Jump to
S1C2
Energy calculated at wB97X-D/6-311G*
| | hartrees |
| Energy at 0K | -217.119772 |
| Energy at 298.15K | |
| HF Energy | -217.119772 |
| Nuclear repulsion energy | 116.627195 |
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 wB97X-D/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' |
3256 |
3256 |
8.89 |
53.76 |
0.73 |
0.84 |
| 2 |
A' |
3173 |
3173 |
7.54 |
158.53 |
0.16 |
0.28 |
| 3 |
A' |
3157 |
3157 |
14.22 |
26.34 |
0.74 |
0.85 |
| 4 |
A' |
3043 |
3043 |
43.82 |
161.74 |
0.11 |
0.21 |
| 5 |
A' |
1754 |
1754 |
4.44 |
21.33 |
0.14 |
0.24 |
| 6 |
A' |
1524 |
1524 |
3.88 |
15.20 |
0.62 |
0.76 |
| 7 |
A' |
1463 |
1463 |
8.60 |
11.03 |
0.55 |
0.71 |
| 8 |
A' |
1440 |
1440 |
12.29 |
6.37 |
0.75 |
0.86 |
| 9 |
A' |
1331 |
1331 |
0.13 |
17.29 |
0.33 |
0.49 |
| 10 |
A' |
1148 |
1148 |
51.91 |
1.97 |
0.75 |
0.86 |
| 11 |
A' |
1028 |
1028 |
44.33 |
4.74 |
0.70 |
0.82 |
| 12 |
A' |
921 |
921 |
1.85 |
3.90 |
0.13 |
0.22 |
| 13 |
A' |
620 |
620 |
6.57 |
1.82 |
0.74 |
0.85 |
| 14 |
A' |
274 |
274 |
2.55 |
1.22 |
0.55 |
0.71 |
| 15 |
A" |
3084 |
3084 |
38.22 |
94.41 |
0.75 |
0.86 |
| 16 |
A" |
1285 |
1285 |
0.04 |
9.03 |
0.75 |
0.86 |
| 17 |
A" |
1060 |
1060 |
13.09 |
1.34 |
0.75 |
0.86 |
| 18 |
A" |
1032 |
1032 |
11.17 |
0.11 |
0.75 |
0.86 |
| 19 |
A" |
964 |
964 |
55.35 |
1.27 |
0.75 |
0.86 |
| 20 |
A" |
565 |
565 |
12.00 |
7.61 |
0.75 |
0.86 |
| 21 |
A" |
176 |
176 |
3.08 |
4.23 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 16147.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 16147.9 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 wB97X-D/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.940 |
-0.209 |
0.000 |
| C2 |
0.000 |
0.952 |
0.000 |
| C3 |
1.320 |
0.851 |
0.000 |
| F4 |
-0.266 |
-1.415 |
0.000 |
| H5 |
1.951 |
1.734 |
0.000 |
| H6 |
1.811 |
-0.116 |
0.000 |
| H7 |
-0.482 |
1.928 |
0.000 |
| H8 |
-1.582 |
-0.185 |
0.888 |
| H9 |
-1.582 |
-0.185 |
-0.888 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4940 | 2.4970 | 1.3817 | 3.4831 | 2.7533 | 2.1856 | 1.0960 | 1.0960 |
C2 | 1.4940 | | 1.3243 | 2.3820 | 2.1015 | 2.1025 | 1.0887 | 2.1409 | 2.1409 | C3 | 2.4970 | 1.3243 | | 2.7667 | 1.0844 | 1.0842 | 2.0998 | 3.2074 | 3.2074 | F4 | 1.3817 | 2.3820 | 2.7667 | | 3.8510 | 2.4508 | 3.3502 | 2.0088 | 2.0088 | H5 | 3.4831 | 2.1015 | 1.0844 | 3.8510 | | 1.8543 | 2.4407 | 4.1171 | 4.1171 | H6 | 2.7533 | 2.1025 | 1.0842 | 2.4508 | 1.8543 | | 3.0719 | 3.5088 | 3.5088 | H7 | 2.1856 | 1.0887 | 2.0998 | 3.3502 | 2.4407 | 3.0719 | | 2.5418 | 2.5418 | H8 | 1.0960 | 2.1409 | 3.2074 | 2.0088 | 4.1171 | 3.5088 | 2.5418 | | 1.7754 | H9 | 1.0960 | 2.1409 | 3.2074 | 2.0088 | 4.1171 | 3.5088 | 2.5418 | 1.7754 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
