Jump to
S1C2
Energy calculated at TPSSh/STO-3G
| | hartrees |
| Energy at 0K | -215.553932 |
| Energy at 298.15K | -215.561511 |
| HF Energy | -215.553932 |
| Nuclear repulsion energy | 125.271067 |
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 TPSSh/STO-3G
| 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' |
3485 |
3485 |
1.97 |
|
|
|
| 2 |
A' |
3348 |
3348 |
3.64 |
|
|
|
| 3 |
A' |
3318 |
3318 |
2.47 |
|
|
|
| 4 |
A' |
3216 |
3216 |
18.75 |
|
|
|
| 5 |
A' |
1704 |
1704 |
1.70 |
|
|
|
| 6 |
A' |
1682 |
1682 |
0.16 |
|
|
|
| 7 |
A' |
1664 |
1664 |
0.40 |
|
|
|
| 8 |
A' |
1581 |
1581 |
0.17 |
|
|
|
| 9 |
A' |
1536 |
1536 |
9.34 |
|
|
|
| 10 |
A' |
1436 |
1436 |
14.39 |
|
|
|
| 11 |
A' |
1217 |
1217 |
7.70 |
|
|
|
| 12 |
A' |
1173 |
1173 |
9.93 |
|
|
|
| 13 |
A' |
1112 |
1112 |
0.65 |
|
|
|
| 14 |
A' |
954 |
954 |
7.82 |
|
|
|
| 15 |
A' |
442 |
442 |
1.26 |
|
|
|
| 16 |
A' |
269 |
269 |
0.54 |
|
|
|
| 17 |
A" |
3486 |
3486 |
3.93 |
|
|
|
| 18 |
A" |
3454 |
3454 |
1.96 |
|
|
|
| 19 |
A" |
3310 |
3310 |
17.97 |
|
|
|
| 20 |
A" |
1698 |
1698 |
3.18 |
|
|
|
| 21 |
A" |
1413 |
1413 |
0.06 |
|
|
|
| 22 |
A" |
1362 |
1362 |
0.70 |
|
|
|
| 23 |
A" |
1246 |
1246 |
1.68 |
|
|
|
| 24 |
A" |
957 |
957 |
1.83 |
|
|
|
| 25 |
A" |
794 |
794 |
3.18 |
|
|
|
| 26 |
A" |
225 |
225 |
0.00 |
|
|
|
| 27 |
A" |
110 |
110 |
0.73 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 23094.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 23094.9 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 TPSSh/STO-3G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.141 |
-0.802 |
0.000 |
| C2 |
0.000 |
0.766 |
0.000 |
| C3 |
-1.491 |
1.203 |
0.000 |
| F4 |
1.493 |
-1.207 |
0.000 |
| H5 |
-0.383 |
-1.211 |
0.901 |
| H6 |
-0.383 |
-1.211 |
-0.901 |
| H7 |
0.509 |
1.173 |
-0.892 |
| H8 |
0.509 |
1.173 |
0.892 |
| H9 |
-1.571 |
2.302 |
0.000 |
| H10 |
-2.009 |
0.818 |
-0.893 |
| H11 |
-2.009 |
0.818 |
0.893 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
H11 |
| C1 | | 1.5746 | 2.5853 | 1.4109 | 1.1197 | 1.1197 | 2.1979 | 2.1979 | 3.5446 | 2.8365 | 2.8365 |
C2 | 1.5746 | | 1.5537 | 2.4740 | 2.2064 | 2.2064 | 1.1046 | 1.1046 | 2.1966 | 2.1992 | 2.1992 | C3 | 2.5853 | 1.5537 | | 3.8352 | 2.8049 | 2.8049 | 2.1905 | 2.1905 | 1.1018 | 1.1020 | 1.1020 | F4 | 1.4109 | 2.4740 | 3.8352 | | 2.0807 | 2.0807 | 2.7247 | 2.7247 | 4.6576 | 4.1424 | 4.1424 | H5 | 1.1197 | 2.2064 | 2.8049 | 2.0807 | | 1.8021 | 3.1134 | 2.5454 | 3.8162 | 3.1594 | 2.6004 | H6 | 1.1197 | 2.2064 | 2.8049 | 2.0807 | 1.8021 | | 2.5454 | 3.1134 | 3.8162 | 2.6004 | 3.1594 | H7 | 2.1979 | 1.1046 | 2.1905 | 2.7247 | 3.1134 | 2.5454 | | 1.7834 | 2.5291 | 2.5433 | 3.1072 | H8 | 2.1979 | 1.1046 | 2.1905 | 2.7247 | 2.5454 | 3.1134 | 1.7834 | | 2.5291 | 3.1072 | 2.5433 | H9 | 3.5446 | 2.1966 | 1.1018 | 4.6576 | 3.8162 | 3.8162 | 2.5291 | 2.5291 | | 1.7866 | 1.7866 | H10 | 2.8365 | 2.1992 | 1.1020 | 4.1424 | 3.1594 | 2.6004 | 2.5433 | 3.1072 | 1.7866 | | 1.7866 | H11 | 2.8365 | 2.1992 | 1.1020 | 4.1424 | 2.6004 | 3.1594 | 3.1072 | 2.5433 | 1.7866 | 1.7866 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
