Jump to
S1C2
Energy calculated at B2PLYP/daug-cc-pVDZ
| | hartrees |
| Energy at 0K | -278.105357 |
| Energy at 298.15K | |
| HF Energy | -277.876915 |
| Nuclear repulsion energy | 124.707918 |
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 B2PLYP/daug-cc-pVDZ
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Ag |
3092 |
3092 |
0.00 |
248.28 |
0.05 |
0.10 |
| 2 |
Ag |
1503 |
1503 |
0.00 |
6.73 |
0.75 |
0.85 |
| 3 |
Ag |
1429 |
1429 |
0.00 |
2.63 |
0.49 |
0.66 |
| 4 |
Ag |
1103 |
1103 |
0.00 |
6.92 |
0.37 |
0.54 |
| 5 |
Ag |
1031 |
1031 |
0.00 |
11.67 |
0.36 |
0.53 |
| 6 |
Ag |
452 |
452 |
0.00 |
2.80 |
0.33 |
0.49 |
| 7 |
Au |
3173 |
3173 |
36.66 |
0.00 |
0.00 |
0.00 |
| 8 |
Au |
1219 |
1219 |
4.07 |
0.00 |
0.00 |
0.00 |
| 9 |
Au |
811 |
811 |
0.01 |
0.00 |
0.00 |
0.00 |
| 10 |
Au |
116 |
116 |
13.97 |
0.00 |
0.00 |
0.00 |
| 11 |
Bg |
3149 |
3149 |
0.00 |
104.99 |
0.75 |
0.86 |
| 12 |
Bg |
1290 |
1290 |
0.00 |
6.50 |
0.75 |
0.86 |
| 13 |
Bg |
1163 |
1163 |
0.00 |
1.48 |
0.75 |
0.86 |
| 14 |
Bu |
3098 |
3098 |
51.82 |
0.00 |
0.00 |
0.00 |
| 15 |
Bu |
1509 |
1509 |
3.83 |
0.00 |
0.74 |
0.85 |
| 16 |
Bu |
1338 |
1338 |
5.73 |
0.00 |
0.00 |
0.00 |
| 17 |
Bu |
1038 |
1038 |
219.09 |
0.00 |
0.00 |
0.00 |
| 18 |
Bu |
280 |
280 |
20.56 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 13395.5 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 13395.5 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 B2PLYP/daug-cc-pVDZ
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.430 |
0.625 |
0.000 |
| C2 |
-0.430 |
-0.625 |
0.000 |
| F3 |
-0.430 |
1.737 |
0.000 |
| F4 |
0.430 |
-1.737 |
0.000 |
| H5 |
1.055 |
0.679 |
0.899 |
| H6 |
1.055 |
0.679 |
-0.899 |
| H7 |
-1.055 |
-0.679 |
0.899 |
| H8 |
-1.055 |
-0.679 |
-0.899 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5176 | 1.4060 | 2.3620 | 1.0965 | 1.0965 | 2.1720 | 2.1720 |
C2 | 1.5176 | | 2.3620 | 1.4060 | 2.1720 | 2.1720 | 1.0965 | 1.0965 | F3 | 1.4060 | 2.3620 | | 3.5789 | 2.0332 | 2.0332 | 2.6530 | 2.6530 | F4 | 2.3620 | 1.4060 | 3.5789 | | 2.6530 | 2.6530 | 2.0332 | 2.0332 | H5 | 1.0965 | 2.1720 | 2.0332 | 2.6530 | | 1.7982 | 2.5105 | 3.0881 | H6 | 1.0965 | 2.1720 | 2.0332 | 2.6530 | 1.7982 | | 3.0881 | 2.5105 | H7 | 2.1720 | 1.0965 | 2.6530 | 2.0332 | 2.5105 | 3.0881 | | 1.7982 | H8 | 2.1720 | 1.0965 | 2.6530 | 2.0332 | 3.0881 | 2.5105 | 1.7982 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
107.724 |
|
C1 |
C2 |
H7 |
111.358 |
| C1 |
C2 |
H8 |
111.358 |
|
C2 |
C1 |
F3 |
107.724 |
| C2 |
C1 |
H5 |
111.358 |
|
C2 |
C1 |
H6 |
111.358 |
| F3 |
C1 |
H5 |
108.044 |
|
F3 |
C1 |
H6 |
108.044 |
| F4 |
C2 |
H7 |
108.044 |
|
F4 |
C2 |
H8 |
108.044 |
| H5 |
C1 |
H6 |
110.166 |
|
H7 |
C2 |
H8 |
110.166 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/daug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
1.381 |
|
|
|
| 2 |
C |
1.381 |
|
|
|
| 3 |
F |
-0.678 |
|
|
|
| 4 |
F |
-0.678 |
|
|
|
| 5 |
H |
-0.352 |
|
|
|
| 6 |
H |
-0.352 |
|
|
|
| 7 |
H |
-0.352 |
|
|
|
| 8 |
H |
-0.352 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.529 |
3.306 |
0.000 |
| y |
3.306 |
-30.075 |
0.000 |
| z |
0.000 |
0.000 |
-21.861 |
|
| Traceless |
| | x | y | z |
| x |
3.438 |
3.306 |
0.000 |
| y |
3.306 |
-7.880 |
0.000 |
| z |
0.000 |
0.000 |
4.441 |
|
| Polar |
| 3z2-r2 | 8.883 |
| x2-y2 | 7.545 |
| xy | 3.306 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.470 |
-0.091 |
0.000 |
| y |
-0.091 |
4.743 |
0.000 |
| z |
0.000 |
0.000 |
4.091 |
<r2> (average value of r
2) Å
2
| <r2> |
89.587 |
| (<r2>)1/2 |
9.465 |
Jump to
S1C1
