Jump to
S1C2
Energy calculated at B1B95/Def2TZVPP
| hartrees |
Energy at 0K | -217.137389 |
Energy at 298.15K | |
HF Energy | -217.137389 |
Nuclear repulsion energy | 117.140293 |
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 B1B95/Def2TZVPP
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' |
3271 |
3271 |
4.12 |
52.12 |
0.70 |
0.83 |
2 |
A' |
3183 |
3183 |
4.24 |
175.71 |
0.12 |
0.22 |
3 |
A' |
3170 |
3170 |
9.00 |
27.56 |
0.73 |
0.85 |
4 |
A' |
3043 |
3043 |
33.50 |
184.72 |
0.10 |
0.18 |
5 |
A' |
1739 |
1739 |
5.75 |
29.91 |
0.09 |
0.16 |
6 |
A' |
1494 |
1494 |
5.15 |
13.66 |
0.53 |
0.70 |
7 |
A' |
1450 |
1450 |
6.61 |
10.06 |
0.44 |
0.61 |
8 |
A' |
1415 |
1415 |
10.52 |
4.84 |
0.75 |
0.86 |
9 |
A' |
1318 |
1318 |
0.18 |
17.55 |
0.26 |
0.42 |
10 |
A' |
1150 |
1150 |
61.51 |
1.75 |
0.75 |
0.86 |
11 |
A' |
1019 |
1019 |
34.45 |
5.05 |
0.66 |
0.80 |
12 |
A' |
923 |
923 |
1.23 |
4.45 |
0.06 |
0.12 |
13 |
A' |
616 |
616 |
6.49 |
1.67 |
0.72 |
0.84 |
14 |
A' |
266 |
266 |
2.09 |
1.17 |
0.51 |
0.68 |
15 |
A" |
3079 |
3079 |
22.22 |
89.63 |
0.75 |
0.86 |
16 |
A" |
1271 |
1271 |
0.01 |
5.86 |
0.75 |
0.86 |
17 |
A" |
1048 |
1048 |
12.54 |
1.27 |
0.75 |
0.86 |
18 |
A" |
1025 |
1025 |
6.37 |
0.02 |
0.75 |
0.86 |
19 |
A" |
967 |
967 |
47.77 |
1.38 |
0.75 |
0.86 |
20 |
A" |
564 |
564 |
10.93 |
3.33 |
0.75 |
0.86 |
21 |
A" |
184 |
184 |
3.00 |
1.88 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 16096.1 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 16096.1 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 B1B95/Def2TZVPP
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.937 |
-0.205 |
0.000 |
C2 |
0.000 |
0.947 |
0.000 |
C3 |
1.317 |
0.844 |
0.000 |
F4 |
-0.265 |
-1.407 |
0.000 |
H5 |
1.945 |
1.721 |
0.000 |
H6 |
1.798 |
-0.122 |
0.000 |
H7 |
-0.478 |
1.920 |
0.000 |
H8 |
-1.579 |
-0.182 |
0.883 |
H9 |
-1.579 |
-0.182 |
-0.883 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
C1 | | 1.4852 | 2.4853 | 1.3770 | 3.4660 | 2.7361 | 2.1739 | 1.0923 | 1.0923 |
C2 | 1.4852 | | 1.3206 | 2.3696 | 2.0929 | 2.0923 | 1.0837 | 2.1330 | 2.1330 | C3 | 2.4853 | 1.3206 | | 2.7511 | 1.0791 | 1.0794 | 2.0927 | 3.1965 | 3.1965 | F4 | 1.3770 | 2.3696 | 2.7511 | | 3.8301 | 2.4306 | 3.3340 | 2.0019 | 2.0019 | H5 | 3.4660 | 2.0929 | 1.0791 | 3.8301 | | 1.8493 | 2.4311 | 4.1013 | 4.1013 | H6 | 2.7361 | 2.0923 | 1.0794 | 2.4306 | 1.8493 | | 3.0582 | 3.4914 | 3.4914 | H7 | 2.1739 | 1.0837 | 2.0927 | 3.3340 | 2.4311 | 3.0582 | | 2.5319 | 2.5319 | H8 | 1.0923 | 2.1330 | 3.1965 | 2.0019 | 4.1013 | 3.4914 | 2.5319 | | 1.7660 | H9 | 1.0923 | 2.1330 | 3.1965 | 2.0019 | 4.1013 | 3.4914 | 2.5319 | 1.7660 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
