Jump to
S1C2
Energy calculated at TPSSh/6-311G*
| | hartrees |
| Energy at 0K | -278.360502 |
| Energy at 298.15K | |
| HF Energy | -278.360502 |
| Nuclear repulsion energy | 125.194082 |
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/6-311G*
| 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 |
2948 |
0.00 |
220.06 |
0.09 |
0.16 |
| 2 |
Ag |
1540 |
1483 |
0.00 |
17.57 |
0.74 |
0.85 |
| 3 |
Ag |
1470 |
1416 |
0.00 |
4.33 |
0.50 |
0.67 |
| 4 |
Ag |
1085 |
1045 |
0.00 |
6.73 |
0.40 |
0.57 |
| 5 |
Ag |
1048 |
1009 |
0.00 |
8.65 |
0.64 |
0.78 |
| 6 |
Ag |
451 |
434 |
0.00 |
3.32 |
0.52 |
0.68 |
| 7 |
Au |
3133 |
3018 |
80.62 |
0.00 |
0.00 |
0.00 |
| 8 |
Au |
1243 |
1197 |
3.52 |
0.00 |
0.00 |
0.00 |
| 9 |
Au |
817 |
787 |
0.11 |
0.00 |
0.00 |
0.00 |
| 10 |
Au |
125 |
121 |
13.51 |
0.00 |
0.00 |
0.00 |
| 11 |
Bg |
3105 |
2991 |
0.00 |
138.00 |
0.75 |
0.86 |
| 12 |
Bg |
1314 |
1265 |
0.00 |
15.02 |
0.75 |
0.86 |
| 13 |
Bg |
1186 |
1142 |
0.00 |
5.39 |
0.75 |
0.86 |
| 14 |
Bu |
3065 |
2952 |
77.47 |
0.00 |
0.00 |
0.00 |
| 15 |
Bu |
1550 |
1493 |
1.40 |
0.00 |
0.00 |
0.00 |
| 16 |
Bu |
1376 |
1325 |
14.00 |
0.00 |
0.00 |
0.00 |
| 17 |
Bu |
1060 |
1021 |
210.41 |
0.00 |
0.00 |
0.00 |
| 18 |
Bu |
266 |
257 |
19.96 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 13446.9 cm
-1
Scaled (by 0.9632) Zero Point Vibrational Energy (zpe) 12952.0 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/6-311G*
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.427 |
0.627 |
0.000 |
| C2 |
-0.427 |
-0.627 |
0.000 |
| F3 |
-0.427 |
1.731 |
0.000 |
| F4 |
0.427 |
-1.731 |
0.000 |
| H5 |
1.053 |
0.675 |
0.894 |
| H6 |
1.053 |
0.675 |
-0.894 |
| H7 |
-1.053 |
-0.675 |
0.894 |
| H8 |
-1.053 |
-0.675 |
-0.894 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5180 | 1.3961 | 2.3587 | 1.0925 | 1.0925 | 2.1652 | 2.1652 |
C2 | 1.5180 | | 2.3587 | 1.3961 | 2.1652 | 2.1652 | 1.0925 | 1.0925 | F3 | 1.3961 | 2.3587 | | 3.5667 | 2.0262 | 2.0262 | 2.6428 | 2.6428 | F4 | 2.3587 | 1.3961 | 3.5667 | | 2.6428 | 2.6428 | 2.0262 | 2.0262 | H5 | 1.0925 | 2.1652 | 2.0262 | 2.6428 | | 1.7886 | 2.5020 | 3.0755 | H6 | 1.0925 | 2.1652 | 2.0262 | 2.6428 | 1.7886 | | 3.0755 | 2.5020 | H7 | 2.1652 | 1.0925 | 2.6428 | 2.0262 | 2.5020 | 3.0755 | | 1.7886 | H8 | 2.1652 | 1.0925 | 2.6428 | 2.0262 | 3.0755 | 2.5020 | 1.7886 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
108.010 |
|
C1 |
C2 |
H7 |
111.027 |
| C1 |
C2 |
H8 |
111.027 |
|
C2 |
C1 |
F3 |
108.010 |
| C2 |
C1 |
H5 |
111.027 |
|
C2 |
C1 |
H6 |
111.027 |
| F3 |
C1 |
H5 |
108.401 |
|
F3 |
C1 |
H6 |
108.401 |
| F4 |
C2 |
H7 |
108.401 |
|
F4 |
C2 |
H8 |
108.401 |
| H5 |
C1 |
H6 |
109.880 |
|
H7 |
C2 |
H8 |
109.880 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at TPSSh/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.119 |
|
|
|
| 2 |
C |
-0.119 |
|
|
|
| 3 |
F |
-0.279 |
|
|
|
| 4 |
F |
-0.279 |
|
|
|
| 5 |
H |
0.199 |
|
|
|
| 6 |
H |
0.199 |
|
|
|
| 7 |
H |
0.199 |
|
|
|
| 8 |
H |
0.199 |
|
|
|
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 |
3.649 |
0.030 |
0.000 |
| y |
0.030 |
3.657 |
0.000 |
| z |
0.000 |
0.000 |
3.378 |
<r2> (average value of r
2) Å
2
| <r2> |
88.674 |
| (<r2>)1/2 |
9.417 |
Jump to
S1C1
Energy calculated at TPSSh/6-311G*
