Jump to
S1C2
Energy calculated at B1B95/6-311G*
| | hartrees |
| Energy at 0K | -217.097139 |
| Energy at 298.15K | |
| HF Energy | -217.097139 |
| Nuclear repulsion energy | 117.046084 |
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 B1B95/6-311G*
| 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' |
3269 |
3133 |
8.70 |
55.26 |
0.72 |
0.84 |
| 2 |
A' |
3182 |
3050 |
6.56 |
161.40 |
0.15 |
0.26 |
| 3 |
A' |
3167 |
3036 |
14.21 |
30.93 |
0.73 |
0.84 |
| 4 |
A' |
3049 |
2923 |
42.65 |
170.15 |
0.12 |
0.21 |
| 5 |
A' |
1748 |
1676 |
4.30 |
20.48 |
0.13 |
0.23 |
| 6 |
A' |
1516 |
1453 |
4.22 |
15.91 |
0.60 |
0.75 |
| 7 |
A' |
1456 |
1396 |
8.08 |
11.83 |
0.54 |
0.70 |
| 8 |
A' |
1431 |
1372 |
12.62 |
7.16 |
0.75 |
0.86 |
| 9 |
A' |
1323 |
1269 |
0.14 |
16.63 |
0.32 |
0.49 |
| 10 |
A' |
1151 |
1104 |
56.33 |
2.17 |
0.75 |
0.86 |
| 11 |
A' |
1025 |
982 |
37.92 |
4.76 |
0.70 |
0.83 |
| 12 |
A' |
927 |
889 |
1.57 |
3.58 |
0.13 |
0.22 |
| 13 |
A' |
618 |
592 |
5.94 |
1.72 |
0.74 |
0.85 |
| 14 |
A' |
270 |
259 |
2.47 |
1.10 |
0.53 |
0.69 |
| 15 |
A" |
3087 |
2960 |
37.44 |
98.91 |
0.75 |
0.86 |
| 16 |
A" |
1279 |
1226 |
0.03 |
8.96 |
0.75 |
0.86 |
| 17 |
A" |
1051 |
1007 |
12.41 |
1.01 |
0.75 |
0.86 |
| 18 |
A" |
1027 |
985 |
12.46 |
0.10 |
0.75 |
0.86 |
| 19 |
A" |
950 |
911 |
50.72 |
1.01 |
0.75 |
0.86 |
| 20 |
A" |
561 |
538 |
11.81 |
7.51 |
0.75 |
0.86 |
| 21 |
A" |
184 |
176 |
3.06 |
4.08 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 16136.0 cm
-1
Scaled (by 0.9586) Zero Point Vibrational Energy (zpe) 15467.9 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 B1B95/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.939 |
-0.202 |
0.000 |
| C2 |
0.000 |
0.951 |
0.000 |
| C3 |
1.318 |
0.835 |
0.000 |
| F4 |
-0.265 |
-1.405 |
0.000 |
| H5 |
1.960 |
1.706 |
0.000 |
| H6 |
1.792 |
-0.137 |
0.000 |
| H7 |
-0.473 |
1.930 |
0.000 |
| H8 |
-1.582 |
-0.180 |
0.885 |
| H9 |
-1.582 |
-0.180 |
-0.885 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4874 | 2.4841 | 1.3785 | 3.4708 | 2.7322 | 2.1823 | 1.0943 | 1.0943 |
C2 | 1.4874 | | 1.3230 | 2.3706 | 2.1002 | 2.0968 | 1.0867 | 2.1368 | 2.1368 | C3 | 2.4841 | 1.3230 | | 2.7427 | 1.0821 | 1.0820 | 2.0984 | 3.1976 | 3.1976 | F4 | 1.3785 | 2.3706 | 2.7427 | | 3.8247 | 2.4163 | 3.3407 | 2.0048 | 2.0048 | H5 | 3.4708 | 2.1002 | 1.0821 | 3.8247 | | 1.8513 | 2.4425 | 4.1094 | 4.1094 | H6 | 2.7322 | 2.0968 | 1.0820 | 2.4163 | 1.8513 | | 3.0661 | 3.4890 | 3.4890 | H7 | 2.1823 | 1.0867 | 2.0984 | 3.3407 | 2.4425 | 3.0661 | | 2.5424 | 2.5424 | H8 | 1.0943 | 2.1368 | 3.1976 | 2.0048 | 4.1094 | 3.4890 | 2.5424 | | 1.7699 | H9 | 1.0943 | 2.1368 | 3.1976 | 2.0048 | 4.1094 | 3.4890 | 2.5424 | 1.7699 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
