Jump to
S1C2
Energy calculated at HF/6-311+G(3df,2p)
| hartrees |
Energy at 0K | -216.000051 |
Energy at 298.15K | |
HF Energy | -216.000051 |
Nuclear repulsion energy | 117.511047 |
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 HF/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' |
3378 |
3069 |
6.91 |
48.63 |
0.73 |
0.85 |
2 |
A' |
3300 |
2999 |
5.86 |
148.88 |
0.13 |
0.23 |
3 |
A' |
3282 |
2982 |
13.43 |
29.43 |
0.72 |
0.84 |
4 |
A' |
3176 |
2886 |
42.35 |
153.33 |
0.10 |
0.18 |
5 |
A' |
1849 |
1680 |
5.76 |
59.68 |
0.07 |
0.12 |
6 |
A' |
1629 |
1480 |
2.12 |
9.22 |
0.59 |
0.74 |
7 |
A' |
1569 |
1426 |
12.77 |
7.72 |
0.41 |
0.58 |
8 |
A' |
1550 |
1408 |
13.35 |
2.77 |
0.33 |
0.49 |
9 |
A' |
1421 |
1291 |
0.52 |
28.02 |
0.21 |
0.35 |
10 |
A' |
1238 |
1125 |
76.60 |
1.53 |
0.72 |
0.84 |
11 |
A' |
1101 |
1000 |
41.41 |
5.42 |
0.62 |
0.77 |
12 |
A' |
961 |
874 |
1.68 |
9.70 |
0.04 |
0.08 |
13 |
A' |
658 |
598 |
10.40 |
1.81 |
0.66 |
0.80 |
14 |
A' |
284 |
258 |
2.45 |
1.45 |
0.51 |
0.67 |
15 |
A" |
3209 |
2916 |
30.46 |
75.20 |
0.75 |
0.86 |
16 |
A" |
1386 |
1259 |
0.25 |
3.41 |
0.75 |
0.86 |
17 |
A" |
1160 |
1054 |
14.20 |
2.85 |
0.75 |
0.86 |
18 |
A" |
1108 |
1006 |
8.30 |
0.13 |
0.75 |
0.86 |
19 |
A" |
1085 |
986 |
58.49 |
5.04 |
0.75 |
0.86 |
20 |
A" |
616 |
559 |
11.60 |
1.50 |
0.75 |
0.86 |
21 |
A" |
188 |
171 |
3.75 |
1.10 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 17073.3 cm
-1
Scaled (by 0.9086) Zero Point Vibrational Energy (zpe) 15512.8 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 HF/6-311+G(3df,2p)
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.933 |
-0.226 |
0.000 |
C2 |
0.000 |
0.941 |
0.000 |
C3 |
1.311 |
0.867 |
0.000 |
F4 |
-0.264 |
-1.407 |
0.000 |
H5 |
1.914 |
1.756 |
0.000 |
H6 |
1.822 |
-0.076 |
0.000 |
H7 |
-0.491 |
1.900 |
0.000 |
H8 |
-1.568 |
-0.205 |
0.878 |
H9 |
-1.568 |
-0.205 |
-0.878 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
C1 | | 1.4949 | 2.4968 | 1.3578 | 3.4689 | 2.7596 | 2.1721 | 1.0841 | 1.0841 |
C2 | 1.4949 | | 1.3133 | 2.3636 | 2.0796 | 2.0869 | 1.0773 | 2.1320 | 2.1320 | C3 | 2.4968 | 1.3133 | | 2.7668 | 1.0733 | 1.0727 | 2.0772 | 3.1958 | 3.1958 | F4 | 1.3578 | 2.3636 | 2.7668 | | 3.8400 | 2.4746 | 3.3155 | 1.9798 | 1.9798 | H5 | 3.4689 | 2.0796 | 1.0733 | 3.8400 | | 1.8339 | 2.4089 | 4.0914 | 4.0914 | H6 | 2.7596 | 2.0869 | 1.0727 | 2.4746 | 1.8339 | | 3.0424 | 3.5048 | 3.5048 | H7 | 2.1721 | 1.0773 | 2.0772 | 3.3155 | 2.4089 | 3.0424 | | 2.5227 | 2.5227 | H8 | 1.0841 | 2.1320 | 3.1958 | 1.9798 | 4.0914 | 3.5048 | 2.5227 | | 1.7568 | H9 | 1.0841 | 2.1320 | 3.1958 | 1.9798 | 4.0914 | 3.5048 | 2.5227 | 1.7568 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
