Jump to
S1C2
Energy calculated at HF/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -375.931874 |
| Energy at 298.15K | |
| HF Energy | -375.931874 |
| Nuclear repulsion energy | 193.599223 |
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/6-311+G(3df,2p)
| 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 |
3277 |
2977 |
40.15 |
23.80 |
0.38 |
0.55 |
| 2 |
A |
3254 |
2956 |
15.65 |
92.72 |
0.35 |
0.52 |
| 3 |
A |
3215 |
2922 |
21.97 |
109.69 |
0.06 |
0.12 |
| 4 |
A |
1630 |
1481 |
8.18 |
3.13 |
0.74 |
0.85 |
| 5 |
A |
1607 |
1460 |
12.29 |
1.77 |
0.34 |
0.50 |
| 6 |
A |
1537 |
1397 |
25.58 |
1.84 |
0.74 |
0.85 |
| 7 |
A |
1474 |
1339 |
22.04 |
1.15 |
0.75 |
0.86 |
| 8 |
A |
1382 |
1256 |
21.71 |
3.45 |
0.67 |
0.80 |
| 9 |
A |
1280 |
1163 |
112.91 |
3.43 |
0.61 |
0.76 |
| 10 |
A |
1244 |
1131 |
138.84 |
3.09 |
0.75 |
0.86 |
| 11 |
A |
1230 |
1117 |
129.84 |
1.51 |
0.23 |
0.38 |
| 12 |
A |
1199 |
1090 |
83.45 |
5.07 |
0.36 |
0.53 |
| 13 |
A |
990 |
900 |
35.58 |
4.62 |
0.22 |
0.36 |
| 14 |
A |
637 |
578 |
5.27 |
1.49 |
0.24 |
0.39 |
| 15 |
A |
520 |
473 |
24.01 |
0.40 |
0.73 |
0.85 |
| 16 |
A |
465 |
423 |
6.17 |
1.23 |
0.37 |
0.53 |
| 17 |
A |
267 |
243 |
9.38 |
0.05 |
0.49 |
0.66 |
| 18 |
A |
130 |
118 |
9.81 |
0.02 |
0.73 |
0.84 |
Unscaled Zero Point Vibrational Energy (zpe) 12668.7 cm
-1
Scaled (by 0.9086) Zero Point Vibrational Energy (zpe) 11510.8 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/6-311+G(3df,2p)
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.780 |
-0.579 |
-0.278 |
| C2 |
0.468 |
0.019 |
0.322 |
| F3 |
-1.855 |
0.123 |
0.150 |
| F4 |
1.504 |
-0.753 |
-0.007 |
| F5 |
0.691 |
1.229 |
-0.182 |
| H6 |
-0.728 |
-0.528 |
-1.357 |
| H7 |
-0.880 |
-1.607 |
0.042 |
| H8 |
0.417 |
0.102 |
1.398 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
F5 |
H6 |
H7 |
H8 |
| C1 | | 1.5089 | 1.3530 | 2.3072 | 2.3334 | 1.0812 | 1.0809 | 2.1697 |
C2 | 1.5089 | | 2.3312 | 1.3338 | 1.3296 | 2.1330 | 2.1304 | 1.0804 | F3 | 1.3530 | 2.3312 | | 3.4748 | 2.7955 | 1.9914 | 1.9883 | 2.5918 | F4 | 2.3072 | 1.3338 | 3.4748 | | 2.1497 | 2.6182 | 2.5328 | 1.9719 | F5 | 2.3334 | 1.3296 | 2.7955 | 2.1497 | | 2.5464 | 3.2497 | 1.9603 | H6 | 1.0812 | 2.1330 | 1.9914 | 2.6182 | 2.5464 | | 1.7728 | 3.0494 | H7 | 1.0809 | 2.1304 | 1.9883 | 2.5328 | 3.2497 | 1.7728 | | 2.5376 | H8 | 2.1697 | 1.0804 | 2.5918 | 1.9719 | 1.9603 | 3.0494 | 2.5376 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
