Jump to
S1C2
Energy calculated at B3LYP/LANL2DZ
| | hartrees |
| Energy at 0K | -217.131087 |
| Energy at 298.15K | |
| HF Energy | -217.131087 |
| Nuclear repulsion energy | 114.466308 |
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 B3LYP/LANL2DZ
| 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' |
3283 |
3156 |
12.48 |
42.30 |
0.70 |
0.83 |
| 2 |
A' |
3183 |
3059 |
10.62 |
161.78 |
0.12 |
0.22 |
| 3 |
A' |
3162 |
3039 |
11.87 |
23.19 |
0.73 |
0.84 |
| 4 |
A' |
3058 |
2940 |
42.29 |
169.75 |
0.11 |
0.19 |
| 5 |
A' |
1714 |
1648 |
4.04 |
23.36 |
0.10 |
0.19 |
| 6 |
A' |
1506 |
1448 |
6.53 |
17.67 |
0.61 |
0.76 |
| 7 |
A' |
1463 |
1406 |
10.09 |
11.09 |
0.48 |
0.65 |
| 8 |
A' |
1403 |
1349 |
5.59 |
11.49 |
0.56 |
0.72 |
| 9 |
A' |
1323 |
1271 |
0.22 |
15.75 |
0.48 |
0.65 |
| 10 |
A' |
1112 |
1069 |
16.23 |
1.36 |
0.75 |
0.86 |
| 11 |
A' |
981 |
943 |
50.37 |
6.18 |
0.74 |
0.85 |
| 12 |
A' |
899 |
864 |
11.68 |
7.85 |
0.13 |
0.23 |
| 13 |
A' |
594 |
571 |
5.14 |
3.18 |
0.75 |
0.86 |
| 14 |
A' |
258 |
248 |
4.17 |
1.69 |
0.59 |
0.74 |
| 15 |
A" |
3115 |
2994 |
35.01 |
78.40 |
0.75 |
0.86 |
| 16 |
A" |
1217 |
1170 |
0.19 |
11.69 |
0.75 |
0.86 |
| 17 |
A" |
1050 |
1010 |
1.57 |
1.92 |
0.75 |
0.86 |
| 18 |
A" |
1027 |
987 |
38.38 |
0.08 |
0.75 |
0.86 |
| 19 |
A" |
1005 |
966 |
70.17 |
4.04 |
0.75 |
0.86 |
| 20 |
A" |
572 |
549 |
19.52 |
6.85 |
0.75 |
0.86 |
| 21 |
A" |
160 |
154 |
4.85 |
4.50 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 16042.7 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 15420.2 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 B3LYP/LANL2DZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.967 |
-0.182 |
0.000 |
| C2 |
0.000 |
0.972 |
0.000 |
| C3 |
1.340 |
0.850 |
0.000 |
| F4 |
-0.262 |
-1.450 |
0.000 |
| H5 |
1.985 |
1.726 |
0.000 |
| H6 |
1.817 |
-0.126 |
0.000 |
| H7 |
-0.471 |
1.957 |
0.000 |
| H8 |
-1.603 |
-0.174 |
0.896 |
| H9 |
-1.603 |
-0.174 |
-0.896 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.5054 | 2.5278 | 1.4515 | 3.5146 | 2.7844 | 2.1953 | 1.0986 | 1.0986 |
C2 | 1.5054 | | 1.3458 | 2.4367 | 2.1231 | 2.1224 | 1.0918 | 2.1646 | 2.1646 | C3 | 2.5278 | 1.3458 | | 2.8041 | 1.0870 | 1.0861 | 2.1226 | 3.2425 | 3.2425 | F4 | 1.4515 | 2.4367 | 2.8041 | | 3.8909 | 2.4653 | 3.4138 | 2.0564 | 2.0564 | H5 | 3.5146 | 2.1231 | 1.0870 | 3.8909 | | 1.8590 | 2.4668 | 4.1573 | 4.1573 | H6 | 2.7844 | 2.1224 | 1.0861 | 2.4653 | 1.8590 | | 3.0936 | 3.5352 | 3.5352 | H7 | 2.1953 | 1.0918 | 2.1226 | 3.4138 | 2.4668 | 3.0936 | | 2.5739 | 2.5739 | H8 | 1.0986 | 2.1646 | 3.2425 | 2.0564 | 4.1573 | 3.5352 | 2.5739 | | 1.7922 | H9 | 1.0986 | 2.1646 | 3.2425 | 2.0564 | 4.1573 | 3.5352 | 2.5739 | 1.7922 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
