Jump to
S1C2
Energy calculated at HF/LANL2DZ
| | hartrees |
| Energy at 0K | -217.085394 |
| Energy at 298.15K | -217.093386 |
| HF Energy | -217.085394 |
| Nuclear repulsion energy | 127.157893 |
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 HF/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' |
3289 |
2960 |
85.58 |
|
|
|
| 2 |
A' |
3281 |
2952 |
35.68 |
|
|
|
| 3 |
A' |
3235 |
2911 |
26.73 |
|
|
|
| 4 |
A' |
3195 |
2876 |
47.88 |
|
|
|
| 5 |
A' |
1667 |
1500 |
7.30 |
|
|
|
| 6 |
A' |
1662 |
1495 |
3.67 |
|
|
|
| 7 |
A' |
1649 |
1484 |
3.68 |
|
|
|
| 8 |
A' |
1573 |
1416 |
10.00 |
|
|
|
| 9 |
A' |
1558 |
1402 |
13.74 |
|
|
|
| 10 |
A' |
1477 |
1329 |
1.69 |
|
|
|
| 11 |
A' |
1246 |
1121 |
0.34 |
|
|
|
| 12 |
A' |
1135 |
1022 |
18.23 |
|
|
|
| 13 |
A' |
1063 |
956 |
106.26 |
|
|
|
| 14 |
A' |
970 |
873 |
18.32 |
|
|
|
| 15 |
A' |
466 |
419 |
9.86 |
|
|
|
| 16 |
A' |
286 |
257 |
7.28 |
|
|
|
| 17 |
A" |
3349 |
3013 |
79.10 |
|
|
|
| 18 |
A" |
3291 |
2961 |
58.59 |
|
|
|
| 19 |
A" |
3264 |
2938 |
15.63 |
|
|
|
| 20 |
A" |
1650 |
1485 |
10.95 |
|
|
|
| 21 |
A" |
1435 |
1291 |
0.23 |
|
|
|
| 22 |
A" |
1377 |
1239 |
0.46 |
|
|
|
| 23 |
A" |
1289 |
1160 |
2.77 |
|
|
|
| 24 |
A" |
985 |
886 |
1.81 |
|
|
|
| 25 |
A" |
846 |
761 |
2.33 |
|
|
|
| 26 |
A" |
243 |
219 |
0.00 |
|
|
|
| 27 |
A" |
130 |
117 |
7.19 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 22804.4 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 20521.7 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 HF/LANL2DZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.101 |
-0.787 |
0.000 |
| C2 |
0.000 |
0.729 |
0.000 |
| C3 |
-1.467 |
1.192 |
0.000 |
| F4 |
1.483 |
-1.169 |
0.000 |
| H5 |
-0.335 |
-1.228 |
0.885 |
| H6 |
-0.335 |
-1.228 |
-0.885 |
| H7 |
0.514 |
1.116 |
-0.872 |
| H8 |
0.514 |
1.116 |
0.872 |
| H9 |
-1.525 |
2.274 |
0.000 |
| H10 |
-1.994 |
0.833 |
-0.878 |
| H11 |
-1.994 |
0.833 |
0.878 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
H11 |
| C1 | | 1.5196 | 2.5245 | 1.4345 | 1.0801 | 1.0801 | 2.1335 | 2.1335 | 3.4658 | 2.7901 | 2.7901 |
