Jump to
S1C2
Energy calculated at B1B95/6-31G*
| hartrees |
Energy at 0K | -551.375287 |
Energy at 298.15K | |
HF Energy | -551.375287 |
Nuclear repulsion energy | 354.590395 |
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 B1B95/6-31G*
Geometric Data calculated at B1B95/6-31G*
Point Group is D4h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
1.011 |
0.000 |
C2 |
1.011 |
0.000 |
0.000 |
C3 |
0.000 |
-1.011 |
0.000 |
C4 |
-1.011 |
0.000 |
0.000 |
F5 |
0.000 |
2.322 |
0.000 |
F6 |
2.322 |
0.000 |
0.000 |
F7 |
0.000 |
-2.322 |
0.000 |
F8 |
-2.322 |
0.000 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
C3 |
C4 |
F5 |
F6 |
F7 |
F8 |
C1 | | 1.4299 | 2.0222 | 1.4299 | 1.3106 | 2.5324 | 3.3329 | 2.5324 |
C2 | 1.4299 | | 1.4299 | 2.0222 | 2.5324 | 1.3106 | 2.5324 | 3.3329 | C3 | 2.0222 | 1.4299 | | 1.4299 | 3.3329 | 2.5324 | 1.3106 | 2.5324 | C4 | 1.4299 | 2.0222 | 1.4299 | | 2.5324 | 3.3329 | 2.5324 | 1.3106 | F5 | 1.3106 | 2.5324 | 3.3329 | 2.5324 | | 3.2834 | 4.6435 | 3.2834 | F6 | 2.5324 | 1.3106 | 2.5324 | 3.3329 | 3.2834 | | 3.2834 | 4.6435 | F7 | 3.3329 | 2.5324 | 1.3106 | 2.5324 | 4.6435 | 3.2834 | | 3.2834 | F8 | 2.5324 | 3.3329 | 2.5324 | 1.3106 | 3.2834 | 4.6435 | 3.2834 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
C3 |
90.000 |
|
C1 |
C2 |
F6 |
135.000 |
C1 |
C4 |
C3 |
90.000 |
|
C1 |
C4 |
F8 |
135.000 |
C2 |
C1 |
C4 |
90.000 |
|
C2 |
C1 |
F5 |
135.000 |
C2 |
C3 |
C4 |
90.000 |
|
C2 |
C3 |
F7 |
135.000 |
C3 |
C2 |
F6 |
135.000 |
|
C3 |
C4 |
F8 |
135.000 |
C4 |
C1 |
F5 |
135.000 |
|
C4 |
C3 |
F7 |
135.000 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.400 |
|
|
|
2 |
C |
0.050 |
|
|
|
3 |
C |
0.400 |
|
|
|
4 |
C |
0.050 |
|
|
|
5 |
F |
-0.190 |
|
|
|
6 |
F |
-0.260 |
|
|
|
7 |
F |
-0.190 |
|
|
|
8 |
F |
-0.260 |
|
|
|
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 |
-47.224 |
0.000 |
0.000 |
y |
0.000 |
-36.661 |
0.000 |
z |
0.000 |
0.000 |
-39.719 |
|
Traceless |
| x | y | z |
x |
-9.034 |
0.000 |
0.000 |
y |
0.000 |
6.811 |
0.000 |
z |
0.000 |
0.000 |
2.223 |
|
Polar |
3z2-r2 | 4.447 |
x2-y2 | -10.563 |
xy | 0.000 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
6.907 |
0.000 |
0.000 |
y |
0.000 |
7.528 |
0.000 |
z |
0.000 |
0.000 |
3.012 |
<r2> (average value of r
2) Å
2
<r2> |
244.329 |
(<r2>)1/2 |
15.631 |
Jump to
S1C1
Energy calculated at B1B95/6-31G*
| hartrees |
Energy at 0K | -551.455522 |
Energy at 298.15K | -551.455438 |
HF Energy | -551.455522 |
Nuclear repulsion energy | 355.104502 |
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 B1B95/6-31G*
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 |
1910 |
1813 |
0.00 |
|
|
|
2 |
Ag |
1255 |
1191 |
0.00 |
|
|
|
3 |
Ag |
715 |
679 |
0.00 |
|
|
|
4 |
Ag |
293 |
278 |
0.00 |
|
|
|
