Jump to
S1C2
Energy calculated at HSEh1PBE/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -377.333432 |
| Energy at 298.15K | |
| HF Energy | -377.333432 |
| Nuclear repulsion energy | 191.426324 |
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 HSEh1PBE/6-311+G(3df,2p)
| 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 |
3131 |
3131 |
16.99 |
34.32 |
0.68 |
0.81 |
| 2 |
A |
3086 |
3086 |
23.22 |
82.89 |
0.29 |
0.45 |
| 3 |
A |
3067 |
3067 |
14.90 |
128.96 |
0.06 |
0.11 |
| 4 |
A |
1490 |
1490 |
6.24 |
3.82 |
0.74 |
0.85 |
| 5 |
A |
1453 |
1453 |
14.08 |
1.43 |
0.48 |
0.65 |
| 6 |
A |
1396 |
1396 |
15.71 |
2.32 |
0.74 |
0.85 |
| 7 |
A |
1341 |
1341 |
10.61 |
1.43 |
0.75 |
0.86 |
| 8 |
A |
1270 |
1270 |
14.47 |
3.61 |
0.68 |
0.81 |
| 9 |
A |
1171 |
1171 |
89.34 |
3.95 |
0.54 |
0.70 |
| 10 |
A |
1138 |
1138 |
7.47 |
1.88 |
0.47 |
0.64 |
| 11 |
A |
1126 |
1126 |
278.33 |
0.09 |
0.58 |
0.73 |
| 12 |
A |
1104 |
1104 |
19.86 |
6.24 |
0.39 |
0.56 |
| 13 |
A |
914 |
914 |
31.61 |
4.04 |
0.26 |
0.41 |
| 14 |
A |
583 |
583 |
3.47 |
1.81 |
0.26 |
0.41 |
| 15 |
A |
478 |
478 |
18.06 |
0.52 |
0.73 |
0.85 |
| 16 |
A |
429 |
429 |
5.21 |
1.30 |
0.41 |
0.59 |
| 17 |
A |
243 |
243 |
7.89 |
0.06 |
0.53 |
0.69 |
| 18 |
A |
118 |
118 |
8.07 |
0.04 |
0.70 |
0.83 |
Unscaled Zero Point Vibrational Energy (zpe) 11769.2 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 11769.2 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 HSEh1PBE/6-311+G(3df,2p)
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.775 |
-0.583 |
-0.284 |
| C2 |
0.467 |
0.020 |
0.325 |
| F3 |
-1.875 |
0.112 |
0.152 |
| F4 |
1.523 |
-0.762 |
-0.006 |
| F5 |
0.687 |
1.253 |
-0.181 |
| H6 |
-0.716 |
-0.519 |
-1.373 |
| H7 |
-0.865 |
-1.625 |
0.027 |
| H8 |
0.415 |
0.103 |
1.414 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
F5 |
H6 |
H7 |
H8 |
| C1 | | 1.5087 | 1.3721 | 2.3221 | 2.3489 | 1.0921 | 1.0918 | 2.1841 |
C2 | 1.5087 | | 2.3499 | 1.3559 | 1.3508 | 2.1378 | 2.1375 | 1.0934 | F3 | 1.3721 | 2.3499 | | 3.5127 | 2.8246 | 2.0166 | 2.0131 | 2.6146 | F4 | 2.3221 | 1.3559 | 3.5127 | | 2.1886 | 2.6343 | 2.5399 | 1.9990 | F5 | 2.3489 | 1.3508 | 2.8246 | 2.1886 | | 2.5544 | 3.2766 | 1.9849 | H6 | 1.0921 | 2.1378 | 2.0166 | 2.6343 | 2.5544 | | 1.7909 | 3.0710 | H7 | 1.0918 | 2.1375 | 2.0131 | 2.5399 | 3.2766 | 1.7909 | | 2.5592 | H8 | 2.1841 | 1.0934 | 2.6146 | 1.9990 | 1.9849 | 3.0710 | 2.5592 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
