Jump to
S1C2
Energy calculated at PBE1PBE/Def2TZVPP
| hartrees |
Energy at 0K | -216.984004 |
Energy at 298.15K | |
HF Energy | -216.984004 |
Nuclear repulsion energy | 116.870721 |
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/Def2TZVPP
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' |
3260 |
3260 |
3.58 |
51.82 |
0.70 |
0.82 |
2 |
A' |
3172 |
3172 |
3.36 |
171.05 |
0.12 |
0.21 |
3 |
A' |
3159 |
3159 |
8.53 |
29.49 |
0.68 |
0.81 |
4 |
A' |
3029 |
3029 |
33.03 |
185.77 |
0.10 |
0.18 |
5 |
A' |
1734 |
1734 |
6.13 |
30.91 |
0.09 |
0.17 |
6 |
A' |
1487 |
1487 |
6.04 |
13.59 |
0.53 |
0.69 |
7 |
A' |
1445 |
1445 |
7.49 |
10.18 |
0.44 |
0.61 |
8 |
A' |
1413 |
1413 |
9.40 |
4.77 |
0.75 |
0.86 |
9 |
A' |
1315 |
1315 |
0.17 |
18.01 |
0.26 |
0.41 |
10 |
A' |
1150 |
1150 |
61.95 |
1.72 |
0.75 |
0.86 |
11 |
A' |
1019 |
1019 |
33.91 |
4.99 |
0.66 |
0.79 |
12 |
A' |
923 |
923 |
1.18 |
4.26 |
0.06 |
0.11 |
13 |
A' |
615 |
615 |
6.22 |
1.67 |
0.72 |
0.84 |
14 |
A' |
264 |
264 |
2.00 |
1.27 |
0.51 |
0.68 |
15 |
A" |
3065 |
3065 |
21.45 |
89.19 |
0.75 |
0.86 |
16 |
A" |
1268 |
1268 |
0.00 |
5.81 |
0.75 |
0.86 |
17 |
A" |
1046 |
1046 |
12.63 |
1.35 |
0.75 |
0.86 |
18 |
A" |
1023 |
1023 |
6.90 |
0.03 |
0.75 |
0.86 |
19 |
A" |
963 |
963 |
48.96 |
1.50 |
0.75 |
0.86 |
20 |
A" |
563 |
563 |
11.37 |
3.20 |
0.75 |
0.86 |
21 |
A" |
185 |
185 |
2.94 |
1.85 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 16049.4 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 16049.4 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/Def2TZVPP
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.936 |
-0.209 |
0.000 |
C2 |
0.000 |
0.947 |
0.000 |
C3 |
1.320 |
0.852 |
0.000 |
F4 |
-0.268 |
-1.413 |
0.000 |
H5 |
1.943 |
1.736 |
0.000 |
H6 |
1.811 |
-0.113 |
0.000 |
H7 |
-0.484 |
1.920 |
0.000 |
H8 |
-1.582 |
-0.182 |
0.886 |
H9 |
-1.582 |
-0.182 |
-0.886 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
C1 | | 1.4868 | 2.4927 | 1.3773 | 3.4747 | 2.7491 | 2.1759 | 1.0961 | 1.0961 |
C2 | 1.4868 | | 1.3234 | 2.3748 | 2.0977 | 2.0988 | 1.0872 | 2.1355 | 2.1355 | C3 | 2.4927 | 1.3234 | | 2.7657 | 1.0824 | 1.0828 | 2.0971 | 3.2050 | 3.2050 | F4 | 1.3773 | 2.3748 | 2.7657 | | 3.8481 | 2.4521 | 3.3399 | 2.0060 | 2.0060 | H5 | 3.4747 | 2.0977 | 1.0824 | 3.8481 | | 1.8544 | 2.4348 | 4.1099 | 4.1099 | H6 | 2.7491 | 2.0988 | 1.0828 | 2.4521 | 1.8544 | | 3.0668 | 3.5073 | 3.5073 | H7 | 2.1759 | 1.0872 | 2.0971 | 3.3399 | 2.4348 | 3.0668 | | 2.5313 | 2.5313 | H8 | 1.0961 | 2.1355 | 3.2050 | 2.0060 | 4.1099 | 3.5073 | 2.5313 | | 1.7710 | H9 | 1.0961 | 2.1355 | 3.2050 | 2.0060 | 4.1099 | 3.5073 | 2.5313 | 1.7710 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
