Jump to
S1C2
Energy calculated at TPSSh/3-21G*
| | hartrees |
| Energy at 0K | -276.766451 |
| Energy at 298.15K | |
| HF Energy | -276.766451 |
| Nuclear repulsion energy | 123.686187 |
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 TPSSh/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 |
Ag |
3060 |
2955 |
0.00 |
191.62 |
0.10 |
0.18 |
| 2 |
Ag |
1583 |
1528 |
0.00 |
30.27 |
0.72 |
0.84 |
| 3 |
Ag |
1466 |
1416 |
0.00 |
5.46 |
0.74 |
0.85 |
| 4 |
Ag |
1048 |
1012 |
0.00 |
9.70 |
0.74 |
0.85 |
| 5 |
Ag |
1045 |
1009 |
0.00 |
7.28 |
0.20 |
0.33 |
| 6 |
Ag |
427 |
412 |
0.00 |
3.44 |
0.54 |
0.70 |
| 7 |
Au |
3125 |
3018 |
82.83 |
0.00 |
0.00 |
0.00 |
| 8 |
Au |
1224 |
1182 |
0.31 |
0.00 |
0.00 |
0.00 |
| 9 |
Au |
850 |
821 |
0.06 |
0.00 |
0.00 |
0.00 |
| 10 |
Au |
118 |
114 |
13.16 |
0.00 |
0.00 |
0.00 |
| 11 |
Bg |
3094 |
2988 |
0.00 |
129.90 |
0.75 |
0.86 |
| 12 |
Bg |
1345 |
1299 |
0.00 |
19.48 |
0.75 |
0.86 |
| 13 |
Bg |
1172 |
1132 |
0.00 |
12.67 |
0.75 |
0.86 |
| 14 |
Bu |
3068 |
2963 |
62.73 |
0.00 |
0.00 |
0.00 |
| 15 |
Bu |
1598 |
1543 |
1.02 |
0.00 |
0.00 |
0.00 |
| 16 |
Bu |
1389 |
1342 |
9.80 |
0.00 |
0.00 |
0.00 |
| 17 |
Bu |
1078 |
1041 |
99.37 |
0.00 |
0.00 |
0.00 |
| 18 |
Bu |
218 |
211 |
19.40 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 13452.9 cm
-1
Scaled (by 0.9657) Zero Point Vibrational Energy (zpe) 12991.5 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 TPSSh/3-21G*
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.437 |
0.626 |
0.000 |
| C2 |
-0.437 |
-0.626 |
0.000 |
| F3 |
-0.437 |
1.754 |
0.000 |
| F4 |
0.437 |
-1.754 |
0.000 |
| H5 |
1.071 |
0.637 |
0.892 |
| H6 |
1.071 |
0.637 |
-0.892 |
| H7 |
-1.071 |
-0.637 |
0.892 |
| H8 |
-1.071 |
-0.637 |
-0.892 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5266 | 1.4264 | 2.3795 | 1.0945 | 1.0945 | 2.1600 | 2.1600 |
C2 | 1.5266 | | 2.3795 | 1.4264 | 2.1600 | 2.1600 | 1.0945 | 1.0945 | F3 | 1.4264 | 2.3795 | | 3.6142 | 2.0772 | 2.0772 | 2.6296 | 2.6296 | F4 | 2.3795 | 1.4264 | 3.6142 | | 2.6296 | 2.6296 | 2.0772 | 2.0772 | H5 | 1.0945 | 2.1600 | 2.0772 | 2.6296 | | 1.7839 | 2.4928 | 3.0654 | H6 | 1.0945 | 2.1600 | 2.0772 | 2.6296 | 1.7839 | | 3.0654 | 2.4928 | H7 | 2.1600 | 1.0945 | 2.6296 | 2.0772 | 2.4928 | 3.0654 | | 1.7839 | H8 | 2.1600 | 1.0945 | 2.6296 | 2.0772 | 3.0654 | 2.4928 | 1.7839 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
107.326 |
|
C1 |
C2 |
H7 |
109.891 |
| C1 |
C2 |
H8 |
109.891 |
|
C2 |
C1 |
F3 |
107.326 |
| C2 |
C1 |
H5 |
109.891 |
|
C2 |
C1 |
H6 |
109.891 |
| F3 |
C1 |
H5 |
110.281 |
|
F3 |
C1 |
H6 |
110.281 |
| F4 |
C2 |
H7 |
110.281 |
|
F4 |
C2 |
H8 |
110.281 |
| H5 |
C1 |
H6 |
109.155 |
|
H7 |
C2 |
H8 |
109.155 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at TPSSh/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.138 |
|
|
|
| 2 |
C |
-0.138 |
|
|
|
| 3 |
F |
-0.296 |
|
|
|
| 4 |
F |
-0.296 |
|
|
|
| 5 |
H |
0.217 |
|
|
|
| 6 |
H |
0.217 |
|
|
|
| 7 |
H |
0.217 |
|
|
|
| 8 |
H |
0.217 |
|
|
|
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
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.240 |
-0.090 |
0.000 |
| y |
-0.090 |
3.206 |
0.000 |
| z |
0.000 |
0.000 |
3.020 |
<r2> (average value of r
2) Å
2
| <r2> |
90.084 |
| (<r2>)1/2 |
9.491 |
