Jump to
S1C2
Energy calculated at B1B95/6-31G*
| | hartrees |
| Energy at 0K | -377.417921 |
| Energy at 298.15K | |
| HF Energy | -377.417921 |
| Nuclear repulsion energy | 191.579401 |
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 B1B95/6-31G*
| 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 |
3165 |
3005 |
35.79 |
37.81 |
0.69 |
0.81 |
| 2 |
A |
3129 |
2970 |
33.20 |
92.53 |
0.35 |
0.52 |
| 3 |
A |
3102 |
2944 |
18.31 |
100.71 |
0.09 |
0.17 |
| 4 |
A |
1534 |
1457 |
2.90 |
9.43 |
0.73 |
0.84 |
| 5 |
A |
1491 |
1416 |
16.15 |
3.31 |
0.67 |
0.81 |
| 6 |
A |
1445 |
1372 |
33.14 |
5.09 |
0.74 |
0.85 |
| 7 |
A |
1369 |
1300 |
29.10 |
3.36 |
0.75 |
0.86 |
| 8 |
A |
1284 |
1219 |
13.17 |
9.53 |
0.73 |
0.84 |
| 9 |
A |
1199 |
1139 |
108.43 |
4.79 |
0.69 |
0.82 |
| 10 |
A |
1169 |
1109 |
195.60 |
1.73 |
0.69 |
0.81 |
| 11 |
A |
1160 |
1101 |
20.89 |
2.65 |
0.61 |
0.76 |
| 12 |
A |
1140 |
1082 |
16.74 |
5.60 |
0.43 |
0.60 |
| 13 |
A |
932 |
885 |
26.84 |
5.21 |
0.36 |
0.52 |
| 14 |
A |
580 |
551 |
4.04 |
1.68 |
0.43 |
0.60 |
| 15 |
A |
479 |
455 |
16.90 |
0.75 |
0.73 |
0.84 |
| 16 |
A |
427 |
405 |
5.79 |
1.47 |
0.53 |
0.69 |
| 17 |
A |
233 |
221 |
7.76 |
0.04 |
0.54 |
0.70 |
| 18 |
A |
119 |
113 |
6.67 |
0.01 |
0.71 |
0.83 |
Unscaled Zero Point Vibrational Energy (zpe) 11978.0 cm
-1
Scaled (by 0.9493) Zero Point Vibrational Energy (zpe) 11370.7 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 B1B95/6-31G*
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.766 |
-0.600 |
-0.272 |
| C2 |
0.469 |
0.022 |
0.330 |
| F3 |
-1.867 |
0.105 |
0.144 |
| F4 |
1.534 |
-0.746 |
-0.013 |
| F5 |
0.655 |
1.260 |
-0.182 |
| H6 |
-0.690 |
-0.561 |
-1.361 |
| H7 |
-0.851 |
-1.639 |
0.054 |
| H8 |
0.419 |
0.101 |
1.418 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
F5 |
H6 |
H7 |
H8 |
| C1 | | 1.5079 | 1.3716 | 2.3194 | 2.3421 | 1.0929 | 1.0925 | 2.1801 |
C2 | 1.5079 | | 2.3447 | 1.3574 | 1.3519 | 2.1310 | 2.1397 | 1.0929 | F3 | 1.3716 | 2.3447 | | 3.5095 | 2.7924 | 2.0231 | 2.0206 | 2.6175 | F4 | 2.3194 | 1.3574 | 3.5095 | | 2.1970 | 2.6075 | 2.5477 | 2.0025 | F5 | 2.3421 | 1.3519 | 2.7924 | 2.1970 | | 2.5520 | 3.2753 | 1.9897 | H6 | 1.0929 | 2.1310 | 2.0231 | 2.6075 | 2.5520 | | 1.7869 | 3.0650 | H7 | 1.0925 | 2.1397 | 2.0206 | 2.5477 | 3.2753 | 1.7869 | | 2.5501 | H8 | 2.1801 | 1.0929 | 2.6175 | 2.0025 | 1.9897 | 3.0650 | 2.5501 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
