Jump to
S1C2
Energy calculated at BLYP/6-311G*
| hartrees |
Energy at 0K | -278.302299 |
Energy at 298.15K | |
HF Energy | -278.302299 |
Nuclear repulsion energy | 123.948888 |
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 BLYP/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 |
2970 |
2963 |
0.00 |
|
|
|
2 |
Ag |
1487 |
1483 |
0.00 |
|
|
|
3 |
Ag |
1420 |
1417 |
0.00 |
|
|
|
4 |
Ag |
1041 |
1039 |
0.00 |
|
|
|
5 |
Ag |
986 |
983 |
0.00 |
|
|
|
6 |
Ag |
437 |
436 |
0.00 |
|
|
|
7 |
Au |
3038 |
3030 |
81.05 |
|
|
|
8 |
Au |
1198 |
1195 |
2.23 |
|
|
|
9 |
Au |
808 |
806 |
0.06 |
|
|
|
10 |
Au |
123 |
123 |
12.71 |
|
|
|
11 |
Bg |
3010 |
3003 |
0.00 |
|
|
|
12 |
Bg |
1273 |
1270 |
0.00 |
|
|
|
13 |
Bg |
1148 |
1145 |
0.00 |
|
|
|
14 |
Bu |
2976 |
2969 |
78.97 |
|
|
|
15 |
Bu |
1500 |
1496 |
1.13 |
|
|
|
16 |
Bu |
1337 |
1333 |
10.65 |
|
|
|
17 |
Bu |
998 |
995 |
191.59 |
|
|
|
18 |
Bu |
269 |
268 |
19.27 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13009.5 cm
-1
Scaled (by 0.9975) Zero Point Vibrational Energy (zpe) 12977.0 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 BLYP/6-311G*
Point Group is C2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.430 |
0.631 |
0.000 |
C2 |
-0.430 |
-0.631 |
0.000 |
F3 |
-0.430 |
1.752 |
0.000 |
F4 |
0.430 |
-1.752 |
0.000 |
H5 |
1.062 |
0.677 |
0.900 |
H6 |
1.062 |
0.677 |
-0.900 |
H7 |
-1.062 |
-0.677 |
0.900 |
H8 |
-1.062 |
-0.677 |
-0.900 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5282 | 1.4130 | 2.3832 | 1.1000 | 1.1000 | 2.1788 | 2.1788 |
C2 | 1.5282 | | 2.3832 | 1.4130 | 2.1788 | 2.1788 | 1.1000 | 1.1000 | F3 | 1.4130 | 2.3832 | | 3.6080 | 2.0474 | 2.0474 | 2.6658 | 2.6658 | F4 | 2.3832 | 1.4130 | 3.6080 | | 2.6658 | 2.6658 | 2.0474 | 2.0474 | H5 | 1.1000 | 2.1788 | 2.0474 | 2.6658 | | 1.7990 | 2.5184 | 3.0950 | H6 | 1.1000 | 2.1788 | 2.0474 | 2.6658 | 1.7990 | | 3.0950 | 2.5184 | H7 | 2.1788 | 1.1000 | 2.6658 | 2.0474 | 2.5184 | 3.0950 | | 1.7990 | H8 | 2.1788 | 1.1000 | 2.6658 | 2.0474 | 3.0950 | 2.5184 | 1.7990 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
F4 |
108.185 |
|
C1 |
C2 |
H7 |
110.946 |
C1 |
C2 |
H8 |
110.946 |
|
C2 |
C1 |
F3 |
108.185 |
C2 |
C1 |
H5 |
110.946 |
|
C2 |
C1 |
H6 |
110.946 |
F3 |
C1 |
H5 |
108.480 |
|
F3 |
C1 |
H6 |
108.480 |
F4 |
C2 |
H7 |
108.480 |
|
F4 |
C2 |
H8 |
108.480 |
H5 |
C1 |
H6 |
109.724 |
|
H7 |
C2 |
H8 |
109.724 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.127 |
|
|
|
2 |
C |
-0.127 |
|
|
|
3 |
F |
-0.257 |
|
|
|
4 |
F |
-0.257 |
|
|
|
5 |
H |
0.192 |
|
|
|
6 |
H |
0.192 |
|
|
|
7 |
H |
0.192 |
|
|
|
8 |
H |
0.192 |
|
|
|
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 |
-22.245 |
2.719 |
0.000 |
y |
2.719 |
-29.241 |
0.000 |
z |
0.000 |
0.000 |
-21.707 |
|
Traceless |
| x | y | z |
x |
3.229 |
2.719 |
0.000 |
y |
2.719 |
-7.265 |
0.000 |
z |
0.000 |
0.000 |
4.036 |
|
Polar |
3z2-r2 | 8.073 |
x2-y2 | 6.996 |
xy | 2.719 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.812 |
0.042 |
0.000 |
y |
0.042 |
3.843 |
0.000 |
z |
0.000 |
0.000 |
3.518 |
<r2> (average value of r
2) Å
2
<r2> |
90.402 |
(<r2>)1/2 |
9.508 |
Jump to
S1C1