C3 |
125.403 |
|
C1 |
C2 |
H7 |
114.248 |
C2 |
C1 |
F4 |
111.813 |
|
C2 |
C1 |
H8 |
110.510 |
C2 |
C1 |
H9 |
110.510 |
|
C2 |
C3 |
H5 |
120.906 |
C2 |
C3 |
H6 |
121.676 |
|
C3 |
C2 |
H7 |
120.349 |
F4 |
C1 |
H8 |
107.818 |
|
F4 |
C1 |
H9 |
107.818 |
H5 |
C3 |
H6 |
117.418 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311+G(3df,2p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.389 |
|
|
|
2 |
C |
-0.168 |
|
|
|
3 |
C |
-0.270 |
|
|
|
4 |
F |
-0.575 |
|
|
|
5 |
H |
0.133 |
|
|
|
6 |
H |
0.134 |
|
|
|
7 |
H |
0.109 |
|
|
|
8 |
H |
0.124 |
|
|
|
9 |
H |
0.124 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.950 |
1.588 |
0.000 |
1.851 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-20.989 |
-0.243 |
0.000 |
y |
-0.243 |
-25.808 |
0.000 |
z |
0.000 |
0.000 |
-25.501 |
|
Traceless |
| x | y | z |
x |
4.665 |
-0.243 |
0.000 |
y |
-0.243 |
-2.563 |
0.000 |
z |
0.000 |
0.000 |
-2.102 |
|
Polar |
3z2-r2 | -4.205 |
x2-y2 | 4.819 |
xy | -0.243 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
7.133 |
0.287 |
0.000 |
y |
0.287 |
5.133 |
0.000 |
z |
0.000 |
0.000 |
4.502 |
<r2> (average value of r
2) Å
2
<r2> |
79.656 |
(<r2>)1/2 |
8.925 |
Jump to
S1C1
Energy calculated at HF/6-311+G(3df,2p)
| hartrees |
Energy at 0K | -215.999923 |
Energy at 298.15K | |
HF Energy | -215.999923 |
Nuclear repulsion energy | 115.347744 |
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 HF/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 |
3361 |
3054 |
13.97 |
56.15 |
0.60 |
0.75 |
2 |
A |
3300 |
2998 |
6.22 |
109.91 |
0.25 |
0.40 |
3 |
A |
3278 |
2978 |
13.24 |
58.53 |
0.14 |
0.24 |
4 |
A |
3239 |
2943 |
22.97 |
55.85 |
0.69 |
0.81 |
5 |
A |
3190 |
2899 |
37.81 |
116.85 |
0.09 |
0.17 |
6 |
A |
1847 |
1678 |
0.66 |
60.64 |
0.08 |
0.14 |
7 |
A |
1636 |
1486 |
2.96 |
2.86 |
0.74 |
0.85 |
8 |
A |
1585 |
1440 |
28.61 |
7.74 |
0.55 |
0.71 |
9 |
A |
1517 |
1379 |
16.52 |
6.61 |
0.13 |
0.23 |
10 |
A |
1419 |
1290 |
0.15 |
22.42 |
0.24 |
0.38 |
11 |
A |
1384 |
1258 |
5.36 |
7.74 |
0.61 |
0.75 |
12 |
A |
1276 |
1159 |
3.91 |
1.68 |
0.66 |
0.80 |
13 |
A |
1159 |
1053 |
168.84 |
5.33 |
0.68 |
0.81 |
14 |
A |
1133 |
1029 |
5.78 |
3.32 |
0.73 |
0.85 |
15 |
A |
1090 |
991 |
65.31 |
3.49 |
0.75 |
0.86 |
16 |
A |
1063 |
966 |
9.05 |
2.52 |
0.08 |
0.15 |
17 |
A |
996 |
905 |
4.28 |
5.06 |
0.07 |
0.13 |
18 |
A |
711 |
646 |
8.25 |
2.10 |
0.27 |
0.43 |
19 |
A |
468 |
425 |
2.35 |
3.62 |
0.30 |
0.46 |
20 |
A |
364 |
330 |
8.42 |
1.04 |
0.73 |
0.85 |
