Jump to
S1C2
Energy calculated at B1B95/STO-3G
| hartrees |
Energy at 0K | -631.264280 |
Energy at 298.15K | -631.268937 |
HF Energy | -631.264280 |
Nuclear repulsion energy | 153.600846 |
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/STO-3G
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' |
3381 |
2985 |
0.20 |
|
|
|
2 |
A' |
3285 |
2901 |
5.53 |
|
|
|
3 |
A' |
1660 |
1466 |
0.94 |
|
|
|
4 |
A' |
1627 |
1436 |
2.37 |
|
|
|
5 |
A' |
1512 |
1335 |
4.11 |
|
|
|
6 |
A' |
1362 |
1203 |
14.24 |
|
|
|
7 |
A' |
1221 |
1078 |
17.62 |
|
|
|
8 |
A' |
1091 |
964 |
1.77 |
|
|
|
9 |
A' |
881 |
778 |
26.85 |
|
|
|
10 |
A' |
383 |
338 |
0.70 |
|
|
|
11 |
A' |
233 |
206 |
7.60 |
|
|
|
12 |
A" |
3507 |
3096 |
0.10 |
|
|
|
13 |
A" |
3385 |
2989 |
4.77 |
|
|
|
14 |
A" |
1378 |
1216 |
0.06 |
|
|
|
15 |
A" |
1265 |
1117 |
3.81 |
|
|
|
16 |
A" |
1110 |
980 |
0.04 |
|
|
|
17 |
A" |
817 |
721 |
1.35 |
|
|
|
18 |
A" |
98 |
86 |
5.76 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14096.9 cm
-1
Scaled (by 0.883) Zero Point Vibrational Energy (zpe) 12447.6 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/STO-3G
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.635 |
0.000 |
C2 |
1.024 |
-0.546 |
0.000 |
Cl3 |
-1.708 |
-0.016 |
0.000 |
F4 |
2.332 |
-0.048 |
0.000 |
H5 |
0.115 |
1.261 |
0.900 |
H6 |
0.115 |
1.261 |
-0.900 |
H7 |
0.840 |
-1.177 |
0.899 |
H8 |
0.840 |
-1.177 |
-0.899 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Cl3 |
F4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5635 | 1.8279 | 2.4294 | 1.1023 | 1.1023 | 2.1903 | 2.1903 |
C2 | 1.5635 | | 2.7832 | 1.3993 | 2.2145 | 2.2145 | 1.1136 | 1.1136 | Cl3 | 1.8279 | 2.7832 | | 4.0397 | 2.4006 | 2.4006 | 2.9407 | 2.9407 | F4 | 2.4294 | 1.3993 | 4.0397 | | 2.7271 | 2.7271 | 2.0760 | 2.0760 | H5 | 1.1023 | 2.2145 | 2.4006 | 2.7271 | | 1.7999 | 2.5438 | 3.1156 | H6 | 1.1023 | 2.2145 | 2.4006 | 2.7271 | 1.7999 | | 3.1156 | 2.5438 | H7 | 2.1903 | 1.1136 | 2.9407 | 2.0760 | 2.5438 | 3.1156 | | 1.7979 | H8 | 2.1903 | 1.1136 | 2.9407 | 2.0760 | 3.1156 | 2.5438 | 1.7979 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
F4 |
110.038 |
|
C1 |
C2 |
H7 |
108.637 |
C1 |
C2 |
H8 |
108.637 |
|
C2 |
C1 |
Cl3 |
110.058 |
C2 |
C1 |
H5 |
111.165 |
|
C2 |
C1 |
H6 |
111.165 |
Cl3 |
C1 |
H5 |
107.424 |
|
Cl3 |
C1 |
H6 |
107.424 |
F4 |
C2 |
H7 |
110.894 |
|
F4 |
C2 |
H8 |
110.894 |
H5 |
C1 |
H6 |
109.464 |
|
H7 |
C2 |
H8 |
107.661 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/STO-3G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.114 |
|
|
|
2 |
C |
-0.028 |
|
|
|
3 |
Cl |
-0.162 |
|
|
|
4 |
F |
-0.100 |
|
|
|
5 |
H |
0.114 |
|
|
|
6 |
H |
0.114 |
|
|
|
7 |
H |
0.088 |
|
|
|
8 |
H |
0.088 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
1.306 |
0.368 |
0.000 |
1.357 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-33.999 |
-0.341 |
0.000 |
y |
-0.341 |
-26.718 |
0.000 |
z |
0.000 |
0.000 |
-27.265 |
|
Traceless |
| x | y | z |
x |
-7.008 |
-0.341 |
0.000 |
y |
-0.341 |
3.914 |
0.000 |
z |
0.000 |
0.000 |
3.093 |
|
Polar |
3z2-r2 | 6.187 |
x2-y2 | -7.282 |
xy | -0.341 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.563 |
0.454 |
0.000 |
y |
0.454 |
1.864 |
0.000 |
z |
0.000 |
0.000 |
1.662 |
<r2> (average value of r
2) Å
2
<r2> |
137.991 |
(<r2>)1/2 |
11.747 |
Jump to
S1C1