C2 | 1.5196 | | 1.5380 | 2.4087 | 2.1739 | 2.1739 | 1.0833 | 1.0833 | 2.1706 | 2.1816 | 2.1816 | C3 | 2.5245 | 1.5380 | | 3.7783 | 2.8146 | 2.8146 | 2.1654 | 2.1654 | 1.0834 | 1.0855 | 1.0855 | F4 | 1.4345 | 2.4087 | 3.7783 | | 2.0228 | 2.0228 | 2.6302 | 2.6302 | 4.5718 | 4.1076 | 4.1076 | H5 | 1.0801 | 2.1739 | 2.8146 | 2.0228 | | 1.7693 | 3.0495 | 2.4930 | 3.8032 | 3.1797 | 2.6464 | H6 | 1.0801 | 2.1739 | 2.8146 | 2.0228 | 1.7693 | | 2.4930 | 3.0495 | 3.8032 | 2.6464 | 3.1797 | H7 | 2.1335 | 1.0833 | 2.1654 | 2.6302 | 3.0495 | 2.4930 | | 1.7432 | 2.5017 | 2.5245 | 3.0715 | H8 | 2.1335 | 1.0833 | 2.1654 | 2.6302 | 2.4930 | 3.0495 | 1.7432 | | 2.5017 | 3.0715 | 2.5245 | H9 | 3.4658 | 2.1706 | 1.0834 | 4.5718 | 3.8032 | 3.8032 | 2.5017 | 2.5017 | | 1.7514 | 1.7514 | H10 | 2.7901 | 2.1816 | 1.0855 | 4.1076 | 3.1797 | 2.6464 | 2.5245 | 3.0715 | 1.7514 | | 1.7559 | H11 | 2.7901 | 2.1816 | 1.0855 | 4.1076 | 2.6464 | 3.1797 | 3.0715 | 2.5245 | 1.7514 | 1.7559 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
111.313 |
|
C1 |
C2 |
H7 |
108.951 |
| C1 |
C2 |
H8 |
108.951 |
|
C2 |
C1 |
F4 |
109.217 |
| C2 |
C1 |
H5 |
112.385 |
|
C2 |
C1 |
H6 |
112.385 |
| C2 |
C3 |
H9 |
110.605 |
|
C2 |
C3 |
H10 |
111.352 |
| C2 |
C3 |
H11 |
111.352 |
|
C3 |
C2 |
H7 |
110.190 |
| C3 |
C2 |
H8 |
110.190 |
|
F4 |
C1 |
H5 |
106.250 |
| F4 |
C1 |
H6 |
106.250 |
|
H5 |
C1 |
H6 |
109.981 |
| H7 |
C2 |
H8 |
107.139 |
|
H9 |
C3 |
H10 |
107.706 |
| H9 |
C3 |
H11 |
107.706 |
|
H10 |
C3 |
H11 |
107.959 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.036 |
|
|
|
| 2 |
C |
-0.294 |
|
|
|
| 3 |
C |
-0.548 |
|
|
|
| 4 |
F |
-0.405 |
|
|
|
| 5 |
H |
0.161 |
|
|
|
| 6 |
H |
0.161 |
|
|
|
| 7 |
H |
0.179 |
|
|
|
| 8 |
H |
0.179 |
|
|
|
| 9 |
H |
0.193 |
|
|
|
| 10 |
H |
0.169 |
|
|
|
| 11 |
H |
0.169 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.697 |
1.093 |
0.000 |
2.910 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-30.255 |
3.517 |
0.000 |
| y |
3.517 |
-26.307 |
0.000 |
| z |
0.000 |
0.000 |
-24.524 |
|
| Traceless |
| | x | y | z |
| x |
-4.840 |
3.517 |
0.000 |
| y |
3.517 |
1.082 |
0.000 |
| z |
0.000 |
0.000 |
3.757 |
|
| Polar |
| 3z2-r2 | 7.515 |
| x2-y2 | -3.948 |
| xy | 3.517 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.771 |
-0.275 |
0.000 |
| y |
-0.275 |
4.561 |
0.000 |
| z |
0.000 |
0.000 |
4.254 |
<r2> (average value of r
2) Å
2
| <r2> |
105.103 |
| (<r2>)1/2 |
10.252 |
Jump to
S1C1
Energy calculated at HF/LANL2DZ
| | hartrees |
| Energy at 0K | -217.085213 |
| Energy at 298.15K | |
| HF Energy | -217.085213 |
| Nuclear repulsion energy | 129.439241 |