107.975 |
|
C1 |
C2 |
F5 |
109.842 |
| C1 |
C2 |
H8 |
112.939 |
|
C2 |
C1 |
F3 |
108.938 |
| C2 |
C1 |
H6 |
108.998 |
|
C2 |
C1 |
H7 |
109.702 |
| F3 |
C1 |
H6 |
109.830 |
|
F3 |
C1 |
H7 |
109.653 |
| F4 |
C2 |
F5 |
108.366 |
|
F4 |
C2 |
H8 |
109.144 |
| F5 |
C2 |
H8 |
108.479 |
|
H6 |
C1 |
H7 |
109.703 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.037 |
|
|
|
| 2 |
C |
0.410 |
|
|
|
| 3 |
F |
-0.304 |
|
|
|
| 4 |
F |
-0.290 |
|
|
|
| 5 |
F |
-0.281 |
|
|
|
| 6 |
H |
0.178 |
|
|
|
| 7 |
H |
0.168 |
|
|
|
| 8 |
H |
0.154 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.178 |
-1.351 |
0.355 |
1.408 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.094 |
1.378 |
1.188 |
| y |
1.378 |
-26.973 |
0.470 |
| z |
1.188 |
0.470 |
-24.348 |
|
| Traceless |
| | x | y | z |
| x |
-5.433 |
1.378 |
1.188 |
| y |
1.378 |
0.748 |
0.470 |
| z |
1.188 |
0.470 |
4.685 |
|
| Polar |
| 3z2-r2 | 9.369 |
| x2-y2 | -4.121 |
| xy | 1.378 |
| xz | 1.188 |
| yz | 0.470 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.438 |
-0.002 |
0.019 |
| y |
-0.002 |
3.477 |
0.033 |
| z |
0.019 |
0.033 |
3.424 |
<r2> (average value of r
2) Å
2
| <r2> |
109.801 |
| (<r2>)1/2 |
10.479 |
Jump to
S1C1
Energy calculated at B1B95/6-31G*
| | hartrees |
| Energy at 0K | -377.415502 |
| Energy at 298.15K | |
| HF Energy | -377.415502 |
| Nuclear repulsion energy | 194.516101 |
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 B1B95/6-31G*
| 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' |
3105 |
2947 |
69.84 |
113.10 |
0.05 |
0.10 |
| 2 |
A' |
3088 |
2931 |
7.99 |
60.14 |
0.45 |
0.62 |
| 3 |
A' |
1532 |
1454 |
4.64 |
8.35 |
0.73 |
0.84 |
| 4 |
A' |
1468 |
1394 |
27.26 |
3.02 |
0.57 |
0.73 |
| 5 |
A' |
1447 |
1373 |
32.75 |
4.38 |
0.72 |
0.84 |
| 6 |
A' |
1218 |
1156 |
118.82 |
5.47 |
0.40 |
0.57 |
| 7 |
A' |
1146 |
1088 |
17.81 |
3.01 |
0.74 |
0.85 |
| 8 |
A' |
901 |
856 |
29.67 |
7.10 |
0.21 |
0.35 |
| 9 |
A' |
774 |
735 |
46.73 |
2.68 |
0.54 |
0.70 |
| 10 |
A' |
514 |
488 |
11.94 |
1.49 |
0.75 |
0.86 |
| 11 |
A' |
221 |
210 |
1.71 |
0.09 |
0.38 |
0.55 |
| 12 |
A" |
3148 |
2989 |
27.93 |
55.10 |
0.75 |
0.86 |
| 13 |
A" |
1439 |
1366 |
43.23 |
1.74 |
0.75 |
0.86 |
| 14 |
A" |
1300 |
1234 |
17.28 |
16.86 |
0.75 |
0.86 |
| 15 |
A" |
1187 |
1127 |
97.78 |
1.01 |
0.75 |
0.86 |
| 16 |
A" |
988 |
938 |
49.86 |
3.81 |
0.75 |
0.86 |
| 17 |
A" |
