Jump to
S1C2
Energy calculated at B97D3/Def2TZVPP
| hartrees |
Energy at 0K | -217.106216 |
Energy at 298.15K | |
HF Energy | -217.106216 |
Nuclear repulsion energy | 115.804025 |
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 B97D3/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' |
3189 |
3145 |
7.58 |
55.37 |
0.72 |
0.84 |
2 |
A' |
3104 |
3061 |
4.92 |
154.01 |
0.11 |
0.20 |
3 |
A' |
3083 |
3041 |
15.17 |
62.32 |
0.40 |
0.57 |
4 |
A' |
2949 |
2908 |
42.18 |
200.18 |
0.10 |
0.18 |
5 |
A' |
1674 |
1651 |
6.63 |
26.66 |
0.08 |
0.15 |
6 |
A' |
1458 |
1438 |
4.59 |
15.25 |
0.50 |
0.67 |
7 |
A' |
1422 |
1402 |
3.42 |
12.01 |
0.40 |
0.57 |
8 |
A' |
1379 |
1360 |
11.58 |
7.62 |
0.69 |
0.82 |
9 |
A' |
1293 |
1275 |
0.12 |
18.61 |
0.26 |
0.42 |
10 |
A' |
1098 |
1083 |
41.86 |
1.47 |
0.73 |
0.84 |
11 |
A' |
983 |
969 |
52.49 |
5.17 |
0.64 |
0.78 |
12 |
A' |
884 |
872 |
2.99 |
3.98 |
0.07 |
0.13 |
13 |
A' |
598 |
590 |
6.64 |
1.92 |
0.72 |
0.84 |
14 |
A' |
259 |
255 |
1.96 |
1.41 |
0.51 |
0.68 |
15 |
A" |
2979 |
2939 |
29.29 |
99.60 |
0.75 |
0.86 |
16 |
A" |
1235 |
1218 |
0.03 |
6.41 |
0.75 |
0.86 |
17 |
A" |
1016 |
1002 |
10.52 |
0.86 |
0.75 |
0.86 |
18 |
A" |
996 |
983 |
9.69 |
0.09 |
0.75 |
0.86 |
19 |
A" |
923 |
910 |
42.19 |
1.42 |
0.75 |
0.86 |
20 |
A" |
543 |
536 |
10.48 |
3.37 |
0.75 |
0.86 |
21 |
A" |
170 |
167 |
2.71 |
1.96 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 15616.0 cm
-1
Scaled (by 0.9863) Zero Point Vibrational Energy (zpe) 15402.0 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 B97D3/Def2TZVPP
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.940 |
-0.211 |
0.000 |
C2 |
0.000 |
0.952 |
0.000 |
C3 |
1.329 |
0.876 |
0.000 |
F4 |
-0.272 |
-1.437 |
0.000 |
H5 |
1.941 |
1.772 |
0.000 |
H6 |
1.841 |
-0.082 |
0.000 |
H7 |
-0.499 |
1.922 |
0.000 |
H8 |
-1.588 |
-0.187 |
0.889 |
H9 |
-1.588 |
-0.187 |
-0.889 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
C1 | | 1.4954 | 2.5160 | 1.3959 | 3.4979 | 2.7835 | 2.1786 | 1.1003 | 1.1003 |
C2 | 1.4954 | | 1.3314 | 2.4043 | 2.1075 | 2.1111 | 1.0910 | 2.1467 | 2.1467 | C3 | 2.5160 | 1.3314 | | 2.8128 | 1.0857 | 1.0855 | 2.1063 | 3.2292 | 3.2292 | F4 | 1.3959 | 2.4043 | 2.8128 | | 3.8984 | 2.5098 | 3.3668 | 2.0210 | 2.0210 | H5 | 3.4979 | 2.1075 | 1.0857 | 3.8984 | | 1.8570 | 2.4445 | 4.1331 | 4.1331 | H6 | 2.7835 | 2.1111 | 1.0855 | 2.5098 | 1.8570 | | 3.0804 | 3.5433 | 3.5433 | H7 | 2.1786 | 1.0910 | 2.1063 | 3.3668 | 2.4445 | 3.0804 | | 2.5348 | 2.5348 | H8 | 1.1003 | 2.1467 | 3.2292 | 2.0210 | 4.1331 | 3.5433 | 2.5348 | | 1.7782 | H9 | 1.1003 | 2.1467 | 3.2292 | 2.0210 | 4.1331 | 3.5433 | 2.5348 | 1.7782 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
