Jump to
S1C2
Energy calculated at B1B95/3-21G
| | hartrees |
| Energy at 0K | -375.366790 |
| Energy at 298.15K | |
| HF Energy | -375.366790 |
| Nuclear repulsion energy | 188.846760 |
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 B1B95/3-21G
| 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 |
3175 |
3037 |
33.79 |
30.79 |
0.54 |
0.70 |
| 2 |
A |
3146 |
3010 |
25.96 |
86.07 |
0.45 |
0.62 |
| 3 |
A |
3116 |
2981 |
9.78 |
99.94 |
0.10 |
0.18 |
| 4 |
A |
1570 |
1502 |
3.45 |
11.98 |
0.74 |
0.85 |
| 5 |
A |
1481 |
1417 |
11.83 |
4.84 |
0.74 |
0.85 |
| 6 |
A |
1465 |
1401 |
21.97 |
8.11 |
0.74 |
0.85 |
| 7 |
A |
1381 |
1321 |
17.45 |
4.71 |
0.75 |
0.86 |
| 8 |
A |
1291 |
1235 |
7.82 |
10.76 |
0.73 |
0.85 |
| 9 |
A |
1183 |
1132 |
99.27 |
4.72 |
0.73 |
0.85 |
| 10 |
A |
1153 |
1103 |
17.11 |
3.91 |
0.70 |
0.82 |
| 11 |
A |
1140 |
1091 |
103.28 |
1.85 |
0.44 |
0.61 |
| 12 |
A |
1103 |
1056 |
8.22 |
7.46 |
0.47 |
0.64 |
| 13 |
A |
937 |
897 |
19.53 |
5.95 |
0.32 |
0.49 |
| 14 |
A |
554 |
530 |
4.94 |
2.18 |
0.45 |
0.62 |
| 15 |
A |
446 |
426 |
19.00 |
0.95 |
0.74 |
0.85 |
| 16 |
A |
410 |
392 |
7.95 |
1.78 |
0.56 |
0.72 |
| 17 |
A |
212 |
203 |
10.50 |
0.06 |
0.60 |
0.75 |
| 18 |
A |
124 |
118 |
9.07 |
0.04 |
0.72 |
0.84 |
Unscaled Zero Point Vibrational Energy (zpe) 11943.3 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 11426.2 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 B1B95/3-21G
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.754 |
-0.586 |
-0.308 |
| C2 |
0.460 |
0.026 |
0.336 |
| F3 |
-1.899 |
0.083 |
0.160 |
| F4 |
1.544 |
-0.776 |
0.004 |
| F5 |
0.673 |
1.292 |
-0.181 |
| H6 |
-0.660 |
-0.482 |
-1.390 |
| H7 |
-0.793 |
-1.643 |
-0.045 |
| H8 |
0.357 |
0.091 |
1.417 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
F5 |
H6 |
H7 |
H8 |
| C1 | | 1.5048 | 1.4069 | 2.3269 | 2.3621 | 1.0904 | 1.0894 | 2.1612 |
C2 | 1.5048 | | 2.3668 | 1.3884 | 1.3833 | 2.1194 | 2.1215 | 1.0882 | F3 | 1.4069 | 2.3668 | | 3.5523 | 2.8624 | 2.0633 | 2.0601 | 2.5830 | F4 | 2.3269 | 1.3884 | 3.5523 | | 2.2509 | 2.6244 | 2.4933 | 2.0388 | F5 | 2.3621 | 1.3833 | 2.8624 | 2.2509 | | 2.5272 | 3.2830 | 2.0235 | H6 | 1.0904 | 2.1194 | 2.0633 | 2.6244 | 2.5272 | | 1.7812 | 3.0402 | H7 | 1.0894 | 2.1215 | 2.0601 | 2.4933 | 3.2830 | 1.7812 | | 2.5428 | H8 | 2.1612 | 1.0882 | 2.5830 | 2.0388 | 2.0235 | 3.0402 | 2.5428 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
