Jump to
S1C2
Energy calculated at B3LYP/6-311G*
| | hartrees |
| Energy at 0K | -217.192966 |
| Energy at 298.15K | |
| HF Energy | -217.192966 |
| Nuclear repulsion energy | 116.288545 |
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/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' |
3234 |
3125 |
10.65 |
57.33 |
0.73 |
0.84 |
| 2 |
A' |
3151 |
3045 |
6.03 |
147.35 |
0.14 |
0.25 |
| 3 |
A' |
3133 |
3027 |
17.83 |
50.63 |
0.52 |
0.68 |
| 4 |
A' |
3017 |
2915 |
44.82 |
172.05 |
0.12 |
0.21 |
| 5 |
A' |
1724 |
1666 |
4.52 |
18.34 |
0.12 |
0.22 |
| 6 |
A' |
1514 |
1463 |
3.42 |
16.89 |
0.59 |
0.74 |
| 7 |
A' |
1455 |
1406 |
5.81 |
10.76 |
0.50 |
0.67 |
| 8 |
A' |
1427 |
1379 |
14.23 |
9.44 |
0.71 |
0.83 |
| 9 |
A' |
1324 |
1279 |
0.11 |
17.57 |
0.33 |
0.49 |
| 10 |
A' |
1129 |
1091 |
42.68 |
2.03 |
0.75 |
0.85 |
| 11 |
A' |
1012 |
978 |
49.03 |
4.84 |
0.70 |
0.82 |
| 12 |
A' |
909 |
878 |
2.37 |
3.53 |
0.12 |
0.22 |
| 13 |
A' |
612 |
591 |
6.47 |
1.86 |
0.74 |
0.85 |
| 14 |
A' |
267 |
258 |
2.46 |
1.22 |
0.53 |
0.69 |
| 15 |
A" |
3049 |
2946 |
40.73 |
101.93 |
0.75 |
0.86 |
| 16 |
A" |
1269 |
1226 |
0.01 |
9.26 |
0.75 |
0.86 |
| 17 |
A" |
1049 |
1014 |
10.75 |
0.88 |
0.75 |
0.86 |
| 18 |
A" |
1022 |
988 |
14.09 |
0.15 |
0.75 |
0.86 |
| 19 |
A" |
946 |
914 |
48.33 |
1.03 |
0.75 |
0.86 |
| 20 |
A" |
560 |
541 |
11.56 |
7.73 |
0.75 |
0.86 |
| 21 |
A" |
176 |
170 |
2.90 |
4.27 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 15988.0 cm
-1
Scaled (by 0.9663) Zero Point Vibrational Energy (zpe) 15449.2 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 B3LYP/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.942 |
-0.207 |
0.000 |
| C2 |
0.000 |
0.955 |
0.000 |
| C3 |
1.323 |
0.854 |
0.000 |
| F4 |
-0.266 |
-1.422 |
0.000 |
| H5 |
1.957 |
1.734 |
0.000 |
| H6 |
1.815 |
-0.112 |
0.000 |
| H7 |
-0.484 |
1.931 |
0.000 |
| H8 |
-1.587 |
-0.186 |
0.887 |
| H9 |
-1.587 |
-0.186 |
-0.887 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4957 | 2.5018 | 1.3908 | 3.4889 | 2.7588 | 2.1861 | 1.0968 | 1.0968 |
C2 | 1.4957 | | 1.3270 | 2.3917 | 2.1063 | 2.1048 | 1.0893 | 2.1462 | 2.1462 | C3 | 2.5018 | 1.3270 | | 2.7765 | 1.0843 | 1.0838 | 2.1031 | 3.2154 | 3.2154 | F4 | 1.3908 | 2.3917 | 2.7765 | | 3.8608 | 2.4593 | 3.3599 | 2.0149 | 2.0149 | H5 | 3.4889 | 2.1063 | 1.0843 | 3.8608 | | 1.8515 | 2.4482 | 4.1270 | 4.1270 | H6 | 2.7588 | 2.1048 | 1.0838 | 2.4593 | 1.8515 | | 3.0746 | 3.5163 | 3.5163 | H7 | 2.1861 | 1.0893 | 2.1031 | 3.3599 | 2.4482 | 3.0746 | | 2.5464 | 2.5464 | H8 | 1.0968 | 2.1462 | 3.2154 | 2.0149 | 4.1270 | 3.5163 | 2.5464 | | 1.7741 | H9 | 1.0968 | 2.1462 | 3.2154 | 2.0149 | 4.1270 | 3.5163 | 2.5464 | 1.7741 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
