Jump to
S1C2
Energy calculated at B2PLYP/6-31G(2df,p)
| hartrees |
Energy at 0K | -278.093125 |
Energy at 298.15K | |
HF Energy | -277.847262 |
Nuclear repulsion energy | 126.104586 |
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 B2PLYP/6-31G(2df,p)
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 |
2935 |
0.00 |
181.97 |
0.09 |
0.16 |
2 |
Ag |
1539 |
1469 |
0.00 |
17.25 |
0.72 |
0.84 |
3 |
Ag |
1475 |
1409 |
0.00 |
2.39 |
0.66 |
0.79 |
4 |
Ag |
1107 |
1058 |
0.00 |
8.64 |
0.69 |
0.82 |
5 |
Ag |
1094 |
1045 |
0.00 |
6.55 |
0.18 |
0.30 |
6 |
Ag |
465 |
444 |
0.00 |
2.51 |
0.46 |
0.63 |
7 |
Au |
3145 |
3004 |
61.01 |
0.00 |
0.00 |
0.00 |
8 |
Au |
1252 |
1195 |
3.82 |
0.00 |
0.00 |
0.00 |
9 |
Au |
818 |
782 |
0.06 |
0.00 |
0.00 |
0.00 |
10 |
Au |
128 |
122 |
10.40 |
0.00 |
0.00 |
0.00 |
11 |
Bg |
3119 |
2979 |
0.00 |
111.13 |
0.75 |
0.86 |
12 |
Bg |
1312 |
1253 |
0.00 |
14.93 |
0.75 |
0.86 |
13 |
Bg |
1202 |
1148 |
0.00 |
3.74 |
0.75 |
0.86 |
14 |
Bu |
3079 |
2941 |
59.98 |
0.00 |
0.08 |
0.16 |
15 |
Bu |
1550 |
1480 |
2.15 |
0.00 |
0.00 |
0.00 |
16 |
Bu |
1384 |
1322 |
14.31 |
0.00 |
0.00 |
0.00 |
17 |
Bu |
1117 |
1067 |
175.95 |
0.00 |
0.00 |
0.00 |
18 |
Bu |
272 |
260 |
15.41 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 13566.2 cm
-1
Scaled (by 0.955) Zero Point Vibrational Energy (zpe) 12955.7 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 B2PLYP/6-31G(2df,p)
Point Group is C2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.422 |
0.631 |
0.000 |
C2 |
-0.422 |
-0.631 |
0.000 |
F3 |
-0.422 |
1.717 |
0.000 |
F4 |
0.422 |
-1.717 |
0.000 |
H5 |
1.057 |
0.665 |
0.890 |
H6 |
1.057 |
0.665 |
-0.890 |
H7 |
-1.057 |
-0.665 |
0.890 |
H8 |
-1.057 |
-0.665 |
-0.890 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5179 | 1.3762 | 2.3475 | 1.0934 | 1.0934 | 2.1580 | 2.1580 |
C2 | 1.5179 | | 2.3475 | 1.3762 | 2.1580 | 2.1580 | 1.0934 | 1.0934 | F3 | 1.3762 | 2.3475 | | 3.5363 | 2.0217 | 2.0217 | 2.6203 | 2.6203 | F4 | 2.3475 | 1.3762 | 3.5363 | | 2.6203 | 2.6203 | 2.0217 | 2.0217 | H5 | 1.0934 | 2.1580 | 2.0217 | 2.6203 | | 1.7795 | 2.4968 | 3.0661 | H6 | 1.0934 | 2.1580 | 2.0217 | 2.6203 | 1.7795 | | 3.0661 | 2.4968 | H7 | 2.1580 | 1.0934 | 2.6203 | 2.0217 | 2.4968 | 3.0661 | | 1.7795 | H8 | 2.1580 | 1.0934 | 2.6203 | 2.0217 | 3.0661 | 2.4968 | 1.7795 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
F4 |
108.322 |
|
C1 |
C2 |
H7 |
110.413 |
C1 |
C2 |
H8 |
110.413 |
|
C2 |
C1 |
F3 |
108.322 |
C2 |
C1 |
H5 |
110.413 |
|
C2 |
C1 |
H6 |
110.413 |
F3 |
C1 |
H5 |
109.368 |
|
F3 |
C1 |
H6 |
109.368 |
F4 |
C2 |
H7 |
109.368 |
|
F4 |
C2 |
H8 |
109.368 |
H5 |
C1 |
H6 |
108.937 |
|
H7 |
C2 |
H8 |
108.937 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-31G(2df,p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.071 |
|
|
|
2 |
C |
-0.071 |
|
|
|
3 |
F |
-0.178 |
|
|
|
4 |
F |
-0.178 |
|
|
|
5 |
H |
0.125 |
|
|
|
6 |
H |
0.125 |
|
|
|
7 |
H |
0.125 |
|
|
|
8 |
H |
0.125 |
|
|
|
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 |
-21.794 |
2.578 |
0.000 |
y |
2.578 |
-27.994 |
0.000 |
z |
0.000 |
0.000 |
-21.295 |
|
Traceless |
| x | y | z |
x |
2.851 |
2.578 |
0.000 |
y |
2.578 |
-6.449 |
0.000 |
z |
0.000 |
0.000 |
3.599 |
|
Polar |
3z2-r2 | 7.198 |
x2-y2 | 6.200 |
xy | 2.578 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.730 |
0.011 |
0.000 |
y |
0.011 |
3.767 |
0.000 |
z |
0.000 |
0.000 |
3.567 |
<r2> (average value of r
2) Å
2
<r2> |
87.387 |
(<r2>)1/2 |
9.348 |
Jump to
S1C1