C3 |
124.893 |
|
C1 |
C2 |
H7 |
114.523 |
C2 |
C1 |
F4 |
111.966 |
|
C2 |
C1 |
H8 |
110.622 |
C2 |
C1 |
H9 |
110.622 |
|
C2 |
C3 |
H5 |
121.040 |
C2 |
C3 |
H6 |
121.117 |
|
C3 |
C2 |
H7 |
120.584 |
F4 |
C1 |
H8 |
107.851 |
|
F4 |
C1 |
H9 |
107.851 |
H5 |
C3 |
H6 |
117.844 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/Def2TZVPP
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.139 |
|
|
|
2 |
C |
-0.146 |
|
|
|
3 |
C |
-0.207 |
|
|
|
4 |
F |
-0.228 |
|
|
|
5 |
H |
0.098 |
|
|
|
6 |
H |
0.102 |
|
|
|
7 |
H |
0.091 |
|
|
|
8 |
H |
0.076 |
|
|
|
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 |
|
-0.898 |
1.439 |
0.000 |
1.696 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-21.242 |
-0.313 |
0.000 |
y |
-0.313 |
-25.271 |
0.000 |
z |
0.000 |
0.000 |
-25.226 |
|
Traceless |
| x | y | z |
x |
4.007 |
-0.313 |
0.000 |
y |
-0.313 |
-2.037 |
0.000 |
z |
0.000 |
0.000 |
-1.970 |
|
Polar |
3z2-r2 | -3.939 |
x2-y2 | 4.029 |
xy | -0.313 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
7.286 |
0.336 |
0.000 |
y |
0.336 |
5.277 |
0.000 |
z |
0.000 |
0.000 |
4.182 |
<r2> (average value of r
2) Å
2
<r2> |
79.894 |
(<r2>)1/2 |
8.938 |
Jump to
S1C1
Energy calculated at PBE1PBE/Def2TZVPP
| hartrees |
Energy at 0K | -216.983375 |
Energy at 298.15K | |
HF Energy | -216.983375 |
Nuclear repulsion energy | 114.579610 |
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/Def2TZVPP
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 |
3243 |
3243 |
8.64 |
60.72 |
0.59 |
0.74 |
2 |
A |
3171 |
3171 |
5.16 |
119.39 |
0.22 |
0.37 |
3 |
A |
3151 |
3151 |
7.88 |
72.55 |
0.12 |
0.21 |
4 |
A |
3098 |
3098 |
20.26 |
68.48 |
0.69 |
0.82 |
5 |
A |
3043 |
3043 |
30.89 |
138.65 |
0.09 |
0.16 |
6 |
A |
1732 |
1732 |
0.66 |
31.48 |
0.11 |
0.19 |
7 |
A |
1497 |
1497 |
4.00 |
4.95 |
0.61 |
0.75 |
8 |
A |
1458 |
1458 |
19.92 |
9.22 |
0.56 |
0.72 |
9 |
A |
1389 |
1389 |
11.29 |
3.96 |
0.34 |
0.51 |
10 |
A |
1315 |
1315 |
0.10 |
13.45 |
0.34 |
0.50 |
11 |
A |
1270 |
1270 |
4.15 |
8.95 |
0.67 |
0.80 |
12 |
A |
1185 |
1185 |
2.67 |
1.13 |
0.68 |
0.81 |
13 |
A |
1070 |
1070 |
122.88 |
4.95 |
0.60 |
0.75 |
14 |
A |
1036 |
1036 |
23.21 |
1.57 |
0.72 |
0.84 |
15 |
A |
994 |
994 |
2.67 |
1.75 |
0.13 |
0.23 |
16 |
A |
976 |
976 |
53.52 |
1.25 |
0.50 |
0.66 |
17 |
A |
932 |
932 |
1.90 |
2.54 |
0.14 |
0.25 |
18 |
A |
662 |
662 |
7.90 |
2.18 |
0.50 |
0.67 |
19 |
A |
438 |
438 |
2.48 |
3.66 |
0.42 |
0.59 |
20 |
A |
330 |
330 |
6.67 |
1.83 |
0.75 |
