Jump to
S1C2
Energy calculated at HSEh1PBE/STO-3G
| hartrees |
Energy at 0K | -214.055423 |
Energy at 298.15K | |
HF Energy | -214.055423 |
Nuclear repulsion energy | 114.905922 |
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/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' |
3597 |
3177 |
0.61 |
30.90 |
0.70 |
0.82 |
2 |
A' |
3491 |
3083 |
1.62 |
54.47 |
0.27 |
0.43 |
3 |
A' |
3438 |
3036 |
19.80 |
25.24 |
0.15 |
0.26 |
4 |
A' |
3251 |
2871 |
10.57 |
62.77 |
0.12 |
0.21 |
5 |
A' |
1889 |
1668 |
1.22 |
6.15 |
0.07 |
0.13 |
6 |
A' |
1665 |
1471 |
1.25 |
18.81 |
0.71 |
0.83 |
7 |
A' |
1557 |
1375 |
1.64 |
11.18 |
0.58 |
0.73 |
8 |
A' |
1516 |
1339 |
19.34 |
8.38 |
0.58 |
0.74 |
9 |
A' |
1404 |
1240 |
1.26 |
16.56 |
0.57 |
0.72 |
10 |
A' |
1252 |
1106 |
10.91 |
2.29 |
0.75 |
0.86 |
11 |
A' |
1090 |
963 |
6.49 |
4.79 |
0.73 |
0.85 |
12 |
A' |
963 |
850 |
1.54 |
4.47 |
0.23 |
0.38 |
13 |
A' |
613 |
542 |
0.65 |
1.53 |
0.74 |
0.85 |
14 |
A' |
233 |
206 |
0.57 |
0.82 |
0.53 |
0.69 |
15 |
A" |
3337 |
2947 |
9.20 |
48.85 |
0.75 |
0.86 |
16 |
A" |
1329 |
1174 |
1.04 |
8.76 |
0.75 |
0.86 |
17 |
A" |
1120 |
989 |
8.92 |
0.18 |
0.75 |
0.86 |
18 |
A" |
1096 |
968 |
0.39 |
0.51 |
0.75 |
0.86 |
19 |
A" |
1017 |
898 |
21.28 |
0.12 |
0.75 |
0.86 |
20 |
A" |
586 |
517 |
5.69 |
6.05 |
0.75 |
0.86 |
21 |
A" |
139 |
123 |
0.82 |
2.69 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 17291.7 cm
-1
Scaled (by 0.8831) Zero Point Vibrational Energy (zpe) 15270.3 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/STO-3G
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
-0.977 |
0.000 |
C2 |
-0.956 |
0.230 |
0.000 |
C3 |
-0.534 |
1.490 |
0.000 |
F4 |
1.344 |
-0.586 |
0.000 |
H5 |
-1.225 |
2.337 |
0.000 |
H6 |
0.536 |
1.721 |
0.000 |
H7 |
-2.025 |
-0.019 |
0.000 |
H8 |
-0.221 |
-1.609 |
0.895 |
H9 |
-0.221 |
-1.609 |
-0.895 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
C1 | | 1.5395 | 2.5237 | 1.3998 | 3.5330 | 2.7500 | 2.2397 | 1.1181 | 1.1181 |
C2 | 1.5395 | | 1.3285 | 2.4409 | 2.1243 | 2.1088 | 1.0974 | 2.1735 | 2.1735 | C3 | 2.5237 | 1.3285 | | 2.7999 | 1.0932 | 1.0946 | 2.1210 | 3.2410 | 3.2410 | F4 | 1.3998 | 2.4409 | 2.7999 | | 3.8921 | 2.4446 | 3.4164 | 2.0732 | 2.0732 | H5 | 3.5330 | 2.1243 | 1.0932 | 3.8921 | | 1.8654 | 2.4885 | 4.1694 | 4.1694 | H6 | 2.7500 | 2.1088 | 1.0946 | 2.4446 | 1.8654 | | 3.0956 | 3.5303 | 3.5303 | H7 | 2.2397 | 1.0974 | 2.1210 | 3.4164 | 2.4885 | 3.0956 | | 2.5656 | 2.5656 | H8 | 1.1181 | 2.1735 | 3.2410 | 2.0732 | 4.1694 | 3.5303 | 2.5656 | | 1.7897 | H9 | 1.1181 | 2.1735 | 3.2410 | 2.0732 | 4.1694 | 3.5303 | 2.5656 | 1.7897 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