124.722 |
|
C1 |
C2 |
H7 |
114.585 |
| C2 |
C1 |
F4 |
111.857 |
|
C2 |
C1 |
H8 |
110.826 |
| C2 |
C1 |
H9 |
110.826 |
|
C2 |
C3 |
H5 |
121.410 |
| C2 |
C3 |
H6 |
121.302 |
|
C3 |
C2 |
H7 |
120.693 |
| F4 |
C1 |
H8 |
107.601 |
|
F4 |
C1 |
H9 |
107.601 |
| H5 |
C3 |
H6 |
117.288 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.087 |
|
|
|
| 2 |
C |
-0.252 |
|
|
|
| 3 |
C |
-0.405 |
|
|
|
| 4 |
F |
-0.274 |
|
|
|
| 5 |
H |
0.206 |
|
|
|
| 6 |
H |
0.217 |
|
|
|
| 7 |
H |
0.193 |
|
|
|
| 8 |
H |
0.201 |
|
|
|
| 9 |
H |
0.201 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.910 |
1.515 |
0.000 |
1.767 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-21.197 |
-0.345 |
0.000 |
| y |
-0.345 |
-25.372 |
0.000 |
| z |
0.000 |
0.000 |
-25.248 |
|
| Traceless |
| | x | y | z |
| x |
4.113 |
-0.345 |
0.000 |
| y |
-0.345 |
-2.149 |
0.000 |
| z |
0.000 |
0.000 |
-1.964 |
|
| Polar |
| 3z2-r2 | -3.928 |
| x2-y2 | 4.175 |
| xy | -0.345 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.866 |
0.275 |
0.000 |
| y |
0.275 |
4.748 |
0.000 |
| z |
0.000 |
0.000 |
3.262 |
<r2> (average value of r
2) Å
2
| <r2> |
80.516 |
| (<r2>)1/2 |
8.973 |
Jump to
S1C1
Energy calculated at B3LYP/6-311G*
| | hartrees |
| Energy at 0K | -217.191943 |
| Energy at 298.15K | |
| HF Energy | -217.191943 |
| Nuclear repulsion energy | 113.943481 |
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/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 |
3214 |
3106 |
19.82 |
67.69 |
0.60 |
0.75 |
| 2 |
A |
3147 |
3041 |
10.11 |
119.25 |
0.27 |
0.43 |
| 3 |
A |
3129 |
3024 |
15.67 |
70.79 |
0.15 |
0.26 |
| 4 |
A |
3084 |
2980 |
31.29 |
75.09 |
0.70 |
0.82 |
| 5 |
A |
3032 |
2930 |
43.47 |
127.77 |
0.12 |
0.21 |
| 6 |
A |
1720 |
1662 |
0.64 |
18.92 |
0.14 |
0.25 |
| 7 |
A |
1517 |
1466 |
2.09 |
7.72 |
0.69 |
0.81 |
| 8 |
A |
1473 |
1423 |
19.83 |
10.69 |
0.60 |
0.75 |
| 9 |
A |
1407 |
1359 |
15.24 |
4.80 |
0.54 |
0.70 |
| 10 |
A |
1323 |
1278 |
0.11 |
13.67 |
0.39 |
0.56 |
| 11 |
A |
1274 |
1231 |
3.95 |
14.27 |
0.71 |
0.83 |
| 12 |
A |
1186 |
1146 |
2.01 |
1.27 |
0.75 |
0.86 |
| 13 |
A |
1034 |
999 |
20.17 |
0.98 |
0.49 |
0.66 |
| 14 |
A |
1028 |
993 |
125.56 |
5.63 |
0.66 |
0.80 |
| 15 |
A |
990 |
957 |
3.96 |
0.77 |
0.25 |
0.41 |
| 16 |
A |
957 |
925 |
53.80 |
0.94 |
0.54 |
0.70 |
| 17 |
A |
933 |
902 |
4.20 |
2.66 |
0.16 |
0.27 |
| 18 |
A |
652 |
630 |
7.78 |
4.40 |
0.62 |
0.77 |
| 19 |
A |
438 |
423 |
2.84 |
4.49 |
0.48 |
0.65 |
| 20 |
A |
329 |