C3 |
124.591 |
|
C1 |
C2 |
H7 |
114.714 |
C2 |
C1 |
F4 |
111.711 |
|
C2 |
C1 |
H8 |
110.773 |
C2 |
C1 |
H9 |
110.773 |
|
C2 |
C3 |
H5 |
121.091 |
C2 |
C3 |
H6 |
121.006 |
|
C3 |
C2 |
H7 |
120.695 |
F4 |
C1 |
H8 |
107.776 |
|
F4 |
C1 |
H9 |
107.776 |
H5 |
C3 |
H6 |
117.903 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/Def2TZVPP
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.117 |
|
|
|
2 |
C |
-0.141 |
|
|
|
3 |
C |
-0.213 |
|
|
|
4 |
F |
-0.235 |
|
|
|
5 |
H |
0.100 |
|
|
|
6 |
H |
0.103 |
|
|
|
7 |
H |
0.095 |
|
|
|
8 |
H |
0.087 |
|
|
|
9 |
H |
0.087 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.902 |
1.464 |
0.000 |
1.720 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-21.191 |
-0.300 |
0.000 |
y |
-0.300 |
-25.268 |
0.000 |
z |
0.000 |
0.000 |
-25.115 |
|
Traceless |
| x | y | z |
x |
4.001 |
-0.300 |
0.000 |
y |
-0.300 |
-2.115 |
0.000 |
z |
0.000 |
0.000 |
-1.886 |
|
Polar |
3z2-r2 | -3.772 |
x2-y2 | 4.077 |
xy | -0.300 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
7.227 |
0.322 |
0.000 |
y |
0.322 |
5.250 |
0.000 |
z |
0.000 |
0.000 |
4.148 |
<r2> (average value of r
2) Å
2
<r2> |
79.451 |
(<r2>)1/2 |
8.914 |
Jump to
S1C1
Energy calculated at B1B95/Def2TZVPP
| hartrees |
Energy at 0K | -217.136654 |
Energy at 298.15K | |
HF Energy | -217.136654 |
Nuclear repulsion energy | 114.780874 |
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 B1B95/Def2TZVPP
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 |
3252 |
3252 |
10.01 |
61.81 |
0.59 |
0.74 |
2 |
A |
3181 |
3181 |
5.77 |
118.22 |
0.23 |
0.37 |
3 |
A |
3160 |
3160 |
8.52 |
75.75 |
0.12 |
0.21 |
4 |
A |
3110 |
3110 |
20.91 |
69.54 |
0.69 |
0.82 |
5 |
A |
3055 |
3055 |
31.47 |
138.50 |
0.09 |
0.16 |
6 |
A |
1736 |
1736 |
0.60 |
30.57 |
0.10 |
0.19 |
7 |
A |
1503 |
1503 |
3.51 |
5.02 |
0.63 |
0.77 |
8 |
A |
1462 |
1462 |
18.82 |
9.32 |
0.55 |
0.71 |
9 |
A |
1392 |
1392 |
12.78 |
3.95 |
0.35 |
0.52 |
10 |
A |
1317 |
1317 |
0.09 |
13.63 |
0.34 |
0.51 |
11 |
A |
1272 |
1272 |
4.01 |
8.82 |
0.67 |
0.80 |
12 |
A |
1185 |
1185 |
2.81 |
1.19 |
0.68 |
0.81 |
13 |
A |
1069 |
1069 |
123.58 |
4.92 |
0.60 |
0.75 |
14 |
A |
1039 |
1039 |
23.23 |
1.55 |
0.71 |
0.83 |
15 |
A |
994 |
994 |
3.26 |
1.77 |
0.14 |
0.24 |
16 |
A |
979 |
979 |
51.95 |
1.19 |
0.43 |
0.60 |
17 |
A |
932 |
932 |
1.96 |
2.62 |
0.14 |
0.25 |
18 |
A |
663 |
663 |
7.65 |
2.26 |
0.51 |
0.67 |
19 |
A |
435 |
435 |
2.48 |
3.63 |
0.42 |
0.60 |
20 |
A |
327 |
327 |
6.73 |
1.84 |