Energy calculated at B1B95/STO-3G
| hartrees |
Energy at 0K | -631.264063 |
Energy at 298.15K | -631.268812 |
HF Energy | -631.264063 |
Nuclear repulsion energy | 157.603438 |
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/STO-3G
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 |
3505 |
3095 |
0.32 |
|
|
|
2 |
A |
3379 |
2984 |
0.15 |
|
|
|
3 |
A |
3365 |
2971 |
4.22 |
|
|
|
4 |
A |
3263 |
2881 |
7.30 |
|
|
|
5 |
A |
1647 |
1454 |
0.87 |
|
|
|
6 |
A |
1609 |
1420 |
3.89 |
|
|
|
7 |
A |
1518 |
1341 |
15.48 |
|
|
|
8 |
A |
1421 |
1255 |
22.88 |
|
|
|
9 |
A |
1330 |
1174 |
0.61 |
|
|
|
10 |
A |
1284 |
1134 |
8.24 |
|
|
|
11 |
A |
1211 |
1069 |
9.99 |
|
|
|
12 |
A |
1113 |
983 |
0.23 |
|
|
|
13 |
A |
1031 |
911 |
6.32 |
|
|
|
14 |
A |
905 |
799 |
1.33 |
|
|
|
15 |
A |
777 |
686 |
15.62 |
|
|
|
16 |
A |
465 |
411 |
6.04 |
|
|
|
17 |
A |
259 |
229 |
0.88 |
|
|
|
18 |
A |
98 |
87 |
1.46 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14089.9 cm
-1
Scaled (by 0.883) Zero Point Vibrational Energy (zpe) 12441.4 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 B1B95/STO-3G
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.105 |
0.876 |
-0.294 |
C2 |
1.237 |
0.413 |
0.353 |
Cl3 |
-1.459 |
-0.299 |
0.065 |
F4 |
1.709 |
-0.777 |
-0.203 |
H5 |
-0.404 |
1.856 |
0.111 |
H6 |
-0.016 |
0.940 |
-1.391 |
H7 |
1.971 |
1.240 |
0.196 |
H8 |
1.083 |
0.305 |
1.451 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Cl3 |
F4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5604 | 1.8286 | 2.4558 | 1.1024 | 1.1023 | 2.1638 | 2.1870 |
C2 | 1.5604 | | 2.8040 | 1.3955 | 2.1992 | 2.2108 | 1.1166 | 1.1140 | Cl3 | 1.8286 | 2.8040 | | 3.2157 | 2.4004 | 2.3960 | 3.7621 | 2.9579 | F4 | 2.4558 | 1.3955 | 3.2157 | | 3.3910 | 2.7079 | 2.0725 | 2.0728 | H5 | 1.1024 | 2.1992 | 2.4004 | 3.3910 | | 1.8018 | 2.4552 | 2.5329 | H6 | 1.1023 | 2.2108 | 2.3960 | 2.7079 | 1.8018 | | 2.5598 | 3.1122 | H7 | 2.1638 | 1.1166 | 3.7621 | 2.0725 | 2.4552 | 2.5598 | | 1.7996 | H8 | 2.1870 | 1.1140 | 2.9579 | 2.0728 | 2.5329 | 3.1122 | 1.7996 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
F4 |
112.248 |
|
C1 |
C2 |
H7 |
106.685 |
C1 |
C2 |
H8 |
108.570 |
|
C2 |
C1 |
Cl3 |
111.418 |
C2 |
C1 |
H5 |
110.179 |
|
C2 |
C1 |
H6 |
111.095 |
Cl3 |
C1 |
H5 |
107.356 |
|
Cl3 |
C1 |
H6 |
107.047 |
F4 |
C2 |
H7 |
110.689 |
|
F4 |
C2 |
H8 |
110.878 |
H5 |
C1 |
H6 |
109.623 |
|
H7 |
C2 |
H8 |
107.567 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/STO-3G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.115 |
|
|
|
2 |
C |
-0.024 |
|
|
|
3 |
Cl |
-0.163 |
|
|
|
4 |
F |
-0.097 |
|
|
|
5 |
H |
0.114 |
|
|
|
6 |
H |
0.115 |
|
|
|
7 |
H |
0.083 |
|
|
|
8 |
H |
0.089 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
1.476 |
2.213 |
-0.015 |
2.660 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-30.894 |
0.735 |
0.671 |
y |
0.735 |
-26.943 |
-0.304 |
z |
0.671 |
-0.304 |
-27.158 |
|
Traceless |
| x | y | z |
x |
-3.843 |
0.735 |
0.671 |
y |
0.735 |
2.083 |
-0.304 |
z |
0.671 |
-0.304 |
1.760 |
|
Polar |
3z2-r2 | 3.520 |
x2-y2 | -3.950 |
xy | 0.735 |
xz | 0.671 |
yz | -0.304 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.866 |
0.642 |
-0.185 |
y |
0.642 |
2.432 |
-0.057 |
z |
-0.185 |
-0.057 |
1.754 |
<r2> (average value of r
2) Å
2
<r2> |
119.008 |
(<r2>)1/2 |
10.909 |