Jump to
S1C1
Energy calculated at TPSSh/3-21G*
| | hartrees |
| Energy at 0K | -276.766430 |
| Energy at 298.15K | |
| HF Energy | -276.766430 |
| Nuclear repulsion energy | 125.567367 |
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 TPSSh/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 |
3087 |
2982 |
26.49 |
108.36 |
0.73 |
0.84 |
| 2 |
A |
3051 |
2947 |
36.91 |
162.92 |
0.03 |
0.05 |
| 3 |
A |
1563 |
1509 |
0.07 |
3.46 |
0.64 |
0.78 |
| 4 |
A |
1452 |
1402 |
11.48 |
7.97 |
0.74 |
0.85 |
| 5 |
A |
1327 |
1281 |
0.01 |
27.47 |
0.73 |
0.85 |
| 6 |
A |
1129 |
1090 |
3.10 |
3.45 |
0.45 |
0.62 |
| 7 |
A |
1094 |
1056 |
42.67 |
4.16 |
0.75 |
0.86 |
| 8 |
A |
864 |
834 |
13.30 |
7.26 |
0.24 |
0.38 |
| 9 |
A |
300 |
290 |
0.69 |
0.33 |
0.42 |
0.59 |
| 10 |
A |
141 |
137 |
3.68 |
0.12 |
0.72 |
0.84 |
| 11 |
B |
3104 |
2998 |
58.20 |
10.46 |
0.75 |
0.86 |
| 12 |
B |
3036 |
2932 |
19.71 |
46.03 |
0.75 |
0.86 |
| 13 |
B |
1563 |
1510 |
4.47 |
22.66 |
0.75 |
0.86 |
| 14 |
B |
1462 |
1412 |
9.00 |
2.25 |
0.75 |
0.86 |
| 15 |
B |
1265 |
1221 |
0.89 |
8.25 |
0.75 |
0.86 |
| 16 |
B |
1081 |
1044 |
20.48 |
3.09 |
0.75 |
0.86 |
| 17 |
B |
926 |
894 |
25.05 |
4.90 |
0.75 |
0.86 |
| 18 |
B |
445 |
429 |
14.83 |
0.77 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13443.8 cm
-1
Scaled (by 0.9657) Zero Point Vibrational Energy (zpe) 12982.7 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 TPSSh/3-21G*
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.282 |
0.704 |
0.519 |
| C2 |
-0.282 |
-0.704 |
0.519 |
| F3 |
-0.282 |
1.452 |
-0.555 |
| F4 |
0.282 |
-1.452 |
-0.555 |
| H5 |
0.039 |
1.191 |
1.472 |
| H6 |
1.370 |
0.656 |
0.403 |
| H7 |
-0.039 |
-1.191 |
1.472 |
| H8 |
-1.370 |
-0.656 |
0.403 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5178 | 1.4250 | 2.4089 | 1.0971 | 1.0953 | 2.1457 | 2.1436 |
C2 | 1.5178 | | 2.4089 | 1.4250 | 2.1457 | 2.1436 | 1.0971 | 1.0953 | F3 | 1.4250 | 2.4089 | | 2.9581 | 2.0681 | 2.0689 | 3.3395 | 2.5578 | F4 | 2.4089 | 1.4250 | 2.9581 | | 3.3395 | 2.5578 | 2.0681 | 2.0689 | H5 | 1.0971 | 2.1457 | 2.0681 | 3.3395 | | 1.7898 | 2.3839 | 2.5574 | H6 | 1.0953 | 2.1436 | 2.0689 | 2.5578 | 1.7898 | | 2.5574 | 3.0383 | H7 | 2.1457 | 1.0971 | 3.3395 | 2.0681 | 2.3839 | 2.5574 | | 1.7898 | H8 | 2.1436 | 1.0953 | 2.5578 | 2.0689 | 2.5574 | 3.0383 | 1.7898 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
109.848 |
|
C1 |
C2 |
H7 |
109.228 |
| C1 |
C2 |
H8 |
109.167 |
|
C2 |
C1 |
F3 |
109.848 |
| C2 |
C1 |
H5 |
109.228 |
|
C2 |
C1 |
H6 |
109.167 |
| F3 |
C1 |
H5 |
109.477 |
|
F3 |
C1 |
H6 |
109.658 |
| F4 |
C2 |
H7 |
109.477 |
|
F4 |
C2 |
H8 |
109.658 |
| H5 |
C1 |
H6 |
109.448 |
|
H7 |
C2 |
H8 |
109.448 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at TPSSh/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.127 |
|
|
|
| 2 |
C |
-0.127 |
|
|
|
| 3 |
F |
-0.293 |
|
|
|
| 4 |
F |
-0.293 |
|
|
|
| 5 |
H |
0.198 |
|
|
|
| 6 |
H |
0.222 |
|
|
|
| 7 |
H |
0.198 |
|
|
|
| 8 |
H |
0.222 |
|
|
|
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 |
2.640 |
2.640 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.108 |
-0.015 |
0.000 |
| y |
-0.015 |
3.245 |
0.000 |
| z |
0.000 |
0.000 |
3.259 |
<r2> (average value of r
2) Å
2
| <r2> |
81.582 |
| (<r2>)1/2 |
9.032 |