Jump to
S1C2
Energy calculated at wB97X-D/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -278.313448 |
| Energy at 298.15K | |
| HF Energy | -278.313448 |
| Nuclear repulsion energy | 125.992838 |
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 wB97X-D/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 |
Ag |
3061 |
3061 |
0.00 |
228.07 |
0.06 |
0.11 |
| 2 |
Ag |
1524 |
1524 |
0.00 |
7.35 |
0.75 |
0.86 |
| 3 |
Ag |
1456 |
1456 |
0.00 |
1.93 |
0.36 |
0.53 |
| 4 |
Ag |
1094 |
1094 |
0.00 |
6.81 |
0.59 |
0.74 |
| 5 |
Ag |
1081 |
1081 |
0.00 |
8.76 |
0.27 |
0.42 |
| 6 |
Ag |
464 |
464 |
0.00 |
2.44 |
0.36 |
0.53 |
| 7 |
Au |
3135 |
3135 |
41.43 |
0.00 |
0.00 |
0.00 |
| 8 |
Au |
1246 |
1246 |
4.68 |
0.00 |
0.00 |
0.00 |
| 9 |
Au |
820 |
820 |
0.05 |
0.00 |
0.00 |
0.00 |
| 10 |
Au |
116 |
116 |
13.12 |
0.00 |
0.00 |
0.00 |
| 11 |
Bg |
3109 |
3109 |
0.00 |
104.93 |
0.75 |
0.86 |
| 12 |
Bg |
1307 |
1307 |
0.00 |
7.15 |
0.75 |
0.86 |
| 13 |
Bg |
1182 |
1182 |
0.00 |
1.29 |
0.75 |
0.86 |
| 14 |
Bu |
3066 |
3066 |
56.37 |
0.00 |
0.00 |
0.00 |
| 15 |
Bu |
1530 |
1530 |
5.57 |
0.00 |
0.00 |
0.00 |
| 16 |
Bu |
1367 |
1367 |
5.77 |
0.00 |
0.00 |
0.00 |
| 17 |
Bu |
1090 |
1090 |
225.05 |
0.00 |
0.00 |
0.00 |
| 18 |
Bu |
286 |
286 |
19.58 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 13466.2 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 13466.2 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 wB97X-D/6-311+G(3df,2p)
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.423 |
0.629 |
0.000 |
| C2 |
-0.423 |
-0.629 |
0.000 |
| F3 |
-0.423 |
1.720 |
0.000 |
| F4 |
0.423 |
-1.720 |
0.000 |
| H5 |
1.051 |
0.676 |
0.891 |
| H6 |
1.051 |
0.676 |
-0.891 |
| H7 |
-1.051 |
-0.676 |
0.891 |
| H8 |
-1.051 |
-0.676 |
-0.891 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5155 | 1.3803 | 2.3487 | 1.0909 | 1.0909 | 2.1601 | 2.1601 |
C2 | 1.5155 | | 2.3487 | 1.3803 | 2.1601 | 2.1601 | 1.0909 | 1.0909 | F3 | 1.3803 | 2.3487 | | 3.5420 | 2.0137 | 2.0137 | 2.6317 | 2.6317 | F4 | 2.3487 | 1.3803 | 3.5420 | | 2.6317 | 2.6317 | 2.0137 | 2.0137 | H5 | 1.0909 | 2.1601 | 2.0137 | 2.6317 | | 1.7819 | 2.4981 | 3.0685 | H6 | 1.0909 | 2.1601 | 2.0137 | 2.6317 | 1.7819 | | 3.0685 | 2.4981 | H7 | 2.1601 | 1.0909 | 2.6317 | 2.0137 | 2.4981 | 3.0685 | | 1.7819 | H8 | 2.1601 | 1.0909 | 2.6317 | 2.0137 | 3.0685 | 2.4981 | 1.7819 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
108.308 |
|
C1 |
C2 |
H7 |
110.894 |
| C1 |
C2 |
H8 |
110.894 |
|
C2 |
C1 |
F3 |
108.308 |
| C2 |
C1 |
H5 |
110.894 |
|
C2 |
C1 |
H6 |
110.894 |
| F3 |
C1 |
H5 |
108.582 |
|
F3 |
C1 |
H6 |
108.582 |
| F4 |
C2 |
H7 |
108.582 |
|
F4 |
C2 |
H8 |
108.582 |
| H5 |
C1 |
H6 |
109.512 |
|
H7 |
C2 |
H8 |
109.512 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.106 |
|
|
|
| 2 |
C |
0.106 |
|
|
|
| 3 |
F |
-0.412 |
|
|
|
| 4 |
F |
-0.412 |
|
|
|
| 5 |
H |
0.153 |
|
|
|
| 6 |
H |
0.153 |
|
|
|
| 7 |
H |
0.153 |
|
|
|
| 8 |
H |
0.153 |
|
|
|
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 |
-22.142 |
3.242 |
0.000 |
| y |
3.242 |
-29.337 |
0.000 |
| z |
0.000 |
0.000 |
-21.486 |
|
| Traceless |
| | x | y | z |
| x |
3.270 |
3.242 |
0.000 |
| y |
3.242 |
-7.523 |
0.000 |
| z |
0.000 |
0.000 |
4.253 |
|
| Polar |
| 3z2-r2 | 8.506 |
| x2-y2 | 7.195 |
| xy | 3.242 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.258 |
-0.071 |
0.000 |
| y |
-0.071 |
4.490 |
0.000 |
| z |
0.000 |
0.000 |
3.915 |
<r2> (average value of r
2) Å
2
| <r2> |
87.954 |
| (<r2>)1/2 |
9.378 |
Jump to
S1C1
