Jump to
S1C2
Energy calculated at B3PW91/aug-cc-pVDZ
| hartrees |
Energy at 0K | -278.225242 |
Energy at 298.15K | |
HF Energy | -278.225242 |
Nuclear repulsion energy | 125.088049 |
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 B3PW91/aug-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 |
3068 |
2959 |
0.00 |
251.70 |
0.05 |
0.10 |
2 |
Ag |
1487 |
1435 |
0.00 |
7.17 |
0.73 |
0.85 |
3 |
Ag |
1422 |
1372 |
0.00 |
2.56 |
0.47 |
0.64 |
4 |
Ag |
1096 |
1057 |
0.00 |
6.32 |
0.42 |
0.60 |
5 |
Ag |
1052 |
1015 |
0.00 |
9.75 |
0.39 |
0.56 |
6 |
Ag |
454 |
438 |
0.00 |
2.50 |
0.37 |
0.54 |
7 |
Au |
3146 |
3035 |
39.87 |
0.00 |
0.00 |
0.00 |
8 |
Au |
1215 |
1172 |
3.95 |
0.00 |
0.00 |
0.00 |
9 |
Au |
806 |
778 |
0.09 |
0.00 |
0.00 |
0.00 |
10 |
Au |
111 |
107 |
12.85 |
0.00 |
0.00 |
0.00 |
11 |
Bg |
3122 |
3011 |
0.00 |
110.96 |
0.75 |
0.86 |
12 |
Bg |
1280 |
1235 |
0.00 |
6.67 |
0.75 |
0.86 |
13 |
Bg |
1156 |
1115 |
0.00 |
1.27 |
0.75 |
0.86 |
14 |
Bu |
3073 |
2964 |
56.31 |
0.00 |
0.00 |
0.00 |
15 |
Bu |
1492 |
1439 |
4.53 |
0.00 |
0.00 |
0.00 |
16 |
Bu |
1329 |
1282 |
4.64 |
0.00 |
0.00 |
0.00 |
17 |
Bu |
1062 |
1025 |
218.01 |
0.00 |
0.00 |
0.00 |
18 |
Bu |
279 |
269 |
19.25 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 13325.1 cm
-1
Scaled (by 0.9646) Zero Point Vibrational Energy (zpe) 12853.4 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 B3PW91/aug-cc-pVDZ
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 |
1.732 |
0.000 |
F4 |
0.427 |
-1.732 |
0.000 |
H5 |
1.057 |
0.679 |
0.899 |
H6 |
1.057 |
0.679 |
-0.899 |
H7 |
-1.057 |
-0.679 |
0.899 |
H8 |
-1.057 |
-0.679 |
-0.899 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5161 | 1.3963 | 2.3583 | 1.0988 | 1.0988 | 2.1710 | 2.1710 |
C2 | 1.5161 | | 2.3583 | 1.3963 | 2.1710 | 2.1710 | 1.0988 | 1.0988 | F3 | 1.3963 | 2.3583 | | 3.5670 | 2.0290 | 2.0290 | 2.6488 | 2.6488 | F4 | 2.3583 | 1.3963 | 3.5670 | | 2.6488 | 2.6488 | 2.0290 | 2.0290 | H5 | 1.0988 | 2.1710 | 2.0290 | 2.6488 | | 1.7972 | 2.5125 | 3.0891 | H6 | 1.0988 | 2.1710 | 2.0290 | 2.6488 | 1.7972 | | 3.0891 | 2.5125 | H7 | 2.1710 | 1.0988 | 2.6488 | 2.0290 | 2.5125 | 3.0891 | | 1.7972 | H8 | 2.1710 | 1.0988 | 2.6488 | 2.0290 | 3.0891 | 2.5125 | 1.7972 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
F4 |
108.066 |
|
C1 |
C2 |
H7 |
111.244 |
C1 |
C2 |
H8 |
111.244 |
|
C2 |
C1 |
F3 |
108.066 |
C2 |
C1 |
H5 |
111.244 |
|
C2 |
C1 |
H6 |
111.244 |
F3 |
C1 |
H5 |
108.223 |
|
F3 |
C1 |
H6 |
108.223 |
F4 |
C2 |
H7 |
108.223 |
|
F4 |
C2 |
H8 |
108.223 |
H5 |
C1 |
H6 |
109.729 |
|
H7 |
C2 |
H8 |
109.729 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/aug-cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.797 |
|
|
|
2 |
C |
0.797 |
|
|
|
3 |
F |
-0.436 |
|
|
|
4 |
F |
-0.436 |
|
|
|
5 |
H |
-0.181 |
|
|
|
6 |
H |
-0.181 |
|
|
|
7 |
H |
-0.181 |
|
|
|
8 |
H |
-0.181 |
|
|
|
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 |
-22.232 |
3.206 |
0.000 |
y |
3.206 |
-29.510 |
0.000 |
z |
0.000 |
0.000 |
-21.571 |
|
Traceless |
| x | y | z |
x |
3.308 |
3.206 |
0.000 |
y |
3.206 |
-7.609 |
0.000 |
z |
0.000 |
0.000 |
4.300 |
|
Polar |
3z2-r2 | 8.600 |
x2-y2 | 7.278 |
xy | 3.206 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
4.405 |
-0.078 |
0.000 |
y |
-0.078 |
4.660 |
0.000 |
z |
0.000 |
0.000 |
4.018 |
<r2> (average value of r
2) Å
2
<r2> |
88.958 |
(<r2>)1/2 |
9.432 |
Jump to
S1C1
Energy calculated at B3PW91/aug-cc-pVDZ
| hartrees |