| | hartrees |
| Energy at 0K | -278.360961 |
| Energy at 298.15K | |
| HF Energy | -278.360961 |
| Nuclear repulsion energy | 127.290085 |
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/6-311G*
| 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 |
3097 |
2983 |
22.35 |
113.03 |
0.72 |
0.83 |
| 2 |
A |
3051 |
2938 |
49.31 |
187.82 |
0.02 |
0.04 |
| 3 |
A |
1517 |
1461 |
0.01 |
1.84 |
0.73 |
0.85 |
| 4 |
A |
1453 |
1400 |
15.51 |
4.75 |
0.49 |
0.65 |
| 5 |
A |
1311 |
1263 |
1.67 |
18.97 |
0.72 |
0.84 |
| 6 |
A |
1138 |
1096 |
0.61 |
0.90 |
0.14 |
0.25 |
| 7 |
A |
1101 |
1061 |
88.15 |
3.96 |
0.75 |
0.85 |
| 8 |
A |
869 |
837 |
28.60 |
5.28 |
0.27 |
0.43 |
| 9 |
A |
318 |
306 |
0.33 |
0.47 |
0.43 |
0.61 |
| 10 |
A |
147 |
141 |
3.69 |
0.07 |
0.74 |
0.85 |
| 11 |
B |
3111 |
2997 |
61.49 |
12.83 |
0.75 |
0.86 |
| 12 |
B |
3037 |
2925 |
18.21 |
45.85 |
0.75 |
0.86 |
| 13 |
B |
1514 |
1458 |
6.35 |
13.55 |
0.75 |
0.86 |
| 14 |
B |
1423 |
1371 |
12.77 |
1.09 |
0.75 |
0.86 |
| 15 |
B |
1267 |
1221 |
4.55 |
5.46 |
0.75 |
0.86 |
| 16 |
B |
1081 |
1041 |
45.61 |
3.25 |
0.75 |
0.86 |
| 17 |
B |
903 |
870 |
49.67 |
3.92 |
0.75 |
0.86 |
| 18 |
B |
485 |
467 |
16.18 |
0.73 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13411.0 cm
-1
Scaled (by 0.9632) Zero Point Vibrational Energy (zpe) 12917.5 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/6-311G*
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.269 |
0.704 |
0.513 |
| C2 |
-0.269 |
-0.704 |
0.513 |
| F3 |
-0.269 |
1.431 |
-0.547 |
| F4 |
0.269 |
-1.431 |
-0.547 |
| H5 |
-0.009 |
1.210 |
1.443 |
| H6 |
1.356 |
0.701 |
0.401 |
| H7 |
0.009 |
-1.210 |
1.443 |
| H8 |
-1.356 |
-0.701 |
0.401 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5067 | 1.3932 | 2.3831 | 1.0955 | 1.0932 | 2.1440 | 2.1509 |
C2 | 1.5067 | | 2.3831 | 1.3932 | 2.1440 | 2.1509 | 1.0955 | 1.0932 | F3 | 1.3932 | 2.3831 | | 2.9120 | 2.0193 | 2.0185 | 3.3188 | 2.5739 | F4 | 2.3831 | 1.3932 | 2.9120 | | 3.3188 | 2.5739 | 2.0193 | 2.0185 | H5 | 1.0955 | 2.1440 | 2.0193 | 3.3188 | | 1.7917 | 2.4205 | 2.5599 | H6 | 1.0932 | 2.1509 | 2.0185 | 2.5739 | 1.7917 | | 2.5599 | 3.0534 | H7 | 2.1440 | 1.0955 | 3.3188 | 2.0193 | 2.4205 | 2.5599 | | 1.7917 | H8 | 2.1509 | 1.0932 | 2.5739 | 2.0185 | 2.5599 | 3.0534 | 1.7917 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
110.473 |
|
C1 |
C2 |
H7 |
109.957 |
| C1 |
C2 |
H8 |
110.642 |
|
C2 |
C1 |
F3 |
110.473 |
| C2 |
C1 |
H5 |
109.957 |
|
C2 |
C1 |
H6 |
110.642 |
| F3 |
C1 |
H5 |
107.867 |
|
F3 |
C1 |
H6 |
107.943 |
| F4 |
C2 |
H7 |
107.867 |
|
F4 |
C2 |
H8 |
107.943 |
| H5 |
C1 |
H6 |
109.895 |
|
H7 |
C2 |
H8 |
109.895 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at TPSSh/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.113 |
|
|
|
| 2 |
C |
-0.113 |
|
|
|
| 3 |
F |
-0.274 |
|
|
|
| 4 |
F |
-0.274 |
|
|
|
| 5 |
H |
0.185 |
|
|
|
| 6 |
H |
0.202 |
|
|
|
| 7 |
H |
0.185 |
|
|
|
| 8 |
H |
0.202 |
|
|
|
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 |
2.691 |
2.691 |
| 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 |
3.509 |
0.066 |
0.000 |
| y |
0.066 |
3.718 |
0.000 |
| z |
0.000 |
0.000 |
3.579 |
<r2> (average value of r
2) Å
2
| <r2> |
80.106 |
| (<r2>)1/2 |
8.950 |