Jump to
S1C2
Energy calculated at B1B95/daug-cc-pVTZ
| | hartrees |
| Energy at 0K | -278.310615 |
| Energy at 298.15K | |
| HF Energy | -278.310615 |
| Nuclear repulsion energy | 126.212912 |
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 B1B95/daug-cc-pVTZ
| 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 |
3074 |
3074 |
0.00 |
254.36 |
0.05 |
0.10 |
| 2 |
Ag |
1514 |
1514 |
0.00 |
7.61 |
0.72 |
0.84 |
| 3 |
Ag |
1446 |
1446 |
0.00 |
1.91 |
0.43 |
0.60 |
| 4 |
Ag |
1100 |
1100 |
0.00 |
6.85 |
0.60 |
0.75 |
| 5 |
Ag |
1085 |
1085 |
0.00 |
8.54 |
0.26 |
0.41 |
| 6 |
Ag |
460 |
460 |
0.00 |
2.48 |
0.35 |
0.52 |
| 7 |
Au |
3146 |
3146 |
40.38 |
0.00 |
0.00 |
0.00 |
| 8 |
Au |
1236 |
1236 |
4.61 |
0.00 |
0.00 |
0.00 |
| 9 |
Au |
811 |
811 |
0.04 |
0.00 |
0.00 |
0.00 |
| 10 |
Au |
112 |
112 |
12.68 |
0.00 |
0.00 |
0.00 |
| 11 |
Bg |
3119 |
3119 |
0.00 |
109.14 |
0.75 |
0.86 |
| 12 |
Bg |
1303 |
1303 |
0.00 |
6.90 |
0.75 |
0.86 |
| 13 |
Bg |
1174 |
1174 |
0.00 |
1.15 |
0.75 |
0.86 |
| 14 |
Bu |
3080 |
3080 |
56.00 |
0.00 |
0.00 |
0.00 |
| 15 |
Bu |
1523 |
1523 |
4.70 |
0.00 |
0.00 |
0.00 |
| 16 |
Bu |
1357 |
1357 |
6.64 |
0.00 |
0.00 |
0.00 |
| 17 |
Bu |
1098 |
1098 |
221.33 |
0.00 |
0.00 |
0.00 |
| 18 |
Bu |
275 |
275 |
18.77 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 13456.1 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 13456.1 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 B1B95/daug-cc-pVTZ
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.422 |
0.625 |
0.000 |
| C2 |
-0.422 |
-0.625 |
0.000 |
| F3 |
-0.422 |
1.717 |
0.000 |
| F4 |
0.422 |
-1.717 |
0.000 |
| H5 |
1.049 |
0.671 |
0.889 |
| H6 |
1.049 |
0.671 |
-0.889 |
| H7 |
-1.049 |
-0.671 |
0.889 |
| H8 |
-1.049 |
-0.671 |
-0.889 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5088 | 1.3804 | 2.3422 | 1.0884 | 1.0884 | 2.1526 | 2.1526 |
C2 | 1.5088 | | 2.3422 | 1.3804 | 2.1526 | 2.1526 | 1.0884 | 1.0884 | F3 | 1.3804 | 2.3422 | | 3.5364 | 2.0121 | 2.0121 | 2.6239 | 2.6239 | F4 | 2.3422 | 1.3804 | 3.5364 | | 2.6239 | 2.6239 | 2.0121 | 2.0121 | H5 | 1.0884 | 2.1526 | 2.0121 | 2.6239 | | 1.7777 | 2.4899 | 3.0594 | H6 | 1.0884 | 2.1526 | 2.0121 | 2.6239 | 1.7777 | | 3.0594 | 2.4899 | H7 | 2.1526 | 1.0884 | 2.6239 | 2.0121 | 2.4899 | 3.0594 | | 1.7777 | H8 | 2.1526 | 1.0884 | 2.6239 | 2.0121 | 3.0594 | 2.4899 | 1.7777 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
108.242 |
|
C1 |
C2 |
H7 |
110.917 |
| C1 |
C2 |
H8 |
110.917 |
|
C2 |
C1 |
F3 |
108.242 |
| C2 |
C1 |
H5 |
110.917 |
|
C2 |
C1 |
H6 |
110.917 |
| F3 |
C1 |
H5 |
108.596 |
|
F3 |
C1 |
H6 |
108.596 |
| F4 |
C2 |
H7 |
108.596 |
|
F4 |
C2 |
H8 |
108.596 |
| H5 |
C1 |
H6 |
109.505 |
|
H7 |
C2 |
H8 |
109.505 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/daug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.188 |
|
|
|
| 2 |
C |
-0.188 |
|
|
|
| 3 |
F |
-0.843 |
|
|
|
| 4 |
F |
-0.843 |
|
|
|
| 5 |
H |
0.515 |
|
|
|
| 6 |
H |
0.515 |
|
|
|
| 7 |
H |
0.515 |
|
|
|
| 8 |
H |
0.515 |
|
|
|
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 |
-22.177 |
3.143 |
0.000 |
| y |
3.143 |
-29.223 |
0.000 |
| z |
0.000 |
0.000 |
-21.508 |
|
| Traceless |
| | x | y | z |
| x |
3.189 |
3.143 |
0.000 |
| y |
3.143 |
-7.381 |
0.000 |
| z |
0.000 |
0.000 |
4.192 |
|
| Polar |
| 3z2-r2 | 8.384 |
| x2-y2 | 7.047 |
| xy | 3.143 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.393 |
-0.037 |
0.000 |
| y |
-0.037 |
4.599 |
0.000 |
| z |
0.000 |
0.000 |
4.034 |
<r2> (average value of r
2) Å
2
| <r2> |
87.646 |
| (<r2>)1/2 |
9.362 |
Jump to
S1C1
