Jump to
S1C2
Energy calculated at B2PLYP/6-31G
| hartrees |
Energy at 0K | -216.801350 |
Energy at 298.15K | |
HF Energy | -216.670121 |
Nuclear repulsion energy | 115.031647 |
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
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' |
3295 |
3295 |
8.81 |
49.55 |
0.73 |
0.84 |
2 |
A' |
3205 |
3205 |
6.48 |
136.24 |
0.11 |
0.20 |
3 |
A' |
3182 |
3182 |
11.45 |
43.52 |
0.52 |
0.69 |
4 |
A' |
3074 |
3074 |
35.38 |
151.30 |
0.12 |
0.21 |
5 |
A' |
1732 |
1732 |
2.05 |
8.05 |
0.10 |
0.18 |
6 |
A' |
1565 |
1565 |
0.95 |
23.78 |
0.62 |
0.76 |
7 |
A' |
1499 |
1499 |
4.92 |
10.29 |
0.49 |
0.66 |
8 |
A' |
1433 |
1433 |
10.47 |
12.08 |
0.62 |
0.77 |
9 |
A' |
1359 |
1359 |
0.11 |
17.45 |
0.42 |
0.60 |
10 |
A' |
1131 |
1131 |
11.06 |
2.62 |
0.74 |
0.85 |
11 |
A' |
1001 |
1001 |
40.78 |
5.54 |
0.74 |
0.85 |
12 |
A' |
918 |
918 |
8.26 |
6.02 |
0.15 |
0.26 |
13 |
A' |
602 |
602 |
5.32 |
2.11 |
0.75 |
0.86 |
14 |
A' |
276 |
276 |
4.63 |
1.05 |
0.56 |
0.72 |
15 |
A" |
3122 |
3122 |
36.17 |
92.95 |
0.75 |
0.86 |
16 |
A" |
1243 |
1243 |
0.12 |
13.86 |
0.75 |
0.86 |
17 |
A" |
1078 |
1078 |
7.23 |
0.98 |
0.75 |
0.86 |
18 |
A" |
1040 |
1040 |
21.18 |
0.05 |
0.75 |
0.86 |
19 |
A" |
988 |
988 |
46.82 |
0.64 |
0.75 |
0.86 |
20 |
A" |
581 |
581 |
11.21 |
13.76 |
0.75 |
0.86 |
21 |
A" |
157 |
157 |
4.38 |
6.31 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 16241.3 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 16241.3 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 B2PLYP/6-31G
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.965 |
-0.177 |
0.000 |
C2 |
0.000 |
0.972 |
0.000 |
C3 |
1.332 |
0.834 |
0.000 |
F4 |
-0.257 |
-1.438 |
0.000 |
H5 |
1.991 |
1.695 |
0.000 |
H6 |
1.793 |
-0.146 |
0.000 |
H7 |
-0.465 |
1.957 |
0.000 |
H8 |
-1.603 |
-0.169 |
0.890 |
H9 |
-1.603 |
-0.169 |
-0.890 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
C1 | | 1.5006 | 2.5102 | 1.4461 | 3.4993 | 2.7587 | 2.1916 | 1.0953 | 1.0953 |
C2 | 1.5006 | | 1.3392 | 2.4234 | 2.1183 | 2.1133 | 1.0889 | 2.1598 | 2.1598 | C3 | 2.5102 | 1.3392 | | 2.7728 | 1.0841 | 1.0837 | 2.1185 | 3.2274 | 3.2274 | F4 | 1.4461 | 2.4234 | 2.7728 | | 3.8562 | 2.4231 | 3.4008 | 2.0531 | 2.0531 | H5 | 3.4993 | 2.1183 | 1.0841 | 3.8562 | | 1.8522 | 2.4696 | 4.1457 | 4.1457 | H6 | 2.7587 | 2.1133 | 1.0837 | 2.4231 | 1.8522 | | 3.0856 | 3.5113 | 3.5113 | H7 | 2.1916 | 1.0889 | 2.1185 | 3.4008 | 2.4696 | 3.0856 | | 2.5703 | 2.5703 | H8 | 1.0953 | 2.1598 | 3.2274 | 2.0531 | 4.1457 | 3.5113 | 2.5703 | | 1.7804 | H9 | 1.0953 | 2.1598 | 3.2274 | 2.0531 | 4.1457 | 3.5113 | 2.5703 | 1.7804 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