124.134 |
|
C1 |
C2 |
H7 |
115.064 |
| C2 |
C1 |
F4 |
111.564 |
|
C2 |
C1 |
H8 |
110.804 |
| C2 |
C1 |
H9 |
110.804 |
|
C2 |
C3 |
H5 |
121.353 |
| C2 |
C3 |
H6 |
121.025 |
|
C3 |
C2 |
H7 |
120.802 |
| F4 |
C1 |
H8 |
107.789 |
|
F4 |
C1 |
H9 |
107.789 |
| H5 |
C3 |
H6 |
117.622 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.110 |
|
|
|
| 2 |
C |
-0.272 |
|
|
|
| 3 |
C |
-0.425 |
|
|
|
| 4 |
F |
-0.269 |
|
|
|
| 5 |
H |
0.217 |
|
|
|
| 6 |
H |
0.230 |
|
|
|
| 7 |
H |
0.205 |
|
|
|
| 8 |
H |
0.211 |
|
|
|
| 9 |
H |
0.211 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.910 |
1.494 |
0.000 |
1.749 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.947 |
-0.342 |
0.000 |
| y |
-0.342 |
-25.044 |
0.000 |
| z |
0.000 |
0.000 |
-25.074 |
|
| Traceless |
| | x | y | z |
| x |
4.113 |
-0.342 |
0.000 |
| y |
-0.342 |
-2.034 |
0.000 |
| z |
0.000 |
0.000 |
-2.079 |
|
| Polar |
| 3z2-r2 | -4.157 |
| x2-y2 | 4.098 |
| xy | -0.342 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.785 |
0.256 |
0.000 |
| y |
0.256 |
4.671 |
0.000 |
| z |
0.000 |
0.000 |
3.239 |
<r2> (average value of r
2) Å
2
| <r2> |
79.325 |
| (<r2>)1/2 |
8.906 |
Jump to
S1C1
Energy calculated at B1B95/6-311G*
| | hartrees |
| Energy at 0K | -217.095635 |
| Energy at 298.15K | |
| HF Energy | -217.095635 |
| Nuclear repulsion energy | 114.566150 |
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 B1B95/6-311G*
| 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 |
3248 |
3113 |
17.47 |
65.27 |
0.60 |
0.75 |
| 2 |
A |
3181 |
3049 |
9.11 |
116.04 |
0.27 |
0.42 |
| 3 |
A |
3157 |
3027 |
13.78 |
69.01 |
0.15 |
0.26 |
| 4 |
A |
3116 |
2987 |
30.88 |
74.89 |
0.71 |
0.83 |
| 5 |
A |
3061 |
2934 |
41.49 |
127.12 |
0.11 |
0.19 |
| 6 |
A |
1746 |
1674 |
0.54 |
20.28 |
0.14 |
0.25 |
| 7 |
A |
1519 |
1456 |
2.30 |
7.50 |
0.70 |
0.82 |
| 8 |
A |
1474 |
1413 |
23.65 |
9.59 |
0.63 |
0.77 |
| 9 |
A |
1409 |
1351 |
14.70 |
5.13 |
0.51 |
0.68 |
| 10 |
A |
1322 |
1267 |
0.13 |
13.02 |
0.40 |
0.57 |
| 11 |
A |
1284 |
1231 |
3.68 |
12.98 |
0.71 |
0.83 |
| 12 |
A |
1192 |
1143 |
2.25 |
1.30 |
0.74 |
0.85 |
| 13 |
A |
1075 |
1030 |
120.10 |
4.64 |
0.61 |
0.76 |
| 14 |
A |
1037 |
994 |
30.77 |
1.43 |
0.74 |
0.85 |
| 15 |
A |
997 |
956 |
2.66 |
1.12 |
0.18 |
0.31 |
| 16 |
A |
963 |
923 |
54.22 |
0.96 |
0.53 |
0.69 |
| 17 |
A |
936 |
897 |
2.70 |
2.31 |
0.16 |
0.28 |
| 18 |
A |
655 |
628 |
8.33 |
4.32 |
0.64 |
0.78 |
| 19 |
A |
438 |
420 |
3.02 |
4.44 |
0.50 |
0.67 |
| 20 |
A |
