10 |
0.19 |
| 3 |
A' |
3140 |
3006 |
9.51 |
39.56 |
0.55 |
0.71 |
| 4 |
A' |
3013 |
2885 |
32.83 |
177.94 |
0.10 |
0.18 |
| 5 |
A' |
1720 |
1646 |
6.53 |
39.65 |
0.05 |
0.10 |
| 6 |
A' |
1485 |
1422 |
6.50 |
12.75 |
0.51 |
0.67 |
| 7 |
A' |
1442 |
1381 |
6.59 |
9.95 |
0.39 |
0.56 |
| 8 |
A' |
1406 |
1346 |
8.75 |
3.31 |
0.74 |
0.85 |
| 9 |
A' |
1313 |
1256 |
0.22 |
18.94 |
0.23 |
0.37 |
| 10 |
A' |
1137 |
1089 |
59.37 |
1.49 |
0.69 |
0.82 |
| 11 |
A' |
1011 |
968 |
38.84 |
4.78 |
0.67 |
0.80 |
| 12 |
A' |
913 |
874 |
1.37 |
5.18 |
0.03 |
0.06 |
| 13 |
A' |
611 |
585 |
6.61 |
1.64 |
0.68 |
0.81 |
| 14 |
A' |
258 |
247 |
2.10 |
1.35 |
0.45 |
0.62 |
| 15 |
A" |
3048 |
2918 |
18.90 |
85.80 |
0.75 |
0.86 |
| 16 |
A" |
1266 |
1212 |
0.00 |
3.85 |
0.75 |
0.86 |
| 17 |
A" |
1042 |
998 |
11.44 |
1.21 |
0.75 |
0.86 |
| 18 |
A" |
1019 |
976 |
7.69 |
0.08 |
0.75 |
0.86 |
| 19 |
A" |
960 |
919 |
46.55 |
2.44 |
0.75 |
0.86 |
| 20 |
A" |
560 |
536 |
11.81 |
1.28 |
0.75 |
0.86 |
| 21 |
A" |
179 |
171 |
3.06 |
0.83 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 15959.6 cm
-1
Scaled (by 0.9573) Zero Point Vibrational Energy (zpe) 15278.2 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 B3PW91/6-311+G(3df,2p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.936 |
-0.211 |
0.000 |
| C2 |
0.000 |
0.947 |
0.000 |
| C3 |
1.321 |
0.861 |
0.000 |
| F4 |
-0.269 |
-1.419 |
0.000 |
| H5 |
1.939 |
1.749 |
0.000 |
| H6 |
1.823 |
-0.099 |
0.000 |
| H7 |
-0.490 |
1.918 |
0.000 |
| H8 |
-1.581 |
-0.188 |
0.885 |
| H9 |
-1.581 |
-0.188 |
-0.885 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4888 | 2.4985 | 1.3806 | 3.4796 | 2.7607 | 2.1745 | 1.0959 | 1.0959 |
C2 | 1.4888 | | 1.3241 | 2.3819 | 2.0986 | 2.1014 | 1.0872 | 2.1382 | 2.1382 | C3 | 2.4985 | 1.3241 | | 2.7798 | 1.0822 | 1.0824 | 2.0973 | 3.2105 | 3.2105 | F4 | 1.3806 | 2.3819 | 2.7798 | | 3.8620 | 2.4736 | 3.3445 | 2.0059 | 2.0059 | H5 | 3.4796 | 2.0986 | 1.0822 | 3.8620 | | 1.8513 | 2.4353 | 4.1145 | 4.1145 | H6 | 2.7607 | 2.1014 | 1.0824 | 2.4736 | 1.8513 | | 3.0682 | 3.5182 | 3.5182 | H7 | 2.1745 | 1.0872 | 2.0973 | 3.3445 | 2.4353 | 3.0682 | | 2.5312 | 2.5312 | H8 | 1.0959 | 2.1382 | 3.2105 | 2.0059 | 4.1145 | 3.5182 | 2.5312 | | 1.7708 | H9 | 1.0959 | 2.1382 | 3.2105 | 2.0059 | 4.1145 | 3.5182 | 2.5312 | 1.7708 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
125.197 |
|
C1 |
C2 |
H7 |
114.259 |
| C2 |
C1 |
F4 |
112.163 |
|
C2 |
C1 |
H8 |
110.722 |
| C2 |
C1 |
H9 |
110.722 |
|
C2 |
C3 |
H5 |
