Jump to
S1C2
Energy calculated at B2PLYP=FULLultrafine/6-311G*
| | hartrees |
| Energy at 0K | -3112.430493 |
| Energy at 298.15K | |
| HF Energy | -3112.110978 |
| Nuclear repulsion energy | 287.622820 |
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/6-311G*
| 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' |
3144 |
3144 |
12.98 |
11.41 |
0.08 |
0.14 |
| 2 |
A' |
3135 |
3135 |
1.60 |
145.57 |
0.08 |
0.15 |
| 3 |
A' |
1518 |
1518 |
1.10 |
13.03 |
0.72 |
0.84 |
| 4 |
A' |
1517 |
1517 |
6.42 |
2.50 |
0.72 |
0.84 |
| 5 |
A' |
1361 |
1361 |
3.24 |
14.79 |
0.62 |
0.77 |
| 6 |
A' |
1268 |
1268 |
50.07 |
3.09 |
0.52 |
0.69 |
| 7 |
A' |
1081 |
1081 |
1.00 |
9.65 |
0.74 |
0.85 |
| 8 |
A' |
746 |
746 |
28.06 |
56.07 |
0.30 |
0.46 |
| 9 |
A' |
646 |
646 |
60.91 |
12.88 |
0.25 |
0.40 |
| 10 |
A' |
249 |
249 |
0.82 |
4.98 |
0.38 |
0.55 |
| 11 |
A' |
197 |
197 |
7.56 |
0.19 |
0.31 |
0.48 |
| 12 |
A" |
3219 |
3219 |
3.84 |
2.91 |
0.75 |
0.86 |
| 13 |
A" |
3196 |
3196 |
0.48 |
96.57 |
0.75 |
0.86 |
| 14 |
A" |
1326 |
1326 |
0.21 |
5.67 |
0.75 |
0.86 |
| 15 |
A" |
1166 |
1166 |
4.78 |
0.09 |
0.75 |
0.86 |
| 16 |
A" |
1004 |
1004 |
0.19 |
6.47 |
0.75 |
0.86 |
| 17 |
A" |
783 |
783 |
4.85 |
0.03 |
0.75 |
0.86 |
| 18 |
A" |
117 |
117 |
5.84 |
0.02 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12836.4 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 12836.4 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/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.644 |
0.000 |
| C2 |
1.238 |
-0.222 |
0.000 |
| Br3 |
-1.594 |
-0.505 |
0.000 |
| Cl4 |
2.700 |
0.841 |
0.000 |
| H5 |
-0.061 |
1.264 |
0.889 |
| H6 |
-0.061 |
1.264 |
-0.889 |
| H7 |
1.294 |
-0.844 |
0.889 |
| H8 |
1.294 |
-0.844 |
-0.889 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5108 | 1.9650 | 2.7071 | 1.0859 | 1.0859 | 2.1630 | 2.1630 |
C2 | 1.5108 | | 2.8459 | 1.8075 | 2.1651 | 2.1651 | 1.0862 | 1.0862 | Br3 | 1.9650 | 2.8459 | | 4.4998 | 2.5037 | 2.5037 | 3.0404 | 3.0404 | Cl4 | 2.7071 | 1.8075 | 4.4998 | | 2.9318 | 2.9318 | 2.3676 | 2.3676 | H5 | 1.0859 | 2.1651 | 2.5037 | 2.9318 | | 1.7789 | 2.5062 | 3.0729 | H6 | 1.0859 | 2.1651 | 2.5037 | 2.9318 | 1.7789 | | 3.0729 | 2.5062 | H7 | 2.1630 | 1.0862 | 3.0404 | 2.3676 | 2.5062 | 3.0729 | | 1.7773 | H8 | 2.1630 | 1.0862 | 3.0404 | 2.3676 | 3.0729 | 2.5062 | 1.7773 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
109.005 |
|
C1 |
