Jump to
S1C2
Energy calculated at M06-2X/6-311G**
| hartrees |
Energy at 0K | -217.102739 |
Energy at 298.15K | |
HF Energy | -217.102739 |
Nuclear repulsion energy | 116.952209 |
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 M06-2X/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' |
3271 |
3271 |
3.05 |
52.73 |
0.71 |
0.83 |
2 |
A' |
3186 |
3186 |
4.64 |
158.14 |
0.16 |
0.28 |
3 |
A' |
3173 |
3173 |
4.83 |
23.60 |
0.69 |
0.82 |
4 |
A' |
3058 |
3058 |
29.25 |
161.77 |
0.11 |
0.19 |
5 |
A' |
1749 |
1749 |
3.89 |
21.46 |
0.13 |
0.23 |
6 |
A' |
1510 |
1510 |
4.62 |
12.73 |
0.64 |
0.78 |
7 |
A' |
1451 |
1451 |
9.16 |
9.95 |
0.57 |
0.72 |
8 |
A' |
1426 |
1426 |
10.48 |
4.74 |
0.75 |
0.86 |
9 |
A' |
1319 |
1319 |
0.22 |
15.84 |
0.32 |
0.48 |
10 |
A' |
1162 |
1162 |
61.43 |
2.15 |
0.75 |
0.86 |
11 |
A' |
1027 |
1027 |
30.77 |
4.68 |
0.72 |
0.84 |
12 |
A' |
927 |
927 |
1.01 |
4.54 |
0.12 |
0.22 |
13 |
A' |
618 |
618 |
6.31 |
1.74 |
0.74 |
0.85 |
14 |
A' |
284 |
284 |
2.79 |
1.16 |
0.54 |
0.70 |
15 |
A" |
3100 |
3100 |
25.24 |
86.36 |
0.75 |
0.86 |
16 |
A" |
1280 |
1280 |
0.13 |
7.74 |
0.75 |
0.86 |
17 |
A" |
1058 |
1058 |
15.02 |
1.34 |
0.75 |
0.86 |
18 |
A" |
1032 |
1032 |
7.17 |
0.01 |
0.75 |
0.86 |
19 |
A" |
980 |
980 |
54.92 |
0.98 |
0.75 |
0.86 |
20 |
A" |
570 |
570 |
11.54 |
6.62 |
0.75 |
0.86 |
21 |
A" |
186 |
186 |
3.24 |
3.84 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 16182.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 16182.9 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 M06-2X/6-311G**
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.945 |
-0.203 |
0.000 |
C2 |
0.000 |
0.956 |
0.000 |
C3 |
1.318 |
0.829 |
0.000 |
F4 |
-0.261 |
-1.401 |
0.000 |
H5 |
1.965 |
1.697 |
0.000 |
H6 |
1.780 |
-0.151 |
0.000 |
H7 |
-0.468 |
1.937 |
0.000 |
H8 |
-1.585 |
-0.180 |
0.888 |
H9 |
-1.585 |
-0.180 |
-0.888 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
C1 | | 1.4951 | 2.4875 | 1.3800 | 3.4755 | 2.7256 | 2.1922 | 1.0946 | 1.0946 |
C2 | 1.4951 | | 1.3243 | 2.3714 | 2.1003 | 2.0957 | 1.0869 | 2.1421 | 2.1421 | C3 | 2.4875 | 1.3243 | | 2.7329 | 1.0825 | 1.0831 | 2.1016 | 3.1990 | 3.1990 | F4 | 1.3800 | 2.3714 | 2.7329 | | 3.8152 | 2.3937 | 3.3445 | 2.0085 | 2.0085 | H5 | 3.4755 | 2.1003 | 1.0825 | 3.8152 | | 1.8570 | 2.4446 | 4.1124 | 4.1124 | H6 | 2.7256 | 2.0957 | 1.0831 | 2.3937 | 1.8570 | | 3.0675 | 3.4802 | 3.4802 | H7 | 2.1922 | 1.0869 | 2.1016 | 3.3445 | 2.4446 | 3.0675 | | 2.5524 | 2.5524 | H8 | 1.0946 | 2.1421 | 3.1990 | 2.0085 | 4.1124 | 3.4802 | 2.5524 | | 1.7757 | H9 | 1.0946 | 2.1421 | 3.1990 | 2.0085 | 4.1124 | 3.4802 | 2.5524 | 1.7757 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