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 HF/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 |
3349 |
3014 |
61.86 |
50.75 |
0.69 |
0.82 |
| 2 |
A |
3305 |
2975 |
62.94 |
31.27 |
0.75 |
0.86 |
| 3 |
A |
3286 |
2957 |
106.54 |
82.09 |
0.12 |
0.21 |
| 4 |
A |
3280 |
2951 |
30.63 |
88.09 |
0.14 |
0.24 |
| 5 |
A |
3262 |
2935 |
11.10 |
121.22 |
0.67 |
0.80 |
| 6 |
A |
3215 |
2893 |
29.72 |
164.31 |
0.09 |
0.16 |
| 7 |
A |
3199 |
2878 |
56.67 |
71.85 |
0.06 |
0.11 |
| 8 |
A |
1664 |
1497 |
2.68 |
5.51 |
0.74 |
0.85 |
| 9 |
A |
1656 |
1490 |
12.65 |
7.52 |
0.75 |
0.86 |
| 10 |
A |
1644 |
1480 |
9.32 |
17.09 |
0.75 |
0.86 |
| 11 |
A |
1634 |
1471 |
3.94 |
15.24 |
0.74 |
0.85 |
| 12 |
A |
1572 |
1415 |
7.68 |
0.89 |
0.09 |
0.16 |
| 13 |
A |
1542 |
1388 |
11.38 |
1.56 |
0.75 |
0.86 |
| 14 |
A |
1530 |
1377 |
1.55 |
0.86 |
0.61 |
0.76 |
| 15 |
A |
1419 |
1277 |
0.76 |
17.72 |
0.73 |
0.84 |
| 16 |
A |
1368 |
1231 |
1.84 |
10.89 |
0.68 |
0.81 |
| 17 |
A |
1278 |
1150 |
2.84 |
3.01 |
0.49 |
0.66 |
| 18 |
A |
1224 |
1101 |
6.23 |
4.26 |
0.63 |
0.78 |
| 19 |
A |
1171 |
1054 |
26.90 |
9.32 |
0.65 |
0.79 |
| 20 |
A |
1036 |
932 |
50.99 |
4.78 |
0.75 |
0.86 |
| 21 |
A |
1001 |
900 |
42.50 |
5.29 |
0.75 |
0.86 |
| 22 |
A |
929 |
836 |
9.16 |
17.13 |
0.13 |
0.23 |
| 23 |
A |
840 |
756 |
3.81 |
3.19 |
0.26 |
0.41 |
| 24 |
A |
504 |
454 |
7.20 |
0.76 |
0.75 |
0.86 |
| 25 |
A |
333 |
299 |
2.77 |
0.40 |
0.29 |
0.45 |
| 26 |
A |
229 |
206 |
2.72 |
0.04 |
0.45 |
0.62 |
| 27 |
A |
138 |
124 |
5.24 |
0.11 |
0.74 |
0.85 |
Unscaled Zero Point Vibrational Energy (zpe) 22802.6 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 20520.0 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 HF/LANL2DZ
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.789 |
0.537 |
0.309 |
| C2 |
-0.601 |
0.652 |
-0.296 |
| C3 |
-1.539 |
-0.490 |
0.124 |
| F4 |
1.419 |
-0.661 |
-0.171 |
| H5 |
1.434 |
1.351 |
0.015 |
| H6 |
0.764 |
0.451 |
1.385 |
| H7 |
-0.510 |
0.678 |
-1.375 |
| H8 |
-1.018 |
1.607 |
0.012 |
| H9 |
-2.515 |
-0.372 |
-0.336 |
| H10 |
-1.137 |
-1.448 |
-0.179 |
| H11 |
-1.678 |
-0.507 |
1.200 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
H11 |
| C1 | | 1.5202 | 2.5513 | 1.4365 | 1.0794 | 1.0800 | 2.1312 | 2.1210 | 3.4861 | 2.8084 | 2.8234 |
