Jump to
S1C2
Energy calculated at PBE1PBE/3-21G
| hartrees |
Energy at 0K | -375.098385 |
Energy at 298.15K | |
HF Energy | -375.098385 |
Nuclear repulsion energy | 188.604117 |
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 PBE1PBE/3-21G
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 |
3162 |
3037 |
34.20 |
32.23 |
0.55 |
0.71 |
2 |
A |
3132 |
3008 |
28.32 |
83.89 |
0.46 |
0.63 |
3 |
A |
3103 |
2981 |
9.83 |
102.29 |
0.10 |
0.18 |
4 |
A |
1567 |
1505 |
3.63 |
11.95 |
0.74 |
0.85 |
5 |
A |
1480 |
1421 |
12.81 |
4.99 |
0.74 |
0.85 |
6 |
A |
1463 |
1405 |
21.20 |
8.15 |
0.74 |
0.85 |
7 |
A |
1380 |
1325 |
17.08 |
4.71 |
0.75 |
0.86 |
8 |
A |
1292 |
1241 |
7.73 |
10.70 |
0.73 |
0.85 |
9 |
A |
1185 |
1138 |
100.63 |
4.64 |
0.74 |
0.85 |
10 |
A |
1154 |
1108 |
17.38 |
3.80 |
0.71 |
0.83 |
11 |
A |
1141 |
1096 |
100.98 |
1.82 |
0.45 |
0.62 |
12 |
A |
1106 |
1062 |
7.70 |
7.35 |
0.47 |
0.64 |
13 |
A |
938 |
901 |
19.33 |
5.81 |
0.32 |
0.49 |
14 |
A |
557 |
535 |
4.82 |
2.18 |
0.44 |
0.61 |
15 |
A |
450 |
432 |
18.81 |
0.94 |
0.74 |
0.85 |
16 |
A |
413 |
396 |
7.58 |
1.78 |
0.56 |
0.72 |
17 |
A |
217 |
208 |
10.13 |
0.06 |
0.60 |
0.75 |
18 |
A |
124 |
119 |
8.86 |
0.04 |
0.72 |
0.84 |
Unscaled Zero Point Vibrational Energy (zpe) 11931.5 cm
-1
Scaled (by 0.9604) Zero Point Vibrational Energy (zpe) 11459.0 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 PBE1PBE/3-21G
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.756 |
-0.587 |
-0.307 |
C2 |
0.462 |
0.027 |
0.335 |
F3 |
-1.901 |
0.083 |
0.160 |
F4 |
1.546 |
-0.777 |
0.004 |
F5 |
0.673 |
1.294 |
-0.181 |
H6 |
-0.661 |
-0.487 |
-1.392 |
H7 |
-0.793 |
-1.646 |
-0.041 |
H8 |
0.358 |
0.091 |
1.419 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
F3 |
F4 |
F5 |
H6 |
H7 |
H8 |
C1 | | 1.5073 | 1.4072 | 2.3307 | 2.3655 | 1.0938 | 1.0927 | 2.1634 |
C2 | 1.5073 | | 2.3707 | 1.3893 | 1.3844 | 2.1233 | 2.1250 | 1.0916 | F3 | 1.4072 | 2.3707 | | 3.5568 | 2.8652 | 2.0670 | 2.0640 | 2.5864 | F4 | 2.3307 | 1.3893 | 3.5568 | | 2.2549 | 2.6280 | 2.4962 | 2.0421 | F5 | 2.3655 | 1.3844 | 2.8652 | 2.2549 | | 2.5337 | 3.2885 | 2.0267 | H6 | 1.0938 | 2.1233 | 2.0670 | 2.6280 | 2.5337 | | 1.7851 | 3.0460 | H7 | 1.0927 | 2.1250 | 2.0640 | 2.4962 | 3.2885 | 1.7851 | | 2.5448 | H8 | 2.1634 | 1.0916 | 2.5864 | 2.0421 | 2.0267 | 3.0460 | 2.5448 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
F4 |
107.081 |
|
C1 |
C2 |
F5 |
109.703 |
C1 |
C2 |
H8 |
111.703 |
|
C2 |
C1 |
F3 |
108.818 |
C2 |
C1 |
H6 |
108.389 |
|
C2 |
C1 |
H7 |
108.580 |
F3 |
C1 |
H6 |
110.854 |
|
F3 |
C1 |
H7 |
110.679 |
F4 |
C2 |
F5 |
108.770 |
|
F4 |
C2 |
H8 |
110.218 |
F5 |
C2 |
H8 |
109.305 |
|
H6 |
C1 |
H7 |
109.457 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/3-21G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.173 |
|
|
|
2 |
C |
0.342 |
|
|
|
3 |
F |
-0.295 |
|
|
|
4 |
F |
-0.296 |
|
|
|
5 |
F |
-0.290 |
|
|
|
6 |
H |
0.247 |
|
|
|
7 |
H |
0.232 |
|
|
|
8 |
H |
0.233 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.192 |
-1.431 |
0.334 |
1.482 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-32.212 |
1.405 |
1.289 |
y |
1.405 |
-27.487 |
0.585 |
z |
1.289 |
0.585 |
-24.260 |
|
Traceless |
| x | y | z |
x |
-6.338 |
1.405 |
1.289 |
y |
1.405 |
0.749 |
0.585 |
z |
1.289 |
0.585 |
5.589 |
|
Polar |
3z2-r2 | 11.178 |
x2-y2 | -4.725 |
xy | 1.405 |
xz | 1.289 |
yz | 0.585 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.971 |
-0.090 |
-0.047 |
y |
-0.090 |
3.090 |
0.028 |
z |
-0.047 |
0.028 |
2.945 |
<r2> (average value of r
2) Å
2
<r2> |
112.825 |
(<r2>)1/2 |