C3 |
123.725 |
|
C1 |
C2 |
H7 |
115.300 |
C2 |
C1 |
F4 |
111.071 |
|
C2 |
C1 |
H8 |
110.665 |
C2 |
C1 |
H9 |
110.665 |
|
C2 |
C3 |
H5 |
121.211 |
C2 |
C3 |
H6 |
120.719 |
|
C3 |
C2 |
H7 |
120.975 |
F4 |
C1 |
H8 |
107.959 |
|
F4 |
C1 |
H9 |
107.959 |
H5 |
C3 |
H6 |
118.069 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.093 |
|
|
|
2 |
C |
-0.262 |
|
|
|
3 |
C |
-0.236 |
|
|
|
4 |
F |
-0.284 |
|
|
|
5 |
H |
0.135 |
|
|
|
6 |
H |
0.148 |
|
|
|
7 |
H |
0.138 |
|
|
|
8 |
H |
0.133 |
|
|
|
9 |
H |
0.133 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.927 |
1.509 |
0.000 |
1.770 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-21.038 |
-0.305 |
0.000 |
y |
-0.305 |
-25.265 |
0.000 |
z |
0.000 |
0.000 |
-25.189 |
|
Traceless |
| x | y | z |
x |
4.189 |
-0.305 |
0.000 |
y |
-0.305 |
-2.151 |
0.000 |
z |
0.000 |
0.000 |
-2.037 |
|
Polar |
3z2-r2 | -4.075 |
x2-y2 | 4.227 |
xy | -0.305 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
6.763 |
0.225 |
0.000 |
y |
0.225 |
4.675 |
0.000 |
z |
0.000 |
0.000 |
3.314 |
<r2> (average value of r
2) Å
2
<r2> |
79.375 |
(<r2>)1/2 |
8.909 |
Jump to
S1C1
Energy calculated at M06-2X/6-311G**
| hartrees |
Energy at 0K | -217.100929 |
Energy at 298.15K | |
HF Energy | -217.100929 |
Nuclear repulsion energy | 114.436275 |
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 M06-2X/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 |
3255 |
3255 |
7.87 |
60.72 |
0.60 |
0.75 |
2 |
A |
3186 |
3186 |
4.37 |
107.44 |
0.27 |
0.42 |
3 |
A |
3163 |
3163 |
5.92 |
68.45 |
0.14 |
0.25 |
4 |
A |
3122 |
3122 |
21.79 |
66.41 |
0.73 |
0.84 |
5 |
A |
3068 |
3068 |
29.29 |
122.11 |
0.09 |
0.17 |
6 |
A |
1749 |
1749 |
0.56 |
20.87 |
0.14 |
0.25 |
7 |
A |
1512 |
1512 |
2.39 |
6.24 |
0.73 |
0.84 |
8 |
A |
1469 |
1469 |
25.28 |
8.04 |
0.65 |
0.79 |
9 |
A |
1405 |
1405 |
12.52 |
4.45 |
0.46 |
0.63 |
10 |
A |
1315 |
1315 |
0.12 |
12.19 |
0.38 |
0.55 |
11 |
A |
1283 |
1283 |
3.59 |
11.63 |
0.72 |
0.84 |
12 |
A |
1186 |
1186 |
2.46 |
1.57 |
0.70 |
0.82 |
13 |
A |
1102 |
1102 |
122.21 |
4.74 |
0.61 |
0.75 |
14 |
A |
1046 |
1046 |
19.06 |
1.42 |
0.75 |
0.85 |
15 |
A |
998 |
998 |
5.85 |
1.19 |
0.26 |
0.42 |
16 |
A |
986 |
986 |
56.76 |
1.02 |
0.36 |
0.53 |
17 |
A |
934 |
934 |
3.00 |
2.49 |
0.14 |
0.25 |
18 |
A |
660 |
660 |
8.40 |
3.89 |
0.62 |
0.77 |
19 |
A |
445 |
445 |
2.86 |
4.26 |
0.48 |
0.65 |
20 |
A |
331 |
331 |
