Jump to
S1C2
Energy calculated at B2PLYP/6-311G*
| | hartrees |
| Energy at 0K | -216.978114 |
| Energy at 298.15K | |
| HF Energy | -216.779498 |
| Nuclear repulsion energy | 116.427764 |
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 B2PLYP/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' |
3269 |
3269 |
8.66 |
54.74 |
0.73 |
0.84 |
| 2 |
A' |
3182 |
3182 |
6.17 |
152.59 |
0.15 |
0.26 |
| 3 |
A' |
3166 |
3166 |
14.68 |
38.57 |
0.61 |
0.76 |
| 4 |
A' |
3055 |
3055 |
42.67 |
161.23 |
0.11 |
0.21 |
| 5 |
A' |
1722 |
1722 |
3.55 |
13.23 |
0.10 |
0.19 |
| 6 |
A' |
1536 |
1536 |
2.62 |
15.79 |
0.61 |
0.76 |
| 7 |
A' |
1468 |
1468 |
7.03 |
9.53 |
0.52 |
0.69 |
| 8 |
A' |
1444 |
1444 |
14.01 |
7.18 |
0.74 |
0.85 |
| 9 |
A' |
1330 |
1330 |
0.11 |
16.58 |
0.32 |
0.48 |
| 10 |
A' |
1142 |
1142 |
43.78 |
2.14 |
0.75 |
0.85 |
| 11 |
A' |
1022 |
1022 |
45.02 |
4.74 |
0.71 |
0.83 |
| 12 |
A' |
920 |
920 |
2.45 |
4.09 |
0.13 |
0.22 |
| 13 |
A' |
615 |
615 |
6.28 |
1.75 |
0.74 |
0.85 |
| 14 |
A' |
272 |
272 |
2.64 |
1.11 |
0.53 |
0.69 |
| 15 |
A" |
3095 |
3095 |
38.22 |
94.11 |
0.75 |
0.86 |
| 16 |
A" |
1283 |
1283 |
0.03 |
9.05 |
0.75 |
0.86 |
| 17 |
A" |
1061 |
1061 |
12.01 |
0.64 |
0.75 |
0.86 |
| 18 |
A" |
1026 |
1026 |
17.20 |
0.16 |
0.75 |
0.86 |
| 19 |
A" |
941 |
941 |
46.26 |
1.00 |
0.75 |
0.86 |
| 20 |
A" |
562 |
562 |
11.29 |
7.81 |
0.75 |
0.86 |
| 21 |
A" |
175 |
175 |
3.00 |
4.13 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 16142.4 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 16142.4 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 B2PLYP/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.945 |
-0.204 |
0.000 |
| C2 |
0.000 |
0.956 |
0.000 |
| C3 |
1.326 |
0.843 |
0.000 |
| F4 |
-0.267 |
-1.415 |
0.000 |
| H5 |
1.964 |
1.718 |
0.000 |
| H6 |
1.806 |
-0.127 |
0.000 |
| H7 |
-0.474 |
1.935 |
0.000 |
| H8 |
-1.587 |
-0.181 |
0.887 |
| H9 |
-1.587 |
-0.181 |
-0.887 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4957 | 2.5007 | 1.3881 | 3.4863 | 2.7524 | 2.1894 | 1.0946 | 1.0946 |
C2 | 1.4957 | | 1.3307 | 2.3855 | 2.1065 | 2.1057 | 1.0878 | 2.1439 | 2.1439 | C3 | 2.5007 | 1.3307 | | 2.7635 | 1.0829 | 1.0824 | 2.1052 | 3.2122 | 3.2122 | F4 | 1.3881 | 2.3855 | 2.7635 | | 3.8463 | 2.4409 | 3.3559 | 2.0120 | 2.0120 | H5 | 3.4863 | 2.1065 | 1.0829 | 3.8463 | | 1.8519 | 2.4475 | 4.1230 | 4.1230 | H6 | 2.7524 | 2.1057 | 1.0824 | 2.4409 | 1.8519 | | 3.0741 | 3.5071 | 3.5071 | H7 | 2.1894 | 1.0878 | 2.1052 | 3.3559 | 2.4475 | 3.0741 | | 2.5496 | 2.5496 | H8 | 1.0946 | 2.1439 | 3.2122 | 2.0120 | 4.1230 | 3.5071 | 2.5496 | | 1.7734 | H9 | 1.0946 | 2.1439 | 3.2122 | 2.0120 | 4.1230 | 3.5071 | 2.5496 | 1.7734 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