107.008 |
|
C1 |
C2 |
F5 |
109.670 |
| C1 |
C2 |
H8 |
111.912 |
|
C2 |
C1 |
F3 |
108.702 |
| C2 |
C1 |
H6 |
108.441 |
|
C2 |
C1 |
H7 |
108.667 |
| F3 |
C1 |
H6 |
110.786 |
|
F3 |
C1 |
H7 |
110.589 |
| F4 |
C2 |
F5 |
108.604 |
|
F4 |
C2 |
H8 |
110.232 |
| F5 |
C2 |
H8 |
109.341 |
|
H6 |
C1 |
H7 |
109.597 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.158 |
|
|
|
| 2 |
C |
0.346 |
|
|
|
| 3 |
F |
-0.298 |
|
|
|
| 4 |
F |
-0.299 |
|
|
|
| 5 |
F |
-0.292 |
|
|
|
| 6 |
H |
0.243 |
|
|
|
| 7 |
H |
0.228 |
|
|
|
| 8 |
H |
0.230 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.202 |
-1.450 |
0.341 |
1.503 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.197 |
1.425 |
1.317 |
| y |
1.425 |
-27.418 |
0.595 |
| z |
1.317 |
0.595 |
-24.154 |
|
| Traceless |
| | x | y | z |
| x |
-6.411 |
1.425 |
1.317 |
| y |
1.425 |
0.757 |
0.595 |
| z |
1.317 |
0.595 |
5.654 |
|
| Polar |
| 3z2-r2 | 11.307 |
| x2-y2 | -4.779 |
| xy | 1.425 |
| xz | 1.317 |
| yz | 0.595 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.960 |
-0.088 |
-0.047 |
| y |
-0.088 |
3.075 |
0.028 |
| z |
-0.047 |
0.028 |
2.930 |
<r2> (average value of r
2) Å
2
| <r2> |
112.526 |
| (<r2>)1/2 |
10.608 |
Jump to
S1C1
Energy calculated at B1B95/3-21G
| | hartrees |
| Energy at 0K | -375.363244 |
| Energy at 298.15K | |
| HF Energy | -375.363244 |
| Nuclear repulsion energy | 191.617603 |
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 B1B95/3-21G
| 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' |
3119 |
2984 |
57.68 |
106.54 |
0.06 |
0.11 |
| 2 |
A' |
3100 |
2966 |
9.71 |
56.61 |
0.51 |
0.68 |
| 3 |
A' |
1564 |
1496 |
3.17 |
12.84 |
0.74 |
0.85 |
| 4 |
A' |
1498 |
1433 |
6.30 |
2.68 |
0.74 |
0.85 |
| 5 |
A' |
1436 |
1374 |
28.48 |
8.04 |
0.69 |
0.81 |
| 6 |
A' |
1193 |
1141 |
80.76 |
6.03 |
0.46 |
0.63 |
| 7 |
A' |
1099 |
1051 |
8.64 |
3.18 |
0.71 |
0.83 |
| 8 |
A' |
887 |
849 |
30.23 |
7.97 |
0.16 |
0.28 |
| 9 |
A' |
741 |
708 |
39.47 |
3.20 |
0.55 |
0.71 |
| 10 |
A' |
479 |
458 |
15.08 |
2.11 |
0.75 |
0.86 |
| 11 |
A' |
211 |
202 |
1.99 |
0.13 |
0.53 |
0.69 |
| 12 |
A" |
3154 |
3017 |
22.06 |
55.23 |
0.75 |
0.86 |
| 13 |
A" |
1459 |
1396 |
34.34 |
1.84 |
0.75 |
0.86 |
| 14 |
A" |
1323 |
1265 |
7.88 |
24.54 |
0.75 |
0.86 |
| 15 |
A" |
1178 |
1127 |
63.55 |
1.20 |
0.75 |
0.86 |
| 16 |
A" |
1008 |
964 |
38.74 |
4.51 |
0.75 |
0.86 |
| 17 |
A" |
339 |
