Jump to
S1C2
Energy calculated at B2PLYP/6-31+G**
| hartrees |
Energy at 0K | -278.066409 |
Energy at 298.15K | |
HF Energy | -277.857962 |
Nuclear repulsion energy | 124.953589 |
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/6-31+G**
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 |
3118 |
2970 |
0.00 |
210.12 |
0.08 |
0.15 |
2 |
Ag |
1544 |
1470 |
0.00 |
12.10 |
0.74 |
0.85 |
3 |
Ag |
1462 |
1393 |
0.00 |
3.80 |
0.67 |
0.80 |
4 |
Ag |
1104 |
1052 |
0.00 |
7.74 |
0.47 |
0.64 |
5 |
Ag |
1046 |
996 |
0.00 |
12.36 |
0.41 |
0.58 |
6 |
Ag |
455 |
433 |
0.00 |
3.06 |
0.41 |
0.58 |
7 |
Au |
3198 |
3046 |
39.65 |
0.00 |
0.00 |
0.00 |
8 |
Au |
1236 |
1177 |
4.44 |
0.00 |
0.00 |
0.00 |
9 |
Au |
825 |
786 |
0.01 |
0.00 |
0.00 |
0.00 |
10 |
Au |
119 |
113 |
16.21 |
0.00 |
0.00 |
0.00 |
11 |
Bg |
3175 |
3024 |
0.00 |
118.80 |
0.75 |
0.86 |
12 |
Bg |
1310 |
1247 |
0.00 |
12.87 |
0.75 |
0.86 |
13 |
Bg |
1183 |
1127 |
0.00 |
3.60 |
0.75 |
0.86 |
14 |
Bu |
3123 |
2975 |
52.24 |
0.00 |
0.08 |
0.00 |
15 |
Bu |
1549 |
1476 |
2.71 |
0.00 |
0.00 |
0.00 |
16 |
Bu |
1368 |
1303 |
11.53 |
0.00 |
0.00 |
0.00 |
17 |
Bu |
1052 |
1002 |
228.25 |
0.00 |
0.00 |
0.00 |
18 |
Bu |
282 |
269 |
23.67 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 13574.3 cm
-1
Scaled (by 0.9524) Zero Point Vibrational Energy (zpe) 12928.2 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/6-31+G**
Point Group is C2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.430 |
0.624 |
0.000 |
C2 |
-0.430 |
-0.624 |
0.000 |
F3 |
-0.430 |
1.734 |
0.000 |
F4 |
0.430 |
-1.734 |
0.000 |
H5 |
1.052 |
0.678 |
0.894 |
H6 |
1.052 |
0.678 |
-0.894 |
H7 |
-1.052 |
-0.678 |
0.894 |
H8 |
-1.052 |
-0.678 |
-0.894 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5162 | 1.4043 | 2.3584 | 1.0902 | 1.0902 | 2.1661 | 2.1661 |
C2 | 1.5162 | | 2.3584 | 1.4043 | 2.1661 | 2.1661 | 1.0902 | 1.0902 | F3 | 1.4043 | 2.3584 | | 3.5735 | 2.0278 | 2.0278 | 2.6465 | 2.6465 | F4 | 2.3584 | 1.4043 | 3.5735 | | 2.6465 | 2.6465 | 2.0278 | 2.0278 | H5 | 1.0902 | 2.1661 | 2.0278 | 2.6465 | | 1.7875 | 2.5034 | 3.0761 | H6 | 1.0902 | 2.1661 | 2.0278 | 2.6465 | 1.7875 | | 3.0761 | 2.5034 | H7 | 2.1661 | 1.0902 | 2.6465 | 2.0278 | 2.5034 | 3.0761 | | 1.7875 | H8 | 2.1661 | 1.0902 | 2.6465 | 2.0278 | 3.0761 | 2.5034 | 1.7875 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
F4 |
107.651 |
|
C1 |
C2 |
H7 |
111.365 |
C1 |
C2 |
H8 |
111.365 |
|
C2 |
C1 |
F3 |
107.651 |
C2 |
C1 |
H5 |
111.365 |
|
C2 |
C1 |
H6 |
111.365 |
F3 |
C1 |
H5 |
108.098 |
|
F3 |
C1 |
H6 |
108.098 |
F4 |
C2 |
H7 |
108.098 |
|
F4 |
C2 |
H8 |
108.098 |
H5 |
C1 |
H6 |
110.119 |
|
H7 |
C2 |
H8 |
110.119 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-31+G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.041 |
|
|
|
2 |
C |
0.041 |
|
|
|
3 |
F |
-0.342 |
|
|
|
4 |
F |
-0.342 |
|
|
|
5 |
H |
0.151 |
|
|
|
6 |
H |
0.151 |
|
|
|
7 |
H |
0.151 |
|
|
|
8 |
H |
0.151 |
|
|
|
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 |
-22.441 |
3.521 |
0.000 |
y |
3.521 |
-30.493 |
0.000 |
z |
0.000 |
0.000 |
-21.823 |
|
Traceless |
| x | y | z |
x |
3.717 |
3.521 |
0.000 |
y |
3.521 |
-8.361 |
0.000 |
z |
0.000 |
0.000 |
4.644 |
|
Polar |
3z2-r2 | 9.288 |
x2-y2 | 8.052 |
xy | 3.521 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.944 |
-0.121 |
0.000 |
y |
-0.121 |
4.085 |
0.000 |
z |
0.000 |
0.000 |
3.621 |
<r2> (average value of r
2) Å
2
<r2> |
89.386 |
(<r2>)1/2 |
9.454 |
Jump to
S1C1
