Jump to
S1C2
Energy calculated at B3PW91/3-21G
| | hartrees |
| Energy at 0K | -215.873102 |
| Energy at 298.15K | |
| HF Energy | -215.873102 |
| Nuclear repulsion energy | 116.287600 |
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 B3PW91/3-21G
| 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' |
3274 |
3147 |
4.03 |
|
|
|
| 2 |
A' |
3191 |
3067 |
5.25 |
|
|
|
| 3 |
A' |
3176 |
3053 |
4.77 |
|
|
|
| 4 |
A' |
3023 |
2906 |
37.95 |
|
|
|
| 5 |
A' |
1732 |
1665 |
2.95 |
|
|
|
| 6 |
A' |
1558 |
1498 |
2.57 |
|
|
|
| 7 |
A' |
1478 |
1421 |
8.69 |
|
|
|
| 8 |
A' |
1430 |
1375 |
6.52 |
|
|
|
| 9 |
A' |
1347 |
1295 |
0.05 |
|
|
|
| 10 |
A' |
1138 |
1094 |
20.83 |
|
|
|
| 11 |
A' |
1033 |
993 |
32.45 |
|
|
|
| 12 |
A' |
912 |
877 |
1.74 |
|
|
|
| 13 |
A' |
612 |
588 |
1.94 |
|
|
|
| 14 |
A' |
296 |
284 |
4.27 |
|
|
|
| 15 |
A" |
3052 |
2933 |
40.99 |
|
|
|
| 16 |
A" |
1271 |
1221 |
0.30 |
|
|
|
| 17 |
A" |
1071 |
1029 |
0.84 |
|
|
|
| 18 |
A" |
1042 |
1002 |
23.74 |
|
|
|
| 19 |
A" |
990 |
952 |
59.26 |
|
|
|
| 20 |
A" |
585 |
563 |
16.57 |
|
|
|
| 21 |
A" |
196 |
189 |
3.63 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16203.9 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 15575.2 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 B3PW91/3-21G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
-0.972 |
0.000 |
| C2 |
-0.961 |
0.181 |
0.000 |
| C3 |
-0.538 |
1.440 |
0.000 |
| F4 |
1.337 |
-0.504 |
0.000 |
| H5 |
-1.223 |
2.281 |
0.000 |
| H6 |
0.526 |
1.649 |
0.000 |
| H7 |
-2.017 |
-0.081 |
0.000 |
| H8 |
-0.163 |
-1.600 |
0.888 |
| H9 |
-0.163 |
-1.600 |
-0.888 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.5008 | 2.4708 | 1.4165 | 3.4747 | 2.6735 | 2.2047 | 1.0999 | 1.0999 |
C2 | 1.5008 | | 1.3279 | 2.3979 | 2.1160 | 2.0899 | 1.0879 | 2.1442 | 2.1442 | C3 | 2.4708 | 1.3279 | | 2.7007 | 1.0845 | 1.0846 | 2.1213 | 3.1891 | 3.1891 | F4 | 1.4165 | 2.3979 | 2.7007 | | 3.7825 | 2.3011 | 3.3804 | 2.0593 | 2.0593 | H5 | 3.4747 | 2.1160 | 1.0845 | 3.7825 | | 1.8592 | 2.4918 | 4.1198 | 4.1198 | H6 | 2.6735 | 2.0899 | 1.0846 | 2.3011 | 1.8592 | | 3.0759 | 3.4386 | 3.4386 | H7 | 2.2047 | 1.0879 | 2.1213 | 3.3804 | 2.4918 | 3.0759 | | 2.5557 | 2.5557 | H8 | 1.0999 | 2.1442 | 3.1891 | 2.0593 | 4.1198 | 3.4386 | 2.5557 | | 1.7757 | H9 | 1.0999 | 2.1442 | 3.1891 | 2.0593 | 4.1198 | 3.4386 | 2.5557 | 1.7757 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
121.613 |
|
C1 |
C2 |
H7 |
115.871 |
| C2 |
C1 |
F4 |
110.532 |
|
C2 |
C1 |
H8 |
110.111 |
| C2 |
C1 |
H9 |
110.111 |
|
C2 |
C3 |
H5 |
122.277 |
| C2 |
C3 |
H6 |
119.723 |
|
C3 |
C2 |
H7 |
122.516 |
| F4 |
C1 |
H8 |
109.194 |
|
F4 |
C1 |
H9 |
109.194 |
| H5 |
C3 |
H6 |
118.001 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.125 |
|
|
|
| 2 |
C |
-0.278 |
|
|
|
| 3 |
C |
-0.401 |
|
|
|
| 4 |
F |
-0.296 |
|
|
|
| 5 |
H |
0.211 |
|
|
|
| 6 |
H |
0.229 |
|
|
|
| 7 |
H |
0.219 |
|
|
|
| 8 |
H |
0.220 |
|
|
|
| 9 |
H |
0.220 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.605 |
-0.654 |
0.000 |
1.733 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.470 |
1.120 |
0.000 |
| y |
1.120 |
-20.792 |
0.000 |
| z |
0.000 |
0.000 |
-25.031 |
|
| Traceless |
| | x | y | z |
| x |
-1.559 |
1.120 |
0.000 |
| y |
1.120 |
3.959 |
0.000 |
| z |
0.000 |
0.000 |
-2.401 |
|
| Polar |
| 3z2-r2 | -4.801 |
| x2-y2 | -3.678 |
| xy | 1.120 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.224 |
0.243 |
0.000 |
| y |
0.243 |
6.155 |
0.000 |
| z |
0.000 |
0.000 |
2.399 |
<r2> (average value of r
2) Å
2
| <r2> |
79.107 |
| (<r2>)1/2 |
8.894 |
Jump to
S1C1
