Jump to
S1C2
Energy calculated at HF/6-311G*
| hartrees |
Energy at 0K | -637.046419 |
Energy at 298.15K | -637.051472 |
HF Energy | -637.046419 |
Nuclear repulsion energy | 157.829866 |
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/6-311G*
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' |
3279 |
2965 |
29.46 |
|
|
|
2 |
A' |
3257 |
2945 |
25.12 |
|
|
|
3 |
A' |
1664 |
1505 |
0.70 |
|
|
|
4 |
A' |
1635 |
1478 |
8.90 |
|
|
|
5 |
A' |
1573 |
1423 |
6.11 |
|
|
|
6 |
A' |
1421 |
1285 |
25.48 |
|
|
|
7 |
A' |
1169 |
1057 |
149.31 |
|
|
|
8 |
A' |
1147 |
1037 |
14.12 |
|
|
|
9 |
A' |
827 |
748 |
76.20 |
|
|
|
10 |
A' |
411 |
372 |
3.48 |
|
|
|
11 |
A' |
265 |
239 |
14.18 |
|
|
|
12 |
A" |
3346 |
3026 |
26.52 |
|
|
|
13 |
A" |
3308 |
2992 |
21.07 |
|
|
|
14 |
A" |
1429 |
1293 |
0.91 |
|
|
|
15 |
A" |
1344 |
1216 |
2.49 |
|
|
|
16 |
A" |
1170 |
1058 |
4.75 |
|
|
|
17 |
A" |
858 |
776 |
0.22 |
|
|
|
18 |
A" |
141 |
128 |
13.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14121.2 cm
-1
Scaled (by 0.9044) Zero Point Vibrational Energy (zpe) 12771.2 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 HF/6-311G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.610 |
0.000 |
C2 |
1.002 |
-0.523 |
0.000 |
Cl3 |
-1.664 |
-0.055 |
0.000 |
F4 |
2.252 |
0.027 |
0.000 |
H5 |
0.105 |
1.222 |
0.881 |
H6 |
0.105 |
1.222 |
-0.881 |
H7 |
0.901 |
-1.137 |
0.883 |
H8 |
0.901 |
-1.137 |
-0.883 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Cl3 |
F4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5121 | 1.7918 | 2.3260 | 1.0775 | 1.0775 | 2.1545 | 2.1545 |
C2 | 1.5121 | | 2.7065 | 1.3660 | 2.1501 | 2.1501 | 1.0803 | 1.0803 | Cl3 | 1.7918 | 2.7065 | | 3.9168 | 2.3527 | 2.3527 | 2.9204 | 2.9204 | F4 | 2.3260 | 1.3660 | 3.9168 | | 2.6096 | 2.6096 | 1.9903 | 1.9903 | H5 | 1.0775 | 2.1501 | 2.3527 | 2.6096 | | 1.7612 | 2.4892 | 3.0507 | H6 | 1.0775 | 2.1501 | 2.3527 | 2.6096 | 1.7612 | | 3.0507 | 2.4892 | H7 | 2.1545 | 1.0803 | 2.9204 | 1.9903 | 2.4892 | 3.0507 | | 1.7660 | H8 | 2.1545 | 1.0803 | 2.9204 | 1.9903 | 3.0507 | 2.4892 | 1.7660 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
F4 |
107.732 |
|
C1 |
C2 |
H7 |
111.338 |
C1 |
C2 |
H8 |
111.338 |
|
C2 |
C1 |
Cl3 |
109.719 |
C2 |
C1 |
H5 |
111.145 |
|
C2 |
C1 |
H6 |
111.145 |
Cl3 |
C1 |
H5 |
107.536 |
|
Cl3 |
C1 |
H6 |
107.536 |
F4 |
C2 |
H7 |
108.337 |
|
F4 |
C2 |
H8 |
108.337 |
H5 |
C1 |
H6 |
109.625 |
|
H7 |
C2 |
H8 |
109.645 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.491 |
|
|
|
2 |
C |
0.008 |
|
|
|
3 |
Cl |
-0.131 |
|
|
|
4 |
F |
-0.345 |
|
|
|
5 |
H |
0.268 |
|
|
|
6 |
H |
0.268 |
|
|
|
7 |
H |
0.211 |
|
|
|
8 |
H |
0.211 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.279 |
0.028 |
0.000 |
0.280 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-39.299 |
-0.827 |
0.000 |
y |
-0.827 |
-29.171 |
0.000 |
z |
0.000 |
0.000 |
-29.773 |
|
Traceless |
| x | y | z |
x |
-9.827 |
-0.827 |
0.000 |
y |
-0.827 |
5.366 |
0.000 |
z |
0.000 |
0.000 |
4.462 |
|
Polar |
3z2-r2 | 8.923 |
x2-y2 | -10.129 |
xy | -0.827 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.890 |
0.485 |
0.000 |
y |
0.485 |
4.065 |
0.000 |
z |
0.000 |
0.000 |
3.627 |
<r2> (average value of r
2) Å
2
<r2> |
133.442 |
(<r2>)1/2 |
11.552 |
Jump to