124.645 |
|
C1 |
C2 |
H7 |
114.704 |
| C2 |
C1 |
F4 |
111.800 |
|
C2 |
C1 |
H8 |
110.569 |
| C2 |
C1 |
H9 |
110.569 |
|
C2 |
C3 |
H5 |
121.177 |
| C2 |
C3 |
H6 |
121.286 |
|
C3 |
C2 |
H7 |
120.651 |
| F4 |
C1 |
H8 |
107.788 |
|
F4 |
C1 |
H9 |
107.788 |
| H5 |
C3 |
H6 |
117.537 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.100 |
|
|
|
| 2 |
C |
-0.280 |
|
|
|
| 3 |
C |
-0.431 |
|
|
|
| 4 |
F |
-0.271 |
|
|
|
| 5 |
H |
0.219 |
|
|
|
| 6 |
H |
0.233 |
|
|
|
| 7 |
H |
0.210 |
|
|
|
| 8 |
H |
0.210 |
|
|
|
| 9 |
H |
0.210 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.916 |
1.521 |
0.000 |
1.776 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.900 |
-0.347 |
0.000 |
| y |
-0.347 |
-25.122 |
0.000 |
| z |
0.000 |
0.000 |
-25.118 |
|
| Traceless |
| | x | y | z |
| x |
4.219 |
-0.347 |
0.000 |
| y |
-0.347 |
-2.112 |
0.000 |
| z |
0.000 |
0.000 |
-2.107 |
|
| Polar |
| 3z2-r2 | -4.214 |
| x2-y2 | 4.221 |
| xy | -0.347 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.812 |
0.242 |
0.000 |
| y |
0.242 |
4.655 |
0.000 |
| z |
0.000 |
0.000 |
3.241 |
<r2> (average value of r
2) Å
2
| <r2> |
79.995 |
| (<r2>)1/2 |
8.944 |
Jump to
S1C1
Energy calculated at wB97X-D/6-311G*
| | hartrees |
| Energy at 0K | -217.118733 |
| Energy at 298.15K | |
| HF Energy | -217.118733 |
| Nuclear repulsion energy | 114.290676 |
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 wB97X-D/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 |
3238 |
3238 |
17.23 |
62.43 |
0.60 |
0.75 |
| 2 |
A |
3175 |
3175 |
8.87 |
112.24 |
0.28 |
0.44 |
| 3 |
A |
3147 |
3147 |
14.33 |
66.65 |
0.15 |
0.27 |
| 4 |
A |
3109 |
3109 |
31.89 |
72.01 |
0.74 |
0.85 |
| 5 |
A |
3055 |
3055 |
42.26 |
120.18 |
0.10 |
0.17 |
| 6 |
A |
1751 |
1751 |
0.62 |
20.91 |
0.15 |
0.26 |
| 7 |
A |
1526 |
1526 |
2.47 |
7.14 |
0.70 |
0.83 |
| 8 |
A |
1482 |
1482 |
24.91 |
9.27 |
0.64 |
0.78 |
| 9 |
A |
1417 |
1417 |
13.68 |
5.16 |
0.48 |
0.65 |
| 10 |
A |
1331 |
1331 |
0.11 |
12.62 |
0.38 |
0.55 |
| 11 |
A |
1289 |
1289 |
3.85 |
14.06 |
0.71 |
0.83 |
| 12 |
A |
1195 |
1195 |
2.07 |
1.31 |
0.74 |
0.85 |
| 13 |
A |
1066 |
1066 |
121.58 |
4.66 |
0.63 |
0.77 |
| 14 |
A |
1044 |
1044 |
28.47 |
1.78 |
0.74 |
0.85 |
| 15 |
A |
1000 |
1000 |
2.61 |
1.01 |
0.22 |
0.36 |
| 16 |
A |
974 |
974 |
60.23 |
1.10 |
0.57 |
0.72 |
| 17 |
A |
942 |
942 |
4.06 |
2.50 |
0.14 |
0.25 |
| 18 |
A |
657 |
657 |
8.53 |
4.41 |
0.64 |
0.78 |
| 19 |
A |
446 |
446 |
2.92 |
4.38 |
0.49 |
