Jump to
S1C2
Energy calculated at HF/LANL2DZ
| hartrees |
Energy at 0K | -181.080096 |
Energy at 298.15K | -181.082743 |
HF Energy | -181.080096 |
Nuclear repulsion energy | 127.950042 |
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/LANL2DZ
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' |
3446 |
3101 |
0.41 |
|
|
|
2 |
A' |
3318 |
2986 |
25.33 |
|
|
|
3 |
A' |
1903 |
1713 |
172.72 |
|
|
|
4 |
A' |
1529 |
1376 |
13.03 |
|
|
|
5 |
A' |
1367 |
1230 |
19.03 |
|
|
|
6 |
A' |
1182 |
1064 |
15.62 |
|
|
|
7 |
A' |
815 |
733 |
42.86 |
|
|
|
8 |
A' |
450 |
405 |
9.64 |
|
|
|
9 |
A' |
348 |
313 |
39.90 |
|
|
|
10 |
A' |
266 |
239 |
2.21 |
|
|
|
11 |
A" |
1370 |
1233 |
30.85 |
|
|
|
12 |
A" |
1133 |
1020 |
29.01 |
|
|
|
13 |
A" |
739 |
665 |
130.17 |
|
|
|
14 |
A" |
307 |
277 |
4.05 |
|
|
|
15 |
A" |
96 |
87 |
18.35 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 9135.3 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 8220.8 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/LANL2DZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.397 |
0.014 |
0.000 |
C2 |
-0.174 |
1.414 |
0.000 |
H3 |
1.466 |
0.010 |
0.000 |
Cl4 |
-0.174 |
-0.858 |
1.508 |
Cl5 |
-0.174 |
-0.858 |
-1.508 |
O6 |
0.544 |
2.389 |
0.000 |
H7 |
-1.253 |
1.482 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
H3 |
Cl4 |
Cl5 |
O6 |
H7 |
C1 | | 1.5123 | 1.0690 | 1.8328 | 1.8328 | 2.3801 | 2.2095 |
C2 | 1.5123 | | 2.1590 | 2.7266 | 2.7266 | 1.2113 | 1.0818 | H3 | 1.0690 | 2.1590 | | 2.3909 | 2.3909 | 2.5517 | 3.0927 | Cl4 | 1.8328 | 2.7266 | 2.3909 | | 3.0156 | 3.6514 | 2.9858 | Cl5 | 1.8328 | 2.7266 | 2.3909 | 3.0156 | | 3.6514 | 2.9858 | O6 | 2.3801 | 1.2113 | 2.5517 | 3.6514 | 3.6514 | | 2.0137 | H7 | 2.2095 | 1.0818 | 3.0927 | 2.9858 | 2.9858 | 2.0137 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
O6 |
121.439 |
|
C1 |
C2 |
H7 |
115.813 |
C2 |
C1 |
H3 |
112.394 |
|
C2 |
C1 |
Cl4 |
108.817 |
C2 |
C1 |
Cl5 |
108.817 |
|
H3 |
C1 |
Cl4 |
108.057 |
H3 |
C1 |
Cl5 |
108.057 |
|
Cl4 |
C1 |
Cl5 |
110.707 |
O6 |
C2 |
H7 |
122.748 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/LANL2DZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.442 |
|
|
|
2 |
C |
0.238 |
|
|
|
3 |
H |
0.325 |
|
|
|
4 |
Cl |
-0.019 |
|
|
|
5 |
Cl |
-0.019 |
|
|
|
6 |
O |
-0.294 |
|
|
|
7 |
H |
0.210 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.485 |
-0.483 |
0.000 |
0.684 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-39.517 |
-4.492 |
0.000 |
y |
-4.492 |
-50.902 |
0.000 |
z |
0.000 |
0.000 |
-44.188 |
|
Traceless |
| x | y | z |
x |
8.028 |
-4.492 |
0.000 |
y |
-4.492 |
-9.049 |
0.000 |
z |
0.000 |
0.000 |
1.021 |
|
Polar |
3z2-r2 | 2.042 |
x2-y2 | 11.384 |
xy | -4.492 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.673 |
1.218 |
0.000 |
y |
1.218 |
5.507 |
0.000 |
z |
0.000 |
0.000 |
6.511 |
<r2> (average value of r
2) Å
2
<r2> |
137.656 |
(<r2>)1/2 |
11.733 |
Jump to
S1C1
Energy calculated at HF/LANL2DZ
| hartrees |
Energy at 0K | -181.076072 |
Energy at 298.15K | |
HF Energy | -181.076072 |