111.467 |
|
C1 |
C2 |
H7 |
108.983 |
| C1 |
C2 |
H8 |
108.983 |
|
C2 |
C1 |
F4 |
111.810 |
| C2 |
C1 |
H5 |
108.780 |
|
C2 |
C1 |
H6 |
108.780 |
| C2 |
C3 |
H9 |
110.463 |
|
C2 |
C3 |
H10 |
110.662 |
| C2 |
C3 |
H11 |
110.662 |
|
C3 |
C2 |
H7 |
109.828 |
| C3 |
C2 |
H8 |
109.828 |
|
F4 |
C1 |
H5 |
110.087 |
| F4 |
C1 |
H6 |
110.087 |
|
H5 |
C1 |
H6 |
107.169 |
| H7 |
C2 |
H8 |
107.666 |
|
H9 |
C3 |
H10 |
108.326 |
| H9 |
C3 |
H11 |
108.326 |
|
H10 |
C3 |
H11 |
108.320 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at TPSSh/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.022 |
|
|
|
| 2 |
C |
-0.129 |
|
|
|
| 3 |
C |
-0.202 |
|
|
|
| 4 |
F |
-0.103 |
|
|
|
| 5 |
H |
0.058 |
|
|
|
| 6 |
H |
0.058 |
|
|
|
| 7 |
H |
0.068 |
|
|
|
| 8 |
H |
0.068 |
|
|
|
| 9 |
H |
0.071 |
|
|
|
| 10 |
H |
0.067 |
|
|
|
| 11 |
H |
0.067 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.865 |
0.392 |
0.000 |
0.950 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.835 |
-0.257 |
0.000 |
| y |
-0.257 |
2.670 |
0.000 |
| z |
0.000 |
0.000 |
2.407 |
<r2> (average value of r
2) Å
2
| <r2> |
106.089 |
| (<r2>)1/2 |
10.300 |
Jump to
S1C1
Energy calculated at TPSSh/STO-3G
| | hartrees |
| Energy at 0K | -215.553903 |
| Energy at 298.15K | |
| HF Energy | -215.553903 |
| Nuclear repulsion energy | 127.603482 |
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 TPSSh/STO-3G
| 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 |
3487 |
3487 |
2.40 |
|
|
|
| 2 |
A |
3486 |
3486 |
2.62 |
|
|
|
| 3 |
A |
3452 |
3452 |
1.81 |
|
|
|
| 4 |
A |
3346 |
3346 |
4.80 |
|
|
|
| 5 |
A |
3319 |
3319 |
1.92 |
|
|
|
| 6 |
A |
3308 |
3308 |
17.18 |
|
|
|
| 7 |
A |
3214 |
3214 |
19.76 |
|
|
|
| 8 |
A |
1702 |
1702 |
2.33 |
|
|
|
| 9 |
A |
1694 |
1694 |
2.77 |
|
|
|
| 10 |
A |
1669 |
1669 |
0.51 |
|
|
|
| 11 |
A |
1662 |
1662 |
0.75 |
|
|
|
| 12 |
A |
1579 |
1579 |
0.49 |
|
|
|
| 13 |
A |
1516 |
1516 |
17.85 |
|
|
|
| 14 |
A |
1492 |
1492 |
6.68 |
|
|
|
| 15 |
A |
1394 |
1394 |
0.82 |
|
|
|
| 16 |
A |
1346 |
1346 |
1.82 |
|
|
|
| 17 |
A |
1240 |
1240 |
4.54 |
|
|
|
| 18 |
A |
1219 |
1219 |
4.51 |
|
|
|
| 19 |
A |
1164 |
1164 |
9.65 |
|
|
|
| 20 |
A |
1073 |
1073 |
5.62 |
|
|
|
| 21 |
A |
980 |
980 |
2.36 |
|
|
|
| 22 |
A |
915 |
915 |
2.47 |
|
|
|
| 23 |
A |
822 |
822 |
3.03 |
|
|
|
| 24 |
A |
478 |
478 |
0.56 |
|
|
|
| 25 |
A |
295 |
295 |
0.42 |
|
|
|
| 26 |
A |
192 |
192 |
0.30 |
|
|
|
| 27 |
A |
112 |
112 |
