Jump to
S1C2
Energy calculated at HSEh1PBE/6-311G*
| hartrees |
Energy at 0K | -3112.424408 |
Energy at 298.15K | |
HF Energy | -3112.424408 |
Nuclear repulsion energy | 288.979842 |
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 HSEh1PBE/6-311G*
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' |
3134 |
3007 |
12.30 |
17.73 |
0.07 |
0.12 |
2 |
A' |
3123 |
2997 |
2.35 |
145.49 |
0.07 |
0.13 |
3 |
A' |
1500 |
1439 |
0.99 |
12.97 |
0.73 |
0.85 |
4 |
A' |
1497 |
1437 |
7.85 |
1.70 |
0.73 |
0.85 |
5 |
A' |
1345 |
1290 |
3.00 |
14.86 |
0.65 |
0.79 |
6 |
A' |
1253 |
1202 |
45.40 |
3.01 |
0.53 |
0.69 |
7 |
A' |
1090 |
1046 |
1.14 |
8.97 |
0.73 |
0.84 |
8 |
A' |
754 |
723 |
32.06 |
54.05 |
0.29 |
0.45 |
9 |
A' |
656 |
630 |
60.61 |
14.57 |
0.25 |
0.40 |
10 |
A' |
251 |
241 |
0.86 |
4.17 |
0.39 |
0.56 |
11 |
A' |
195 |
187 |
7.97 |
0.14 |
0.31 |
0.48 |
12 |
A" |
3209 |
3079 |
3.40 |
4.22 |
0.75 |
0.86 |
13 |
A" |
3183 |
3055 |
0.61 |
97.19 |
0.75 |
0.86 |
14 |
A" |
1314 |
1261 |
0.23 |
5.60 |
0.75 |
0.86 |
15 |
A" |
1156 |
1109 |
4.88 |
0.07 |
0.75 |
0.86 |
16 |
A" |
993 |
953 |
0.18 |
6.15 |
0.75 |
0.86 |
17 |
A" |
775 |
744 |
5.78 |
0.03 |
0.75 |
0.86 |
18 |
A" |
117 |
112 |
5.72 |
0.02 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12771.0 cm
-1
Scaled (by 0.9596) Zero Point Vibrational Energy (zpe) 12255.0 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 HSEh1PBE/6-311G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.642 |
0.000 |
C2 |
1.231 |
-0.225 |
0.000 |
Br3 |
-1.587 |
-0.496 |
0.000 |
Cl4 |
2.689 |
0.825 |
0.000 |
H5 |
-0.059 |
1.265 |
0.890 |
H6 |
-0.059 |
1.265 |
-0.890 |
H7 |
1.284 |
-0.851 |
0.889 |
H8 |
1.284 |
-0.851 |
-0.889 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5057 | 1.9530 | 2.6956 | 1.0879 | 1.0879 | 2.1601 | 2.1601 |
C2 | 1.5057 | | 2.8315 | 1.7967 | 2.1622 | 2.1622 | 1.0884 | 1.0884 | Br3 | 1.9530 | 2.8315 | | 4.4760 | 2.4958 | 2.4958 | 3.0263 | 3.0263 | Cl4 | 2.6956 | 1.7967 | 4.4760 | | 2.9219 | 2.9219 | 2.3609 | 2.3609 | H5 | 1.0879 | 2.1622 | 2.4958 | 2.9219 | | 1.7798 | 2.5056 | 3.0728 | H6 | 1.0879 | 2.1622 | 2.4958 | 2.9219 | 1.7798 | | 3.0728 | 2.5056 | H7 | 2.1601 | 1.0884 | 3.0263 | 2.3609 | 2.5056 | 3.0728 | | 1.7778 | H8 | 2.1601 | 1.0884 | 3.0263 | 2.3609 | 3.0728 | 2.5056 | 1.7778 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
109.107 |
|
C1 |
C2 |
H7 |
111.742 |
C1 |
C2 |
H8 |
111.742 |
|
C2 |
C1 |
Br3 |
109.222 |
C2 |
C1 |
Cl4 |
39.036 |
|
C2 |
C1 |
H6 |
111.948 |
Br3 |
C1 |
H5 |
106.847 |
|
Br3 |
C1 |
H6 |
106.847 |
Cl4 |
C2 |
H7 |
107.269 |
|
Cl4 |
C2 |
H8 |
107.269 |
H5 |
C1 |
H6 |
109.768 |
|
H7 |
C2 |
H8 |
109.510 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.542 |
|
|
|
2 |
C |
-0.517 |
|
|
|
3 |
Br |
-0.034 |
|
|
|
4 |
Cl |
-0.075 |
|
|
|
5 |
H |
0.292 |
|
|
|
6 |
H |
0.292 |
|
|
|
7 |
H |
0.291 |
|
|
|
8 |
H |
0.291 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.196 |
-0.061 |
0.000 |
0.206 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-50.869 |
-2.302 |
0.000 |
y |
-2.302 |
-43.699 |
0.000 |
z |
0.000 |
0.000 |
-43.854 |
|
Traceless |
| x | y | z |
x |
-7.093 |
-2.302 |
0.000 |
y |
-2.302 |
3.663 |
0.000 |
z |
0.000 |
0.000 |
3.430 |
|
Polar |
3z2-r2 | 6.861 |
x2-y2 | -7.171 |
xy | -2.302 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
10.550 |
2.208 |
0.000 |
y |
2.208 |
6.424 |
0.000 |
z |
0.000 |
0.000 |
4.862 |
<r2> (average value of r
2) Å
2
<r2> |
283.120 |
(<r2>)1/2 |
16.826 |
Jump to
S1C1
