Jump to
S1C2
Energy calculated at B2PLYP/6-311+G(3df,2p)
| hartrees |
Energy at 0K | -377.452309 |
Energy at 298.15K | |
HF Energy | -377.104268 |
Nuclear repulsion energy | 190.852876 |
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/6-311+G(3df,2p)
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 |
3152 |
3152 |
16.42 |
31.36 |
0.67 |
0.80 |
2 |
A |
3115 |
3115 |
18.61 |
87.48 |
0.28 |
0.44 |
3 |
A |
3086 |
3086 |
15.27 |
116.91 |
0.06 |
0.11 |
4 |
A |
1511 |
1511 |
5.82 |
3.69 |
0.75 |
0.86 |
5 |
A |
1462 |
1462 |
11.40 |
1.39 |
0.49 |
0.66 |
6 |
A |
1407 |
1407 |
14.50 |
2.26 |
0.74 |
0.85 |
7 |
A |
1353 |
1353 |
11.48 |
1.40 |
0.75 |
0.86 |
8 |
A |
1277 |
1277 |
12.06 |
3.63 |
0.67 |
0.80 |
9 |
A |
1163 |
1163 |
85.60 |
4.09 |
0.54 |
0.70 |
10 |
A |
1144 |
1144 |
5.75 |
1.86 |
0.29 |
0.45 |
11 |
A |
1104 |
1104 |
270.80 |
0.42 |
0.51 |
0.67 |
12 |
A |
1084 |
1084 |
26.70 |
7.00 |
0.39 |
0.56 |
13 |
A |
914 |
914 |
37.87 |
4.51 |
0.24 |
0.39 |
14 |
A |
579 |
579 |
3.59 |
2.01 |
0.24 |
0.38 |
15 |
A |
480 |
480 |
19.57 |
0.55 |
0.73 |
0.84 |
16 |
A |
427 |
427 |
5.04 |
1.36 |
0.42 |
0.59 |
17 |
A |
245 |
245 |
8.40 |
0.07 |
0.53 |
0.69 |
18 |
A |
119 |
119 |
8.59 |
0.05 |
0.72 |
0.84 |
Unscaled Zero Point Vibrational Energy (zpe) 11810.1 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 11810.1 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/6-311+G(3df,2p)
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.774 |
-0.589 |
-0.286 |
C2 |
0.466 |
0.020 |
0.328 |
F3 |
-1.880 |
0.110 |
0.153 |
F4 |
1.531 |
-0.761 |
-0.006 |
F5 |
0.684 |
1.258 |
-0.182 |
H6 |
-0.716 |
-0.521 |
-1.371 |
H7 |
-0.866 |
-1.627 |
0.026 |
H8 |
0.417 |
0.103 |
1.413 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
F3 |
F4 |
F5 |
H6 |
H7 |
H8 |
C1 | | 1.5111 | 1.3806 | 2.3281 | 2.3549 | 1.0886 | 1.0885 | 2.1868 |
C2 | 1.5111 | | 2.3544 | 1.3626 | 1.3568 | 2.1393 | 2.1394 | 1.0891 | F3 | 1.3806 | 2.3544 | | 3.5246 | 2.8295 | 2.0190 | 2.0156 | 2.6197 | F4 | 2.3281 | 1.3626 | 3.5246 | | 2.1968 | 2.6405 | 2.5490 | 2.0008 | F5 | 2.3549 | 1.3568 | 2.8295 | 2.1968 | | 2.5571 | 3.2818 | 1.9868 | H6 | 1.0886 | 2.1393 | 2.0190 | 2.6405 | 2.5571 | | 1.7888 | 3.0697 | H7 | 1.0885 | 2.1394 | 2.0156 | 2.5490 | 3.2818 | 1.7888 | | 2.5617 | H8 | 2.1868 | 1.0891 | 2.6197 | 2.0008 | 1.9868 | 3.0697 | 2.5617 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
F4 |
108.112 |
|
C1 |
C2 |
F5 |
110.279 |
C1 |
C2 |
H8 |
113.500 |
|
C2 |
C1 |
F3 |
108.931 |
C2 |
C1 |
H6 |
109.680 |
|
C2 |
C1 |
H7 |
109.698 |
F3 |
C1 |
H6 |
109.134 |
|
F3 |
C1 |
H7 |
108.868 |
F4 |
C2 |
F5 |
107.768 |
|
F4 |
C2 |
H8 |
108.882 |
F5 |
C2 |
H8 |
108.144 |
|
H6 |
C1 |
H7 |
110.501 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-311+G(3df,2p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.135 |
|
|
|
2 |
C |
0.741 |
|
|
|
3 |
F |
-0.450 |
|
|
|
4 |
F |
-0.454 |
|
|
|
5 |
F |
-0.457 |
|
|
|
6 |
H |
0.167 |
|
|
|
7 |
H |
0.161 |
|
|
|
8 |
H |
0.159 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.294 |
-1.521 |
0.384 |
1.596 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-32.995 |
1.767 |
1.609 |
y |
1.767 |
-28.342 |
0.536 |
z |
1.609 |
0.536 |
-25.075 |
|
Traceless |
| x | y | z |
x |
-6.286 |
1.767 |
1.609 |
y |
1.767 |
0.693 |
0.536 |
z |
1.609 |
0.536 |
5.593 |
|
Polar |
3z2-r2 | 11.186 |
x2-y2 | -4.653 |
xy | 1.767 |
xz | 1.609 |
yz | 0.536 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
4.554 |
-0.070 |
-0.026 |
y |
-0.070 |
4.386 |
0.056 |
z |
-0.026 |
0.056 |
4.094 |
<r2> (average value of r
2) Å
2
<r2> |
111.552 |
(<r2>)1/2 |
10.562 |