S1C1
Energy calculated at HF/6-311G*
| hartrees |
Energy at 0K | -637.045159 |
Energy at 298.15K | -637.050316 |
HF Energy | -637.045159 |
Nuclear repulsion energy | 161.734721 |
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/6-311G*
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 |
3331 |
3013 |
17.23 |
|
|
|
2 |
A |
3294 |
2979 |
35.72 |
|
|
|
3 |
A |
3268 |
2955 |
27.74 |
|
|
|
4 |
A |
3230 |
2921 |
35.75 |
|
|
|
5 |
A |
1650 |
1492 |
1.33 |
|
|
|
6 |
A |
1608 |
1455 |
13.03 |
|
|
|
7 |
A |
1575 |
1425 |
18.82 |
|
|
|
8 |
A |
1475 |
1334 |
50.21 |
|
|
|
9 |
A |
1404 |
1270 |
0.20 |
|
|
|
10 |
A |
1339 |
1211 |
3.26 |
|
|
|
11 |
A |
1212 |
1096 |
89.42 |
|
|
|
12 |
A |
1168 |
1056 |
32.76 |
|
|
|
13 |
A |
1056 |
955 |
5.08 |
|
|
|
14 |
A |
932 |
843 |
15.32 |
|
|
|
15 |
A |
724 |
655 |
50.16 |
|
|
|
16 |
A |
503 |
455 |
16.61 |
|
|
|
17 |
A |
305 |
276 |
1.09 |
|
|
|
18 |
A |
143 |
129 |
3.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14108.1 cm
-1
Scaled (by 0.9044) Zero Point Vibrational Energy (zpe) 12759.4 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/6-311G*
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.079 |
0.836 |
-0.293 |
C2 |
1.204 |
0.399 |
0.364 |
Cl3 |
-1.436 |
-0.280 |
0.064 |
F4 |
1.665 |
-0.747 |
-0.206 |
H5 |
-0.370 |
1.810 |
0.069 |
H6 |
0.031 |
0.865 |
-1.365 |
H7 |
1.953 |
1.168 |
0.217 |
H8 |
1.069 |
0.223 |
1.421 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Cl3 |
F4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5065 | 1.7921 | 2.3567 | 1.0791 | 1.0780 | 2.1220 | 2.1522 |
C2 | 1.5065 | | 2.7427 | 1.3602 | 2.1347 | 2.1405 | 1.0838 | 1.0805 | Cl3 | 1.7921 | 2.7427 | | 3.1473 | 2.3458 | 2.3460 | 3.6891 | 2.8933 | F4 | 2.3567 | 1.3602 | 3.1473 | | 3.2794 | 2.5711 | 1.9827 | 1.9859 | H5 | 1.0791 | 2.1347 | 2.3458 | 3.2794 | | 1.7631 | 2.4152 | 2.5336 | H6 | 1.0780 | 2.1405 | 2.3460 | 2.5711 | 1.7631 | | 2.5078 | 3.0416 | H7 | 2.1220 | 1.0838 | 3.6891 | 1.9827 | 2.4152 | 2.5078 | | 1.7682 | H8 | 2.1522 | 1.0805 | 2.8933 | 1.9859 | 2.5336 | 3.0416 | 1.7682 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
F4 |
110.486 |
|
C1 |
C2 |
H7 |
108.917 |
C1 |
C2 |
H8 |
111.534 |
|
C2 |
C1 |
Cl3 |
112.211 |
C2 |
C1 |
H5 |
110.203 |
|
C2 |
C1 |
H6 |
110.734 |
Cl3 |
C1 |
H5 |
106.932 |
|
Cl3 |
C1 |
H6 |
106.998 |
F4 |
C2 |
H7 |
107.900 |
|
F4 |
C2 |
H8 |
108.364 |
H5 |
C1 |
H6 |
109.631 |
|
H7 |
C2 |
H8 |
109.566 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.487 |
|
|
|
2 |
C |
0.001 |
|
|
|
3 |
Cl |
-0.123 |
|
|
|
4 |
F |
-0.334 |
|
|
|
5 |
H |
0.256 |
|
|
|
6 |
H |
0.269 |
|
|
|
7 |
H |
0.200 |
|
|
|
8 |
H |
0.218 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
1.069 |
3.001 |
0.379 |
3.209 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-34.242 |
2.568 |
1.150 |
y |
2.568 |
-29.885 |
-0.560 |
z |
1.150 |
-0.560 |
-29.702 |
|
Traceless |
| x | y | z |
x |
-4.448 |
2.568 |
1.150 |
y |
2.568 |
2.087 |
-0.560 |
z |
1.150 |
-0.560 |
2.361 |
|
Polar |
3z2-r2 | 4.722 |
x2-y2 | -4.357 |
xy | 2.568 |
xz | 1.150 |
yz | -0.560 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.414 |
1.020 |
-0.143 |
y |
1.020 |
4.460 |
-0.205 |
z |
-0.143 |
-0.205 |
3.781 |
<r2> (average value of r
2) Å
2
<r2> |
116.000 |
(<r2>)1/2 |
10.770 |