108.355 |
|
C1 |
C2 |
F5 |
110.418 |
| C1 |
C2 |
H8 |
112.806 |
|
C2 |
C1 |
F3 |
108.969 |
| C2 |
C1 |
H6 |
109.777 |
|
C2 |
C1 |
H7 |
109.581 |
| F3 |
C1 |
H6 |
109.289 |
|
F3 |
C1 |
H7 |
109.044 |
| F4 |
C2 |
F5 |
107.631 |
|
F4 |
C2 |
H8 |
109.081 |
| F5 |
C2 |
H8 |
108.416 |
|
H6 |
C1 |
H7 |
110.158 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.268 |
|
|
|
| 2 |
C |
0.998 |
|
|
|
| 3 |
F |
-0.549 |
|
|
|
| 4 |
F |
-0.555 |
|
|
|
| 5 |
F |
-0.562 |
|
|
|
| 6 |
H |
0.139 |
|
|
|
| 7 |
H |
0.133 |
|
|
|
| 8 |
H |
0.128 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.321 |
-1.592 |
0.428 |
1.680 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.770 |
1.907 |
1.710 |
| y |
1.907 |
-28.029 |
0.551 |
| z |
1.710 |
0.551 |
-24.544 |
|
| Traceless |
| | x | y | z |
| x |
-6.484 |
1.907 |
1.710 |
| y |
1.907 |
0.628 |
0.551 |
| z |
1.710 |
0.551 |
5.856 |
|
| Polar |
| 3z2-r2 | 11.711 |
| x2-y2 | -4.742 |
| xy | 1.907 |
| xz | 1.710 |
| yz | 0.551 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.007 |
-0.033 |
-0.007 |
| y |
-0.033 |
3.895 |
0.045 |
| z |
-0.007 |
0.045 |
3.724 |
<r2> (average value of r
2) Å
2
| <r2> |
108.945 |
| (<r2>)1/2 |
10.438 |
Jump to
S1C1
Energy calculated at HF/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -375.929734 |
| Energy at 298.15K | |
| HF Energy | -375.929734 |
| Nuclear repulsion energy | 196.317346 |
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/6-311+G(3df,2p)
| 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' |
3233 |
2938 |
60.84 |
108.82 |
0.08 |
0.14 |
| 2 |
A' |
3203 |
2910 |
9.95 |
73.74 |
0.18 |
0.31 |
| 3 |
A' |
1624 |
1475 |
10.49 |
2.44 |
0.74 |
0.85 |
| 4 |
A' |
1581 |
1437 |
22.17 |
2.45 |
0.27 |
0.42 |
| 5 |
A' |
1547 |
1405 |
24.26 |
1.31 |
0.66 |
0.80 |
| 6 |
A' |
1307 |
1187 |
154.07 |
3.75 |
0.30 |
0.46 |
| 7 |
A' |
1217 |
1106 |
33.48 |
3.48 |
0.75 |
0.85 |
| 8 |
A' |
944 |
858 |
41.77 |
7.55 |
0.11 |
0.20 |
| 9 |
A' |
829 |
753 |
64.44 |
2.20 |
0.39 |
0.57 |
| 10 |
A' |
571 |
519 |
16.39 |
0.80 |
0.75 |
0.86 |
| 11 |
A' |
258 |
235 |
2.08 |
0.16 |
0.36 |
0.53 |
| 12 |
A" |
3257 |
2959 |
24.12 |
44.03 |
0.75 |
0.86 |
| 13 |
A" |
1531 |
1391 |
32.65 |
0.96 |
0.75 |
0.86 |
| 14 |
A" |
1402 |
1274 |
29.15 |
5.83 |
0.75 |
0.86 |
| 15 |
A" |
1267 |
1151 |
132.07 |
1.62 |
0.75 |
0.86 |
| 16 |
A" |
1056 |
959 |
63.99 |
2.02 |
0.75 |
0.86 |
| 17 |
A" |