369 |
350 |
0.15 |
0.15 |
0.75 |
0.86 |
| 18 |
A" |
104 |
98 |
1.88 |
0.01 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 11973.9 cm
-1
Scaled (by 0.9493) Zero Point Vibrational Energy (zpe) 11366.8 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 B1B95/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.740 |
-0.827 |
0.000 |
| C2 |
0.356 |
0.630 |
0.000 |
| F3 |
-0.388 |
-1.600 |
0.000 |
| F4 |
-0.388 |
0.911 |
1.095 |
| F5 |
-0.388 |
0.911 |
-1.095 |
| H6 |
1.333 |
-1.045 |
-0.893 |
| H7 |
1.333 |
-1.045 |
0.893 |
| H8 |
1.237 |
1.280 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
F5 |
H6 |
H7 |
H8 |
| C1 | | 1.5068 | 1.3681 | 2.3434 | 2.3434 | 1.0937 | 1.0937 | 2.1647 |
C2 | 1.5068 | | 2.3510 | 1.3535 | 1.3535 | 2.1355 | 2.1355 | 1.0953 | F3 | 1.3681 | 2.3510 | | 2.7391 | 2.7391 | 2.0169 | 2.0169 | 3.3073 | F4 | 2.3434 | 1.3535 | 2.7391 | | 2.1909 | 3.2774 | 2.6135 | 1.9946 | F5 | 2.3434 | 1.3535 | 2.7391 | 2.1909 | | 2.6135 | 3.2774 | 1.9946 | H6 | 1.0937 | 2.1355 | 2.0169 | 3.2774 | 2.6135 | | 1.7850 | 2.4930 | H7 | 1.0937 | 2.1355 | 2.0169 | 2.6135 | 3.2774 | 1.7850 | | 2.4930 | H8 | 2.1647 | 1.0953 | 3.3073 | 1.9946 | 1.9946 | 2.4930 | 2.4930 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
109.907 |
|
C1 |
C2 |
F5 |
109.907 |
| C1 |
C2 |
H8 |
111.617 |
|
C2 |
C1 |
F3 |
109.633 |
| C2 |
C1 |
H6 |
109.379 |
|
C2 |
C1 |
H7 |
109.379 |
| F3 |
C1 |
H6 |
109.525 |
|
F3 |
C1 |
H7 |
109.525 |
| F4 |
C2 |
F5 |
108.068 |
|
F4 |
C2 |
H8 |
108.629 |
| F5 |
C2 |
H8 |
108.629 |
|
H6 |
C1 |
H7 |
109.385 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.025 |
|
|
|
| 2 |
C |
0.421 |
|
|
|
| 3 |
F |
-0.297 |
|
|
|
| 4 |
F |
-0.284 |
|
|
|
| 5 |
F |
-0.284 |
|
|
|
| 6 |
H |
0.166 |
|
|
|
| 7 |
H |
0.166 |
|
|
|
| 8 |
H |
0.138 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.873 |
0.100 |
0.000 |
2.875 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.587 |
-0.298 |
0.000 |
| y |
-0.298 |
-27.980 |
0.000 |
| z |
0.000 |
0.000 |
-27.688 |
|
| Traceless |
| | x | y | z |
| x |
3.247 |
-0.298 |
0.000 |
| y |
-0.298 |
-1.842 |
0.000 |
| z |
0.000 |
0.000 |
-1.405 |
|
| Polar |
| 3z2-r2 | -2.810 |
| x2-y2 | 3.393 |
| xy | -0.298 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.467 |
0.012 |
0.000 |
| y |
0.012 |
3.464 |
0.000 |
| z |
0.000 |
0.000 |
3.468 |
<r2> (average value of r
2) Å
2
| <r2> |
101.376 |
| (<r2>)1/2 |
10.069 |