318 |
7.31 |
3.44 |
0.75 |
0.86 |
| 21 |
A |
117 |
113 |
1.15 |
5.93 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 15991.8 cm
-1
Scaled (by 0.9663) Zero Point Vibrational Energy (zpe) 15452.8 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 B3LYP/6-311G*
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.605 |
0.444 |
0.303 |
| C2 |
0.646 |
-0.370 |
0.245 |
| C3 |
1.809 |
0.082 |
-0.210 |
| F4 |
-1.653 |
-0.236 |
-0.332 |
| H5 |
2.703 |
-0.532 |
-0.207 |
| H6 |
1.918 |
1.091 |
-0.601 |
| H7 |
0.559 |
-1.387 |
0.623 |
| H8 |
-0.922 |
0.611 |
1.338 |
| H9 |
-0.480 |
1.410 |
-0.193 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4935 | 2.4944 | 1.4015 | 3.4862 | 2.7568 | 2.1927 | 1.0955 | 1.0935 |
C2 | 1.4935 | | 1.3286 | 2.3740 | 2.1121 | 2.1136 | 1.0882 | 2.1489 | 2.1516 | C3 | 2.4944 | 1.3286 | | 3.4790 | 1.0847 | 1.0868 | 2.1015 | 3.1840 | 2.6464 | F4 | 1.4015 | 2.3740 | 3.4790 | | 4.3678 | 3.8188 | 2.6700 | 2.0102 | 2.0260 | H5 | 3.4862 | 2.1121 | 1.0847 | 4.3678 | | 1.8456 | 2.4525 | 4.1030 | 3.7288 | H6 | 2.7568 | 2.1136 | 1.0868 | 3.8188 | 1.8456 | | 3.0795 | 3.4723 | 2.4531 | H7 | 2.1927 | 1.0882 | 2.1015 | 2.6700 | 2.4525 | 3.0795 | | 2.5878 | 3.0933 | H8 | 1.0955 | 2.1489 | 3.1840 | 2.0102 | 4.1030 | 3.4723 | 2.5878 | | 1.7834 | H9 | 1.0935 | 2.1516 | 2.6464 | 2.0260 | 3.7288 | 2.4531 | 3.0933 | 1.7834 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
124.119 |
|
C1 |
C2 |
H7 |
115.387 |
| C2 |
C1 |
F4 |
110.135 |
|
C2 |
C1 |
H8 |
111.265 |
| C2 |
C1 |
H9 |
111.609 |
|
C2 |
C3 |
H5 |
121.808 |
| C2 |
C3 |
H6 |
121.788 |
|
C3 |
C2 |
H7 |
120.486 |
| F4 |
C1 |
H8 |
106.589 |
|
F4 |
C1 |
H9 |
107.949 |
| H5 |
C3 |
H6 |
116.404 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.109 |
|
|
|
| 2 |
C |
-0.200 |
|
|
|
| 3 |
C |
-0.419 |
|
|
|
| 4 |
F |
-0.282 |
|
|
|
| 5 |
H |
0.213 |
|
|
|
| 6 |
H |
0.205 |
|
|
|
| 7 |
H |
0.202 |
|
|
|
| 8 |
H |
0.195 |
|
|
|
| 9 |
H |
0.195 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.527 |
0.775 |
0.846 |
1.910 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.811 |
-1.146 |
-1.826 |
| y |
-1.146 |
-22.486 |
-1.017 |
| z |
-1.826 |
-1.017 |
-24.815 |
|
| Traceless |
| | x | y | z |
| x |
-2.160 |
-1.146 |
-1.826 |
| y |
-1.146 |
2.827 |
-1.017 |
| z |
-1.826 |
-1.017 |
-0.667 |
|
| Polar |
| 3z2-r2 | -1.333 |
| x2-y2 | -3.324 |
| xy | -1.146 |
| xz | -1.826 |
| yz | -1.017 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.629 |
0.202 |
-0.850 |
| y |
0.202 |
4.642 |
-0.495 |
| z |
-0.850 |
-0.495 |
3.668 |
<r2> (average value of r
2) Å
2
| <r2> |
89.621 |
| (<r2>)1/2 |
9.467 |