Jump to
S1C2
Energy calculated at B3LYP/daug-cc-pVDZ
| | hartrees |
| Energy at 0K | -278.330183 |
| Energy at 298.15K | |
| HF Energy | -278.330183 |
| Nuclear repulsion energy | 124.673065 |
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 B3LYP/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 |
3061 |
3061 |
0.00 |
256.74 |
0.05 |
0.10 |
| 2 |
Ag |
1486 |
1486 |
0.00 |
7.34 |
0.73 |
0.85 |
| 3 |
Ag |
1415 |
1415 |
0.00 |
2.41 |
0.51 |
0.67 |
| 4 |
Ag |
1084 |
1084 |
0.00 |
6.66 |
0.35 |
0.52 |
| 5 |
Ag |
1028 |
1028 |
0.00 |
10.76 |
0.41 |
0.58 |
| 6 |
Ag |
450 |
450 |
0.00 |
2.80 |
0.34 |
0.51 |
| 7 |
Au |
3137 |
3137 |
39.45 |
0.00 |
0.00 |
0.00 |
| 8 |
Au |
1211 |
1211 |
3.99 |
0.00 |
0.00 |
0.00 |
| 9 |
Au |
805 |
805 |
0.04 |
0.00 |
0.00 |
0.00 |
| 10 |
Au |
111 |
111 |
13.62 |
0.00 |
0.00 |
0.00 |
| 11 |
Bg |
3113 |
3113 |
0.00 |
112.36 |
0.75 |
0.86 |
| 12 |
Bg |
1280 |
1280 |
0.00 |
6.89 |
0.75 |
0.86 |
| 13 |
Bg |
1154 |
1154 |
0.00 |
1.41 |
0.75 |
0.86 |
| 14 |
Bu |
3067 |
3067 |
54.35 |
0.00 |
0.00 |
0.00 |
| 15 |
Bu |
1493 |
1493 |
4.18 |
0.00 |
0.00 |
0.00 |
| 16 |
Bu |
1327 |
1327 |
5.08 |
0.00 |
0.00 |
0.00 |
| 17 |
Bu |
1035 |
1035 |
222.29 |
0.00 |
0.00 |
0.00 |
| 18 |
Bu |
281 |
281 |
20.09 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 13268.6 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 13268.6 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 B3LYP/daug-cc-pVDZ
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.429 |
0.627 |
0.000 |
| C2 |
-0.429 |
-0.627 |
0.000 |
| F3 |
-0.429 |
1.738 |
0.000 |
| F4 |
0.429 |
-1.738 |
0.000 |
| H5 |
1.056 |
0.682 |
0.899 |
| H6 |
1.056 |
0.682 |
-0.899 |
| H7 |
-1.056 |
-0.682 |
0.899 |
| H8 |
-1.056 |
-0.682 |
-0.899 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5196 | 1.4044 | 2.3650 | 1.0976 | 1.0976 | 2.1746 | 2.1746 |
C2 | 1.5196 | | 2.3650 | 1.4044 | 2.1746 | 2.1746 | 1.0976 | 1.0976 | F3 | 1.4044 | 2.3650 | | 3.5807 | 2.0324 | 2.0324 | 2.6569 | 2.6569 | F4 | 2.3650 | 1.4044 | 3.5807 | | 2.6569 | 2.6569 | 2.0324 | 2.0324 | H5 | 1.0976 | 2.1746 | 2.0324 | 2.6569 | | 1.7987 | 2.5146 | 3.0917 | H6 | 1.0976 | 2.1746 | 2.0324 | 2.6569 | 1.7987 | | 3.0917 | 2.5146 | H7 | 2.1746 | 1.0976 | 2.6569 | 2.0324 | 2.5146 | 3.0917 | | 1.7987 | H8 | 2.1746 | 1.0976 | 2.6569 | 2.0324 | 3.0917 | 2.5146 | 1.7987 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
107.894 |
|
C1 |
C2 |
H7 |
111.360 |
| C1 |
C2 |
H8 |
111.360 |
|
C2 |
C1 |
F3 |
107.894 |
| C2 |
C1 |
H5 |
111.360 |
|
C2 |
C1 |
H6 |
111.360 |
| F3 |
C1 |
H5 |
108.020 |
|
F3 |
C1 |
H6 |
108.020 |
| F4 |
C2 |
H7 |
108.020 |
|
F4 |
C2 |
H8 |
108.020 |
| H5 |
C1 |
H6 |
110.045 |
|
H7 |
C2 |
H8 |
110.045 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/daug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
1.538 |
|
|
|
| 2 |
C |
1.538 |
|
|
|
| 3 |
F |
-0.619 |
|
|
|
| 4 |
F |
-0.619 |
|
|
|
| 5 |
H |
-0.460 |
|
|
|
| 6 |
H |
-0.460 |
|
|
|
| 7 |
H |
-0.460 |
|
|
|
| 8 |
H |
-0.460 |
|
|
|
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 |
-22.471 |
3.301 |
0.000 |
| y |
3.301 |
-29.960 |
0.000 |
| z |
0.000 |
0.000 |
-21.794 |
|
| Traceless |
| | x | y | z |
| x |
3.407 |
3.301 |
0.000 |
| y |
3.301 |
-7.828 |
0.000 |
| z |
0.000 |
0.000 |
4.421 |
|
| Polar |
| 3z2-r2 | 8.842 |
| x2-y2 | 7.490 |
| xy | 3.301 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.527 |
-0.072 |
0.000 |
| y |
-0.072 |
4.792 |
0.000 |
| z |
0.000 |
0.000 |
4.145 |
<r2> (average value of r
2) Å
2
| <r2> |
89.636 |
| (<r2>)1/2 |
9.468 |
Jump to
S1C1
