Jump to
S1C2
Energy calculated at B1B95/cc-pVDZ
| | hartrees |
| Energy at 0K | -1073.087688 |
| Energy at 298.15K | -1073.090178 |
| HF Energy | -1073.087688 |
| Nuclear repulsion energy | 263.893874 |
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/cc-pVDZ
| 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' |
3185 |
3062 |
0.91 |
|
|
|
| 2 |
A' |
2981 |
2865 |
45.87 |
|
|
|
| 3 |
A' |
1874 |
1801 |
174.98 |
|
|
|
| 4 |
A' |
1382 |
1328 |
3.89 |
|
|
|
| 5 |
A' |
1196 |
1150 |
8.84 |
|
|
|
| 6 |
A' |
1081 |
1039 |
25.28 |
|
|
|
| 7 |
A' |
790 |
759 |
25.72 |
|
|
|
| 8 |
A' |
442 |
425 |
4.34 |
|
|
|
| 9 |
A' |
316 |
304 |
23.75 |
|
|
|
| 10 |
A' |
255 |
245 |
2.53 |
|
|
|
| 11 |
A" |
1220 |
1173 |
22.10 |
|
|
|
| 12 |
A" |
1014 |
975 |
17.30 |
|
|
|
| 13 |
A" |
741 |
713 |
127.40 |
|
|
|
| 14 |
A" |
274 |
263 |
3.06 |
|
|
|
| 15 |
A" |
87 |
83 |
6.56 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8418.3 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 8091.7 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/cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.391 |
-0.019 |
0.000 |
| C2 |
-0.171 |
1.392 |
0.000 |
| H3 |
1.484 |
-0.004 |
0.000 |
| Cl4 |
-0.171 |
-0.839 |
1.472 |
| Cl5 |
-0.171 |
-0.839 |
-1.472 |
| O6 |
0.536 |
2.359 |
0.000 |
| H7 |
-1.283 |
1.435 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
Cl4 |
Cl5 |
O6 |
H7 |
| C1 | | 1.5188 | 1.0928 | 1.7766 | 1.7766 | 2.3818 | 2.2175 |
C2 | 1.5188 | | 2.1652 | 2.6736 | 2.6736 | 1.1972 | 1.1132 | H3 | 1.0928 | 2.1652 | | 2.3668 | 2.3668 | 2.5459 | 3.1190 | Cl4 | 1.7766 | 2.6736 | 2.3668 | | 2.9445 | 3.5909 | 2.9291 | Cl5 | 1.7766 | 2.6736 | 2.3668 | 2.9445 | | 3.5909 | 2.9291 | O6 | 2.3818 | 1.1972 | 2.5459 | 3.5909 | 3.5909 | | 2.0401 | H7 | 2.2175 | 1.1132 | 3.1190 | 2.9291 | 2.9291 | 2.0401 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
O6 |
122.107 |
|
C1 |
C2 |
H7 |
113.925 |
| C2 |
C1 |
H3 |
110.951 |
|
C2 |
C1 |
Cl4 |
108.192 |
| C2 |
C1 |
Cl5 |
108.192 |
|
H3 |
C1 |
Cl4 |
108.798 |
| H3 |
C1 |
Cl5 |
108.798 |
|
Cl4 |
C1 |
Cl5 |
111.924 |
| O6 |
C2 |
H7 |
123.969 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.184 |
|
|
|
| 2 |
C |
0.244 |
|
|
|
| 3 |
H |
0.127 |
|
|
|
| 4 |
Cl |
-0.027 |
|
|
|
| 5 |
Cl |
-0.027 |
|
|
|
| 6 |
O |
-0.166 |
|
|
|
| 7 |
H |
0.032 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.256 |
-0.620 |
0.000 |
0.670 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-40.270 |
-2.563 |
0.000 |
| y |
-2.563 |
-47.452 |
0.000 |
| z |
0.000 |
0.000 |
-42.112 |
|
| Traceless |
| | x | y | z |
| x |
4.512 |
-2.563 |
0.000 |
| y |
-2.563 |
-6.261 |
0.000 |
| z |
0.000 |
0.000 |
1.749 |
|
| Polar |
| 3z2-r2 | 3.498 |
| x2-y2 | 7.181 |
| xy | -2.563 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.043 |
0.635 |
0.000 |
| y |
0.635 |
6.772 |
0.000 |
| z |
0.000 |
0.000 |
7.098 |
<r2> (average value of r
2) Å
2
| <r2> |
191.109 |
| (<r2>)1/2 |
13.824 |
Jump to
S1C1
Energy calculated at B1B95/cc-pVDZ
| | hartrees |
| Energy at 0K | -1073.085352 |
| Energy at 298.15K | |