Energy calculated at B2PLYP/6-31G(2df,p)
| hartrees |
Energy at 0K | -278.094103 |
Energy at 298.15K | |
HF Energy | -277.847908 |
Nuclear repulsion energy | 128.457997 |
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 B2PLYP/6-31G(2df,p)
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 |
2974 |
20.92 |
85.92 |
0.75 |
0.86 |
2 |
A |
3067 |
2929 |
34.80 |
161.02 |
0.03 |
0.06 |
3 |
A |
1520 |
1451 |
0.39 |
2.17 |
0.63 |
0.77 |
4 |
A |
1462 |
1396 |
14.64 |
3.50 |
0.62 |
0.77 |
5 |
A |
1319 |
1260 |
1.71 |
16.38 |
0.71 |
0.83 |
6 |
A |
1158 |
1105 |
27.37 |
1.70 |
0.14 |
0.24 |
7 |
A |
1141 |
1089 |
54.41 |
3.58 |
0.75 |
0.85 |
8 |
A |
892 |
851 |
18.35 |
6.37 |
0.23 |
0.37 |
9 |
A |
321 |
307 |
0.32 |
0.20 |
0.32 |
0.48 |
10 |
A |
145 |
138 |
2.75 |
0.04 |
0.75 |
0.86 |
11 |
B |
3127 |
2986 |
46.50 |
13.55 |
0.75 |
0.86 |
12 |
B |
3058 |
2920 |
14.59 |
34.06 |
0.75 |
0.86 |
13 |
B |
1515 |
1447 |
6.72 |
12.21 |
0.75 |
0.86 |
14 |
B |
1432 |
1368 |
10.28 |
1.12 |
0.75 |
0.86 |
15 |
B |
1281 |
1224 |
5.52 |
4.57 |
0.75 |
0.86 |
16 |
B |
1120 |
1069 |
38.45 |
2.79 |
0.75 |
0.86 |
17 |
B |
922 |
880 |
32.96 |
3.16 |
0.75 |
0.86 |
18 |
B |
498 |
476 |
13.39 |
0.43 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13545.5 cm
-1
Scaled (by 0.955) Zero Point Vibrational Energy (zpe) 12936.0 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 B2PLYP/6-31G(2df,p)
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.260 |
0.708 |
0.516 |
C2 |
-0.260 |
-0.708 |
0.516 |
F3 |
-0.260 |
1.398 |
-0.553 |
F4 |
0.260 |
-1.398 |
-0.553 |
H5 |
-0.034 |
1.209 |
1.444 |
H6 |
1.351 |
0.706 |
0.438 |
H7 |
0.034 |
-1.209 |
1.444 |
H8 |
-1.351 |
-0.706 |
0.438 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5073 | 1.3747 | 2.3616 | 1.0953 | 1.0941 | 2.1416 | 2.1442 |
C2 | 1.5073 | | 2.3616 | 1.3747 | 2.1416 | 2.1442 | 1.0953 | 1.0941 | F3 | 1.3747 | 2.3616 | | 2.8440 | 2.0191 | 2.0138 | 3.2978 | 2.5694 | F4 | 2.3616 | 1.3747 | 2.8440 | | 3.2978 | 2.5694 | 2.0191 | 2.0138 | H5 | 1.0953 | 2.1416 | 2.0191 | 3.2978 | | 1.7843 | 2.4196 | 2.5326 | H6 | 1.0941 | 2.1442 | 2.0138 | 2.5694 | 1.7843 | | 2.5326 | 3.0485 | H7 | 2.1416 | 1.0953 | 3.2978 | 2.0191 | 2.4196 | 2.5326 | | 1.7843 | H8 | 2.1442 | 1.0941 | 2.5694 | 2.0138 | 2.5326 | 3.0485 | 1.7843 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
F4 |
109.972 |
|
C1 |
C2 |
H7 |
109.738 |
C1 |
C2 |
H8 |
110.014 |
|
C2 |
C1 |
F3 |
109.972 |
C2 |
C1 |
H5 |
109.738 |
|
C2 |
C1 |
H6 |
110.014 |
F3 |
C1 |
H5 |
109.133 |
|
F3 |
C1 |
H6 |
108.784 |
F4 |
C2 |
H7 |
109.133 |
|
F4 |
C2 |
H8 |
108.784 |
H5 |
C1 |
H6 |
109.176 |
|
H7 |
C2 |
H8 |
109.176 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-31G(2df,p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.057 |
|
|
|
2 |
C |
-0.057 |
|
|
|
3 |
F |
-0.180 |
|
|
|
4 |
F |
-0.180 |
|
|
|
5 |
H |
0.112 |
|
|
|
6 |
H |
0.126 |
|
|
|
7 |
H |
0.112 |
|
|
|
8 |
H |
0.126 |
|
|
|
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 |
2.391 |
2.391 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-21.451 |
1.364 |
0.000 |
y |
1.364 |
-25.297 |
0.000 |
z |
0.000 |
0.000 |
-22.028 |
|
Traceless |
| x | y | z |
x |
2.211 |
1.364 |
0.000 |
y |
1.364 |
-3.558 |
0.000 |
z |
0.000 |
0.000 |
1.346 |
|
Polar |
3z2-r2 | 2.693 |
x2-y2 | 3.846 |
xy | 1.364 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.632 |
0.037 |
0.000 |
y |
0.037 |
3.823 |
0.000 |
z |
0.000 |
0.000 |
3.715 |
<r2> (average value of r
2) Å
2
<r2> |
78.371 |
(<r2>)1/2 |
8.853 |