121.080 |
| C2 |
C3 |
H6 |
121.340 |
|
C3 |
C2 |
H7 |
120.544 |
| F4 |
C1 |
H8 |
107.634 |
|
F4 |
C1 |
H9 |
107.634 |
| H5 |
C3 |
H6 |
117.580 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.265 |
|
|
|
| 2 |
C |
-0.127 |
|
|
|
| 3 |
C |
-0.310 |
|
|
|
| 4 |
F |
-0.459 |
|
|
|
| 5 |
H |
0.135 |
|
|
|
| 6 |
H |
0.135 |
|
|
|
| 7 |
H |
0.108 |
|
|
|
| 8 |
H |
0.126 |
|
|
|
| 9 |
H |
0.126 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.917 |
1.498 |
0.000 |
1.756 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-21.156 |
-0.277 |
0.000 |
| y |
-0.277 |
-25.478 |
0.000 |
| z |
0.000 |
0.000 |
-25.272 |
|
| Traceless |
| | x | y | z |
| x |
4.219 |
-0.277 |
0.000 |
| y |
-0.277 |
-2.264 |
0.000 |
| z |
0.000 |
0.000 |
-1.955 |
|
| Polar |
| 3z2-r2 | -3.911 |
| x2-y2 | 4.322 |
| xy | -0.277 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.405 |
0.369 |
0.000 |
| y |
0.369 |
5.602 |
0.000 |
| z |
0.000 |
0.000 |
4.655 |
<r2> (average value of r
2) Å
2
| <r2> |
80.287 |
| (<r2>)1/2 |
8.960 |
Jump to
S1C1
Energy calculated at B3PW91/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -217.133726 |
| Energy at 298.15K | |
| HF Energy | -217.133726 |
| Nuclear repulsion energy | 114.412256 |
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 B3PW91/6-311+G(3df,2p)
| 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 |
3224 |
3086 |
9.20 |
61.36 |
0.59 |
0.74 |
| 2 |
A |
3154 |
3019 |
4.96 |
118.34 |
0.22 |
0.36 |
| 3 |
A |
3135 |
3001 |
8.50 |
69.97 |
0.10 |
0.19 |
| 4 |
A |
3084 |
2952 |
18.13 |
65.00 |
0.68 |
0.81 |
| 5 |
A |
3029 |
2900 |
29.33 |
133.28 |
0.09 |
0.16 |
| 6 |
A |
1716 |
1643 |
0.75 |
41.20 |
0.07 |
0.13 |
| 7 |
A |
1495 |
1432 |
4.36 |
3.87 |
0.65 |
0.79 |
| 8 |
A |
1455 |
1393 |
17.60 |
9.82 |
0.50 |
0.66 |
| 9 |
A |
1383 |
1324 |
11.00 |
3.92 |
0.24 |
0.39 |
| 10 |
A |
1313 |
1257 |
0.07 |
14.41 |
0.31 |
0.47 |
| 11 |
A |
1264 |
1210 |
4.33 |
7.23 |
0.65 |
0.79 |
| 12 |
A |
1180 |
1130 |
2.54 |
1.10 |
0.62 |
0.76 |
| 13 |
A |
1045 |
1000 |
114.58 |
5.45 |
0.54 |
0.70 |
| 14 |
A |
1032 |
988 |
35.20 |
2.20 |
0.70 |
0.83 |
| 15 |
A |
988 |
946 |
3.77 |
1.73 |
0.14 |
0.24 |
| 16 |
A |
972 |
930 |
52.77 |
2.13 |
0.54 |
0.70 |
| 17 |
A |
928 |
888 |
2.31 |
3.16 |
0.12 |
0.21 |
| 18 |
A |
658 |
630 |
7.77 |
1.49 |
0.30 |
0.46 |
| 19 |
A |
435 |
417 |
2.50 |
3.55 |
0.32 |
0.49 |
| 20 |
A |
329 |
315 |
7.22 |
1.17 |
0.73 |
0.85 |
| 21 |
A |
116 |
111 |
1.01 |
2.52 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 15967.9 cm