124.795 |
|
C1 |
C2 |
H7 |
114.458 |
| C2 |
C1 |
F4 |
110.972 |
|
C2 |
C1 |
H8 |
111.496 |
| C2 |
C1 |
H9 |
111.496 |
|
C2 |
C3 |
H5 |
121.184 |
| C2 |
C3 |
H6 |
121.197 |
|
C3 |
C2 |
H7 |
120.747 |
| F4 |
C1 |
H8 |
106.671 |
|
F4 |
C1 |
H9 |
106.671 |
| H5 |
C3 |
H6 |
117.619 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.179 |
|
|
|
| 2 |
C |
-0.097 |
|
|
|
| 3 |
C |
-0.501 |
|
|
|
| 4 |
F |
-0.280 |
|
|
|
| 5 |
H |
0.210 |
|
|
|
| 6 |
H |
0.242 |
|
|
|
| 7 |
H |
0.201 |
|
|
|
| 8 |
H |
0.202 |
|
|
|
| 9 |
H |
0.202 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.161 |
2.088 |
0.000 |
2.389 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.081 |
-0.405 |
0.000 |
| y |
-0.405 |
-25.862 |
0.000 |
| z |
0.000 |
0.000 |
-25.157 |
|
| Traceless |
| | x | y | z |
| x |
5.429 |
-0.405 |
0.000 |
| y |
-0.405 |
-3.243 |
0.000 |
| z |
0.000 |
0.000 |
-2.186 |
|
| Polar |
| 3z2-r2 | -4.372 |
| x2-y2 | 5.781 |
| xy | -0.405 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.421 |
0.166 |
0.000 |
| y |
0.166 |
4.343 |
0.000 |
| z |
0.000 |
0.000 |
2.752 |
<r2> (average value of r
2) Å
2
| <r2> |
82.045 |
| (<r2>)1/2 |
9.058 |
Jump to
S1C1
Energy calculated at B3LYP/LANL2DZ
| | hartrees |
| Energy at 0K | -217.131470 |
| Energy at 298.15K | |
| HF Energy | -217.131470 |
| Nuclear repulsion energy | 112.059710 |
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 B3LYP/LANL2DZ
| 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 |
3266 |
3139 |
25.08 |
53.84 |
0.56 |
0.72 |
| 2 |
A |
3192 |
3068 |
11.30 |
88.14 |
0.21 |
0.35 |
| 3 |
A |
3158 |
3035 |
15.84 |
79.88 |
0.17 |
0.29 |
| 4 |
A |
3151 |
3029 |
17.91 |
54.24 |
0.75 |
0.86 |
| 5 |
A |
3079 |
2960 |
43.53 |
124.49 |
0.09 |
0.16 |
| 6 |
A |
1707 |
1641 |
0.80 |
30.02 |
0.12 |
0.22 |
| 7 |
A |
1513 |
1454 |
7.53 |
6.81 |
0.63 |
0.77 |
| 8 |
A |
1477 |
1420 |
19.22 |
13.84 |
0.52 |
0.69 |
| 9 |
A |
1392 |
1338 |
7.14 |
4.95 |
0.73 |
0.84 |
| 10 |
A |
1323 |
1272 |
0.08 |
14.49 |
0.52 |
0.68 |
| 11 |
A |
1242 |
1194 |
4.21 |
16.86 |
0.72 |
0.84 |
| 12 |
A |
1179 |
1133 |
0.55 |
4.89 |
0.66 |
0.79 |
| 13 |
A |
1050 |
1009 |
11.13 |
3.36 |
0.73 |
0.84 |
| 14 |
A |
1011 |
972 |
86.29 |
3.30 |
0.75 |
0.86 |
| 15 |
A |
993 |
955 |
8.93 |
1.29 |
0.34 |
0.51 |
| 16 |
A |
973 |
935 |
80.46 |
4.38 |
0.49 |
0.66 |
| 17 |
A |
916 |
881 |
43.18 |
12.67 |
0.26 |
0.42 |
| 18 |
A |
657 |
631 |
9.51 |
4.28 |
0.49 |
0.66 |
| 19 |
A |
431 |
415 |
2.85 |
5.43 |
0.47 |
0.64 |
| 20 |
A |