Energy at 0K | -278.226923 |
Energy at 298.15K | |
HF Energy | -278.226923 |
Nuclear repulsion energy | 127.067173 |
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 B3PW91/aug-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 |
3115 |
3005 |
11.00 |
89.73 |
0.73 |
0.84 |
2 |
A |
3060 |
2952 |
39.05 |
233.98 |
0.01 |
0.03 |
3 |
A |
1457 |
1406 |
1.95 |
1.30 |
0.71 |
0.83 |
4 |
A |
1416 |
1365 |
10.02 |
1.41 |
0.26 |
0.42 |
5 |
A |
1287 |
1242 |
3.48 |
8.35 |
0.66 |
0.80 |
6 |
A |
1119 |
1080 |
31.32 |
1.81 |
0.64 |
0.78 |
7 |
A |
1110 |
1071 |
61.36 |
2.94 |
0.27 |
0.42 |
8 |
A |
869 |
838 |
25.00 |
5.83 |
0.15 |
0.27 |
9 |
A |
319 |
308 |
0.50 |
0.40 |
0.32 |
0.49 |
10 |
A |
148 |
143 |
3.66 |
0.15 |
0.75 |
0.86 |
11 |
B |
3127 |
3017 |
30.16 |
12.43 |
0.75 |
0.86 |
12 |
B |
3050 |
2942 |
8.76 |
33.19 |
0.75 |
0.86 |
13 |
B |
1454 |
1402 |
10.04 |
6.86 |
0.75 |
0.86 |
14 |
B |
1369 |
1321 |
5.62 |
0.02 |
0.75 |
0.86 |
15 |
B |
1242 |
1198 |
6.69 |
2.11 |
0.75 |
0.86 |
16 |
B |
1076 |
1037 |
61.69 |
3.93 |
0.75 |
0.86 |
17 |
B |
891 |
860 |
42.35 |
2.58 |
0.75 |
0.86 |
18 |
B |
489 |
472 |
15.96 |
0.48 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13299.4 cm
-1
Scaled (by 0.9646) Zero Point Vibrational Energy (zpe) 12828.6 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 B3PW91/aug-cc-pVDZ
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.268 |
0.702 |
0.510 |
C2 |
-0.268 |
-0.702 |
0.510 |
F3 |
-0.268 |
1.439 |
-0.545 |
F4 |
0.268 |
-1.439 |
-0.545 |
H5 |
-0.014 |
1.204 |
1.449 |
H6 |
1.362 |
0.706 |
0.400 |
H7 |
0.014 |
-1.204 |
1.449 |
H8 |
-1.362 |
-0.706 |
0.400 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5029 | 1.3940 | 2.3871 | 1.1013 | 1.0994 | 2.1396 | 2.1569 |
C2 | 1.5029 | | 2.3871 | 1.3940 | 2.1396 | 2.1569 | 1.1013 | 1.0994 | F3 | 1.3940 | 2.3871 | | 2.9284 | 2.0236 | 2.0217 | 3.3226 | 2.5875 | F4 | 2.3871 | 1.3940 | 2.9284 | | 3.3226 | 2.5875 | 2.0236 | 2.0217 | H5 | 1.1013 | 2.1396 | 2.0236 | 3.3226 | | 1.7998 | 2.4073 | 2.5620 | H6 | 1.0994 | 2.1569 | 2.0217 | 2.5875 | 1.7998 | | 2.5620 | 3.0684 | H7 | 2.1396 | 1.1013 | 3.3226 | 2.0236 | 2.4073 | 2.5620 | | 1.7998 | H8 | 2.1569 | 1.0994 | 2.5875 | 2.0217 | 2.5620 | 3.0684 | 1.7998 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
F4 |
110.922 |
|
C1 |
C2 |
H7 |
109.521 |
C1 |
C2 |
H8 |
111.010 |
|
C2 |
C1 |
F3 |
110.922 |
C2 |
C1 |
H5 |
109.521 |
|
C2 |
C1 |
H6 |
111.010 |
F3 |
C1 |
H5 |
107.804 |
|
F3 |
C1 |
H6 |
107.775 |
F4 |
C2 |
H7 |
107.804 |
|
F4 |
C2 |
H8 |
107.775 |
H5 |
C1 |
H6 |
109.738 |
|
H7 |
C2 |
H8 |
109.738 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/aug-cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.819 |
|
|
|
2 |
C |
0.819 |
|
|
|
3 |
F |
-0.436 |
|
|
|
4 |
F |
-0.436 |
|
|
|
5 |
H |
-0.190 |
|
|
|
6 |
H |
-0.193 |
|
|
|
7 |
H |
-0.190 |
|
|
|
8 |
H |
-0.193 |
|
|
|
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 |
2.748 |
2.748 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-21.802 |
1.745 |
0.000 |
y |
1.745 |
-26.440 |
0.000 |
z |
0.000 |
0.000 |
-22.521 |
|
Traceless |
| x | y | z |
x |
2.679 |
1.745 |
0.000 |
y |
1.745 |
-4.279 |
0.000 |
z |
0.000 |
0.000 |
1.600 |
|
Polar |
3z2-r2 | 3.199 |
x2-y2 | 4.638 |
xy | 1.745 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
4.190 |
0.033 |
0.000 |
y |
0.033 |
4.605 |
0.000 |
z |
0.000 |
0.000 |
4.400 |
<r2> (average value of r
2) Å
2
<r2> |
80.683 |
(<r2>)1/2 |
8.982 |