| HF Energy | -1073.085352 |
| Nuclear repulsion energy | 266.727519 |
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/cc-pVDZ
| 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 |
3133 |
3012 |
4.24 |
89.34 |
0.19 |
0.32 |
| 2 |
A |
2969 |
2854 |
56.61 |
146.98 |
0.31 |
0.47 |
| 3 |
A |
1889 |
1815 |
149.96 |
14.04 |
0.50 |
0.66 |
| 4 |
A |
1379 |
1326 |
14.27 |
4.38 |
0.56 |
0.72 |
| 5 |
A |
1254 |
1205 |
12.15 |
3.46 |
0.72 |
0.84 |
| 6 |
A |
1198 |
1151 |
11.03 |
8.50 |
0.73 |
0.85 |
| 7 |
A |
1038 |
998 |
12.16 |
1.57 |
0.58 |
0.74 |
| 8 |
A |
940 |
903 |
8.42 |
6.02 |
0.65 |
0.79 |
| 9 |
A |
824 |
792 |
85.31 |
5.48 |
0.72 |
0.83 |
| 10 |
A |
656 |
630 |
39.25 |
9.03 |
0.09 |
0.17 |
| 11 |
A |
618 |
594 |
33.91 |
6.58 |
0.44 |
0.61 |
| 12 |
A |
343 |
329 |
1.48 |
3.10 |
0.24 |
0.39 |
| 13 |
A |
273 |
263 |
3.38 |
5.93 |
0.66 |
0.79 |
| 14 |
A |
215 |
207 |
2.62 |
1.49 |
0.70 |
0.82 |
| 15 |
A |
95 |
91 |
8.86 |
2.05 |
0.72 |
0.84 |
Unscaled Zero Point Vibrational Energy (zpe) 8411.1 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 8084.7 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/cc-pVDZ
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.100 |
-0.023 |
0.519 |
| C2 |
-0.692 |
-1.286 |
0.193 |
| H3 |
0.231 |
0.065 |
1.604 |
| Cl4 |
1.736 |
-0.236 |
-0.168 |
| Cl5 |
-0.698 |
1.432 |
-0.058 |
| O6 |
-1.772 |
-1.291 |
-0.316 |
| H7 |
-0.147 |
-2.213 |
0.487 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
Cl4 |
Cl5 |
O6 |
H7 |
| C1 | | 1.5261 | 1.0967 | 1.7874 | 1.7568 | 2.4098 | 2.2040 |
C2 | 1.5261 | | 2.1608 | 2.6696 | 2.7303 | 1.1937 | 1.1142 | H3 | 1.0967 | 2.1608 | | 2.3444 | 2.3440 | 3.0880 | 2.5648 | Cl4 | 1.7874 | 2.6696 | 2.3444 | | 2.9531 | 3.6657 | 2.8077 | Cl5 | 1.7568 | 2.7303 | 2.3440 | 2.9531 | | 2.9390 | 3.7266 | O6 | 2.4098 | 1.1937 | 3.0880 | 3.6657 | 2.9390 | | 2.0329 | H7 | 2.2040 | 1.1142 | 2.5648 | 2.8077 | 3.7266 | 2.0329 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
O6 |
124.303 |
|
C1 |
C2 |
H7 |
112.246 |
| C2 |
C1 |
H3 |
109.861 |
|
C2 |
C1 |
Cl4 |
107.087 |
| C2 |
C1 |
Cl5 |
112.350 |
|
H3 |
C1 |
Cl4 |
106.275 |
| H3 |
C1 |
Cl5 |
108.226 |
|
Cl4 |
C1 |
Cl5 |
112.857 |
| O6 |
C2 |
H7 |
123.451 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.211 |
|
|
|
| 2 |
C |
0.237 |
|
|
|
| 3 |
H |
0.137 |
|
|
|
| 4 |
Cl |
-0.040 |
|
|
|
| 5 |
Cl |
-0.006 |
|
|
|
| 6 |
O |
-0.148 |
|
|
|
| 7 |
H |
0.031 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.125 |
-0.759 |
1.865 |
2.306 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-46.508 |
-2.019 |
-1.096 |
| y |
-2.019 |
-41.173 |
-1.443 |
| z |
-1.096 |
-1.443 |
-39.709 |
|
| Traceless |
| | x | y | z |
| x |
-6.067 |
-2.019 |
-1.096 |
| y |
-2.019 |
1.935 |
-1.443 |
| z |
-1.096 |
-1.443 |
4.131 |
|
| Polar |
| 3z2-r2 | 8.262 |
| x2-y2 | -5.335 |
| xy | -2.019 |
| xz | -1.096 |
| yz | -1.443 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.644 |
-0.758 |
0.169 |
| y |
-0.758 |
6.651 |
-0.354 |
| z |
0.169 |
-0.354 |
4.298 |
<r2> (average value of r
2) Å
2
| <r2> |
184.132 |
| (<r2>)1/2 |
13.570 |