C3 |
123.104 |
|
C1 |
C2 |
H7 |
115.260 |
C2 |
C1 |
F4 |
112.198 |
|
C2 |
C1 |
H8 |
108.707 |
C2 |
C1 |
H9 |
108.707 |
|
C2 |
C3 |
H5 |
122.311 |
C2 |
C3 |
H6 |
120.682 |
|
C3 |
C2 |
H7 |
121.636 |
F4 |
C1 |
H8 |
110.352 |
|
F4 |
C1 |
H9 |
110.352 |
H5 |
C3 |
H6 |
117.006 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/STO-3G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.042 |
|
|
|
2 |
C |
-0.090 |
|
|
|
3 |
C |
-0.173 |
|
|
|
4 |
F |
-0.103 |
|
|
|
5 |
H |
0.083 |
|
|
|
6 |
H |
0.086 |
|
|
|
7 |
H |
0.082 |
|
|
|
8 |
H |
0.079 |
|
|
|
9 |
H |
0.079 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.870 |
-0.384 |
0.000 |
0.951 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-22.125 |
0.679 |
0.000 |
y |
0.679 |
-20.437 |
0.000 |
z |
0.000 |
0.000 |
-22.521 |
|
Traceless |
| x | y | z |
x |
-0.646 |
0.679 |
0.000 |
y |
0.679 |
1.886 |
0.000 |
z |
0.000 |
0.000 |
-1.240 |
|
Polar |
3z2-r2 | -2.480 |
x2-y2 | -1.689 |
xy | 0.679 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.680 |
0.202 |
0.000 |
y |
0.202 |
3.840 |
0.000 |
z |
0.000 |
0.000 |
1.216 |
<r2> (average value of r
2) Å
2
<r2> |
80.653 |
(<r2>)1/2 |
8.981 |
Jump to
S1C1
Energy calculated at HSEh1PBE/STO-3G
| hartrees |
Energy at 0K | -214.054830 |
Energy at 298.15K | |
HF Energy | -214.054830 |
Nuclear repulsion energy | 112.516020 |
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/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 |
3590 |
3170 |
0.07 |
33.23 |
0.71 |
0.83 |
2 |
A |
3492 |
3084 |
2.24 |
49.14 |
0.27 |
0.43 |
3 |
A |
3435 |
3034 |
17.34 |
28.90 |
0.14 |
0.24 |
4 |
A |
3367 |
2973 |
8.49 |
32.94 |
0.75 |
0.86 |
5 |
A |
3262 |
2881 |
11.94 |
47.40 |
0.15 |
0.26 |
6 |
A |
1881 |
1661 |
0.25 |
7.79 |
0.09 |
0.16 |
7 |
A |
1660 |
1466 |
0.43 |
12.72 |
0.75 |
0.86 |
8 |
A |
1586 |
1400 |
6.58 |
11.71 |
0.48 |
0.65 |
9 |
A |
1497 |
1322 |
18.69 |
6.26 |
0.72 |
0.84 |
10 |
A |
1410 |
1246 |
2.68 |
14.78 |
0.58 |
0.73 |
11 |
A |
1344 |
1187 |
3.90 |
14.79 |
0.74 |
0.85 |
12 |
A |
1231 |
1087 |
1.00 |
2.63 |
0.55 |
0.71 |
13 |
A |
1215 |
1073 |
16.85 |
4.03 |
0.58 |
0.73 |
14 |
A |
1120 |
989 |
9.00 |
0.40 |
0.74 |
0.85 |
15 |
A |
1032 |
911 |
4.23 |
0.57 |
0.41 |
0.59 |
16 |
A |
1022 |
902 |
16.68 |
0.42 |
0.28 |
0.44 |
17 |
A |
981 |
866 |
4.47 |
2.40 |
0.24 |
0.38 |
18 |
A |
690 |
609 |
4.97 |
4.12 |
0.61 |
0.76 |
19 |
A |
428 |
378 |
0.43 |
2.25 |
0.52 |
0.68 |
20 |
A |
337 |
298 |
2.21 |
3.03 |
0.75 |
0.86 |
21 |