108.196 |
|
C1 |
C2 |
F5 |
110.341 |
| C1 |
C2 |
H8 |
113.181 |
|
C2 |
C1 |
F3 |
109.223 |
| C2 |
C1 |
H6 |
109.529 |
|
C2 |
C1 |
H7 |
109.524 |
| F3 |
C1 |
H6 |
109.318 |
|
F3 |
C1 |
H7 |
109.050 |
| F4 |
C2 |
F5 |
107.912 |
|
F4 |
C2 |
H8 |
108.933 |
| F5 |
C2 |
H8 |
108.144 |
|
H6 |
C1 |
H7 |
110.178 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.161 |
|
|
|
| 2 |
C |
0.750 |
|
|
|
| 3 |
F |
-0.435 |
|
|
|
| 4 |
F |
-0.439 |
|
|
|
| 5 |
F |
-0.444 |
|
|
|
| 6 |
H |
0.143 |
|
|
|
| 7 |
H |
0.136 |
|
|
|
| 8 |
H |
0.129 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.293 |
-1.468 |
0.367 |
1.541 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.527 |
1.714 |
1.560 |
| y |
1.714 |
-28.078 |
0.516 |
| z |
1.560 |
0.516 |
-24.909 |
|
| Traceless |
| | x | y | z |
| x |
-6.034 |
1.714 |
1.560 |
| y |
1.714 |
0.640 |
0.516 |
| z |
1.560 |
0.516 |
5.394 |
|
| Polar |
| 3z2-r2 | 10.787 |
| x2-y2 | -4.449 |
| xy | 1.714 |
| xz | 1.560 |
| yz | 0.516 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.546 |
-0.050 |
-0.011 |
| y |
-0.050 |
4.385 |
0.060 |
| z |
-0.011 |
0.060 |
4.131 |
<r2> (average value of r
2) Å
2
| <r2> |
110.861 |
| (<r2>)1/2 |
10.529 |
Jump to
S1C1
Energy calculated at HSEh1PBE/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -377.331619 |
| Energy at 298.15K | |
| HF Energy | -377.331619 |
| Nuclear repulsion energy | 194.138071 |
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 HSEh1PBE/6-311+G(3df,2p)
| 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' |
3066 |
3066 |
54.07 |
156.38 |
0.02 |
0.03 |
| 2 |
A' |
3052 |
3052 |
1.97 |
44.69 |
0.69 |
0.82 |
| 3 |
A' |
1483 |
1483 |
7.60 |
3.63 |
0.73 |
0.85 |
| 4 |
A' |
1432 |
1432 |
20.82 |
2.08 |
0.31 |
0.47 |
| 5 |
A' |
1408 |
1408 |
15.96 |
1.48 |
0.67 |
0.80 |
| 6 |
A' |
1201 |
1201 |
125.87 |
4.09 |
0.16 |
0.27 |
| 7 |
A' |
1123 |
1123 |
30.34 |
3.40 |
0.75 |
0.86 |
| 8 |
A' |
881 |
881 |
28.37 |
6.73 |
0.12 |
0.22 |
| 9 |
A' |
770 |
770 |
50.55 |
2.21 |
0.45 |
0.62 |
| 10 |
A' |
522 |
522 |
12.00 |
1.03 |
0.75 |
0.85 |
| 11 |
A' |
235 |
235 |
1.50 |
0.19 |
0.35 |
0.52 |
| 12 |
A" |
3115 |
3115 |
13.51 |
48.37 |
0.75 |
0.86 |
| 13 |
A" |
1386 |
1386 |
21.35 |
1.08 |
0.75 |
0.86 |
| 14 |
A" |
1287 |
1287 |
20.14 |
6.58 |
0.75 |
0.86 |
| 15 |
A" |
1146 |
1146 |
127.25 |
1.52 |
0.75 |
0.86 |
| 16 |
A" |
956 |
956 |
58.88 |
2.03 |
0.75 |
0.86 |