C3 |
124.141 |
|
C1 |
C2 |
H7 |
114.698 |
C2 |
C1 |
F4 |
110.639 |
|
C2 |
C1 |
H8 |
111.656 |
C2 |
C1 |
H9 |
111.656 |
|
C2 |
C3 |
H5 |
121.532 |
C2 |
C3 |
H6 |
121.075 |
|
C3 |
C2 |
H7 |
121.162 |
F4 |
C1 |
H8 |
106.967 |
|
F4 |
C1 |
H9 |
106.967 |
H5 |
C3 |
H6 |
117.393 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-31G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.034 |
|
|
|
2 |
C |
-0.133 |
|
|
|
3 |
C |
-0.278 |
|
|
|
4 |
F |
-0.367 |
|
|
|
5 |
H |
0.134 |
|
|
|
6 |
H |
0.159 |
|
|
|
7 |
H |
0.140 |
|
|
|
8 |
H |
0.155 |
|
|
|
9 |
H |
0.155 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-1.015 |
1.878 |
0.000 |
2.134 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-20.672 |
-0.335 |
0.009 |
y |
-0.335 |
-25.949 |
-0.003 |
z |
0.009 |
-0.003 |
-24.956 |
|
Traceless |
| x | y | z |
x |
4.780 |
-0.335 |
0.009 |
y |
-0.335 |
-3.135 |
-0.003 |
z |
0.009 |
-0.003 |
-1.645 |
|
Polar |
3z2-r2 | -3.290 |
x2-y2 | 5.276 |
xy | -0.335 |
xz | 0.009 |
yz | -0.003 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
6.297 |
0.106 |
-0.002 |
y |
0.106 |
4.445 |
0.000 |
z |
-0.002 |
0.000 |
2.582 |
<r2> (average value of r
2) Å
2
<r2> |
81.276 |
(<r2>)1/2 |
9.015 |
Jump to
S1C1
Energy calculated at B2PLYP/6-31G
| hartrees |
Energy at 0K | -216.800530 |
Energy at 298.15K | |
HF Energy | -216.669244 |
Nuclear repulsion energy | 112.543623 |
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
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 |
3274 |
3274 |
18.39 |
61.46 |
0.57 |
0.72 |
2 |
A |
3207 |
3207 |
7.57 |
97.31 |
0.26 |
0.41 |
3 |
A |
3180 |
3180 |
10.19 |
67.80 |
0.12 |
0.21 |
4 |
A |
3146 |
3146 |
28.03 |
69.17 |
0.75 |
0.85 |
5 |
A |
3087 |
3087 |
33.85 |
115.33 |
0.11 |
0.19 |
6 |
A |
1725 |
1725 |
0.41 |
10.42 |
0.12 |
0.21 |
7 |
A |
1568 |
1568 |
1.53 |
11.96 |
0.68 |
0.81 |
8 |
A |
1514 |
1514 |
11.06 |
13.38 |
0.51 |
0.68 |
9 |
A |
1418 |
1418 |
16.04 |
6.77 |
0.75 |
0.86 |
10 |
A |
1360 |
1360 |
0.12 |
15.34 |
0.46 |
0.63 |
11 |
A |
1267 |
1267 |
3.48 |
17.53 |
0.73 |
0.84 |
12 |
A |
1201 |
1201 |
0.90 |
4.77 |
0.69 |
0.82 |
13 |
A |
1057 |
1057 |
19.04 |
1.01 |
0.68 |
0.81 |
14 |
A |
1014 |
1014 |
5.34 |
0.82 |
0.33 |
0.49 |
15 |
A |
1004 |
1004 |
51.05 |
6.10 |
0.63 |
0.77 |
16 |
A |
992 |
992 |
67.80 |
0.40 |
0.23 |
0.38 |
17 |
A |
942 |
942 |
22.07 |
7.57 |
0.24 |
0.38 |
18 |
A |
660 |
660 |
7.45 |
8.36 |
0.67 |
0.81 |
19 |
A |
441 |
441 |
2.30 |
4.79 |
0.47 |
0.64 |
20 |
A |
321 |
321 |