21 |
A |
126 |
114 |
1.27 |
2.93 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 17071.3 cm
-1
Scaled (by 0.9086) Zero Point Vibrational Energy (zpe) 15510.9 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 HF/6-311+G(3df,2p)
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.614 |
0.428 |
0.308 |
C2 |
0.644 |
-0.376 |
0.238 |
C3 |
1.788 |
0.094 |
-0.207 |
F4 |
-1.625 |
-0.227 |
-0.336 |
H5 |
2.678 |
-0.507 |
-0.213 |
H6 |
1.881 |
1.098 |
-0.579 |
H7 |
0.573 |
-1.388 |
0.598 |
H8 |
-0.930 |
0.565 |
1.335 |
H9 |
-0.491 |
1.396 |
-0.157 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
C1 | | 1.4945 | 2.4794 | 1.3656 | 3.4614 | 2.7315 | 2.1884 | 1.0832 | 1.0813 |
C2 | 1.4945 | | 1.3144 | 2.3455 | 2.0871 | 2.0905 | 1.0764 | 2.1370 | 2.1407 | C3 | 2.4794 | 1.3144 | | 3.4307 | 1.0735 | 1.0753 | 2.0783 | 3.1605 | 2.6250 | F4 | 1.3656 | 2.3455 | 3.4307 | | 4.3137 | 3.7555 | 2.6557 | 1.9755 | 1.9878 | H5 | 3.4614 | 2.0871 | 1.0735 | 4.3137 | | 1.8295 | 2.4212 | 4.0696 | 3.6964 | H6 | 2.7315 | 2.0905 | 1.0753 | 3.7555 | 1.8295 | | 3.0457 | 3.4424 | 2.4269 | H7 | 2.1884 | 1.0764 | 2.0783 | 2.6557 | 2.4212 | 3.0457 | | 2.5725 | 3.0742 | H8 | 1.0832 | 2.1370 | 3.1605 | 1.9755 | 4.0696 | 3.4424 | 2.5725 | | 1.7632 | H9 | 1.0813 | 2.1407 | 2.6250 | 1.9878 | 3.6964 | 2.4269 | 3.0742 | 1.7632 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
C3 |
123.819 |
|
C1 |
C2 |
H7 |
115.738 |
C2 |
C1 |
F4 |
110.100 |
|
C2 |
C1 |
H8 |
110.996 |
C2 |
C1 |
H9 |
111.416 |
|
C2 |
C3 |
H5 |
121.540 |
C2 |
C3 |
H6 |
121.733 |
|
C3 |
C2 |
H7 |
120.434 |
F4 |
C1 |
H8 |
106.986 |
|
F4 |
C1 |
H9 |
108.096 |
H5 |
C3 |
H6 |
116.727 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311+G(3df,2p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.337 |
|
|
|
2 |
C |
-0.057 |
|
|
|
3 |
C |
-0.329 |
|
|
|
4 |
F |
-0.554 |
|
|
|
5 |
H |
0.135 |
|
|
|
6 |
H |
0.120 |
|
|
|
7 |
H |
0.111 |
|
|
|
8 |
H |
0.124 |
|
|
|
9 |
H |
0.114 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
1.557 |
0.836 |
0.898 |
1.982 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-25.976 |
-1.254 |
-2.204 |
y |
-1.254 |
-22.535 |
-1.153 |
z |
-2.204 |
-1.153 |
-25.133 |
|
Traceless |
| x | y | z |
x |
-2.142 |
-1.254 |
-2.204 |
y |
-1.254 |
3.020 |
-1.153 |
z |
-2.204 |
-1.153 |
-0.878 |
|
Polar |
3z2-r2 | -1.755 |
x2-y2 | -3.441 |
xy | -1.254 |
xz | -2.204 |
yz | -1.153 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
7.013 |
0.359 |
-0.627 |
y |
0.359 |
5.059 |
-0.203 |
z |
-0.627 |
-0.203 |
4.785 |
<r2> (average value of r
2) Å
2
<r2> |
88.024 |
(<r2>)1/2 |
9.382 |