399 |
362 |
0.31 |
0.14 |
0.75 |
0.86 |
| 18 |
A" |
130 |
118 |
2.57 |
0.04 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12677.0 cm
-1
Scaled (by 0.9086) Zero Point Vibrational Energy (zpe) 11518.3 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/6-311+G(3df,2p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.725 |
-0.835 |
0.000 |
| C2 |
0.348 |
0.625 |
0.000 |
| F3 |
-0.381 |
-1.606 |
0.000 |
| F4 |
-0.381 |
0.920 |
1.073 |
| F5 |
-0.381 |
0.920 |
-1.073 |
| H6 |
1.307 |
-1.053 |
-0.886 |
| H7 |
1.307 |
-1.053 |
0.886 |
| H8 |
1.230 |
1.253 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
F5 |
H6 |
H7 |
H8 |
| C1 | | 1.5078 | 1.3484 | 2.3354 | 2.3354 | 1.0821 | 1.0821 | 2.1478 |
C2 | 1.5078 | | 2.3475 | 1.3303 | 1.3303 | 2.1262 | 2.1262 | 1.0827 | F3 | 1.3484 | 2.3475 | | 2.7451 | 2.7451 | 1.9847 | 1.9847 | 3.2818 | F4 | 2.3354 | 1.3303 | 2.7451 | | 2.1460 | 3.2526 | 2.6035 | 1.9640 | F5 | 2.3354 | 1.3303 | 2.7451 | 2.1460 | | 2.6035 | 3.2526 | 1.9640 | H6 | 1.0821 | 2.1262 | 1.9847 | 3.2526 | 2.6035 | | 1.7714 | 2.4713 | H7 | 1.0821 | 2.1262 | 1.9847 | 2.6035 | 3.2526 | 1.7714 | | 2.4713 | H8 | 2.1478 | 1.0827 | 3.2818 | 1.9640 | 1.9640 | 2.4713 | 2.4713 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
110.598 |
|
C1 |
C2 |
F5 |
110.598 |
| C1 |
C2 |
H8 |
110.951 |
|
C2 |
C1 |
F3 |
110.429 |
| C2 |
C1 |
H6 |
109.261 |
|
C2 |
C1 |
H7 |
109.261 |
| F3 |
C1 |
H6 |
109.001 |
|
F3 |
C1 |
H7 |
109.001 |
| F4 |
C2 |
F5 |
107.528 |
|
F4 |
C2 |
H8 |
108.531 |
| F5 |
C2 |
H8 |
108.531 |
|
H6 |
C1 |
H7 |
109.876 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.246 |
|
|
|
| 2 |
C |
1.044 |
|
|
|
| 3 |
F |
-0.565 |
|
|
|
| 4 |
F |
-0.558 |
|
|
|
| 5 |
F |
-0.558 |
|
|
|
| 6 |
H |
0.133 |
|
|
|
| 7 |
H |
0.133 |
|
|
|
| 8 |
H |
0.124 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
3.420 |
0.088 |
0.000 |
3.421 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.209 |
-0.388 |
0.000 |
| y |
-0.388 |
-28.878 |
0.000 |
| z |
0.000 |
0.000 |
-28.688 |
|
| Traceless |
| | x | y | z |
| x |
3.574 |
-0.388 |
0.000 |
| y |
-0.388 |
-1.930 |
0.000 |
| z |
0.000 |
0.000 |
-1.644 |
|
| Polar |
| 3z2-r2 | -3.288 |
| x2-y2 | 3.670 |
| xy | -0.388 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.873 |
-0.009 |
0.000 |
| y |
-0.009 |
3.933 |
0.000 |
| z |
0.000 |
0.000 |
3.833 |
<r2> (average value of r
2) Å
2
| <r2> |
101.033 |
| (<r2>)1/2 |
10.052 |