9.06 |
5.37 |
0.75 |
0.86 |
21 |
A |
105 |
105 |
1.64 |
7.03 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 16240.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 16240.9 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
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.589 |
0.471 |
0.301 |
C2 |
0.650 |
-0.366 |
0.261 |
C3 |
1.825 |
0.068 |
-0.220 |
F4 |
-1.684 |
-0.252 |
-0.329 |
H5 |
2.714 |
-0.553 |
-0.204 |
H6 |
1.939 |
1.062 |
-0.644 |
H7 |
0.554 |
-1.367 |
0.674 |
H8 |
-0.914 |
0.678 |
1.325 |
H9 |
-0.462 |
1.412 |
-0.240 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
C1 | | 1.4956 | 2.5022 | 1.4551 | 3.4949 | 2.7622 | 2.1961 | 1.0942 | 1.0931 |
C2 | 1.4956 | | 1.3416 | 2.4097 | 2.1242 | 2.1255 | 1.0872 | 2.1602 | 2.1565 | C3 | 2.5022 | 1.3416 | | 3.5251 | 1.0845 | 1.0870 | 2.1149 | 3.2030 | 2.6534 | F4 | 1.4551 | 2.4097 | 3.5251 | | 4.4099 | 3.8660 | 2.6933 | 2.0473 | 2.0666 | H5 | 3.4949 | 2.1242 | 1.0845 | 4.4099 | | 1.8450 | 2.4699 | 4.1250 | 3.7355 | H6 | 2.7622 | 2.1255 | 1.0870 | 3.8660 | 1.8450 | | 3.0909 | 3.4871 | 2.4595 | H7 | 2.1961 | 1.0872 | 2.1149 | 2.6933 | 2.4699 | 3.0909 | | 2.5998 | 3.0972 | H8 | 1.0942 | 2.1602 | 3.2030 | 2.0473 | 4.1250 | 3.4871 | 2.5998 | | 1.7867 | H9 | 1.0931 | 2.1565 | 2.6534 | 2.0666 | 3.7355 | 2.4595 | 3.0972 | 1.7867 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
C3 |
123.663 |
|
C1 |
C2 |
H7 |
115.583 |
C2 |
C1 |
F4 |
109.493 |
|
C2 |
C1 |
H8 |
112.125 |
C2 |
C1 |
H9 |
111.882 |
|
C2 |
C3 |
H5 |
121.865 |
C2 |
C3 |
H6 |
121.786 |
|
C3 |
C2 |
H7 |
120.740 |
F4 |
C1 |
H8 |
105.983 |
|
F4 |
C1 |
H9 |
107.541 |
H5 |
C3 |
H6 |
116.350 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-31G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.015 |
|
|
|
2 |
C |
-0.087 |
|
|
|
3 |
C |
-0.292 |
|
|
|
4 |
F |
-0.372 |
|
|
|
5 |
H |
0.145 |
|
|
|
6 |
H |
0.137 |
|
|
|
7 |
H |
0.155 |
|
|
|
8 |
H |
0.151 |
|
|
|
9 |
H |
0.147 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
1.918 |
0.989 |
1.002 |
2.379 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-26.343 |
-1.422 |
-1.969 |
y |
-1.422 |
-22.392 |
-0.936 |
z |
-1.969 |
-0.936 |
-24.476 |
|
Traceless |
| x | y | z |
x |
-2.909 |
-1.422 |
-1.969 |
y |
-1.422 |
3.017 |
-0.936 |
z |
-1.969 |
-0.936 |
-0.108 |
|
Polar |
3z2-r2 | -0.217 |
x2-y2 | -3.951 |
xy | -1.422 |
xz | -1.969 |
yz | -0.936 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
6.173 |
0.228 |
-0.873 |
y |
0.228 |
4.185 |
-0.605 |
z |
-0.873 |
-0.605 |
3.098 |
<r2> (average value of r
2) Å
2
<r2> |
91.263 |
(<r2>)1/2 |
9.553 |