| 17 |
A" |
369 |
369 |
0.43 |
0.21 |
0.75 |
0.86 |
| 18 |
A" |
117 |
117 |
1.97 |
0.08 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 11773.6 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 11773.6 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 HSEh1PBE/6-311+G(3df,2p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.732 |
-0.834 |
0.000 |
| C2 |
0.354 |
0.626 |
0.000 |
| F3 |
-0.385 |
-1.622 |
0.000 |
| F4 |
-0.385 |
0.927 |
1.091 |
| F5 |
-0.385 |
0.927 |
-1.091 |
| H6 |
1.322 |
-1.051 |
-0.894 |
| H7 |
1.322 |
-1.051 |
0.894 |
| H8 |
1.245 |
1.263 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
F5 |
H6 |
H7 |
H8 |
| C1 | | 1.5077 | 1.3668 | 2.3531 | 2.3531 | 1.0929 | 1.0929 | 2.1592 |
C2 | 1.5077 | | 2.3660 | 1.3517 | 1.3517 | 2.1324 | 2.1324 | 1.0959 | F3 | 1.3668 | 2.3660 | | 2.7722 | 2.7722 | 2.0096 | 2.0096 | 3.3140 | F4 | 2.3531 | 1.3517 | 2.7722 | | 2.1816 | 3.2810 | 2.6201 | 1.9905 | F5 | 2.3531 | 1.3517 | 2.7722 | 2.1816 | | 2.6201 | 3.2810 | 1.9905 | H6 | 1.0929 | 2.1324 | 2.0096 | 3.2810 | 2.6201 | | 1.7876 | 2.4822 | H7 | 1.0929 | 2.1324 | 2.0096 | 2.6201 | 3.2810 | 1.7876 | | 2.4822 | H8 | 2.1592 | 1.0959 | 3.3140 | 1.9905 | 1.9905 | 2.4822 | 2.4822 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
110.645 |
|
C1 |
C2 |
F5 |
110.645 |
| C1 |
C2 |
H8 |
111.074 |
|
C2 |
C1 |
F3 |
110.702 |
| C2 |
C1 |
H6 |
109.127 |
|
C2 |
C1 |
H7 |
109.127 |
| F3 |
C1 |
H6 |
109.067 |
|
F3 |
C1 |
H7 |
109.067 |
| F4 |
C2 |
F5 |
107.603 |
|
F4 |
C2 |
H8 |
108.380 |
| F5 |
C2 |
H8 |
108.380 |
|
H6 |
C1 |
H7 |
109.739 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.146 |
|
|
|
| 2 |
C |
0.790 |
|
|
|
| 3 |
F |
-0.448 |
|
|
|
| 4 |
F |
-0.442 |
|
|
|
| 5 |
F |
-0.442 |
|
|
|
| 6 |
H |
0.136 |
|
|
|
| 7 |
H |
0.136 |
|
|
|
| 8 |
H |
0.123 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
3.162 |
0.049 |
0.000 |
3.162 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.438 |
-0.371 |
0.000 |
| y |
-0.371 |
-28.919 |
0.000 |
| z |
0.000 |
0.000 |
-28.728 |
|
| Traceless |
| | x | y | z |
| x |
3.385 |
-0.371 |
0.000 |
| y |
-0.371 |
-1.836 |
0.000 |
| z |
0.000 |
0.000 |
-1.549 |
|
| Polar |
| 3z2-r2 | -3.098 |
| x2-y2 | 3.481 |
| xy | -0.371 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.345 |
-0.020 |
0.000 |
| y |
-0.020 |
4.435 |
0.000 |
| z |
0.000 |
0.000 |
4.297 |
<r2> (average value of r
2) Å
2
| <r2> |
102.790 |
| (<r2>)1/2 |
10.139 |