0.58 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 23076.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 23076.8 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 TPSSh/STO-3G
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.820 |
0.516 |
0.293 |
| C2 |
-0.635 |
0.672 |
-0.287 |
| C3 |
-1.556 |
-0.510 |
0.122 |
| F4 |
1.447 |
-0.659 |
-0.172 |
| H5 |
1.422 |
1.414 |
0.002 |
| H6 |
0.763 |
0.502 |
1.412 |
| H7 |
-0.577 |
0.735 |
-1.388 |
| H8 |
-1.053 |
1.626 |
0.083 |
| H9 |
-2.555 |
-0.398 |
-0.329 |
| H10 |
-1.125 |
-1.465 |
-0.218 |
| H11 |
-1.671 |
-0.552 |
1.217 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
H11 |
| C1 | | 1.5746 | 2.5940 | 1.4108 | 1.1198 | 1.1197 | 2.1972 | 2.1871 | 3.5520 | 2.8226 | 2.8638 |
C2 | 1.5746 | | 1.5531 | 2.4740 | 2.2059 | 2.2067 | 1.1046 | 1.1048 | 2.1985 | 2.1931 | 2.1988 | C3 | 2.5940 | 1.5531 | | 3.0216 | 3.5477 | 2.8400 | 2.1889 | 2.1943 | 1.1018 | 1.1019 | 1.1019 | F4 | 1.4108 | 2.4740 | 3.0216 | | 2.0805 | 2.0794 | 2.7422 | 3.3961 | 4.0142 | 2.6956 | 3.4156 | H5 | 1.1198 | 2.2059 | 3.5477 | 2.0805 | | 1.8039 | 2.5273 | 2.4850 | 4.3831 | 3.8499 | 3.8616 | H6 | 1.1197 | 2.2067 | 2.8400 | 2.0794 | 1.8039 | | 3.1127 | 2.5150 | 3.8536 | 3.1761 | 2.6598 | H7 | 2.1972 | 1.1046 | 2.1889 | 2.7422 | 2.5273 | 3.1127 | | 1.7841 | 2.5144 | 2.5514 | 3.1056 | H8 | 2.1871 | 1.1048 | 2.1943 | 3.3961 | 2.4850 | 2.5150 | 1.7841 | | 2.5538 | 3.1058 | 2.5323 | H9 | 3.5520 | 2.1985 | 1.1018 | 4.0142 | 4.3831 | 3.8536 | 2.5144 | 2.5538 | | 1.7881 | 1.7875 | H10 | 2.8226 | 2.1931 | 1.1019 | 2.6956 | 3.8499 | 3.1761 | 2.5514 | 3.1058 | 1.7881 | | 1.7866 | H11 | 2.8638 | 2.1988 | 1.1019 | 3.4156 | 3.8616 | 2.6598 | 3.1056 | 2.5323 | 1.7875 | 1.7866 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
112.064 |
|
C1 |
C2 |
H7 |
108.925 |
| C1 |
C2 |
H8 |
108.142 |
|
C2 |
C1 |
F4 |
111.818 |
| C2 |
C1 |
H5 |
108.734 |
|
C2 |
C1 |
H6 |
108.797 |
| C2 |
C3 |
H9 |
110.657 |
|
C2 |
C3 |
H10 |
110.221 |
| C2 |
C3 |
H11 |
110.674 |
|
C3 |
C2 |
H7 |
109.741 |
| C3 |
C2 |
H8 |
110.147 |
|
F4 |
C1 |
H5 |
110.066 |
| F4 |
C1 |
H6 |
109.991 |
|
H5 |
C1 |
H6 |
107.315 |
| H7 |
C2 |
H8 |
107.706 |
|
H9 |
C3 |
H10 |
108.470 |
| H9 |
C3 |
H11 |
108.419 |
|
H10 |
C3 |
H11 |
108.325 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at TPSSh/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.022 |
|
|
|
| 2 |
C |
-0.128 |
|
|
|
| 3 |
C |
-0.203 |
|
|
|
| 4 |
F |
-0.104 |
|
|
|
| 5 |
H |
0.059 |
|
|
|
| 6 |
H |
0.058 |
|
|
|
| 7 |
H |
0.067 |
|
|
|
| 8 |
H |
0.068 |
|
|
|
| 9 |
H |
0.068 |
|
|
|
| 10 |
H |
0.071 |
|
|
|
| 11 |
H |
0.066 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.495 |
0.716 |
0.235 |
0.902 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.770 |
-0.012 |
-0.012 |
| y |
-0.012 |
2.655 |
0.067 |
| z |
-0.012 |
0.067 |
2.447 |
<r2> (average value of r
2) Å
2
| <r2> |
93.969 |
| (<r2>)1/2 |
9.694 |