Energy calculated at B3LYP/daug-cc-pVDZ
| | hartrees |
| Energy at 0K | -278.331725 |
| Energy at 298.15K | |
| HF Energy | -278.331725 |
| Nuclear repulsion energy | 126.690504 |
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 B3LYP/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 |
3105 |
3105 |
10.85 |
92.92 |
0.72 |
0.84 |
| 2 |
A |
3052 |
3052 |
39.67 |
239.11 |
0.01 |
0.02 |
| 3 |
A |
1458 |
1458 |
1.71 |
1.38 |
0.71 |
0.83 |
| 4 |
A |
1410 |
1410 |
8.94 |
1.39 |
0.28 |
0.44 |
| 5 |
A |
1284 |
1284 |
3.15 |
8.65 |
0.66 |
0.79 |
| 6 |
A |
1113 |
1113 |
1.92 |
1.36 |
0.15 |
0.27 |
| 7 |
A |
1091 |
1091 |
88.83 |
3.63 |
0.49 |
0.66 |
| 8 |
A |
860 |
860 |
28.68 |
6.60 |
0.14 |
0.25 |
| 9 |
A |
320 |
320 |
0.48 |
0.48 |
0.29 |
0.45 |
| 10 |
A |
147 |
147 |
3.85 |
0.14 |
0.75 |
0.86 |
| 11 |
B |
3117 |
3117 |
30.53 |
12.09 |
0.75 |
0.86 |
| 12 |
B |
3043 |
3043 |
7.82 |
34.99 |
0.75 |
0.86 |
| 13 |
B |
1456 |
1456 |
9.54 |
6.99 |
0.75 |
0.86 |
| 14 |
B |
1369 |
1369 |
6.19 |
0.01 |
0.75 |
0.86 |
| 15 |
B |
1238 |
1238 |
6.04 |
2.13 |
0.75 |
0.86 |
| 16 |
B |
1059 |
1059 |
56.21 |
3.75 |
0.75 |
0.86 |
| 17 |
B |
884 |
884 |
49.69 |
2.84 |
0.75 |
0.86 |
| 18 |
B |
490 |
490 |
16.73 |
0.50 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13246.6 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 13246.6 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 B3LYP/daug-cc-pVDZ
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.271 |
0.703 |
0.513 |
| C2 |
-0.271 |
-0.703 |
0.513 |
| F3 |
-0.271 |
1.443 |
-0.547 |
| F4 |
0.271 |
-1.443 |
-0.547 |
| H5 |
-0.011 |
1.208 |
1.449 |
| H6 |
1.363 |
0.707 |
0.397 |
| H7 |
0.011 |
-1.208 |
1.449 |
| H8 |
-1.363 |
-0.707 |
0.397 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5064 | 1.4015 | 2.3934 | 1.1003 | 1.0983 | 2.1438 | 2.1607 |
C2 | 1.5064 | | 2.3934 | 1.4015 | 2.1438 | 2.1607 | 1.1003 | 1.0983 | F3 | 1.4015 | 2.3934 | | 2.9361 | 2.0267 | 2.0252 | 3.3304 | 2.5897 | F4 | 2.3934 | 1.4015 | 2.9361 | | 3.3304 | 2.5897 | 2.0267 | 2.0252 | H5 | 1.1003 | 2.1438 | 2.0267 | 3.3304 | | 1.8009 | 2.4162 | 2.5694 | H6 | 1.0983 | 2.1607 | 2.0252 | 2.5897 | 1.8009 | | 2.5694 | 3.0704 | H7 | 2.1438 | 1.1003 | 3.3304 | 2.0267 | 2.4162 | 2.5694 | | 1.8009 | H8 | 2.1607 | 1.0983 | 2.5897 | 2.0252 | 2.5694 | 3.0704 | 1.8009 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
110.733 |
|
C1 |
C2 |
H7 |
109.673 |
| C1 |
C2 |
H8 |
111.140 |
|
C2 |
C1 |
F3 |
110.733 |
| C2 |
C1 |
H5 |
109.673 |
|
C2 |
C1 |
H6 |
111.140 |
| F3 |
C1 |
H5 |
107.607 |
|
F3 |
C1 |
H6 |
107.606 |
| F4 |
C2 |
H7 |
107.607 |
|
F4 |
C2 |
H8 |
107.606 |
| H5 |
C1 |
H6 |
109.998 |
|
H7 |
C2 |
H8 |
109.998 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/daug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
1.608 |
|
|
|
| 2 |
C |
1.608 |
|
|
|
| 3 |
F |
-0.502 |
|
|
|
| 4 |
F |
-0.502 |
|
|
|
| 5 |
H |
-0.587 |
|
|
|
| 6 |
H |
-0.518 |
|
|
|
| 7 |
H |
-0.587 |
|
|
|
| 8 |
H |
-0.518 |
|
|
|
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 |
2.818 |
2.818 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.029 |
1.806 |
0.000 |
| y |
1.806 |
-26.806 |
0.000 |
| z |
0.000 |
0.000 |
-22.751 |
|
| Traceless |
| | x | y | z |
| x |
2.749 |
1.806 |
0.000 |
| y |
1.806 |
-4.416 |
0.000 |
| z |
0.000 |
0.000 |
1.667 |
|
| Polar |
| 3z2-r2 | 3.334 |
| x2-y2 | 4.777 |
| xy | 1.806 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.310 |
0.036 |
0.000 |
| y |
0.036 |
4.737 |
0.000 |
| z |
0.000 |
0.000 |
4.517 |
<r2> (average value of r
2) Å
2
| <r2> |
81.197 |
| (<r2>)1/2 |
9.011 |