Energy calculated at HSEh1PBE/6-311G*
| hartrees |
Energy at 0K | -3112.421465 |
Energy at 298.15K | |
HF Energy | -3112.421465 |
Nuclear repulsion energy | 304.762342 |
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 HSEh1PBE/6-311G*
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 |
3184 |
3056 |
3.55 |
39.58 |
0.75 |
0.86 |
2 |
A |
3164 |
3037 |
2.11 |
94.18 |
0.75 |
0.86 |
3 |
A |
3113 |
2987 |
15.86 |
167.21 |
0.04 |
0.07 |
4 |
A |
3096 |
2971 |
11.18 |
106.44 |
0.23 |
0.37 |
5 |
A |
1481 |
1421 |
2.82 |
5.75 |
0.71 |
0.83 |
6 |
A |
1474 |
1414 |
13.15 |
12.98 |
0.74 |
0.85 |
7 |
A |
1360 |
1305 |
25.75 |
4.22 |
0.75 |
0.86 |
8 |
A |
1316 |
1263 |
47.59 |
1.73 |
0.56 |
0.72 |
9 |
A |
1236 |
1186 |
5.08 |
14.39 |
0.75 |
0.85 |
10 |
A |
1168 |
1121 |
3.33 |
5.58 |
0.74 |
0.85 |
11 |
A |
1063 |
1020 |
1.36 |
2.66 |
0.68 |
0.81 |
12 |
A |
948 |
910 |
11.10 |
7.05 |
0.42 |
0.59 |
13 |
A |
883 |
847 |
27.29 |
2.06 |
0.75 |
0.86 |
14 |
A |
690 |
662 |
22.76 |
9.09 |
0.43 |
0.60 |
15 |
A |
587 |
563 |
12.06 |
14.73 |
0.20 |
0.34 |
16 |
A |
390 |
374 |
7.43 |
2.45 |
0.71 |
0.83 |
17 |
A |
247 |
237 |
1.23 |
1.46 |
0.54 |
0.70 |
18 |
A |
101 |
97 |
0.52 |
1.82 |
0.74 |
0.85 |
Unscaled Zero Point Vibrational Energy (zpe) 12750.7 cm
-1
Scaled (by 0.9596) Zero Point Vibrational Energy (zpe) 12235.6 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 HSEh1PBE/6-311G*
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.012 |
1.097 |
-0.381 |
C2 |
1.282 |
0.897 |
0.400 |
Br3 |
-1.357 |
-0.224 |
0.036 |
Cl4 |
2.172 |
-0.575 |
-0.086 |
H5 |
-0.420 |
2.068 |
-0.134 |
H6 |
0.184 |
1.041 |
-1.454 |
H7 |
1.950 |
1.741 |
0.218 |
H8 |
1.089 |
0.820 |
1.469 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5048 | 1.9476 | 2.7480 | 1.0905 | 1.0885 | 2.1287 | 2.1588 |
C2 | 1.5048 | | 2.8900 | 1.7872 | 2.1342 | 2.1595 | 1.0921 | 1.0890 | Br3 | 1.9476 | 2.8900 | | 3.5480 | 2.4823 | 2.4888 | 3.8512 | 3.0211 | Cl4 | 2.7480 | 1.7872 | 3.5480 | | 3.7023 | 2.9039 | 2.3464 | 2.3532 | H5 | 1.0905 | 2.1342 | 2.4823 | 3.7023 | | 1.7784 | 2.4186 | 2.5310 | H6 | 1.0885 | 2.1595 | 2.4888 | 2.9039 | 1.7784 | | 2.5307 | 3.0679 | H7 | 2.1287 | 1.0921 | 3.8512 | 2.3464 | 2.4186 | 2.5307 | | 1.7765 | H8 | 2.1588 | 1.0890 | 3.0211 | 2.3532 | 2.5310 | 3.0679 | 1.7765 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
112.897 |
|
C1 |
C2 |
H7 |
109.076 |
C1 |
C2 |
H8 |
111.667 |
|
C2 |
C1 |
Br3 |
113.052 |
C2 |
C1 |
Cl4 |
36.808 |
|
C2 |
C1 |
H6 |
111.762 |
Br3 |
C1 |
H5 |
106.125 |
|
Br3 |
C1 |
H6 |
106.672 |
Cl4 |
C2 |
H7 |
106.654 |
|
Cl4 |
C2 |
H8 |
107.297 |
H5 |
C1 |
H6 |
109.405 |
|
H7 |
C2 |
H8 |
109.070 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.544 |
|
|
|
2 |
C |
-0.512 |
|
|
|
3 |
Br |
-0.022 |
|
|
|
4 |
Cl |
-0.062 |
|
|
|
5 |
H |
0.279 |
|
|
|
6 |
H |
0.293 |
|
|
|
7 |
H |
0.279 |
|
|
|
8 |
H |
0.291 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.277 |
2.802 |
0.113 |
2.818 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-48.205 |
2.915 |
0.398 |
y |
2.915 |
-40.763 |
-0.104 |
z |
0.398 |
-0.104 |
-43.491 |
|
Traceless |
| x | y | z |
x |
-6.078 |
2.915 |
0.398 |
y |
2.915 |
5.085 |
-0.104 |
z |
0.398 |
-0.104 |
0.994 |
|
Polar |
3z2-r2 | 1.987 |
x2-y2 | -7.442 |
xy | 2.915 |
xz | 0.398 |
yz | -0.104 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
8.326 |
0.259 |
-0.293 |
y |
0.259 |
7.327 |
0.075 |
z |
-0.293 |
0.075 |
5.211 |
<r2> (average value of r
2) Å
2
<r2> |
222.084 |
(<r2>)1/2 |
14.902 |