Energy calculated at B3PW91/3-21G
| | hartrees |
| Energy at 0K | -215.869279 |
| Energy at 298.15K | |
| HF Energy | -215.869279 |
| Nuclear repulsion energy | 113.162962 |
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 B3PW91/3-21G
| 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 |
3245 |
3119 |
11.46 |
|
|
|
| 2 |
A |
3187 |
3063 |
3.68 |
|
|
|
| 3 |
A |
3157 |
3035 |
6.28 |
|
|
|
| 4 |
A |
3081 |
2962 |
33.16 |
|
|
|
| 5 |
A |
3031 |
2914 |
35.74 |
|
|
|
| 6 |
A |
1728 |
1661 |
1.04 |
|
|
|
| 7 |
A |
1560 |
1499 |
1.50 |
|
|
|
| 8 |
A |
1504 |
1445 |
13.52 |
|
|
|
| 9 |
A |
1422 |
1367 |
13.62 |
|
|
|
| 10 |
A |
1347 |
1295 |
0.16 |
|
|
|
| 11 |
A |
1276 |
1226 |
2.73 |
|
|
|
| 12 |
A |
1186 |
1140 |
0.42 |
|
|
|
| 13 |
A |
1068 |
1027 |
41.50 |
|
|
|
| 14 |
A |
1054 |
1013 |
36.35 |
|
|
|
| 15 |
A |
1016 |
977 |
4.71 |
|
|
|
| 16 |
A |
983 |
945 |
66.74 |
|
|
|
| 17 |
A |
936 |
900 |
8.37 |
|
|
|
| 18 |
A |
635 |
610 |
11.82 |
|
|
|
| 19 |
A |
452 |
434 |
2.39 |
|
|
|
| 20 |
A |
299 |
287 |
5.85 |
|
|
|
| 21 |
A |
103 |
99 |
1.54 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16134.5 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 15508.5 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 B3PW91/3-21G
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.587 |
0.478 |
0.237 |
| C2 |
0.642 |
-0.379 |
0.195 |
| C3 |
1.842 |
0.062 |
-0.173 |
| F4 |
-1.705 |
-0.248 |
-0.261 |
| H5 |
2.720 |
-0.575 |
-0.141 |
| H6 |
1.994 |
1.080 |
-0.523 |
| H7 |
0.500 |
-1.400 |
0.540 |
| H8 |
-0.803 |
0.769 |
1.275 |
| H9 |
-0.440 |
1.391 |
-0.354 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4991 | 2.4980 | 1.4230 | 3.4914 | 2.7573 | 2.1914 | 1.0994 | 1.0969 |
C2 | 1.4991 | | 1.3297 | 2.3951 | 2.1140 | 2.1149 | 1.0876 | 2.1376 | 2.1455 | C3 | 2.4980 | 1.3297 | | 3.5616 | 1.0856 | 1.0880 | 2.1086 | 3.0963 | 2.6465 | F4 | 1.4230 | 2.3951 | 3.5616 | | 4.4392 | 3.9394 | 2.6143 | 2.0511 | 2.0724 | H5 | 3.4914 | 2.1140 | 1.0856 | 4.4392 | | 1.8480 | 2.4644 | 4.0273 | 3.7277 | H6 | 2.7573 | 2.1149 | 1.0880 | 3.9394 | 1.8480 | | 3.0850 | 3.3393 | 2.4594 | H7 | 2.1914 | 1.0876 | 2.1086 | 2.6143 | 2.4644 | 3.0850 | | 2.6343 | 3.0777 | H8 | 1.0994 | 2.1376 | 3.0963 | 2.0511 | 4.0273 | 3.3393 | 2.6343 | | 1.7808 | H9 | 1.0969 | 2.1455 | 2.6465 | 2.0724 | 3.7277 | 2.4594 | 3.0777 | 1.7808 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
123.919 |
|
C1 |
C2 |
H7 |
114.885 |
| C2 |
C1 |
F4 |
110.073 |
|
C2 |
C1 |
H8 |
109.746 |
| C2 |
C1 |
H9 |
110.519 |
|
C2 |
C3 |
H5 |
121.826 |
| C2 |
C3 |
H6 |
121.713 |
|
C3 |
C2 |
H7 |
121.130 |
| F4 |
C1 |
H8 |
108.122 |
|
F4 |
C1 |
H9 |
109.975 |
| H5 |
C3 |
H6 |
116.461 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.138 |
|
|
|
| 2 |
C |
-0.243 |
|
|
|
| 3 |
C |
-0.414 |
|
|
|
| 4 |
F |
-0.302 |
|
|
|
| 5 |
H |
0.221 |
|
|
|
| 6 |
H |
0.209 |
|
|
|
| 7 |
H |
0.234 |
|
|
|
| 8 |
H |
0.220 |
|
|
|
| 9 |
H |
0.212 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.535 |
0.845 |
0.730 |
1.898 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.361 |
-1.088 |
-1.447 |
| y |
-1.088 |
-21.836 |
-0.916 |
| z |
-1.447 |
-0.916 |
-24.617 |
|
| Traceless |
| | x | y | z |
| x |
-2.135 |
-1.088 |
-1.447 |
| y |
-1.088 |
3.153 |
-0.916 |
| z |
-1.447 |
-0.916 |
-1.018 |
|
| Polar |
| 3z2-r2 | -2.036 |
| x2-y2 | -3.525 |
| xy | -1.088 |
| xz | -1.447 |
| yz | -0.916 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.996 |
0.220 |
-0.750 |
| y |
0.220 |
4.102 |
-0.517 |
| z |
-0.750 |
-0.517 |
2.721 |
<r2> (average value of r
2) Å
2
| <r2> |
90.967 |
| (<r2>)1/2 |
9.538 |