324 |
0.02 |
0.23 |
0.75 |
0.86 |
| 18 |
A" |
115 |
110 |
2.38 |
0.07 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 11950.1 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 11432.7 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 B1B95/3-21G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.755 |
-0.817 |
0.000 |
| C2 |
0.363 |
0.635 |
0.000 |
| F3 |
-0.395 |
-1.624 |
0.000 |
| F4 |
-0.395 |
0.915 |
1.125 |
| F5 |
-0.395 |
0.915 |
-1.125 |
| H6 |
1.354 |
-1.015 |
-0.890 |
| H7 |
1.354 |
-1.015 |
0.890 |
| H8 |
1.252 |
1.267 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
F5 |
H6 |
H7 |
H8 |
| C1 | | 1.5044 | 1.4053 | 2.3636 | 2.3636 | 1.0909 | 1.0909 | 2.1425 |
C2 | 1.5044 | | 2.3830 | 1.3847 | 1.3847 | 2.1210 | 2.1210 | 1.0908 | F3 | 1.4053 | 2.3830 | | 2.7765 | 2.7765 | 2.0547 | 2.0547 | 3.3274 | F4 | 2.3636 | 1.3847 | 2.7765 | | 2.2492 | 3.2928 | 2.6148 | 2.0254 | F5 | 2.3636 | 1.3847 | 2.7765 | 2.2492 | | 2.6148 | 3.2928 | 2.0254 | H6 | 1.0909 | 2.1210 | 2.0547 | 3.2928 | 2.6148 | | 1.7807 | 2.4519 | H7 | 1.0909 | 2.1210 | 2.0547 | 2.6148 | 3.2928 | 1.7807 | | 2.4519 | H8 | 2.1425 | 1.0908 | 3.3274 | 2.0254 | 2.0254 | 2.4519 | 2.4519 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
109.725 |
|
C1 |
C2 |
F5 |
109.725 |
| C1 |
C2 |
H8 |
110.276 |
|
C2 |
C1 |
F3 |
109.924 |
| C2 |
C1 |
H6 |
108.568 |
|
C2 |
C1 |
H7 |
108.568 |
| F3 |
C1 |
H6 |
110.167 |
|
F3 |
C1 |
H7 |
110.167 |
| F4 |
C2 |
F5 |
108.616 |
|
F4 |
C2 |
H8 |
109.235 |
| F5 |
C2 |
H8 |
109.235 |
|
H6 |
C1 |
H7 |
109.410 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.139 |
|
|
|
| 2 |
C |
0.356 |
|
|
|
| 3 |
F |
-0.290 |
|
|
|
| 4 |
F |
-0.292 |
|
|
|
| 5 |
F |
-0.292 |
|
|
|
| 6 |
H |
0.225 |
|
|
|
| 7 |
H |
0.225 |
|
|
|
| 8 |
H |
0.208 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
3.288 |
0.164 |
0.000 |
3.292 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.516 |
-0.259 |
0.000 |
| y |
-0.259 |
-28.509 |
0.000 |
| z |
0.000 |
0.000 |
-28.194 |
|
| Traceless |
| | x | y | z |
| x |
3.836 |
-0.259 |
0.000 |
| y |
-0.259 |
-2.154 |
0.000 |
| z |
0.000 |
0.000 |
-1.681 |
|
| Polar |
| 3z2-r2 | -3.362 |
| x2-y2 | 3.993 |
| xy | -0.259 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.059 |
0.067 |
0.000 |
| y |
0.067 |
2.926 |
0.000 |
| z |
0.000 |
0.000 |
3.071 |
<r2> (average value of r
2) Å
2
| <r2> |
103.806 |
| (<r2>)1/2 |
10.189 |