C3 |
125.657 |
|
C1 |
C2 |
H7 |
113.860 |
C2 |
C1 |
F4 |
112.472 |
|
C2 |
C1 |
H8 |
110.664 |
C2 |
C1 |
H9 |
110.664 |
|
C2 |
C3 |
H5 |
121.029 |
C2 |
C3 |
H6 |
121.390 |
|
C3 |
C2 |
H7 |
120.483 |
F4 |
C1 |
H8 |
107.523 |
|
F4 |
C1 |
H9 |
107.523 |
H5 |
C3 |
H6 |
117.581 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/Def2TZVPP
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.179 |
|
|
|
2 |
C |
-0.126 |
|
|
|
3 |
C |
-0.182 |
|
|
|
4 |
F |
-0.230 |
|
|
|
5 |
H |
0.086 |
|
|
|
6 |
H |
0.091 |
|
|
|
7 |
H |
0.069 |
|
|
|
8 |
H |
0.056 |
|
|
|
9 |
H |
0.056 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.881 |
1.431 |
0.000 |
1.681 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-21.441 |
-0.322 |
0.000 |
y |
-0.322 |
-25.460 |
0.000 |
z |
0.000 |
0.000 |
-25.221 |
|
Traceless |
| x | y | z |
x |
3.900 |
-0.322 |
0.000 |
y |
-0.322 |
-2.129 |
0.000 |
z |
0.000 |
0.000 |
-1.770 |
|
Polar |
3z2-r2 | -3.541 |
x2-y2 | 4.019 |
xy | -0.322 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
7.519 |
0.405 |
0.000 |
y |
0.405 |
5.522 |
0.000 |
z |
0.000 |
0.000 |
4.285 |
<r2> (average value of r
2) Å
2
<r2> |
81.411 |
(<r2>)1/2 |
9.023 |
Jump to
S1C1
Energy calculated at B97D3/Def2TZVPP
| hartrees |
Energy at 0K | -217.106307 |
Energy at 298.15K | |
HF Energy | -217.106307 |
Nuclear repulsion energy | 113.680378 |
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 B97D3/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 |
3170 |
3126 |
15.25 |
66.55 |
0.59 |
0.74 |
2 |
A |
3099 |
3057 |
8.57 |
126.05 |
0.23 |
0.38 |
3 |
A |
3082 |
3040 |
12.61 |
80.76 |
0.12 |
0.21 |
4 |
A |
3021 |
2979 |
26.08 |
74.39 |
0.67 |
0.80 |
5 |
A |
2967 |
2926 |
38.82 |
146.60 |
0.10 |
0.17 |
6 |
A |
1669 |
1646 |
0.71 |
28.22 |
0.10 |
0.18 |
7 |
A |
1470 |
1450 |
3.04 |
5.80 |
0.55 |
0.71 |
8 |
A |
1433 |
1413 |
12.66 |
11.24 |
0.51 |
0.67 |
9 |
A |
1359 |
1341 |
12.72 |
3.97 |
0.40 |
0.57 |
10 |
A |
1294 |
1276 |
0.06 |
13.88 |
0.34 |
0.51 |
11 |
A |
1236 |
1219 |
4.45 |
10.36 |
0.65 |
0.79 |
12 |
A |
1156 |
1140 |
2.26 |
1.06 |
0.71 |
0.83 |
13 |
A |
1006 |
992 |
10.39 |
0.49 |
0.74 |
0.85 |
14 |
A |
980 |
967 |
129.92 |
6.52 |
0.59 |
0.74 |
15 |
A |
965 |
952 |
7.30 |
1.31 |
0.19 |
0.31 |
16 |
A |
939 |
926 |
48.90 |
1.04 |
0.59 |
0.75 |
17 |
A |
912 |
899 |
5.89 |
3.57 |
0.16 |
0.28 |
18 |
A |
644 |
635 |
6.94 |
2.26 |
0.48 |
0.64 |
19 |
A |
429 |
423 |
2.30 |
3.90 |
0.41 |
0.58 |
20 |
A |
328 |
324 |
7.23 |
2.19 |
0.75 |
0.86 |