323 |
309 |
6.67 |
3.14 |
0.75 |
0.86 |
| 21 |
A |
117 |
112 |
1.15 |
5.78 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 16124.4 cm
-1
Scaled (by 0.9586) Zero Point Vibrational Energy (zpe) 15456.9 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 B1B95/6-311G*
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.602 |
0.438 |
0.298 |
| C2 |
0.640 |
-0.375 |
0.235 |
| C3 |
1.802 |
0.085 |
-0.204 |
| F4 |
-1.646 |
-0.231 |
-0.325 |
| H5 |
2.695 |
-0.527 |
-0.202 |
| H6 |
1.908 |
1.097 |
-0.578 |
| H7 |
0.552 |
-1.395 |
0.597 |
| H8 |
-0.908 |
0.609 |
1.333 |
| H9 |
-0.473 |
1.402 |
-0.197 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4863 | 2.4812 | 1.3870 | 3.4718 | 2.7396 | 2.1866 | 1.0934 | 1.0915 |
C2 | 1.4863 | | 1.3241 | 2.3579 | 2.1062 | 2.1064 | 1.0859 | 2.1385 | 2.1409 | C3 | 2.4812 | 1.3241 | | 3.4642 | 1.0826 | 1.0848 | 2.0962 | 3.1596 | 2.6285 | F4 | 1.3870 | 2.3579 | 3.4642 | | 4.3525 | 3.8027 | 2.6522 | 1.9997 | 2.0149 | H5 | 3.4718 | 2.1062 | 1.0826 | 4.3525 | | 1.8436 | 2.4465 | 4.0783 | 3.7089 | H6 | 2.7396 | 2.1064 | 1.0848 | 3.8027 | 1.8436 | | 3.0714 | 3.4391 | 2.4304 | H7 | 2.1866 | 1.0859 | 2.0962 | 2.6522 | 2.4465 | 3.0714 | | 2.5862 | 3.0829 | H8 | 1.0934 | 2.1385 | 3.1596 | 1.9997 | 4.0783 | 3.4391 | 2.5862 | | 1.7784 | H9 | 1.0915 | 2.1409 | 2.6285 | 2.0149 | 3.7089 | 2.4304 | 3.0829 | 1.7784 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
123.881 |
|
C1 |
C2 |
H7 |
115.566 |
| C2 |
C1 |
F4 |
110.245 |
|
C2 |
C1 |
H8 |
111.067 |
| C2 |
C1 |
H9 |
111.387 |
|
C2 |
C3 |
H5 |
121.802 |
| C2 |
C3 |
H6 |
121.642 |
|
C3 |
C2 |
H7 |
120.541 |
| F4 |
C1 |
H8 |
106.850 |
|
F4 |
C1 |
H9 |
108.180 |
| H5 |
C3 |
H6 |
116.555 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.133 |
|
|
|
| 2 |
C |
-0.219 |
|
|
|
| 3 |
C |
-0.437 |
|
|
|
| 4 |
F |
-0.275 |
|
|
|
| 5 |
H |
0.224 |
|
|
|
| 6 |
H |
0.215 |
|
|
|
| 7 |
H |
0.215 |
|
|
|
| 8 |
H |
0.205 |
|
|
|
| 9 |
H |
0.205 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.502 |
0.765 |
0.833 |
1.881 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.517 |
-1.118 |
-1.804 |
| y |
-1.118 |
-22.214 |
-1.011 |
| z |
-1.804 |
-1.011 |
-24.664 |
|
| Traceless |
| | x | y | z |
| x |
-2.079 |
-1.118 |
-1.804 |
| y |
-1.118 |
2.877 |
-1.011 |
| z |
-1.804 |
-1.011 |
-0.798 |
|
| Polar |
| 3z2-r2 | -1.596 |
| x2-y2 | -3.304 |
| xy | -1.118 |
| xz | -1.804 |
| yz | -1.011 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.524 |
0.213 |
-0.823 |
| y |
0.213 |
4.609 |
-0.475 |
| z |
-0.823 |
-0.475 |
3.609 |
<r2> (average value of r
2) Å
2
| <r2> |
88.716 |
| (<r2>)1/2 |
9.419 |