Energy calculated at B1B95/daug-cc-pVTZ
| | hartrees |
| Energy at 0K | -278.312409 |
| Energy at 298.15K | |
| HF Energy | -278.312409 |
| Nuclear repulsion energy | 128.240817 |
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 B1B95/daug-cc-pVTZ
| 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 |
3114 |
3114 |
13.66 |
85.15 |
0.75 |
0.85 |
| 2 |
A |
3069 |
3069 |
36.08 |
238.57 |
0.02 |
0.03 |
| 3 |
A |
1487 |
1487 |
0.70 |
1.45 |
0.66 |
0.80 |
| 4 |
A |
1437 |
1437 |
11.81 |
1.19 |
0.24 |
0.39 |
| 5 |
A |
1308 |
1308 |
3.57 |
8.25 |
0.65 |
0.79 |
| 6 |
A |
1137 |
1137 |
90.32 |
3.41 |
0.39 |
0.56 |
| 7 |
A |
1129 |
1129 |
8.21 |
1.31 |
0.30 |
0.46 |
| 8 |
A |
880 |
880 |
20.83 |
5.90 |
0.16 |
0.27 |
| 9 |
A |
322 |
322 |
0.46 |
0.40 |
0.28 |
0.44 |
| 10 |
A |
149 |
149 |
3.67 |
0.11 |
0.75 |
0.86 |
| 11 |
B |
3127 |
3127 |
30.85 |
11.90 |
0.75 |
0.86 |
| 12 |
B |
3059 |
3059 |
8.65 |
32.30 |
0.75 |
0.86 |
| 13 |
B |
1486 |
1486 |
10.25 |
6.62 |
0.75 |
0.86 |
| 14 |
B |
1398 |
1398 |
7.11 |
0.01 |
0.75 |
0.86 |
| 15 |
B |
1266 |
1266 |
7.64 |
2.06 |
0.75 |
0.86 |
| 16 |
B |
1106 |
1106 |
63.04 |
3.76 |
0.75 |
0.86 |
| 17 |
B |
911 |
911 |
40.30 |
2.18 |
0.75 |
0.86 |
| 18 |
B |
495 |
495 |
15.77 |
0.44 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13439.6 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 13439.6 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 B1B95/daug-cc-pVTZ
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.265 |
0.699 |
0.505 |
| C2 |
-0.265 |
-0.699 |
0.505 |
| F3 |
-0.265 |
1.425 |
-0.541 |
| F4 |
0.265 |
-1.425 |
-0.541 |
| H5 |
-0.010 |
1.194 |
1.437 |
| H6 |
1.349 |
0.699 |
0.399 |
| H7 |
0.010 |
-1.194 |
1.437 |
| H8 |
-1.349 |
-0.699 |
0.399 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.4959 | 1.3787 | 2.3673 | 1.0907 | 1.0891 | 2.1256 | 2.1385 |
C2 | 1.4959 | | 2.3673 | 1.3787 | 2.1256 | 2.1385 | 1.0907 | 1.0891 | F3 | 1.3787 | 2.3673 | | 2.8984 | 2.0072 | 2.0046 | 3.2930 | 2.5628 | F4 | 2.3673 | 1.3787 | 2.8984 | | 3.2930 | 2.5628 | 2.0072 | 2.0046 | H5 | 1.0907 | 2.1256 | 2.0072 | 3.2930 | | 1.7805 | 2.3880 | 2.5401 | H6 | 1.0891 | 2.1385 | 2.0046 | 2.5628 | 1.7805 | | 2.5401 | 3.0392 | H7 | 2.1256 | 1.0907 | 3.2930 | 2.0072 | 2.3880 | 2.5401 | | 1.7805 | H8 | 2.1385 | 1.0891 | 2.5628 | 2.0046 | 2.5401 | 3.0392 | 1.7805 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
110.813 |
|
C1 |
C2 |
H7 |
109.534 |
| C1 |
C2 |
H8 |
110.653 |
|
C2 |
C1 |
F3 |
110.813 |
| C2 |
C1 |
H5 |
109.534 |
|
C2 |
C1 |
H6 |
110.653 |
| F3 |
C1 |
H5 |
108.187 |
|
F3 |
C1 |
H6 |
108.067 |
| F4 |
C2 |
H7 |
108.187 |
|
F4 |
C2 |
H8 |
108.067 |
| H5 |
C1 |
H6 |
109.535 |
|
H7 |
C2 |
H8 |
109.535 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/daug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.310 |
|
|
|
| 2 |
C |
-0.310 |
|
|
|
| 3 |
F |
-0.812 |
|
|
|
| 4 |
F |
-0.812 |
|
|
|
| 5 |
H |
0.685 |
|
|
|
| 6 |
H |
0.436 |
|
|
|
| 7 |
H |
0.685 |
|
|
|
| 8 |
H |
0.436 |
|
|
|
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
| Primitive |
| | x | y | z |
| x |
-21.743 |
1.712 |
0.000 |
| y |
1.712 |
-26.210 |
0.000 |
| z |
0.000 |
0.000 |
-22.457 |
|
| Traceless |
| | x | y | z |
| x |
2.590 |
1.712 |
0.000 |
| y |
1.712 |
-4.110 |
0.000 |
| z |
0.000 |
0.000 |
1.520 |
|
| Polar |
| 3z2-r2 | 3.039 |
| x2-y2 | 4.467 |
| xy | 1.712 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.188 |
0.049 |
0.000 |
| y |
0.049 |
4.567 |
0.000 |
| z |
0.000 |
0.000 |
4.358 |
<r2> (average value of r
2) Å
2
| <r2> |
79.413 |
| (<r2>)1/2 |
8.911 |