Jump to
S1C2
Energy calculated at B2PLYP=FULLultrafine/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -1072.788591 |
| Energy at 298.15K | |
| HF Energy | -1072.439202 |
| Nuclear repulsion energy | 263.653150 |
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/aug-cc-pVTZ
| 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' |
3183 |
3052 |
1.63 |
|
|
|
| 2 |
A' |
2989 |
2867 |
32.26 |
|
|
|
| 3 |
A' |
1790 |
1717 |
161.89 |
|
|
|
| 4 |
A' |
1406 |
1348 |
1.52 |
|
|
|
| 5 |
A' |
1236 |
1185 |
7.51 |
|
|
|
| 6 |
A' |
1074 |
1031 |
26.67 |
|
|
|
| 7 |
A' |
786 |
754 |
20.29 |
|
|
|
| 8 |
A' |
440 |
422 |
4.15 |
|
|
|
| 9 |
A' |
325 |
312 |
22.25 |
|
|
|
| 10 |
A' |
252 |
242 |
1.86 |
|
|
|
| 11 |
A" |
1245 |
1194 |
21.43 |
|
|
|
| 12 |
A" |
1020 |
978 |
19.31 |
|
|
|
| 13 |
A" |
727 |
697 |
111.43 |
|
|
|
| 14 |
A" |
284 |
272 |
4.53 |
|
|
|
| 15 |
A" |
85 |
81 |
7.92 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8420.2 cm
-1
Scaled (by 0.9591) Zero Point Vibrational Energy (zpe) 8075.8 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 B2PLYP=FULLultrafine/aug-cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.393 |
-0.018 |
0.000 |
| C2 |
-0.171 |
1.390 |
0.000 |
| H3 |
1.474 |
-0.010 |
0.000 |
| Cl4 |
-0.171 |
-0.840 |
1.475 |
| Cl5 |
-0.171 |
-0.840 |
-1.475 |
| O6 |
0.534 |
2.362 |
0.000 |
| H7 |
-1.270 |
1.438 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
Cl4 |
Cl5 |
O6 |
H7 |
| C1 | | 1.5171 | 1.0811 | 1.7803 | 1.7803 | 2.3848 | 2.2109 |
C2 | 1.5171 | | 2.1604 | 2.6737 | 2.6737 | 1.2012 | 1.1003 | H3 | 1.0811 | 2.1604 | | 2.3604 | 2.3604 | 2.5521 | 3.1032 | Cl4 | 1.7803 | 2.6737 | 2.3604 | | 2.9500 | 3.5956 | 2.9280 | Cl5 | 1.7803 | 2.6737 | 2.3604 | 2.9500 | | 3.5956 | 2.9280 | O6 | 2.3848 | 1.2012 | 2.5521 | 3.5956 | 3.5956 | | 2.0274 | H7 | 2.2109 | 1.1003 | 3.1032 | 2.9280 | 2.9280 | 2.0274 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
O6 |
122.218 |
|
C1 |
C2 |
H7 |
114.335 |
| C2 |
C1 |
H3 |
111.405 |
|
C2 |
C1 |
Cl4 |
108.095 |
| C2 |
C1 |
Cl5 |
108.095 |
|
H3 |
C1 |
Cl4 |
108.687 |
| H3 |
C1 |
Cl5 |
108.687 |
|
Cl4 |
C1 |
Cl5 |
111.898 |
| O6 |
C2 |
H7 |
123.447 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.276 |
|
|
|
| 2 |
C |
0.017 |
|
|
|
| 3 |
H |
0.243 |
|
|
|
| 4 |
Cl |
-0.232 |
|
|
|
| 5 |
Cl |
-0.232 |
|
|
|
| 6 |
O |
-0.549 |
|
|
|
| 7 |
H |
0.476 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.380 |
-0.919 |
0.000 |
0.995 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-41.269 |
-3.032 |
0.005 |
| y |
-3.032 |
-49.102 |
0.022 |
| z |
0.005 |
0.022 |
-43.027 |
|
| Traceless |
| | x | y | z |
| x |
4.795 |
-3.032 |
0.005 |
| y |
-3.032 |
-6.953 |
0.022 |
| z |
0.005 |
0.022 |
2.158 |
|
| Polar |
| 3z2-r2 | 4.316 |
| x2-y2 | 7.832 |
| xy | -3.032 |
| xz | 0.005 |
| yz | 0.022 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.222 |
0.616 |
0.000 |
| y |
0.616 |
9.173 |
-0.000 |
| z |
0.000 |
-0.000 |
9.208 |
<r2> (average value of r
2) Å
2
| <r2> |
192.215 |
| (<r2>)1/2 |
13.864 |
Jump to
S1C1
Energy calculated at B2PLYP=FULLultrafine/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -1072.785326 |