Energy calculated at wB97X-D/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -278.315052 |
| Energy at 298.15K | |
| HF Energy | -278.315052 |
| Nuclear repulsion energy | 128.011971 |
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 wB97X-D/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 |
3105 |
3105 |
12.67 |
82.63 |
0.74 |
0.85 |
| 2 |
A |
3056 |
3056 |
37.21 |
213.25 |
0.02 |
0.03 |
| 3 |
A |
1495 |
1495 |
1.02 |
1.35 |
0.74 |
0.85 |
| 4 |
A |
1445 |
1445 |
10.92 |
1.39 |
0.19 |
0.31 |
| 5 |
A |
1315 |
1315 |
3.87 |
8.37 |
0.66 |
0.80 |
| 6 |
A |
1137 |
1137 |
33.06 |
2.14 |
0.10 |
0.18 |
| 7 |
A |
1128 |
1128 |
66.33 |
2.59 |
0.75 |
0.86 |
| 8 |
A |
881 |
881 |
22.27 |
5.67 |
0.16 |
0.27 |
| 9 |
A |
329 |
329 |
0.43 |
0.40 |
0.29 |
0.45 |
| 10 |
A |
153 |
153 |
3.83 |
0.13 |
0.75 |
0.86 |
| 11 |
B |
3117 |
3117 |
31.60 |
11.85 |
0.75 |
0.86 |
| 12 |
B |
3046 |
3046 |
8.82 |
31.48 |
0.75 |
0.86 |
| 13 |
B |
1495 |
1495 |
10.61 |
6.41 |
0.75 |
0.86 |
| 14 |
B |
1405 |
1405 |
5.90 |
0.01 |
0.75 |
0.86 |
| 15 |
B |
1273 |
1273 |
7.13 |
2.24 |
0.75 |
0.86 |
| 16 |
B |
1103 |
1103 |
60.69 |
3.67 |
0.75 |
0.86 |
| 17 |
B |
914 |
914 |
43.80 |
2.43 |
0.75 |
0.86 |
| 18 |
B |
506 |
506 |
16.90 |
0.46 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13451.1 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 13451.1 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 wB97X-D/6-311+G(3df,2p)
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.265 |
0.703 |
0.505 |
| C2 |
-0.265 |
-0.703 |
0.505 |
| F3 |
-0.265 |
1.428 |
-0.541 |
| F4 |
0.265 |
-1.428 |
-0.541 |
| H5 |
-0.015 |
1.197 |
1.439 |
| H6 |
1.352 |
0.705 |
0.402 |
| H7 |
0.015 |
-1.197 |
1.439 |
| H8 |
-1.352 |
-0.705 |
0.402 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5024 | 1.3787 | 2.3736 | 1.0932 | 1.0915 | 2.1320 | 2.1462 |
C2 | 1.5024 | | 2.3736 | 1.3787 | 2.1320 | 2.1462 | 1.0932 | 1.0915 | F3 | 1.3787 | 2.3736 | | 2.9047 | 2.0088 | 2.0066 | 3.3000 | 2.5724 | F4 | 2.3736 | 1.3787 | 2.9047 | | 3.3000 | 2.5724 | 2.0088 | 2.0066 | H5 | 1.0932 | 2.1320 | 2.0088 | 3.3000 | | 1.7849 | 2.3948 | 2.5457 | H6 | 1.0915 | 2.1462 | 2.0066 | 2.5724 | 1.7849 | | 2.5457 | 3.0489 | H7 | 2.1320 | 1.0932 | 3.3000 | 2.0088 | 2.3948 | 2.5457 | | 1.7849 | H8 | 2.1462 | 1.0915 | 2.5724 | 2.0066 | 2.5457 | 3.0489 | 1.7849 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
110.873 |
|
C1 |
C2 |
H7 |
109.441 |
| C1 |
C2 |
H8 |
110.668 |
|
C2 |
C1 |
F3 |
110.873 |
| C2 |
C1 |
H5 |
109.441 |
|
C2 |
C1 |
H6 |
110.668 |
| F3 |
C1 |
H5 |
108.157 |
|
F3 |
C1 |
H6 |
108.078 |
| F4 |
C2 |
H7 |
108.157 |
|
F4 |
C2 |
H8 |
108.078 |
| H5 |
C1 |
H6 |
109.572 |
|
H7 |
C2 |
H8 |
109.572 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.110 |
|
|
|
| 2 |
C |
0.110 |
|
|
|
| 3 |
F |
-0.415 |
|
|
|
| 4 |
F |
-0.415 |
|
|
|
| 5 |
H |
0.150 |
|
|
|
| 6 |
H |
0.155 |
|
|
|
| 7 |
H |
0.150 |
|
|
|
| 8 |
H |
0.155 |
|
|
|
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 |
2.741 |
2.741 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-21.710 |
1.763 |
0.000 |
| y |
1.763 |
-26.249 |
0.000 |
| z |
0.000 |
0.000 |
-22.456 |
|
| Traceless |
| | x | y | z |
| x |
2.643 |
1.763 |
0.000 |
| y |
1.763 |
-4.166 |
0.000 |
| z |
0.000 |
0.000 |
1.524 |
|
| Polar |
| 3z2-r2 | 3.047 |
| x2-y2 | 4.539 |
| xy | 1.763 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.061 |
0.027 |
0.000 |
| y |
0.027 |
4.437 |
0.000 |
| z |
0.000 |
0.000 |
4.244 |
<r2> (average value of r
2) Å
2
| <r2> |
79.704 |
| (<r2>)1/2 |
8.928 |