Energy calculated at B2PLYP/6-31+G**
| hartrees |
Energy at 0K | -278.067238 |
Energy at 298.15K | |
HF Energy | -277.858500 |
Nuclear repulsion energy | 127.038506 |
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/6-31+G**
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 |
3164 |
3013 |
9.99 |
100.61 |
0.71 |
0.83 |
2 |
A |
3105 |
2958 |
39.92 |
192.76 |
0.02 |
0.03 |
3 |
A |
1516 |
1444 |
0.66 |
2.25 |
0.72 |
0.84 |
4 |
A |
1454 |
1385 |
15.53 |
2.69 |
0.47 |
0.64 |
5 |
A |
1309 |
1246 |
2.21 |
14.52 |
0.71 |
0.83 |
6 |
A |
1141 |
1087 |
0.36 |
1.46 |
0.23 |
0.37 |
7 |
A |
1111 |
1058 |
87.85 |
5.30 |
0.50 |
0.66 |
8 |
A |
876 |
834 |
33.78 |
6.39 |
0.19 |
0.32 |
9 |
A |
325 |
310 |
0.40 |
0.42 |
0.28 |
0.44 |
10 |
A |
149 |
142 |
4.44 |
0.14 |
0.71 |
0.83 |
11 |
B |
3176 |
3024 |
30.19 |
12.55 |
0.75 |
0.86 |
12 |
B |
3095 |
2948 |
8.27 |
40.24 |
0.75 |
0.86 |
13 |
B |
1514 |
1442 |
7.60 |
11.16 |
0.75 |
0.86 |
14 |
B |
1415 |
1348 |
12.84 |
0.61 |
0.75 |
0.86 |
15 |
B |
1263 |
1203 |
5.20 |
3.77 |
0.75 |
0.86 |
16 |
B |
1081 |
1029 |
51.80 |
4.03 |
0.75 |
0.86 |
17 |
B |
905 |
862 |
52.74 |
3.82 |
0.75 |
0.86 |
18 |
B |
497 |
474 |
18.39 |
0.59 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13547.5 cm
-1
Scaled (by 0.9524) Zero Point Vibrational Energy (zpe) 12902.6 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 B2PLYP/6-31+G**
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.271 |
0.701 |
0.515 |
C2 |
-0.271 |
-0.701 |
0.515 |
F3 |
-0.271 |
1.435 |
-0.548 |
F4 |
0.271 |
-1.435 |
-0.548 |
H5 |
-0.007 |
1.208 |
1.443 |
H6 |
1.356 |
0.701 |
0.398 |
H7 |
0.007 |
-1.208 |
1.443 |
H8 |
-1.356 |
-0.701 |
0.398 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5040 | 1.4008 | 2.3859 | 1.0932 | 1.0910 | 2.1395 | 2.1516 |
C2 | 1.5040 | | 2.3859 | 1.4008 | 2.1395 | 2.1516 | 1.0932 | 1.0910 | F3 | 1.4008 | 2.3859 | | 2.9202 | 2.0207 | 2.0200 | 3.3205 | 2.5756 | F4 | 2.3859 | 1.4008 | 2.9202 | | 3.3205 | 2.5756 | 2.0207 | 2.0200 | H5 | 1.0932 | 2.1395 | 2.0207 | 3.3205 | | 1.7908 | 2.4168 | 2.5609 | H6 | 1.0910 | 2.1516 | 2.0200 | 2.5756 | 1.7908 | | 2.5609 | 3.0532 | H7 | 2.1395 | 1.0932 | 3.3205 | 2.0207 | 2.4168 | 2.5609 | | 1.7908 | H8 | 2.1516 | 1.0910 | 2.5756 | 2.0200 | 2.5609 | 3.0532 | 1.7908 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
F4 |
110.392 |
|
C1 |
C2 |
H7 |
109.916 |
C1 |
C2 |
H8 |
111.023 |
|
C2 |
C1 |
F3 |
110.392 |
C2 |
C1 |
H5 |
109.916 |
|
C2 |
C1 |
H6 |
111.023 |
F3 |
C1 |
H5 |
107.600 |
|
F3 |
C1 |
H6 |
107.677 |
F4 |
C2 |
H7 |
107.600 |
|
F4 |
C2 |
H8 |
107.677 |
H5 |
C1 |
H6 |
110.148 |
|
H7 |
C2 |
H8 |
110.148 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-31+G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.046 |
|
|
|
2 |
C |
0.046 |
|
|
|
3 |
F |
-0.338 |
|
|
|
4 |
F |
-0.338 |
|
|
|
5 |
H |
0.138 |
|
|
|
6 |
H |
0.153 |
|
|
|
7 |
H |
0.138 |
|
|
|
8 |
H |
0.153 |
|
|
|
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 |
3.069 |
3.069 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-22.035 |
1.933 |
0.000 |
y |
1.933 |
-27.082 |
0.000 |
z |
0.000 |
0.000 |
-22.742 |
|
Traceless |
| x | y | z |
x |
2.877 |
1.933 |
0.000 |
y |
1.933 |
-4.693 |
0.000 |
z |
0.000 |
0.000 |
1.816 |
|
Polar |
3z2-r2 | 3.633 |
x2-y2 | 5.047 |
xy | 1.933 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.770 |
-0.003 |
0.000 |
y |
-0.003 |
4.074 |
0.000 |
z |
0.000 |
0.000 |
3.958 |
<r2> (average value of r
2) Å
2
<r2> |
80.773 |
(<r2>)1/2 |
8.987 |