| Energy at 298.15K | |
| HF Energy | -1072.435782 |
| Nuclear repulsion energy | 266.326399 |
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/aug-cc-pVTZ
| 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 |
3129 |
3001 |
5.24 |
78.70 |
0.15 |
0.26 |
| 2 |
A |
2972 |
2850 |
45.65 |
135.09 |
0.27 |
0.43 |
| 3 |
A |
1803 |
1729 |
131.86 |
18.62 |
0.39 |
0.56 |
| 4 |
A |
1402 |
1345 |
11.94 |
3.21 |
0.30 |
0.47 |
| 5 |
A |
1276 |
1224 |
9.65 |
2.14 |
0.75 |
0.86 |
| 6 |
A |
1223 |
1173 |
11.24 |
4.60 |
0.67 |
0.80 |
| 7 |
A |
1036 |
994 |
14.66 |
1.86 |
0.34 |
0.51 |
| 8 |
A |
940 |
902 |
8.39 |
3.01 |
0.56 |
0.72 |
| 9 |
A |
808 |
774 |
72.71 |
5.81 |
0.71 |
0.83 |
| 10 |
A |
646 |
620 |
33.23 |
14.27 |
0.07 |
0.13 |
| 11 |
A |
615 |
590 |
34.05 |
6.18 |
0.43 |
0.60 |
| 12 |
A |
343 |
329 |
1.76 |
3.57 |
0.12 |
0.21 |
| 13 |
A |
273 |
262 |
3.38 |
3.18 |
0.59 |
0.74 |
| 14 |
A |
218 |
209 |
2.75 |
0.98 |
0.65 |
0.78 |
| 15 |
A |
86 |
82 |
10.11 |
1.33 |
0.73 |
0.84 |
Unscaled Zero Point Vibrational Energy (zpe) 8384.6 cm
-1
Scaled (by 0.9591) Zero Point Vibrational Energy (zpe) 8041.7 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 B2PLYP=FULLultrafine/aug-cc-pVTZ
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.095 |
-0.021 |
0.521 |
| C2 |
-0.701 |
-1.283 |
0.201 |
| H3 |
0.225 |
0.065 |
1.595 |
| Cl4 |
1.732 |
-0.251 |
-0.169 |
| Cl5 |
-0.684 |
1.446 |
-0.058 |
| O6 |
-1.779 |
-1.295 |
-0.321 |
| H7 |
-0.175 |
-2.201 |
0.507 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
Cl4 |
Cl5 |
O6 |
H7 |
| C1 | | 1.5256 | 1.0851 | 1.7914 | 1.7594 | 2.4171 | 2.1961 |
C2 | 1.5256 | | 2.1493 | 2.6680 | 2.7415 | 1.1977 | 1.1014 | H3 | 1.0851 | 2.1493 | | 2.3411 | 2.3380 | 3.0885 | 2.5455 | Cl4 | 1.7914 | 2.6680 | 2.3411 | | 2.9544 | 3.6656 | 2.8091 | Cl5 | 1.7594 | 2.7415 | 2.3380 | 2.9544 | | 2.9637 | 3.7255 | O6 | 2.4171 | 1.1977 | 3.0885 | 3.6656 | 2.9637 | | 2.0197 | H7 | 2.1961 | 1.1014 | 2.5455 | 2.8091 | 3.7255 | 2.0197 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
O6 |
124.706 |
|
C1 |
C2 |
H7 |
112.432 |
| C2 |
C1 |
H3 |
109.678 |
|
C2 |
C1 |
Cl4 |
106.824 |
| C2 |
C1 |
Cl5 |
112.946 |
|
H3 |
C1 |
Cl4 |
106.352 |
| H3 |
C1 |
Cl5 |
108.208 |
|
Cl4 |
C1 |
Cl5 |
112.615 |
| O6 |
C2 |
H7 |
122.861 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.194 |
|
|
|
| 2 |
C |
0.018 |
|
|
|
| 3 |
H |
0.237 |
|
|
|
| 4 |
Cl |
-0.222 |
|
|
|
| 5 |
Cl |
-0.188 |
|
|
|
| 6 |
O |
-0.500 |
|
|
|
| 7 |
H |
0.460 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.324 |
-0.693 |
1.931 |
2.441 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-48.002 |
-2.228 |
-1.336 |
| y |
-2.228 |
-42.166 |
-1.661 |
| z |
-1.336 |
-1.661 |
-40.653 |
|
| Traceless |
| | x | y | z |
| x |
-6.592 |
-2.228 |
-1.336 |
| y |
-2.228 |
2.161 |
-1.661 |
| z |
-1.336 |
-1.661 |
4.431 |
|
| Polar |
| 3z2-r2 | 8.862 |
| x2-y2 | -5.836 |
| xy | -2.228 |
| xz | -1.336 |
| yz | -1.661 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
9.814 |
-0.525 |
0.212 |
| y |
-0.525 |
8.812 |
-0.209 |
| z |
0.212 |
-0.209 |
6.654 |
<r2> (average value of r
2) Å
2
| <r2> |
185.379 |
| (<r2>)1/2 |
13.615 |