Jump to
S1C2
Energy calculated at B97D3/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -377.484570 |
| Energy at 298.15K | |
| HF Energy | -377.484570 |
| Nuclear repulsion energy | 189.239724 |
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 B97D3/6-311+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 |
3056 |
3017 |
24.14 |
36.29 |
0.72 |
0.83 |
| 2 |
A |
3012 |
2973 |
27.35 |
93.65 |
0.29 |
0.45 |
| 3 |
A |
2995 |
2956 |
19.31 |
134.25 |
0.06 |
0.11 |
| 4 |
A |
1461 |
1442 |
4.31 |
4.20 |
0.73 |
0.85 |
| 5 |
A |
1403 |
1385 |
8.96 |
1.56 |
0.53 |
0.70 |
| 6 |
A |
1358 |
1340 |
13.92 |
2.55 |
0.74 |
0.85 |
| 7 |
A |
1308 |
1291 |
10.06 |
1.64 |
0.75 |
0.86 |
| 8 |
A |
1238 |
1222 |
9.50 |
3.77 |
0.69 |
0.82 |
| 9 |
A |
1108 |
1094 |
69.77 |
3.49 |
0.30 |
0.46 |
| 10 |
A |
1095 |
1080 |
21.23 |
2.29 |
0.68 |
0.81 |
| 11 |
A |
1045 |
1032 |
269.16 |
0.37 |
0.44 |
0.61 |
| 12 |
A |
1030 |
1017 |
35.99 |
6.52 |
0.43 |
0.60 |
| 13 |
A |
873 |
861 |
43.71 |
4.58 |
0.28 |
0.44 |
| 14 |
A |
558 |
551 |
2.82 |
2.22 |
0.24 |
0.39 |
| 15 |
A |
465 |
459 |
18.08 |
0.63 |
0.73 |
0.85 |
| 16 |
A |
412 |
406 |
3.99 |
1.55 |
0.42 |
0.59 |
| 17 |
A |
240 |
236 |
7.43 |
0.09 |
0.53 |
0.69 |
| 18 |
A |
114 |
113 |
7.76 |
0.05 |
0.68 |
0.81 |
Unscaled Zero Point Vibrational Energy (zpe) 11385.2 cm
-1
Scaled (by 0.987) Zero Point Vibrational Energy (zpe) 11237.2 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 B97D3/6-311+G(3df,2p)
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.784 |
-0.584 |
-0.291 |
| C2 |
0.470 |
0.021 |
0.327 |
| F3 |
-1.900 |
0.112 |
0.156 |
| F4 |
1.538 |
-0.778 |
-0.004 |
| F5 |
0.702 |
1.269 |
-0.182 |
| H6 |
-0.731 |
-0.514 |
-1.383 |
| H7 |
-0.875 |
-1.631 |
0.019 |
| H8 |
0.421 |
0.105 |
1.419 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
F5 |
H6 |
H7 |
H8 |
| C1 | | 1.5229 | 1.3891 | 2.3475 | 2.3779 | 1.0954 | 1.0956 | 2.2025 |
C2 | 1.5229 | | 2.3775 | 1.3741 | 1.3677 | 2.1565 | 2.1518 | 1.0968 | F3 | 1.3891 | 2.3775 | | 3.5547 | 2.8678 | 2.0311 | 2.0264 | 2.6418 | F4 | 2.3475 | 1.3741 | 3.5547 | | 2.2175 | 2.6682 | 2.5594 | 2.0137 | F5 | 2.3779 | 1.3677 | 2.8678 | 2.2175 | | 2.5836 | 3.3070 | 1.9991 | H6 | 1.0954 | 2.1565 | 2.0311 | 2.6682 | 2.5836 | | 1.7987 | 3.0921 | H7 | 1.0956 | 2.1518 | 2.0264 | 2.5594 | 3.3070 | 1.7987 | | 2.5791 | H8 | 2.2025 | 1.0968 | 2.6418 | 2.0137 | 1.9991 | 3.0921 | 2.5791 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