10.622 |
Jump to
S1C1
Energy calculated at PBE1PBE/3-21G
| hartrees |
Energy at 0K | -375.094899 |
Energy at 298.15K | |
HF Energy | -375.094899 |
Nuclear repulsion energy | 191.296596 |
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 PBE1PBE/3-21G
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' |
3106 |
2983 |
58.59 |
109.10 |
0.05 |
0.09 |
2 |
A' |
3087 |
2965 |
10.96 |
54.93 |
0.57 |
0.72 |
3 |
A' |
1560 |
1499 |
3.36 |
12.95 |
0.74 |
0.85 |
4 |
A' |
1497 |
1437 |
6.16 |
2.67 |
0.74 |
0.85 |
5 |
A' |
1435 |
1378 |
28.87 |
8.05 |
0.68 |
0.81 |
6 |
A' |
1195 |
1147 |
79.91 |
5.89 |
0.46 |
0.63 |
7 |
A' |
1101 |
1057 |
8.86 |
3.23 |
0.71 |
0.83 |
8 |
A' |
887 |
852 |
30.51 |
7.75 |
0.16 |
0.28 |
9 |
A' |
744 |
715 |
38.64 |
3.16 |
0.54 |
0.70 |
10 |
A' |
482 |
463 |
14.65 |
2.10 |
0.75 |
0.86 |
11 |
A' |
216 |
208 |
1.96 |
0.14 |
0.52 |
0.68 |
12 |
A" |
3141 |
3017 |
22.45 |
55.65 |
0.75 |
0.86 |
13 |
A" |
1457 |
1400 |
34.61 |
1.76 |
0.75 |
0.86 |
14 |
A" |
1324 |
1271 |
7.65 |
24.53 |
0.75 |
0.86 |
15 |
A" |
1179 |
1132 |
63.84 |
1.27 |
0.75 |
0.86 |
16 |
A" |
1008 |
968 |
37.98 |
4.40 |
0.75 |
0.86 |
17 |
A" |
343 |
330 |
0.02 |
0.23 |
0.75 |
0.86 |
18 |
A" |
117 |
112 |
2.33 |
0.07 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 11938.8 cm
-1
Scaled (by 0.9604) Zero Point Vibrational Energy (zpe) 11466.0 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 PBE1PBE/3-21G
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.754 |
-0.819 |
0.000 |
C2 |
0.362 |
0.636 |
0.000 |
F3 |
-0.395 |
-1.630 |
0.000 |
F4 |
-0.395 |
0.918 |
1.126 |
F5 |
-0.395 |
0.918 |
-1.126 |
H6 |
1.356 |
-1.015 |
-0.892 |
H7 |
1.356 |
-1.015 |
0.892 |
H8 |
1.257 |
1.265 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
F3 |
F4 |
F5 |
H6 |
H7 |
H8 |
C1 | | 1.5068 | 1.4057 | 2.3675 | 2.3675 | 1.0942 | 1.0942 | 2.1441 |
C2 | 1.5068 | | 2.3885 | 1.3858 | 1.3858 | 2.1240 | 2.1240 | 1.0942 | F3 | 1.4057 | 2.3885 | | 2.7856 | 2.7856 | 2.0587 | 2.0587 | 3.3328 | F4 | 2.3675 | 1.3858 | 2.7856 | | 2.2529 | 3.2981 | 2.6186 | 2.0289 | F5 | 2.3675 | 1.3858 | 2.7856 | 2.2529 | | 2.6186 | 3.2981 | 2.0289 | H6 | 1.0942 | 2.1240 | 2.0587 | 3.2981 | 2.6186 | | 1.7846 | 2.4510 | H7 | 1.0942 | 2.1240 | 2.0587 | 2.6186 | 3.2981 | 1.7846 | | 2.4510 | H8 | 2.1441 | 1.0942 | 3.3328 | 2.0289 | 2.0289 | 2.4510 | 2.4510 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
F4 |
109.791 |
|
C1 |
C2 |
F5 |
109.791 |
C1 |
C2 |
H8 |
110.030 |
|
C2 |
C1 |
F3 |
110.135 |
C2 |
C1 |
H6 |
108.449 |
|
C2 |
C1 |
H7 |
108.449 |
F3 |
C1 |
H6 |
110.248 |
|
F3 |
C1 |
H7 |
110.248 |
F4 |
C2 |
F5 |
108.751 |
|
F4 |
C2 |
H8 |
109.227 |
F5 |
C2 |
H8 |
109.227 |
|
H6 |
C1 |
H7 |
109.266 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/3-21G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.154 |
|
|
|
2 |
C |
0.351 |
|
|
|
3 |
F |
-0.287 |
|
|
|
4 |
F |
-0.290 |
|
|
|
5 |
F |
-0.290 |
|
|
|
6 |
H |
0.230 |
|
|
|
7 |
H |
0.230 |
|
|
|
8 |
H |
0.211 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
3.235 |
0.162 |
0.000 |
3.239 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-24.612 |
-0.256 |
0.000 |
y |
-0.256 |
-28.605 |
0.000 |
z |
0.000 |
0.000 |
-28.256 |
|
Traceless |
| x | y | z |
x |
3.819 |
-0.256 |
0.000 |
y |
-0.256 |
-2.171 |
0.000 |
z |
0.000 |
0.000 |
-1.648 |
|
Polar |
3z2-r2 | -3.295 |
x2-y2 | 3.993 |
xy | -0.256 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.073 |
0.069 |
0.000 |
y |
0.069 |
2.936 |
0.000 |
z |
0.000 |
0.000 |
3.087 |
<r2> (average value of r
2) Å
2
<r2> |
104.235 |
(<r2>)1/2 |
10.210 |