C2 | 1.5202 | | 1.5363 | 2.4131 | 2.1743 | 2.1748 | 1.0837 | 1.0866 | 2.1704 | 2.1709 | 2.1776 | C3 | 2.5513 | 1.5363 | | 2.9781 | 3.4989 | 2.7899 | 2.1614 | 2.1637 | 1.0842 | 1.0824 | 1.0857 | F4 | 1.4365 | 2.4131 | 2.9781 | | 2.0208 | 2.0220 | 2.6391 | 3.3348 | 3.9477 | 2.6745 | 3.3910 | H5 | 1.0794 | 2.1743 | 3.4989 | 2.0208 | | 1.7707 | 2.4826 | 2.4658 | 4.3223 | 3.8057 | 3.8137 | H6 | 1.0800 | 2.1748 | 2.7899 | 2.0220 | 1.7707 | | 3.0486 | 2.5295 | 3.7931 | 3.1092 | 2.6303 | H7 | 2.1312 | 1.0837 | 2.1614 | 2.6391 | 2.4826 | 3.0486 | | 1.7455 | 2.4906 | 2.5195 | 3.0666 | H8 | 2.1210 | 1.0866 | 2.1637 | 3.3348 | 2.4658 | 2.5295 | 1.7455 | | 2.5052 | 3.0637 | 2.5134 | H9 | 3.4861 | 2.1704 | 1.0842 | 3.9477 | 4.3223 | 3.7931 | 2.4906 | 2.5052 | | 1.7553 | 1.7538 | H10 | 2.8084 | 2.1709 | 1.0824 | 2.6745 | 3.8057 | 3.1092 | 2.5195 | 3.0637 | 1.7553 | | 1.7550 | H11 | 2.8234 | 2.1776 | 1.0857 | 3.3910 | 3.8137 | 2.6303 | 3.0666 | 2.5134 | 1.7538 | 1.7550 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
113.173 |
|
C1 |
C2 |
H7 |
108.701 |
| C1 |
C2 |
H8 |
107.749 |
|
C2 |
C1 |
F4 |
109.367 |
| C2 |
C1 |
H5 |
112.416 |
|
C2 |
C1 |
H6 |
112.423 |
| C2 |
C3 |
H9 |
110.647 |
|
C2 |
C3 |
H10 |
110.791 |
| C2 |
C3 |
H11 |
111.135 |
|
C3 |
C2 |
H7 |
109.960 |
| C3 |
C2 |
H8 |
109.977 |
|
F4 |
C1 |
H5 |
106.005 |
| F4 |
C1 |
H6 |
106.060 |
|
H5 |
C1 |
H6 |
110.167 |
| H7 |
C2 |
H8 |
107.073 |
|
H9 |
C3 |
H10 |
108.220 |
| H9 |
C3 |
H11 |
107.849 |
|
H10 |
C3 |
H11 |
108.081 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.024 |
|
|
|
| 2 |
C |
-0.283 |
|
|
|
| 3 |
C |
-0.541 |
|
|
|
| 4 |
F |
-0.408 |
|
|
|
| 5 |
H |
0.171 |
|
|
|
| 6 |
H |
0.157 |
|
|
|
| 7 |
H |
0.182 |
|
|
|
| 8 |
H |
0.155 |
|
|
|
| 9 |
H |
0.178 |
|
|
|
| 10 |
H |
0.202 |
|
|
|
| 11 |
H |
0.161 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.467 |
2.215 |
0.757 |
2.762 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-28.063 |
2.876 |
1.100 |
| y |
2.876 |
-25.732 |
-0.076 |
| z |
1.100 |
-0.076 |
-24.675 |
|
| Traceless |
| | x | y | z |
| x |
-2.860 |
2.876 |
1.100 |
| y |
2.876 |
0.637 |
-0.076 |
| z |
1.100 |
-0.076 |
2.223 |
|
| Polar |
| 3z2-r2 | 4.446 |
| x2-y2 | -2.331 |
| xy | 2.876 |
| xz | 1.100 |
| yz | -0.076 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.690 |
0.093 |
-0.025 |
| y |
0.093 |
4.539 |
0.029 |
| z |
-0.025 |
0.029 |
4.307 |
<r2> (average value of r
2) Å
2
| <r2> |
93.023 |
| (<r2>)1/2 |
9.645 |