0.74 |
0.85 |
21 |
A |
116 |
116 |
0.99 |
3.74 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 16088.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 16088.9 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 B1B95/Def2TZVPP
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.602 |
0.427 |
0.316 |
C2 |
0.642 |
-0.379 |
0.242 |
C3 |
1.790 |
0.092 |
-0.213 |
F4 |
-1.636 |
-0.223 |
-0.341 |
H5 |
2.687 |
-0.508 |
-0.223 |
H6 |
1.873 |
1.104 |
-0.587 |
H7 |
0.570 |
-1.397 |
0.606 |
H8 |
-0.922 |
0.564 |
1.350 |
H9 |
-0.467 |
1.404 |
-0.147 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
C1 | | 1.4844 | 2.4725 | 1.3868 | 3.4618 | 2.7200 | 2.1869 | 1.0913 | 1.0893 |
C2 | 1.4844 | | 1.3216 | 2.3571 | 2.1011 | 2.0980 | 1.0831 | 2.1368 | 2.1356 | C3 | 2.4725 | 1.3216 | | 3.4430 | 1.0798 | 1.0819 | 2.0921 | 3.1657 | 2.6113 | F4 | 1.3868 | 2.3571 | 3.4430 | | 4.3343 | 3.7594 | 2.6726 | 1.9976 | 2.0123 | H5 | 3.4618 | 2.1011 | 1.0798 | 4.3343 | | 1.8428 | 2.4412 | 4.0808 | 3.6894 | H6 | 2.7200 | 2.0980 | 1.0819 | 3.7594 | 1.8428 | | 3.0618 | 3.4430 | 2.3997 | H7 | 2.1869 | 1.0831 | 2.0921 | 2.6726 | 2.4412 | 3.0618 | | 2.5740 | 3.0797 | H8 | 1.0913 | 2.1368 | 3.1657 | 1.9976 | 4.0808 | 3.4430 | 2.5740 | | 1.7755 | H9 | 1.0893 | 2.1356 | 2.6113 | 2.0123 | 3.6894 | 2.3997 | 3.0797 | 1.7755 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
C3 |
123.461 |
|
C1 |
C2 |
H7 |
115.934 |
C2 |
C1 |
F4 |
110.311 |
|
C2 |
C1 |
H8 |
111.201 |
C2 |
C1 |
H9 |
111.223 |
|
C2 |
C3 |
H5 |
121.755 |
C2 |
C3 |
H6 |
121.272 |
|
C3 |
C2 |
H7 |
120.595 |
F4 |
C1 |
H8 |
106.826 |
|
F4 |
C1 |
H9 |
108.112 |
H5 |
C3 |
H6 |
116.972 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/Def2TZVPP
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.107 |
|
|
|
2 |
C |
-0.119 |
|
|
|
3 |
C |
-0.195 |
|
|
|
4 |
F |
-0.236 |
|
|
|
5 |
H |
0.103 |
|
|
|
6 |
H |
0.086 |
|
|
|
7 |
H |
0.101 |
|
|
|
8 |
H |
0.080 |
|
|
|
9 |
H |
0.074 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
1.483 |
0.722 |
0.842 |
1.852 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-25.618 |
-1.125 |
-1.897 |
y |
-1.125 |
-22.459 |
-0.976 |
z |
-1.897 |
-0.976 |
-24.739 |
|
Traceless |
| x | y | z |
x |
-2.019 |
-1.125 |
-1.897 |
y |
-1.125 |
2.720 |
-0.976 |
z |
-1.897 |
-0.976 |
-0.700 |
|
Polar |
3z2-r2 | -1.401 |
x2-y2 | -3.160 |
xy | -1.125 |
xz | -1.897 |
yz | -0.976 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
7.102 |
0.236 |
-0.711 |
y |
0.236 |
5.113 |
-0.325 |
z |
-0.711 |
-0.325 |
4.494 |
<r2> (average value of r
2) Å
2
<r2> |
88.295 |
(<r2>)1/2 |
9.397 |