323 |
310 |
10.06 |
3.59 |
0.74 |
0.85 |
| 21 |
A |
111 |
107 |
1.66 |
6.23 |
0.75 |
0.85 |
Unscaled Zero Point Vibrational Energy (zpe) 16071.5 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 15447.9 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 B3LYP/LANL2DZ
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.593 |
0.471 |
0.317 |
| C2 |
0.655 |
-0.362 |
0.276 |
| C3 |
1.827 |
0.070 |
-0.232 |
| F4 |
-1.682 |
-0.254 |
-0.346 |
| H5 |
2.717 |
-0.555 |
-0.218 |
| H6 |
1.933 |
1.060 |
-0.673 |
| H7 |
0.570 |
-1.361 |
0.703 |
| H8 |
-0.943 |
0.642 |
1.342 |
| H9 |
-0.474 |
1.423 |
-0.211 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.5004 | 2.5132 | 1.4668 | 3.5056 | 2.7757 | 2.2035 | 1.0972 | 1.0953 |
C2 | 1.5004 | | 1.3481 | 2.4216 | 2.1288 | 2.1340 | 1.0898 | 2.1677 | 2.1674 | C3 | 2.5132 | 1.3481 | | 3.5263 | 1.0872 | 1.0890 | 2.1215 | 3.2371 | 2.6696 | F4 | 1.4668 | 2.4216 | 3.5263 | | 4.4114 | 3.8603 | 2.7202 | 2.0491 | 2.0710 | H5 | 3.5056 | 2.1288 | 1.0872 | 4.4114 | | 1.8515 | 2.4712 | 4.1550 | 3.7540 | H6 | 2.7757 | 2.1340 | 1.0890 | 3.8603 | 1.8515 | | 3.1000 | 3.5366 | 2.4776 | H7 | 2.2035 | 1.0898 | 2.1215 | 2.7202 | 2.4712 | 3.1000 | | 2.5909 | 3.1105 | H8 | 1.0972 | 2.1677 | 3.2371 | 2.0491 | 4.1550 | 3.5366 | 2.5909 | | 1.8006 | H9 | 1.0953 | 2.1674 | 2.6696 | 2.0710 | 3.7540 | 2.4776 | 3.1105 | 1.8006 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
123.746 |
|
C1 |
C2 |
H7 |
115.659 |
| C2 |
C1 |
F4 |
109.393 |
|
C2 |
C1 |
H8 |
112.195 |
| C2 |
C1 |
H9 |
112.290 |
|
C2 |
C3 |
H5 |
121.519 |
| C2 |
C3 |
H6 |
121.878 |
|
C3 |
C2 |
H7 |
120.591 |
| F4 |
C1 |
H8 |
105.193 |
|
F4 |
C1 |
H9 |
106.973 |
| H5 |
C3 |
H6 |
116.603 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.206 |
|
|
|
| 2 |
C |
-0.040 |
|
|
|
| 3 |
C |
-0.517 |
|
|
|
| 4 |
F |
-0.285 |
|
|
|
| 5 |
H |
0.218 |
|
|
|
| 6 |
H |
0.213 |
|
|
|
| 7 |
H |
0.228 |
|
|
|
| 8 |
H |
0.195 |
|
|
|
| 9 |
H |
0.194 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.065 |
1.091 |
1.134 |
2.596 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.363 |
-1.665 |
-2.416 |
| y |
-1.665 |
-21.976 |
-1.299 |
| z |
-2.416 |
-1.299 |
-24.539 |
|
| Traceless |
| | x | y | z |
| x |
-3.105 |
-1.665 |
-2.416 |
| y |
-1.665 |
3.475 |
-1.299 |
| z |
-2.416 |
-1.299 |
-0.370 |
|
| Polar |
| 3z2-r2 | -0.740 |
| x2-y2 | -4.387 |
| xy | -1.665 |
| xz | -2.416 |
| yz | -1.299 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.436 |
0.313 |
-0.891 |
| y |
0.313 |
4.024 |
-0.521 |
| z |
-0.891 |
-0.521 |
3.263 |
<r2> (average value of r
2) Å
2
| <r2> |
91.661 |
| (<r2>)1/2 |
9.574 |