6.77 |
2.83 |
0.75 |
0.86 |
21 |
A |
116 |
116 |
1.21 |
5.58 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 16165.1 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 16165.1 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 M06-2X/6-311G**
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.605 |
0.444 |
0.295 |
C2 |
0.642 |
-0.378 |
0.235 |
C3 |
1.804 |
0.085 |
-0.202 |
F4 |
-1.646 |
-0.233 |
-0.322 |
H5 |
2.697 |
-0.527 |
-0.203 |
H6 |
1.902 |
1.101 |
-0.573 |
H7 |
0.548 |
-1.399 |
0.594 |
H8 |
-0.906 |
0.621 |
1.331 |
H9 |
-0.468 |
1.402 |
-0.212 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
C1 | | 1.4941 | 2.4851 | 1.3871 | 3.4771 | 2.7331 | 2.1942 | 1.0938 | 1.0924 |
C2 | 1.4941 | | 1.3252 | 2.3592 | 2.1065 | 2.1045 | 1.0864 | 2.1438 | 2.1449 | C3 | 2.4851 | 1.3252 | | 3.4668 | 1.0830 | 1.0855 | 2.1010 | 3.1593 | 2.6261 | F4 | 1.3871 | 2.3592 | 3.4668 | | 4.3547 | 3.7995 | 2.6484 | 2.0027 | 2.0184 | H5 | 3.4771 | 2.1065 | 1.0830 | 4.3547 | | 1.8491 | 2.4520 | 4.0808 | 3.7069 | H6 | 2.7331 | 2.1045 | 1.0855 | 3.7995 | 1.8491 | | 3.0734 | 3.4268 | 2.4169 | H7 | 2.1942 | 1.0864 | 2.1010 | 2.6484 | 2.4520 | 3.0734 | | 2.5958 | 3.0869 | H8 | 1.0938 | 2.1438 | 3.1593 | 2.0027 | 4.0808 | 3.4268 | 2.5958 | | 1.7839 | H9 | 1.0924 | 2.1449 | 2.6261 | 2.0184 | 3.7069 | 2.4169 | 3.0869 | 1.7839 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
C3 |
123.526 |
|
C1 |
C2 |
H7 |
115.583 |
C2 |
C1 |
F4 |
109.877 |
|
C2 |
C1 |
H8 |
110.924 |
C2 |
C1 |
H9 |
111.090 |
|
C2 |
C3 |
H5 |
121.699 |
C2 |
C3 |
H6 |
121.295 |
|
C3 |
C2 |
H7 |
120.882 |
F4 |
C1 |
H8 |
107.064 |
|
F4 |
C1 |
H9 |
108.399 |
H5 |
C3 |
H6 |
117.005 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.070 |
|
|
|
2 |
C |
-0.206 |
|
|
|
3 |
C |
-0.250 |
|
|
|
4 |
F |
-0.289 |
|
|
|
5 |
H |
0.141 |
|
|
|
6 |
H |
0.135 |
|
|
|
7 |
H |
0.146 |
|
|
|
8 |
H |
0.129 |
|
|
|
9 |
H |
0.123 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
1.509 |
0.803 |
0.832 |
1.901 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-25.715 |
-1.155 |
-1.832 |
y |
-1.155 |
-22.359 |
-0.988 |
z |
-1.832 |
-0.988 |
-24.799 |
|
Traceless |
| x | y | z |
x |
-2.136 |
-1.155 |
-1.832 |
y |
-1.155 |
2.898 |
-0.988 |
z |
-1.832 |
-0.988 |
-0.761 |
|
Polar |
3z2-r2 | -1.523 |
x2-y2 | -3.356 |
xy | -1.155 |
xz | -1.832 |
yz | -0.988 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
6.505 |
0.231 |
-0.800 |
y |
0.231 |
4.616 |
-0.460 |
z |
-0.800 |
-0.460 |
3.669 |
<r2> (average value of r
2) Å
2
<r2> |
88.923 |
(<r2>)1/2 |
9.430 |