108.149 |
|
C1 |
C2 |
F5 |
110.587 |
| C1 |
C2 |
H8 |
113.436 |
|
C2 |
C1 |
F3 |
109.372 |
| C2 |
C1 |
H6 |
109.827 |
|
C2 |
C1 |
H7 |
109.440 |
| F3 |
C1 |
H6 |
109.106 |
|
F3 |
C1 |
H7 |
108.711 |
| F4 |
C2 |
F5 |
107.956 |
|
F4 |
C2 |
H8 |
108.647 |
| F5 |
C2 |
H8 |
107.918 |
|
H6 |
C1 |
H7 |
110.362 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.184 |
|
|
|
| 2 |
C |
0.743 |
|
|
|
| 3 |
F |
-0.427 |
|
|
|
| 4 |
F |
-0.432 |
|
|
|
| 5 |
F |
-0.436 |
|
|
|
| 6 |
H |
0.130 |
|
|
|
| 7 |
H |
0.124 |
|
|
|
| 8 |
H |
0.115 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.292 |
-1.434 |
0.340 |
1.503 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.641 |
1.685 |
1.552 |
| y |
1.685 |
-28.184 |
0.517 |
| z |
1.552 |
0.517 |
-25.047 |
|
| Traceless |
| | x | y | z |
| x |
-6.025 |
1.685 |
1.552 |
| y |
1.685 |
0.660 |
0.517 |
| z |
1.552 |
0.517 |
5.366 |
|
| Polar |
| 3z2-r2 | 10.731 |
| x2-y2 | -4.457 |
| xy | 1.685 |
| xz | 1.552 |
| yz | 0.517 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.837 |
-0.055 |
-0.008 |
| y |
-0.055 |
4.636 |
0.067 |
| z |
-0.008 |
0.067 |
4.327 |
<r2> (average value of r
2) Å
2
| <r2> |
113.200 |
| (<r2>)1/2 |
10.640 |
Jump to
S1C1
Energy calculated at B97D3/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -377.482690 |
| Energy at 298.15K | |
| HF Energy | -377.482690 |
| Nuclear repulsion energy | 191.797621 |
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 B97D3/6-311+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' |
2987 |
2948 |
59.47 |
166.99 |
0.01 |
0.02 |
| 2 |
A' |
2971 |
2932 |
10.17 |
51.34 |
0.70 |
0.83 |
| 3 |
A' |
1455 |
1436 |
5.23 |
4.24 |
0.72 |
0.84 |
| 4 |
A' |
1386 |
1368 |
6.00 |
1.19 |
0.26 |
0.42 |
| 5 |
A' |
1368 |
1350 |
25.51 |
3.27 |
0.52 |
0.68 |
| 6 |
A' |
1134 |
1120 |
124.15 |
3.89 |
0.12 |
0.22 |
| 7 |
A' |
1056 |
1043 |
32.84 |
3.45 |
0.75 |
0.86 |
| 8 |
A' |
834 |
823 |
31.22 |
7.17 |
0.13 |
0.22 |
| 9 |
A' |
739 |
729 |
49.66 |
2.82 |
0.42 |
0.59 |
| 10 |
A' |
500 |
494 |
9.74 |
1.17 |
0.74 |
0.85 |
| 11 |
A' |
231 |
228 |
1.42 |
0.26 |
0.35 |
0.52 |
| 12 |
A" |
3035 |
2996 |
19.67 |
53.97 |
0.75 |
0.86 |
| 13 |
A" |
1345 |
1327 |
15.76 |
1.25 |
0.75 |
0.86 |
| 14 |
A" |
1253 |
1237 |
12.96 |
6.94 |
0.75 |
0.86 |
| 15 |
A" |
1082 |
1068 |
107.49 |
1.18 |
0.75 |
0.86 |
| 16 |
A" |
910 |
899 |
95.44 |
2.62 |
0.75 |
0.86 |
| 17 |
A" |
362 |