C2 |
H7 |
111.751 |
| C1 |
C2 |
H8 |
111.751 |
|
C2 |
C1 |
Br3 |
109.230 |
| C2 |
C1 |
Cl4 |
39.146 |
|
C2 |
C1 |
H6 |
111.939 |
| Br3 |
C1 |
H5 |
106.731 |
|
Br3 |
C1 |
H6 |
106.731 |
| Cl4 |
C2 |
H7 |
107.162 |
|
Cl4 |
C2 |
H8 |
107.162 |
| H5 |
C1 |
H6 |
109.998 |
|
H7 |
C2 |
H8 |
109.793 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.498 |
|
|
|
| 2 |
C |
-0.474 |
|
|
|
| 3 |
Br |
-0.046 |
|
|
|
| 4 |
Cl |
-0.085 |
|
|
|
| 5 |
H |
0.276 |
|
|
|
| 6 |
H |
0.276 |
|
|
|
| 7 |
H |
0.275 |
|
|
|
| 8 |
H |
0.275 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.187 |
-0.063 |
0.000 |
0.198 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-51.378 |
-2.386 |
-0.009 |
| y |
-2.386 |
-44.084 |
-0.003 |
| z |
-0.009 |
-0.003 |
-44.168 |
|
| Traceless |
| | x | y | z |
| x |
-7.252 |
-2.386 |
-0.009 |
| y |
-2.386 |
3.689 |
-0.003 |
| z |
-0.009 |
-0.003 |
3.563 |
|
| Polar |
| 3z2-r2 | 7.125 |
| x2-y2 | -7.294 |
| xy | -2.386 |
| xz | -0.009 |
| yz | -0.003 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
10.477 |
2.275 |
0.000 |
| y |
2.275 |
6.422 |
0.000 |
| z |
0.000 |
0.000 |
4.829 |
<r2> (average value of r
2) Å
2
| <r2> |
285.976 |
| (<r2>)1/2 |
16.911 |
Jump to
S1C1
Energy calculated at B2PLYP=FULLultrafine/6-311G*
| | hartrees |
| Energy at 0K | -3112.427310 |
| Energy at 298.15K | |
| HF Energy | -3112.107604 |
| Nuclear repulsion energy | 303.386284 |
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/6-311G*
| 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 |
3193 |
3193 |
4.04 |
36.62 |
0.75 |
0.86 |
| 2 |
A |
3175 |
3175 |
1.97 |
93.80 |
0.75 |
0.86 |
| 3 |
A |
3122 |
3122 |
17.26 |
164.20 |
0.04 |
0.07 |
| 4 |
A |
3106 |
3106 |
10.41 |
95.50 |
0.26 |
0.41 |
| 5 |
A |
1501 |
1501 |
2.06 |
6.21 |
0.69 |
0.82 |
| 6 |
A |
1495 |
1495 |
11.03 |
12.94 |
0.73 |
0.85 |
| 7 |
A |
1375 |
1375 |
28.04 |
3.40 |
0.74 |
0.85 |
| 8 |
A |
1333 |
1333 |
50.21 |
1.87 |
0.58 |
0.73 |
| 9 |
A |
1243 |
1243 |
5.17 |
13.92 |
0.74 |
0.85 |
| 10 |
A |
1177 |
1177 |
3.31 |
5.65 |
0.74 |
0.85 |
| 11 |
A |
1061 |
1061 |
1.12 |
2.61 |
0.74 |
0.85 |
| 12 |
A |
955 |
955 |
10.39 |
7.03 |
0.43 |
0.60 |
| 13 |
A |
891 |
891 |
24.14 |
2.00 |
0.74 |
0.85 |
| 14 |
A |
683 |
683 |
23.12 |
10.48 |
0.43 |
0.60 |
| 15 |
A |
579 |
579 |
12.21 |
15.87 |
0.21 |
0.34 |
| 16 |
A |
391 |
391 |
7.27 |
2.71 |
0.71 |
0.83 |
| 17 |
A |
247 |
247 |
1.19 |
1.51 |
0.53 |
0.69 |