21 |
A |
112 |
111 |
0.85 |
3.83 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 15634.9 cm
-1
Scaled (by 0.9863) Zero Point Vibrational Energy (zpe) 15420.7 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 B97D3/Def2TZVPP
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.604 |
0.428 |
0.331 |
C2 |
0.650 |
-0.378 |
0.253 |
C3 |
1.802 |
0.093 |
-0.224 |
F4 |
-1.650 |
-0.224 |
-0.356 |
H5 |
2.706 |
-0.510 |
-0.234 |
H6 |
1.883 |
1.106 |
-0.613 |
H7 |
0.584 |
-1.397 |
0.634 |
H8 |
-0.940 |
0.545 |
1.370 |
H9 |
-0.474 |
1.419 |
-0.120 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
C1 | | 1.4934 | 2.4924 | 1.4100 | 3.4868 | 2.7452 | 2.1989 | 1.0988 | 1.0965 |
C2 | 1.4934 | | 1.3329 | 2.3839 | 2.1169 | 2.1147 | 1.0896 | 2.1519 | 2.1526 | C3 | 2.4924 | 1.3329 | | 3.4688 | 1.0864 | 1.0883 | 2.1069 | 3.2041 | 2.6366 | F4 | 1.4100 | 2.3839 | 3.4688 | | 4.3665 | 3.7830 | 2.7100 | 2.0185 | 2.0335 | H5 | 3.4868 | 2.1169 | 1.0864 | 4.3665 | | 1.8528 | 2.4582 | 4.1211 | 3.7213 | H6 | 2.7452 | 2.1147 | 1.0883 | 3.7830 | 1.8528 | | 3.0832 | 3.4951 | 2.4281 | H7 | 2.1989 | 1.0896 | 2.1069 | 2.7100 | 2.4582 | 3.0832 | | 2.5768 | 3.1014 | H8 | 1.0988 | 2.1519 | 3.2041 | 2.0185 | 4.1211 | 3.4951 | 2.5768 | | 1.7894 | H9 | 1.0965 | 2.1526 | 2.6366 | 2.0335 | 3.7213 | 2.4281 | 3.1014 | 1.7894 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
C3 |
123.637 |
|
C1 |
C2 |
H7 |
115.829 |
C2 |
C1 |
F4 |
110.355 |
|
C2 |
C1 |
H8 |
111.319 |
C2 |
C1 |
H9 |
111.516 |
|
C2 |
C3 |
H5 |
121.758 |
C2 |
C3 |
H6 |
121.390 |
|
C3 |
C2 |
H7 |
120.524 |
F4 |
C1 |
H8 |
106.482 |
|
F4 |
C1 |
H9 |
107.790 |
H5 |
C3 |
H6 |
116.850 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/Def2TZVPP
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.168 |
|
|
|
2 |
C |
-0.110 |
|
|
|
3 |
C |
-0.154 |
|
|
|
4 |
F |
-0.235 |
|
|
|
5 |
H |
0.089 |
|
|
|
6 |
H |
0.072 |
|
|
|
7 |
H |
0.074 |
|
|
|
8 |
H |
0.050 |
|
|
|
9 |
H |
0.047 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
1.479 |
0.692 |
0.845 |
1.838 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-25.770 |
-1.103 |
-1.888 |
y |
-1.103 |
-22.672 |
-0.961 |
z |
-1.888 |
-0.961 |
-24.817 |
|
Traceless |
| x | y | z |
x |
-2.026 |
-1.103 |
-1.888 |
y |
-1.103 |
2.622 |
-0.961 |
z |
-1.888 |
-0.961 |
-0.596 |
|
Polar |
3z2-r2 | -1.191 |
x2-y2 | -3.099 |
xy | -1.103 |
xz | -1.888 |
yz | -0.961 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
7.452 |
0.203 |
-0.749 |
y |
0.203 |
5.294 |
-0.341 |
z |
-0.749 |
-0.341 |
4.675 |
<r2> (average value of r
2) Å
2
<r2> |
89.684 |
(<r2>)1/2 |
9.470 |