Jump to
S1C2
Energy calculated at B2PLYP=FULLultrafine/6-31+G**
| | hartrees |
| Energy at 0K | -1072.561451 |
| Energy at 298.15K | |
| Nuclear repulsion energy | |
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 B2PLYP=FULLultrafine/6-31+G**
Geometric Data calculated at B2PLYP=FULLultrafine/6-31+G**
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
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S1C1
Energy calculated at B2PLYP=FULLultrafine/6-31+G**
| | hartrees |
| Energy at 0K | -1072.558219 |
| Energy at 298.15K | |
| HF Energy | -1072.309402 |
| Nuclear repulsion energy | 265.022989 |
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 B2PLYP=FULLultrafine/6-31+G**
| 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 |
3150 |
3150 |
5.00 |
85.01 |
0.18 |
0.31 |
| 2 |
A |
3017 |
3017 |
45.52 |
135.02 |
0.31 |
0.47 |
| 3 |
A |
1808 |
1808 |
131.88 |
17.95 |
0.38 |
0.55 |
| 4 |
A |
1412 |
1412 |
12.55 |
3.63 |
0.48 |
0.65 |
| 5 |
A |
1285 |
1285 |
14.96 |
3.81 |
0.71 |
0.83 |
| 6 |
A |
1251 |
1251 |
11.90 |
7.67 |
0.74 |
0.85 |
| 7 |
A |
1042 |
1042 |
13.98 |
2.49 |
0.44 |
0.61 |
| 8 |
A |
947 |
947 |
8.86 |
5.68 |
0.59 |
0.74 |
| 9 |
A |
816 |
816 |
83.47 |
7.70 |
0.67 |
0.80 |
| 10 |
A |
651 |
651 |
36.92 |
11.32 |
0.09 |
0.17 |
| 11 |
A |
608 |
608 |
32.63 |
6.74 |
0.53 |
0.70 |
| 12 |
A |
350 |
350 |
1.44 |
4.26 |
0.18 |
0.30 |
| 13 |
A |
277 |
277 |
3.46 |
4.42 |
0.67 |
0.80 |
| 14 |
A |
220 |
220 |
3.09 |
1.31 |
0.70 |
0.82 |
| 15 |
A |
80 |
80 |
12.13 |
1.99 |
0.74 |
0.85 |
Unscaled Zero Point Vibrational Energy (zpe) 8457.3 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 8457.3 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 B2PLYP=FULLultrafine/6-31+G**
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.097 |
-0.030 |
0.509 |
| C2 |
-0.723 |
-1.280 |
0.175 |
| H3 |
0.215 |
0.041 |
1.591 |
| Cl4 |
1.745 |
-0.273 |
-0.162 |
| Cl5 |
-0.662 |
1.459 |
-0.058 |
| O6 |
-1.834 |
-1.264 |
-0.298 |
| H7 |
-0.198 |
-2.217 |
0.430 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
Cl4 |
Cl5 |
O6 |
H7 |
| C1 | | 1.5319 | 1.0899 | 1.7958 | 1.7653 | 2.4299 | 2.2079 |
C2 | 1.5319 | | 2.1511 | 2.6868 | 2.7496 | 1.2078 | 1.1035 | H3 | 1.0899 | 2.1511 | | 2.3480 | 2.3447 | 3.0768 | 2.5720 | Cl4 | 1.7958 | 2.6868 | 2.3480 | | 2.9674 | 3.7162 | 2.8115 | Cl5 | 1.7653 | 2.7496 | 2.3447 | 2.9674 | | 2.9740 | 3.7369 | O6 | 2.4299 | 1.2078 | 3.0768 | 3.7162 | 2.9740 | | 2.0283 | H7 | 2.2079 | 1.1035 | 2.5720 | 2.8115 | 3.7369 | 2.0283 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
O6 |
124.553 |
|
C1 |
C2 |
H7 |
112.809 |
| C2 |
C1 |
H3 |
109.103 |
|
C2 |
C1 |
Cl4 |
107.419 |
| C2 |
C1 |
Cl5 |
112.813 |
|
H3 |
C1 |
Cl4 |
106.327 |
| H3 |
C1 |
Cl5 |
108.070 |
|
Cl4 |
C1 |
Cl5 |
112.870 |
| O6 |
C2 |
H7 |
122.629 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.250 |
|
|
|
| 2 |
C |
0.135 |
|
|
|
| 3 |
H |
0.244 |
|
|
|
| 4 |
Cl |
0.005 |
|
|
|
| 5 |
Cl |
0.031 |
|
|
|
| 6 |
O |
-0.315 |
|
|
|
| 7 |
H |
0.150 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.350 |
-0.843 |
1.968 |
2.531 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-48.996 |
-2.221 |
-1.279 |
| y |
-2.221 |
-42.257 |
-1.534 |
| z |
-1.279 |
-1.534 |
-40.897 |
|
| Traceless |
| | x | y | z |
| x |
-7.419 |
-2.221 |
-1.279 |
| y |
-2.221 |
2.689 |
-1.534 |
| z |
-1.279 |
-1.534 |
4.730 |
|
| Polar |
| 3z2-r2 | 9.459 |
| x2-y2 | -6.739 |
| xy | -2.221 |
| xz | -1.279 |
| yz | -1.534 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
8.906 |
-0.637 |
0.234 |
| y |
-0.637 |
7.697 |
-0.235 |
| z |
0.234 |
-0.235 |
5.470 |
<r2> (average value of r
2) Å
2
| <r2> |
187.577 |
| (<r2>)1/2 |
13.696 |