| 18 |
A |
102 |
102 |
0.54 |
1.93 |
0.74 |
0.85 |
Unscaled Zero Point Vibrational Energy (zpe) 12814.0 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 12814.0 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 B2PLYP=FULLultrafine/6-311G*
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.014 |
1.101 |
-0.385 |
| C2 |
1.287 |
0.900 |
0.404 |
| Br3 |
-1.364 |
-0.225 |
0.036 |
| Cl4 |
2.184 |
-0.577 |
-0.086 |
| H5 |
-0.417 |
2.070 |
-0.141 |
| H6 |
0.191 |
1.038 |
-1.455 |
| H7 |
1.953 |
1.744 |
0.224 |
| H8 |
1.089 |
0.819 |
1.470 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5108 | 1.9582 | 2.7590 | 1.0887 | 1.0865 | 2.1316 | 2.1622 |
C2 | 1.5108 | | 2.9036 | 1.7965 | 2.1375 | 2.1630 | 1.0901 | 1.0870 | Br3 | 1.9582 | 2.9036 | | 3.5684 | 2.4895 | 2.4970 | 3.8623 | 3.0277 | Cl4 | 2.7590 | 1.7965 | 3.5684 | | 3.7115 | 2.9078 | 2.3527 | 2.3603 | H5 | 1.0887 | 2.1375 | 2.4895 | 3.7115 | | 1.7779 | 2.4199 | 2.5356 | H6 | 1.0865 | 2.1630 | 2.4970 | 2.9078 | 1.7779 | | 2.5348 | 3.0679 | H7 | 2.1316 | 1.0901 | 3.8623 | 2.3527 | 2.4199 | 2.5348 | | 1.7760 | H8 | 2.1622 | 1.0870 | 3.0277 | 2.3603 | 2.5356 | 3.0679 | 1.7760 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
112.783 |
|
C1 |
C2 |
H7 |
109.009 |
| C1 |
C2 |
H8 |
111.637 |
|
C2 |
C1 |
Br3 |
113.017 |
| C2 |
C1 |
Cl4 |
36.894 |
|
C2 |
C1 |
H6 |
111.731 |
| Br3 |
C1 |
H5 |
106.034 |
|
Br3 |
C1 |
H6 |
106.655 |
| Cl4 |
C2 |
H7 |
106.606 |
|
Cl4 |
C2 |
H8 |
107.311 |
| H5 |
C1 |
H6 |
109.637 |
|
H7 |
C2 |
H8 |
109.329 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.502 |
|
|
|
| 2 |
C |
-0.472 |
|
|
|
| 3 |
Br |
-0.033 |
|
|
|
| 4 |
Cl |
-0.071 |
|
|
|
| 5 |
H |
0.263 |
|
|
|
| 6 |
H |
0.277 |
|
|
|
| 7 |
H |
0.263 |
|
|
|
| 8 |
H |
0.275 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.279 |
2.800 |
0.113 |
2.816 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-48.636 |
2.923 |
0.395 |
| y |
2.923 |
-41.139 |
-0.087 |
| z |
0.395 |
-0.087 |
-43.815 |
|
| Traceless |
| | x | y | z |
| x |
-6.159 |
2.923 |
0.395 |
| y |
2.923 |
5.087 |
-0.087 |
| z |
0.395 |
-0.087 |
1.072 |
|
| Polar |
| 3z2-r2 | 2.144 |
| x2-y2 | -7.498 |
| xy | 2.923 |
| xz | 0.395 |
| yz | -0.087 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
8.261 |
0.260 |
-0.327 |
| y |
0.260 |
7.318 |
0.077 |
| z |
-0.327 |
0.077 |
5.176 |
<r2> (average value of r
2) Å
2
| <r2> |
224.257 |
| (<r2>)1/2 |
14.975 |