Energy calculated at B2PLYP/daug-cc-pVDZ
| | hartrees |
| Energy at 0K | -278.106717 |
| Energy at 298.15K | |
| HF Energy | -277.878029 |
| Nuclear repulsion energy | 126.787249 |
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 B2PLYP/daug-cc-pVDZ
| 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 |
3139 |
3139 |
9.97 |
87.41 |
0.72 |
0.84 |
| 2 |
A |
3081 |
3081 |
39.47 |
232.98 |
0.01 |
0.02 |
| 3 |
A |
1475 |
1475 |
1.88 |
1.26 |
0.75 |
0.85 |
| 4 |
A |
1425 |
1425 |
9.52 |
1.34 |
0.23 |
0.37 |
| 5 |
A |
1293 |
1293 |
2.69 |
8.46 |
0.65 |
0.79 |
| 6 |
A |
1128 |
1128 |
7.11 |
1.60 |
0.31 |
0.47 |
| 7 |
A |
1101 |
1101 |
79.22 |
3.90 |
0.38 |
0.56 |
| 8 |
A |
867 |
867 |
30.94 |
7.18 |
0.12 |
0.22 |
| 9 |
A |
320 |
320 |
0.46 |
0.45 |
0.29 |
0.45 |
| 10 |
A |
148 |
148 |
3.81 |
0.15 |
0.75 |
0.86 |
| 11 |
B |
3151 |
3151 |
28.51 |
12.12 |
0.75 |
0.86 |
| 12 |
B |
3072 |
3072 |
7.88 |
32.87 |
0.75 |
0.86 |
| 13 |
B |
1472 |
1472 |
8.61 |
6.68 |
0.75 |
0.86 |
| 14 |
B |
1381 |
1381 |
6.79 |
0.01 |
0.75 |
0.86 |
| 15 |
B |
1247 |
1247 |
5.92 |
2.10 |
0.75 |
0.86 |
| 16 |
B |
1064 |
1064 |
52.59 |
3.72 |
0.75 |
0.86 |
| 17 |
B |
890 |
890 |
49.60 |
2.88 |
0.75 |
0.86 |
| 18 |
B |
492 |
492 |
16.98 |
0.50 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13371.6 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 13371.6 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 B2PLYP/daug-cc-pVDZ
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.270 |
0.703 |
0.516 |
| C2 |
-0.270 |
-0.703 |
0.516 |
| F3 |
-0.270 |
1.436 |
-0.550 |
| F4 |
0.270 |
-1.436 |
-0.550 |
| H5 |
-0.017 |
1.210 |
1.449 |
| H6 |
1.361 |
0.707 |
0.404 |
| H7 |
0.017 |
-1.210 |
1.449 |
| H8 |
-1.361 |
-0.707 |
0.404 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5052 | 1.4026 | 2.3900 | 1.0993 | 1.0972 | 2.1425 | 2.1586 |
C2 | 1.5052 | | 2.3900 | 1.4026 | 2.1425 | 2.1586 | 1.0993 | 1.0972 | F3 | 1.4026 | 2.3900 | | 2.9227 | 2.0275 | 2.0256 | 3.3285 | 2.5874 | F4 | 2.3900 | 1.4026 | 2.9227 | | 3.3285 | 2.5874 | 2.0275 | 2.0256 | H5 | 1.0993 | 2.1425 | 2.0275 | 3.3285 | | 1.8007 | 2.4200 | 2.5637 | H6 | 1.0972 | 2.1586 | 2.0256 | 2.5874 | 1.8007 | | 2.5637 | 3.0677 | H7 | 2.1425 | 1.0993 | 3.3285 | 2.0275 | 2.4200 | 2.5637 | | 1.8007 | H8 | 2.1586 | 1.0972 | 2.5874 | 2.0256 | 2.5637 | 3.0677 | 1.8007 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
110.508 |
|
C1 |
C2 |
H7 |
109.718 |
| C1 |
C2 |
H8 |
111.120 |
|
C2 |
C1 |
F3 |
110.508 |
| C2 |
C1 |
H5 |
109.718 |
|
C2 |
C1 |
H6 |
111.120 |
| F3 |
C1 |
H5 |
107.650 |
|
F3 |
C1 |
H6 |
107.627 |
| F4 |
C2 |
H7 |
107.650 |
|
F4 |
C2 |
H8 |
107.627 |
| H5 |
C1 |
H6 |
110.136 |
|
H7 |
C2 |
H8 |
110.136 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/daug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
1.441 |
|
|
|
| 2 |
C |
1.441 |
|
|
|
| 3 |
F |
-0.576 |
|
|
|
| 4 |
F |
-0.576 |
|
|
|
| 5 |
H |
-0.463 |
|
|
|
| 6 |
H |
-0.402 |
|
|
|
| 7 |
H |
-0.463 |
|
|
|
| 8 |
H |
-0.402 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
2.855 |
2.855 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.097 |
1.792 |
0.000 |
| y |
1.792 |
-26.859 |
0.000 |
| z |
0.000 |
0.000 |
-22.789 |
|
| Traceless |
| | x | y | z |
| x |
2.727 |
1.792 |
0.000 |
| y |
1.792 |
-4.416 |
0.000 |
| z |
0.000 |
0.000 |
1.689 |
|
| Polar |
| 3z2-r2 | 3.377 |
| x2-y2 | 4.762 |
| xy | 1.792 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.252 |
0.025 |
0.000 |
| y |
0.025 |
4.666 |
0.000 |
| z |
0.000 |
0.000 |
4.469 |
<r2> (average value of r
2) Å
2
| <r2> |
80.982 |
| (<r2>)1/2 |
8.999 |