124.343 |
|
C1 |
C2 |
H7 |
114.957 |
| C2 |
C1 |
F4 |
111.578 |
|
C2 |
C1 |
H8 |
110.768 |
| C2 |
C1 |
H9 |
110.768 |
|
C2 |
C3 |
H5 |
121.232 |
| C2 |
C3 |
H6 |
121.188 |
|
C3 |
C2 |
H7 |
120.700 |
| F4 |
C1 |
H8 |
107.688 |
|
F4 |
C1 |
H9 |
107.688 |
| H5 |
C3 |
H6 |
117.581 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.081 |
|
|
|
| 2 |
C |
-0.270 |
|
|
|
| 3 |
C |
-0.412 |
|
|
|
| 4 |
F |
-0.281 |
|
|
|
| 5 |
H |
0.212 |
|
|
|
| 6 |
H |
0.224 |
|
|
|
| 7 |
H |
0.200 |
|
|
|
| 8 |
H |
0.204 |
|
|
|
| 9 |
H |
0.204 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.899 |
1.522 |
0.000 |
1.768 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-21.215 |
-0.364 |
0.006 |
| y |
-0.364 |
-25.413 |
-0.006 |
| z |
0.006 |
-0.006 |
-25.312 |
|
| Traceless |
| | x | y | z |
| x |
4.148 |
-0.364 |
0.006 |
| y |
-0.364 |
-2.150 |
-0.006 |
| z |
0.006 |
-0.006 |
-1.998 |
|
| Polar |
| 3z2-r2 | -3.996 |
| x2-y2 | 4.199 |
| xy | -0.364 |
| xz | 0.006 |
| yz | -0.006 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.711 |
0.224 |
-0.001 |
| y |
0.224 |
4.666 |
0.000 |
| z |
-0.001 |
0.000 |
3.220 |
<r2> (average value of r
2) Å
2
| <r2> |
80.266 |
| (<r2>)1/2 |
8.959 |
Jump to
S1C1
Energy calculated at B2PLYP/6-311G*
| | hartrees |
| Energy at 0K | -216.977101 |
| Energy at 298.15K | |
| HF Energy | -216.778458 |
| Nuclear repulsion energy | 114.043868 |
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 B2PLYP/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 |
3250 |
3250 |
17.07 |
63.87 |
0.61 |
0.76 |
| 2 |
A |
3182 |
3182 |
9.33 |
111.46 |
0.27 |
0.43 |
| 3 |
A |
3160 |
3160 |
13.11 |
72.73 |
0.15 |
0.27 |
| 4 |
A |
3124 |
3124 |
29.97 |
72.15 |
0.74 |
0.85 |
| 5 |
A |
3070 |
3070 |
41.28 |
119.63 |
0.10 |
0.18 |
| 6 |
A |
1719 |
1719 |
0.48 |
13.60 |
0.12 |
0.22 |
| 7 |
A |
1538 |
1538 |
1.91 |
7.34 |
0.71 |
0.83 |
| 8 |
A |
1486 |
1486 |
22.07 |
9.54 |
0.62 |
0.76 |
| 9 |
A |
1421 |
1421 |
14.68 |
4.49 |
0.50 |
0.67 |
| 10 |
A |
1329 |
1329 |
0.11 |
12.71 |
0.38 |
0.55 |
| 11 |
A |
1288 |
1288 |
3.75 |
13.79 |
0.71 |
0.83 |
| 12 |
A |
1198 |
1198 |
2.22 |
1.34 |
0.74 |
0.85 |
| 13 |
A |
1049 |
1049 |
103.19 |
4.65 |
0.60 |
0.75 |
| 14 |
A |
1032 |
1032 |
46.29 |
1.69 |
0.70 |
0.83 |
| 15 |
A |
1000 |
1000 |
3.71 |
0.99 |
0.18 |
0.30 |
| 16 |
A |
953 |
953 |
49.40 |
1.02 |
0.46 |
0.63 |
| 17 |
A |
941 |
941 |
2.81 |
2.67 |
0.17 |
0.29 |
| 18 |
A |
655 |
655 |
7.76 |
4.41 |
0.62 |
0.77 |
| 19 |
A |
439 |
439 |
2.80 |
4.24 |
0.49 |
0.66 |