5 |
Ag |
177 |
168 |
0.00 |
|
|
|
6 |
Au |
1363 |
1294 |
506.88 |
|
|
|
7 |
Au |
942 |
894 |
42.59 |
|
|
|
8 |
Au |
582 |
552 |
50.65 |
|
|
|
9 |
Au |
237 |
225 |
0.04 |
|
|
|
10 |
Au |
157 |
149 |
0.04 |
|
|
|
11 |
Bg |
1392 |
1321 |
0.00 |
|
|
|
12 |
Bg |
762 |
724 |
0.00 |
|
|
|
13 |
Bg |
486 |
461 |
0.00 |
|
|
|
14 |
Bg |
386 |
366 |
0.00 |
|
|
|
15 |
Bu |
1889 |
1793 |
173.64 |
|
|
|
16 |
Bu |
1016 |
965 |
184.22 |
|
|
|
17 |
Bu |
311 |
295 |
5.72 |
|
|
|
18 |
Bu |
190 |
180 |
1.95 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7030.8 cm
-1
Scaled (by 0.9493) Zero Point Vibrational Energy (zpe) 6674.3 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 B1B95/6-31G*
Point Group is C2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.107 |
0.768 |
0.662 |
C2 |
-0.107 |
-0.768 |
0.662 |
C3 |
-0.107 |
-0.768 |
-0.662 |
C4 |
0.107 |
0.768 |
-0.662 |
F5 |
-0.107 |
1.656 |
1.607 |
F6 |
0.107 |
-1.656 |
1.607 |
F7 |
0.107 |
-1.656 |
-1.607 |
F8 |
-0.107 |
1.656 |
-1.607 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
C3 |
C4 |
F5 |
F6 |
F7 |
F8 |
C1 | | 1.5516 | 2.0402 | 1.3248 | 1.3140 | 2.6020 | 3.3209 | 2.4464 |
C2 | 1.5516 | | 1.3248 | 2.0402 | 2.6020 | 1.3140 | 2.4464 | 3.3209 | C3 | 2.0402 | 1.3248 | | 1.5516 | 3.3209 | 2.4464 | 1.3140 | 2.6020 | C4 | 1.3248 | 2.0402 | 1.5516 | | 2.4464 | 3.3209 | 2.6020 | 1.3140 | F5 | 1.3140 | 2.6020 | 3.3209 | 2.4464 | | 3.3192 | 4.6204 | 3.2141 | F6 | 2.6020 | 1.3140 | 2.4464 | 3.3209 | 3.3192 | | 3.2141 | 4.6204 | F7 | 3.3209 | 2.4464 | 1.3140 | 2.6020 | 4.6204 | 3.2141 | | 3.3192 | F8 | 2.4464 | 3.3209 | 2.6020 | 1.3140 | 3.2141 | 4.6204 | 3.3192 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
C3 |
90.000 |
|
C1 |
C2 |
F6 |
130.288 |
C1 |
C4 |
C3 |
90.000 |
|
C1 |
C4 |
F8 |
135.964 |
C2 |
C1 |
C4 |
90.000 |
|
C2 |
C1 |
F5 |
130.288 |
C2 |
C3 |
C4 |
90.000 |
|
C2 |
C3 |
F7 |
135.964 |
C3 |
C2 |
F6 |
135.964 |
|
C3 |
C4 |
F8 |
130.288 |
C4 |
C1 |
F5 |
135.964 |
|
C4 |
C3 |
F7 |
130.288 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.231 |
|
|
|
2 |
C |
0.231 |
|
|
|
3 |
C |
0.231 |
|
|
|
4 |
C |
0.231 |
|
|
|
5 |
F |
-0.231 |
|
|
|
6 |
F |
-0.231 |
|
|
|
7 |
F |
-0.231 |
|
|
|
8 |
F |
-0.231 |
|
|
|
Electric dipole moments
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-39.447 |
-0.013 |
0.000 |
y |
-0.013 |
-42.338 |
0.000 |
z |
0.000 |
0.000 |
-42.027 |
|
Traceless |
| x | y | z |
x |
2.736 |
-0.013 |
0.000 |
y |
-0.013 |
-1.601 |
0.000 |
z |
0.000 |
0.000 |
-1.134 |
|
Polar |
3z2-r2 | -2.268 |
x2-y2 | 2.891 |
xy | -0.013 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.978 |
-0.019 |
0.000 |
y |
-0.019 |
5.750 |
0.000 |
z |
0.000 |
0.000 |
7.404 |
<r2> (average value of r
2) Å
2
<r2> |
242.881 |
(<r2>)1/2 |
15.585 |