0.85 |
21 |
A |
116 |
116 |
0.94 |
3.75 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 16051.0 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 16051.0 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/Def2TZVPP
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.604 |
0.427 |
0.315 |
C2 |
0.643 |
-0.379 |
0.241 |
C3 |
1.794 |
0.092 |
-0.212 |
F4 |
-1.639 |
-0.223 |
-0.341 |
H5 |
2.693 |
-0.512 |
-0.221 |
H6 |
1.880 |
1.108 |
-0.586 |
H7 |
0.570 |
-1.401 |
0.604 |
H8 |
-0.922 |
0.564 |
1.354 |
H9 |
-0.469 |
1.408 |
-0.148 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
C1 | | 1.4863 | 2.4782 | 1.3872 | 3.4695 | 2.7287 | 2.1908 | 1.0950 | 1.0930 |
C2 | 1.4863 | | 1.3244 | 2.3599 | 2.1058 | 2.1036 | 1.0865 | 2.1399 | 2.1403 | C3 | 2.4782 | 1.3244 | | 3.4503 | 1.0830 | 1.0851 | 2.0965 | 3.1712 | 2.6188 | F4 | 1.3872 | 2.3599 | 3.4503 | | 4.3433 | 3.7702 | 2.6756 | 2.0014 | 2.0161 | H5 | 3.4695 | 2.1058 | 1.0830 | 4.3433 | | 1.8483 | 2.4452 | 4.0877 | 3.7000 | H6 | 2.7287 | 2.1036 | 1.0851 | 3.7702 | 1.8483 | | 3.0699 | 3.4515 | 2.4088 | H7 | 2.1908 | 1.0865 | 2.0965 | 2.6756 | 2.4452 | 3.0699 | | 2.5786 | 3.0873 | H8 | 1.0950 | 2.1399 | 3.1712 | 2.0014 | 4.0877 | 3.4515 | 2.5786 | | 1.7807 | H9 | 1.0930 | 2.1403 | 2.6188 | 2.0161 | 3.7000 | 2.4088 | 3.0873 | 1.7807 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
C3 |
123.592 |
|
C1 |
C2 |
H7 |
115.887 |
C2 |
C1 |
F4 |
110.374 |
|
C2 |
C1 |
H8 |
111.086 |
C2 |
C1 |
H9 |
111.237 |
|
C2 |
C3 |
H5 |
121.704 |
C2 |
C3 |
H6 |
121.316 |
|
C3 |
C2 |
H7 |
120.510 |
F4 |
C1 |
H8 |
106.881 |
|
F4 |
C1 |
H9 |
108.171 |
H5 |
C3 |
H6 |
116.978 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/Def2TZVPP
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.128 |
|
|
|
2 |
C |
-0.129 |
|
|
|
3 |
C |
-0.184 |
|
|
|
4 |
F |
-0.230 |
|
|
|
5 |
H |
0.101 |
|
|
|
6 |
H |
0.083 |
|
|
|
7 |
H |
0.097 |
|
|
|
8 |
H |
0.068 |
|
|
|
9 |
H |
0.065 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
1.457 |
0.711 |
0.830 |
1.822 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-25.622 |
-1.112 |
-1.892 |
y |
-1.112 |
-22.490 |
-0.999 |
z |
-1.892 |
-0.999 |
-24.839 |
|
Traceless |
| x | y | z |
x |
-1.958 |
-1.112 |
-1.892 |
y |
-1.112 |
2.741 |
-0.999 |
z |
-1.892 |
-0.999 |
-0.783 |
|
Polar |
3z2-r2 | -1.566 |
x2-y2 | -3.132 |
xy | -1.112 |
xz | -1.892 |
yz | -0.999 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
7.155 |
0.240 |
-0.714 |
y |
0.240 |
5.138 |
-0.322 |
z |
-0.714 |
-0.322 |
4.525 |
<r2> (average value of r
2) Å
2
<r2> |
88.611 |
(<r2>)1/2 |
9.413 |