Energy calculated at BLYP/6-311G*
| hartrees |
Energy at 0K | -278.302909 |
Energy at 298.15K | |
HF Energy | -278.302909 |
Nuclear repulsion energy | 125.986705 |
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 BLYP/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 |
2998 |
2990 |
20.21 |
|
|
|
2 |
A |
2957 |
2949 |
52.78 |
|
|
|
3 |
A |
1464 |
1460 |
0.00 |
|
|
|
4 |
A |
1400 |
1397 |
13.60 |
|
|
|
5 |
A |
1269 |
1266 |
1.10 |
|
|
|
6 |
A |
1099 |
1096 |
0.39 |
|
|
|
7 |
A |
1041 |
1038 |
78.05 |
|
|
|
8 |
A |
835 |
833 |
30.12 |
|
|
|
9 |
A |
317 |
316 |
0.32 |
|
|
|
10 |
A |
147 |
147 |
3.42 |
|
|
|
11 |
B |
3013 |
3006 |
62.49 |
|
|
|
12 |
B |
2943 |
2936 |
16.42 |
|
|
|
13 |
B |
1461 |
1457 |
7.67 |
|
|
|
14 |
B |
1379 |
1376 |
10.21 |
|
|
|
15 |
B |
1224 |
1220 |
3.32 |
|
|
|
16 |
B |
1029 |
1027 |
36.45 |
|
|
|
17 |
B |
867 |
865 |
53.23 |
|
|
|
18 |
B |
477 |
476 |
15.63 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 12959.2 cm
-1
Scaled (by 0.9975) Zero Point Vibrational Energy (zpe) 12926.8 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 BLYP/6-311G*
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.272 |
0.707 |
0.515 |
C2 |
-0.272 |
-0.707 |
0.515 |
F3 |
-0.272 |
1.453 |
-0.550 |
F4 |
0.272 |
-1.453 |
-0.550 |
H5 |
0.001 |
1.213 |
1.458 |
H6 |
1.367 |
0.699 |
0.400 |
H7 |
-0.001 |
-1.213 |
1.458 |
H8 |
-1.367 |
-0.699 |
0.400 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5155 | 1.4097 | 2.4084 | 1.1034 | 1.1009 | 2.1560 | 2.1631 |
C2 | 1.5155 | | 2.4084 | 1.4097 | 2.1560 | 2.1631 | 1.1034 | 1.1009 | F3 | 1.4097 | 2.4084 | | 2.9567 | 2.0403 | 2.0393 | 3.3480 | 2.5947 | F4 | 2.4084 | 1.4097 | 2.9567 | | 3.3480 | 2.5947 | 2.0403 | 2.0393 | H5 | 1.1034 | 2.1560 | 2.0403 | 3.3480 | | 1.8025 | 2.4251 | 2.5780 | H6 | 1.1009 | 2.1631 | 2.0393 | 2.5947 | 1.8025 | | 2.5780 | 3.0712 | H7 | 2.1560 | 1.1034 | 3.3480 | 2.0403 | 2.4251 | 2.5780 | | 1.8025 | H8 | 2.1631 | 1.1009 | 2.5947 | 2.0393 | 2.5780 | 3.0712 | 1.8025 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
F4 |
110.787 |
|
C1 |
C2 |
H7 |
109.821 |
C1 |
C2 |
H8 |
110.530 |
|
C2 |
C1 |
F3 |
110.787 |
C2 |
C1 |
H5 |
109.821 |
|
C2 |
C1 |
H6 |
110.530 |
F3 |
C1 |
H5 |
107.934 |
|
F3 |
C1 |
H6 |
108.002 |
F4 |
C2 |
H7 |
107.934 |
|
F4 |
C2 |
H8 |
108.002 |
H5 |
C1 |
H6 |
109.709 |
|
H7 |
C2 |
H8 |
109.709 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.118 |
|
|
|
2 |
C |
-0.118 |
|
|
|
3 |
F |
-0.253 |
|
|
|
4 |
F |
-0.253 |
|
|
|
5 |
H |
0.178 |
|
|
|
6 |
H |
0.194 |
|
|
|
7 |
H |
0.178 |
|
|
|
8 |
H |
0.194 |
|
|
|
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 |
2.597 |
2.597 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-21.885 |
1.495 |
0.000 |
y |
1.495 |
-26.444 |
0.000 |
z |
0.000 |
0.000 |
-22.383 |
|
Traceless |
| x | y | z |
x |
2.528 |
1.495 |
0.000 |
y |
1.495 |
-4.309 |
0.000 |
z |
0.000 |
0.000 |
1.781 |
|
Polar |
3z2-r2 | 3.562 |
x2-y2 | 4.559 |
xy | 1.495 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.669 |
0.083 |
0.000 |
y |
0.083 |
3.922 |
0.000 |
z |
0.000 |
0.000 |
3.740 |
<r2> (average value of r
2) Å
2
<r2> |
81.803 |
(<r2>)1/2 |
9.045 |