357 |
0.50 |
0.28 |
0.75 |
0.86 |
| 18 |
A" |
116 |
114 |
1.84 |
0.10 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 11381.9 cm
-1
Scaled (by 0.987) Zero Point Vibrational Energy (zpe) 11233.9 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 B97D3/6-311+G(3df,2p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.735 |
-0.843 |
0.000 |
| C2 |
0.356 |
0.631 |
0.000 |
| F3 |
-0.387 |
-1.651 |
0.000 |
| F4 |
-0.387 |
0.943 |
1.106 |
| F5 |
-0.387 |
0.943 |
-1.106 |
| H6 |
1.327 |
-1.059 |
-0.898 |
| H7 |
1.327 |
-1.059 |
0.898 |
| H8 |
1.254 |
1.267 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
F5 |
H6 |
H7 |
H8 |
| C1 | | 1.5214 | 1.3830 | 2.3820 | 2.3820 | 1.0969 | 1.0969 | 2.1725 |
C2 | 1.5214 | | 2.3994 | 1.3687 | 1.3687 | 2.1457 | 2.1457 | 1.1002 | F3 | 1.3830 | 2.3994 | | 2.8199 | 2.8199 | 2.0238 | 2.0238 | 3.3474 | F4 | 2.3820 | 1.3687 | 2.8199 | | 2.2113 | 3.3112 | 2.6446 | 2.0052 | F5 | 2.3820 | 1.3687 | 2.8199 | 2.2113 | | 2.6446 | 3.3112 | 2.0052 | H6 | 1.0969 | 2.1457 | 2.0238 | 3.3112 | 2.6446 | | 1.7954 | 2.4943 | H7 | 1.0969 | 2.1457 | 2.0238 | 2.6446 | 3.3112 | 1.7954 | | 2.4943 | H8 | 2.1725 | 1.1002 | 3.3474 | 2.0052 | 2.0052 | 2.4943 | 2.4943 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
110.896 |
|
C1 |
C2 |
F5 |
110.896 |
| C1 |
C2 |
H8 |
110.905 |
|
C2 |
C1 |
F3 |
111.317 |
| C2 |
C1 |
H6 |
108.993 |
|
C2 |
C1 |
H7 |
108.993 |
| F3 |
C1 |
H6 |
108.838 |
|
F3 |
C1 |
H7 |
108.838 |
| F4 |
C2 |
F5 |
107.759 |
|
F4 |
C2 |
H8 |
108.130 |
| F5 |
C2 |
H8 |
108.130 |
|
H6 |
C1 |
H7 |
109.851 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.171 |
|
|
|
| 2 |
C |
0.778 |
|
|
|
| 3 |
F |
-0.438 |
|
|
|
| 4 |
F |
-0.435 |
|
|
|
| 5 |
F |
-0.435 |
|
|
|
| 6 |
H |
0.125 |
|
|
|
| 7 |
H |
0.125 |
|
|
|
| 8 |
H |
0.110 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
3.101 |
0.038 |
0.000 |
3.101 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.535 |
-0.378 |
0.000 |
| y |
-0.378 |
-29.128 |
0.000 |
| z |
0.000 |
0.000 |
-28.834 |
|
| Traceless |
| | x | y | z |
| x |
3.446 |
-0.378 |
0.000 |
| y |
-0.378 |
-1.944 |
0.000 |
| z |
0.000 |
0.000 |
-1.502 |
|
| Polar |
| 3z2-r2 | -3.005 |
| x2-y2 | 3.594 |
| xy | -0.378 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.578 |
-0.028 |
0.000 |
| y |
-0.028 |
4.709 |
0.000 |
| z |
0.000 |
0.000 |
4.539 |
<r2> (average value of r
2) Å
2
| <r2> |
105.193 |
| (<r2>)1/2 |
10.256 |