Nuclear repulsion energy | 128.785700 |
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/LANL2DZ
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 |
3397 |
3057 |
5.13 |
97.65 |
0.17 |
0.29 |
2 |
A |
3288 |
2959 |
29.10 |
109.52 |
0.30 |
0.46 |
3 |
A |
1911 |
1719 |
158.08 |
28.47 |
0.30 |
0.46 |
4 |
A |
1534 |
1380 |
23.50 |
4.95 |
0.70 |
0.82 |
5 |
A |
1410 |
1269 |
6.24 |
6.87 |
0.62 |
0.77 |
6 |
A |
1356 |
1220 |
16.60 |
12.25 |
0.68 |
0.81 |
7 |
A |
1146 |
1032 |
9.85 |
1.51 |
0.69 |
0.82 |
8 |
A |
1042 |
938 |
3.06 |
8.50 |
0.56 |
0.72 |
9 |
A |
856 |
770 |
91.94 |
15.93 |
0.74 |
0.85 |
10 |
A |
651 |
585 |
47.89 |
24.65 |
0.13 |
0.23 |
11 |
A |
634 |
570 |
52.81 |
16.27 |
0.55 |
0.71 |
12 |
A |
371 |
333 |
1.97 |
7.40 |
0.26 |
0.42 |
13 |
A |
283 |
255 |
6.01 |
7.77 |
0.65 |
0.79 |
14 |
A |
233 |
210 |
3.78 |
2.84 |
0.73 |
0.84 |
15 |
A |
93 |
83 |
24.05 |
2.57 |
0.72 |
0.84 |
Unscaled Zero Point Vibrational Energy (zpe) 9101.6 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 8190.6 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 HF/LANL2DZ
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.076 |
-0.054 |
0.524 |
C2 |
-0.701 |
-1.310 |
0.173 |
H3 |
0.200 |
0.030 |
1.586 |
Cl4 |
1.780 |
-0.240 |
-0.161 |
Cl5 |
-0.709 |
1.471 |
-0.059 |
O6 |
-1.811 |
-1.318 |
-0.304 |
H7 |
-0.171 |
-2.225 |
0.410 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
H3 |
Cl4 |
Cl5 |
O6 |
H7 |
C1 | | 1.5180 | 1.0723 | 1.8455 | 1.8117 | 2.4179 | 2.1876 |
C2 | 1.5180 | | 2.1460 | 2.7224 | 2.7901 | 1.2079 | 1.0838 | H3 | 1.0723 | 2.1460 | | 2.3713 | 2.3677 | 3.0716 | 2.5706 | Cl4 | 1.8455 | 2.7224 | 2.3713 | | 3.0212 | 3.7519 | 2.8411 | Cl5 | 1.8117 | 2.7901 | 2.3677 | 3.0212 | | 3.0090 | 3.7637 | O6 | 2.4179 | 1.2079 | 3.0716 | 3.7519 | 3.0090 | | 2.0051 | H7 | 2.1876 | 1.0838 | 2.5706 | 2.8411 | 3.7637 | 2.0051 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
O6 |
124.608 |
|
C1 |
C2 |
H7 |
113.399 |
C2 |
C1 |
H3 |
110.708 |
|
C2 |
C1 |
Cl4 |
107.675 |
C2 |
C1 |
Cl5 |
113.556 |
|
H3 |
C1 |
Cl4 |
105.648 |
H3 |
C1 |
Cl5 |
107.584 |
|
Cl4 |
C1 |
Cl5 |
111.401 |
O6 |
C2 |
H7 |
121.983 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/LANL2DZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.434 |
|
|
|
2 |
C |
0.219 |
|
|
|
3 |
H |
0.308 |
|
|
|
4 |
Cl |
-0.030 |
|
|
|
5 |
Cl |
0.011 |
|
|
|
6 |
O |
-0.275 |
|
|
|
7 |
H |
0.201 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
1.596 |
-1.399 |
2.668 |
3.410 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-50.745 |
-2.542 |
-1.456 |
y |
-2.542 |
-41.262 |
-1.805 |
z |
-1.456 |
-1.805 |
-39.115 |
|
Traceless |
| x | y | z |
x |
-10.556 |
-2.542 |
-1.456 |
y |
-2.542 |
3.667 |
-1.805 |
z |
-1.456 |
-1.805 |
6.889 |
|
Polar |
3z2-r2 | 13.778 |
x2-y2 | -9.483 |
xy | -2.542 |
xz | -1.456 |
yz | -1.805 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
7.160 |
-1.046 |
0.095 |
y |
-1.046 |
5.222 |
-0.398 |
z |
0.095 |
-0.398 |
3.163 |
<r2> (average value of r
2) Å
2
<r2> |
132.443 |
(<r2>)1/2 |
11.508 |