| 20 |
A |
332 |
332 |
7.24 |
3.37 |
0.75 |
0.86 |
| 21 |
A |
116 |
116 |
1.17 |
5.70 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 16141.6 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 16141.6 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 B2PLYP/6-311G*
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.605 |
0.440 |
0.308 |
| C2 |
0.644 |
-0.375 |
0.246 |
| C3 |
1.807 |
0.086 |
-0.211 |
| F4 |
-1.649 |
-0.232 |
-0.336 |
| H5 |
2.701 |
-0.525 |
-0.214 |
| H6 |
1.907 |
1.096 |
-0.596 |
| H7 |
0.561 |
-1.393 |
0.617 |
| H8 |
-0.924 |
0.599 |
1.342 |
| H9 |
-0.475 |
1.407 |
-0.182 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4931 | 2.4928 | 1.3982 | 3.4838 | 2.7495 | 2.1948 | 1.0934 | 1.0919 |
C2 | 1.4931 | | 1.3321 | 2.3694 | 2.1132 | 2.1140 | 1.0866 | 2.1471 | 2.1476 | C3 | 2.4928 | 1.3321 | | 3.4727 | 1.0832 | 1.0853 | 2.1039 | 3.1835 | 2.6370 | F4 | 1.3982 | 2.3694 | 3.4727 | | 4.3614 | 3.8049 | 2.6720 | 2.0073 | 2.0225 | H5 | 3.4838 | 2.1132 | 1.0832 | 4.3614 | | 1.8454 | 2.4540 | 4.1020 | 3.7180 | H6 | 2.7495 | 2.1140 | 1.0853 | 3.8049 | 1.8454 | | 3.0788 | 3.4667 | 2.4378 | H7 | 2.1948 | 1.0866 | 2.1039 | 2.6720 | 2.4540 | 3.0788 | | 2.5884 | 3.0910 | H8 | 1.0934 | 2.1471 | 3.1835 | 2.0073 | 4.1020 | 3.4667 | 2.5884 | | 1.7819 | H9 | 1.0919 | 2.1476 | 2.6370 | 2.0225 | 3.7180 | 2.4378 | 3.0910 | 1.7819 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
123.756 |
|
C1 |
C2 |
H7 |
115.697 |
| C2 |
C1 |
F4 |
110.026 |
|
C2 |
C1 |
H8 |
111.283 |
| C2 |
C1 |
H9 |
111.416 |
|
C2 |
C3 |
H5 |
121.726 |
| C2 |
C3 |
H6 |
121.634 |
|
C3 |
C2 |
H7 |
120.540 |
| F4 |
C1 |
H8 |
106.698 |
|
F4 |
C1 |
H9 |
107.993 |
| H5 |
C3 |
H6 |
116.639 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.103 |
|
|
|
| 2 |
C |
-0.216 |
|
|
|
| 3 |
C |
-0.427 |
|
|
|
| 4 |
F |
-0.288 |
|
|
|
| 5 |
H |
0.219 |
|
|
|
| 6 |
H |
0.210 |
|
|
|
| 7 |
H |
0.209 |
|
|
|
| 8 |
H |
0.198 |
|
|
|
| 9 |
H |
0.198 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.539 |
0.778 |
0.858 |
1.926 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.862 |
-1.126 |
-1.862 |
| y |
-1.126 |
-22.515 |
-1.013 |
| z |
-1.862 |
-1.013 |
-24.876 |
|
| Traceless |
| | x | y | z |
| x |
-2.166 |
-1.126 |
-1.862 |
| y |
-1.126 |
2.854 |
-1.013 |
| z |
-1.862 |
-1.013 |
-0.688 |
|
| Polar |
| 3z2-r2 | -1.376 |
| x2-y2 | -3.347 |
| xy | -1.126 |
| xz | -1.862 |
| yz | -1.013 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.463 |
0.220 |
-0.825 |
| y |
0.220 |
4.583 |
-0.486 |
| z |
-0.825 |
-0.486 |
3.614 |
<r2> (average value of r
2) Å
2
| <r2> |
89.444 |
| (<r2>)1/2 |
9.457 |