-1
Scaled (by 0.9573) Zero Point Vibrational Energy (zpe) 15286.1 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 B3PW91/6-311+G(3df,2p)
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.604 |
0.427 |
0.318 |
| C2 |
0.645 |
-0.379 |
0.243 |
| C3 |
1.796 |
0.093 |
-0.214 |
| F4 |
-1.641 |
-0.223 |
-0.344 |
| H5 |
2.695 |
-0.511 |
-0.223 |
| H6 |
1.884 |
1.106 |
-0.592 |
| H7 |
0.573 |
-1.398 |
0.610 |
| H8 |
-0.928 |
0.560 |
1.355 |
| H9 |
-0.475 |
1.409 |
-0.143 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4880 | 2.4809 | 1.3921 | 3.4721 | 2.7346 | 2.1917 | 1.0946 | 1.0924 |
C2 | 1.4880 | | 1.3253 | 2.3654 | 2.1067 | 2.1061 | 1.0862 | 2.1429 | 2.1445 | C3 | 2.4809 | 1.3253 | | 3.4544 | 1.0828 | 1.0848 | 2.0971 | 3.1783 | 2.6260 | F4 | 1.3921 | 2.3654 | 3.4544 | | 4.3477 | 3.7758 | 2.6825 | 2.0025 | 2.0166 | H5 | 3.4721 | 2.1067 | 1.0828 | 4.3477 | | 1.8460 | 2.4461 | 4.0942 | 3.7070 | H6 | 2.7346 | 2.1061 | 1.0848 | 3.7758 | 1.8460 | | 3.0714 | 3.4635 | 2.4204 | H7 | 2.1917 | 1.0862 | 2.0971 | 2.6825 | 2.4461 | 3.0714 | | 2.5776 | 3.0900 | H8 | 1.0946 | 2.1429 | 3.1783 | 2.0025 | 4.0942 | 3.4635 | 2.5776 | | 1.7805 | H9 | 1.0924 | 2.1445 | 2.6260 | 2.0166 | 3.7070 | 2.4204 | 3.0900 | 1.7805 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
123.631 |
|
C1 |
C2 |
H7 |
115.854 |
| C2 |
C1 |
F4 |
110.379 |
|
C2 |
C1 |
H8 |
111.229 |
| C2 |
C1 |
H9 |
111.495 |
|
C2 |
C3 |
H5 |
121.719 |
| C2 |
C3 |
H6 |
121.504 |
|
C3 |
C2 |
H7 |
120.503 |
| F4 |
C1 |
H8 |
106.658 |
|
F4 |
C1 |
H9 |
107.906 |
| H5 |
C3 |
H6 |
116.776 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.233 |
|
|
|
| 2 |
C |
-0.032 |
|
|
|
| 3 |
C |
-0.362 |
|
|
|
| 4 |
F |
-0.443 |
|
|
|
| 5 |
H |
0.135 |
|
|
|
| 6 |
H |
0.124 |
|
|
|
| 7 |
H |
0.107 |
|
|
|
| 8 |
H |
0.125 |
|
|
|
| 9 |
H |
0.113 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.529 |
0.747 |
0.861 |
1.908 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.758 |
-1.198 |
-2.039 |
| y |
-1.198 |
-22.512 |
-1.050 |
| z |
-2.039 |
-1.050 |
-24.896 |
|
| Traceless |
| | x | y | z |
| x |
-2.054 |
-1.198 |
-2.039 |
| y |
-1.198 |
2.815 |
-1.050 |
| z |
-2.039 |
-1.050 |
-0.761 |
|
| Polar |
| 3z2-r2 | -1.521 |
| x2-y2 | -3.246 |
| xy | -1.198 |
| xz | -2.039 |
| yz | -1.050 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.439 |
0.242 |
-0.601 |
| y |
0.242 |
5.385 |
-0.205 |
| z |
-0.601 |
-0.205 |
4.967 |
<r2> (average value of r
2) Å
2
| <r2> |
88.871 |
| (<r2>)1/2 |
9.427 |