A |
92 |
81 |
0.22 |
3.30 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 17335.3 cm
-1
Scaled (by 0.8831) Zero Point Vibrational Energy (zpe) 15308.8 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 HSEh1PBE/STO-3G
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.633 |
0.412 |
0.343 |
C2 |
0.679 |
-0.386 |
0.263 |
C3 |
1.812 |
0.104 |
-0.234 |
F4 |
-1.667 |
-0.217 |
-0.371 |
H5 |
2.732 |
-0.487 |
-0.273 |
H6 |
1.876 |
1.126 |
-0.620 |
H7 |
0.633 |
-1.415 |
0.642 |
H8 |
-0.930 |
0.516 |
1.416 |
H9 |
-0.456 |
1.439 |
-0.053 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
C1 | | 1.5378 | 2.5307 | 1.4061 | 3.5371 | 2.7807 | 2.2428 | 1.1178 | 1.1145 |
C2 | 1.5378 | | 1.3305 | 2.4363 | 2.1244 | 2.1213 | 1.0976 | 2.1756 | 2.1723 | C3 | 2.5307 | 1.3305 | | 3.4966 | 1.0943 | 1.0949 | 2.1129 | 3.2267 | 2.6379 | F4 | 1.4061 | 2.4363 | 3.4966 | | 4.4090 | 3.7978 | 2.7845 | 2.0673 | 2.0763 | H5 | 3.5371 | 2.1244 | 1.0943 | 4.4090 | | 1.8589 | 2.4711 | 4.1559 | 3.7312 | H6 | 2.7807 | 2.1213 | 1.0949 | 3.7978 | 1.8589 | | 3.0980 | 3.5204 | 2.4203 | H7 | 2.2428 | 1.0976 | 2.1129 | 2.7845 | 2.4711 | 3.0980 | | 2.6020 | 3.1327 | H8 | 1.1178 | 2.1756 | 3.2267 | 2.0673 | 4.1559 | 3.5204 | 2.6020 | | 1.7984 | H9 | 1.1145 | 2.1723 | 2.6379 | 2.0763 | 3.7312 | 2.4203 | 3.1327 | 1.7984 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
C3 |
123.688 |
|
C1 |
C2 |
H7 |
115.644 |
C2 |
C1 |
F4 |
111.625 |
|
C2 |
C1 |
H8 |
109.002 |
C2 |
C1 |
H9 |
108.928 |
|
C2 |
C3 |
H5 |
122.055 |
C2 |
C3 |
H6 |
121.706 |
|
C3 |
C2 |
H7 |
120.667 |
F4 |
C1 |
H8 |
109.458 |
|
F4 |
C1 |
H9 |
110.381 |
H5 |
C3 |
H6 |
116.237 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/STO-3G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.044 |
|
|
|
2 |
C |
-0.089 |
|
|
|
3 |
C |
-0.167 |
|
|
|
4 |
F |
-0.103 |
|
|
|
5 |
H |
0.085 |
|
|
|
6 |
H |
0.081 |
|
|
|
7 |
H |
0.083 |
|
|
|
8 |
H |
0.077 |
|
|
|
9 |
H |
0.076 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.683 |
0.394 |
0.500 |
0.934 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-22.667 |
-0.548 |
-1.059 |
y |
-0.548 |
-20.851 |
-0.576 |
z |
-1.059 |
-0.576 |
-22.254 |
|
Traceless |
| x | y | z |
x |
-1.115 |
-0.548 |
-1.059 |
y |
-0.548 |
1.609 |
-0.576 |
z |
-1.059 |
-0.576 |
-0.495 |
|
Polar |
3z2-r2 | -0.989 |
x2-y2 | -1.816 |
xy | -0.548 |
xz | -1.059 |
yz | -0.576 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.795 |
0.250 |
-0.592 |
y |
0.250 |
2.378 |
-0.384 |
z |
-0.592 |
-0.384 |
1.650 |
<r2> (average value of r
2) Å
2
<r2> |
89.854 |
(<r2>)1/2 |
9.479 |