0.66 |
| 20 |
A |
334 |
334 |
7.07 |
3.26 |
0.75 |
0.86 |
| 21 |
A |
114 |
114 |
1.20 |
6.04 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 16144.6 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 16144.6 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 wB97X-D/6-311G*
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.605 |
0.440 |
0.298 |
| C2 |
0.643 |
-0.376 |
0.235 |
| C3 |
1.806 |
0.085 |
-0.204 |
| F4 |
-1.650 |
-0.232 |
-0.325 |
| H5 |
2.700 |
-0.529 |
-0.203 |
| H6 |
1.912 |
1.100 |
-0.580 |
| H7 |
0.556 |
-1.397 |
0.599 |
| H8 |
-0.910 |
0.610 |
1.336 |
| H9 |
-0.477 |
1.406 |
-0.200 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4928 | 2.4880 | 1.3902 | 3.4803 | 2.7465 | 2.1939 | 1.0951 | 1.0938 |
C2 | 1.4928 | | 1.3254 | 2.3649 | 2.1081 | 2.1100 | 1.0877 | 2.1443 | 2.1489 | C3 | 2.4880 | 1.3254 | | 3.4721 | 1.0847 | 1.0870 | 2.0990 | 3.1662 | 2.6370 | F4 | 1.3902 | 2.3649 | 3.4721 | | 4.3613 | 3.8115 | 2.6596 | 2.0042 | 2.0184 | H5 | 3.4803 | 2.1081 | 1.0847 | 4.3613 | | 1.8479 | 2.4484 | 4.0864 | 3.7194 | H6 | 2.7465 | 2.1100 | 1.0870 | 3.8115 | 1.8479 | | 3.0765 | 3.4466 | 2.4386 | H7 | 2.1939 | 1.0877 | 2.0990 | 2.6596 | 2.4484 | 3.0765 | | 2.5926 | 3.0918 | H8 | 1.0951 | 2.1443 | 3.1662 | 2.0042 | 4.0864 | 3.4466 | 2.5926 | | 1.7832 | H9 | 1.0938 | 2.1489 | 2.6370 | 2.0184 | 3.7194 | 2.4386 | 3.0918 | 1.7832 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
123.863 |
|
C1 |
C2 |
H7 |
115.573 |
| C2 |
C1 |
F4 |
110.178 |
|
C2 |
C1 |
H8 |
110.978 |
| C2 |
C1 |
H9 |
111.426 |
|
C2 |
C3 |
H5 |
121.699 |
| C2 |
C3 |
H6 |
121.688 |
|
C3 |
C2 |
H7 |
120.552 |
| F4 |
C1 |
H8 |
106.896 |
|
F4 |
C1 |
H9 |
108.107 |
| H5 |
C3 |
H6 |
116.613 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.122 |
|
|
|
| 2 |
C |
-0.228 |
|
|
|
| 3 |
C |
-0.444 |
|
|
|
| 4 |
F |
-0.278 |
|
|
|
| 5 |
H |
0.226 |
|
|
|
| 6 |
H |
0.219 |
|
|
|
| 7 |
H |
0.219 |
|
|
|
| 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 |
| |
1.513 |
0.785 |
0.845 |
1.903 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.576 |
-1.143 |
-1.847 |
| y |
-1.143 |
-22.195 |
-1.040 |
| z |
-1.847 |
-1.040 |
-24.703 |
|
| Traceless |
| | x | y | z |
| x |
-2.127 |
-1.143 |
-1.847 |
| y |
-1.143 |
2.945 |
-1.040 |
| z |
-1.847 |
-1.040 |
-0.818 |
|
| Polar |
| 3z2-r2 | -1.636 |
| x2-y2 | -3.381 |
| xy | -1.143 |
| xz | -1.847 |
| yz | -1.040 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.520 |
0.250 |
-0.835 |
| y |
0.250 |
4.604 |
-0.483 |
| z |
-0.835 |
-0.483 |
3.619 |
<r2> (average value of r
2) Å
2
| <r2> |
89.095 |
| (<r2>)1/2 |
9.439 |