Jump to
S1C1
Energy calculated at B2PLYP/6-311+G(3df,2p)
| hartrees |
Energy at 0K | -377.450262 |
Energy at 298.15K | |
HF Energy | -377.102238 |
Nuclear repulsion energy | 193.620066 |
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/6-311+G(3df,2p)
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' |
3087 |
3087 |
50.37 |
134.52 |
0.05 |
0.09 |
2 |
A' |
3071 |
3071 |
2.72 |
60.94 |
0.30 |
0.46 |
3 |
A' |
1505 |
1505 |
6.88 |
3.56 |
0.74 |
0.85 |
4 |
A' |
1441 |
1441 |
12.79 |
1.80 |
0.27 |
0.42 |
5 |
A' |
1421 |
1421 |
20.61 |
1.88 |
0.61 |
0.76 |
6 |
A' |
1189 |
1189 |
119.09 |
4.40 |
0.17 |
0.30 |
7 |
A' |
1105 |
1105 |
27.99 |
3.43 |
0.75 |
0.86 |
8 |
A' |
879 |
879 |
32.40 |
7.54 |
0.10 |
0.18 |
9 |
A' |
763 |
763 |
52.51 |
2.46 |
0.44 |
0.61 |
10 |
A' |
517 |
517 |
11.86 |
1.08 |
0.74 |
0.85 |
11 |
A' |
238 |
238 |
1.57 |
0.21 |
0.36 |
0.53 |
12 |
A" |
3132 |
3132 |
12.84 |
47.22 |
0.75 |
0.86 |
13 |
A" |
1397 |
1397 |
18.90 |
1.13 |
0.75 |
0.86 |
14 |
A" |
1294 |
1294 |
17.09 |
6.41 |
0.75 |
0.86 |
15 |
A" |
1138 |
1138 |
115.38 |
1.38 |
0.75 |
0.86 |
16 |
A" |
957 |
957 |
75.87 |
2.37 |
0.75 |
0.86 |
17 |
A" |
371 |
371 |
0.41 |
0.23 |
0.75 |
0.86 |
18 |
A" |
119 |
119 |
2.07 |
0.09 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 11812.0 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 11812.0 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/6-311+G(3df,2p)
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.738 |
-0.833 |
0.000 |
C2 |
0.357 |
0.628 |
0.000 |
F3 |
-0.387 |
-1.623 |
0.000 |
F4 |
-0.387 |
0.926 |
1.096 |
F5 |
-0.387 |
0.926 |
-1.096 |
H6 |
1.323 |
-1.052 |
-0.893 |
H7 |
1.323 |
-1.052 |
0.893 |
H8 |
1.241 |
1.270 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
F3 |
F4 |
F5 |
H6 |
H7 |
H8 |
C1 | | 1.5103 | 1.3746 | 2.3582 | 2.3582 | 1.0898 | 1.0898 | 2.1627 |
C2 | 1.5103 | | 2.3711 | 1.3579 | 1.3579 | 2.1341 | 2.1341 | 1.0919 | F3 | 1.3746 | 2.3711 | | 2.7740 | 2.7740 | 2.0120 | 2.0120 | 3.3196 | F4 | 2.3582 | 1.3579 | 2.7740 | | 2.1915 | 3.2852 | 2.6228 | 1.9925 | F5 | 2.3582 | 1.3579 | 2.7740 | 2.1915 | | 2.6228 | 3.2852 | 1.9925 | H6 | 1.0898 | 2.1341 | 2.0120 | 3.2852 | 2.6228 | | 1.7860 | 2.4897 | H7 | 1.0898 | 2.1341 | 2.0120 | 2.6228 | 3.2852 | 1.7860 | | 2.4897 | H8 | 2.1627 | 1.0919 | 3.3196 | 1.9925 | 1.9925 | 2.4897 | 2.4897 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
F4 |
110.494 |
|
C1 |
C2 |
F5 |
110.494 |
C1 |
C2 |
H8 |
111.415 |
|
C2 |
C1 |
F3 |
110.457 |
C2 |
C1 |
H6 |
109.254 |
|
C2 |
C1 |
H7 |
109.254 |
F3 |
C1 |
H6 |
108.906 |
|
F3 |
C1 |
H7 |
108.906 |
F4 |
C2 |
F5 |
107.596 |
|
F4 |
C2 |
H8 |
108.361 |
F5 |
C2 |
H8 |
108.361 |
|
H6 |
C1 |
H7 |
110.053 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-311+G(3df,2p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.115 |
|
|
|
2 |
C |
0.783 |
|
|
|
3 |
F |
-0.461 |
|
|
|
4 |
F |
-0.455 |
|
|
|
5 |
F |
-0.455 |
|
|
|
6 |
H |
0.160 |
|
|
|
7 |
H |
0.160 |
|
|
|
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 |
|
3.276 |
0.074 |
0.000 |
3.276 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-25.611 |
-0.373 |
-0.007 |
y |
-0.373 |
-29.222 |
-0.000 |
z |
-0.007 |
-0.000 |
-29.034 |
|
Traceless |
| x | y | z |
x |
3.517 |
-0.373 |
-0.007 |
y |
-0.373 |
-1.900 |
-0.000 |
z |
-0.007 |
-0.000 |
-1.617 |
|
Polar |
3z2-r2 | -3.234 |
x2-y2 | 3.611 |
xy | -0.373 |
xz | -0.007 |
yz | -0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
4.338 |
-0.015 |
0.001 |
y |
-0.015 |
4.415 |
-0.000 |
z |
0.001 |
-0.000 |
4.301 |
<r2> (average value of r
2) Å
2
<r2> |
103.279 |
(<r2>)1/2 |
10.163 |