Jump to
S1C2
Energy calculated at B2PLYP/6-311G**
| | hartrees |
| Energy at 0K | -3112.302503 |
| Energy at 298.15K | |
| HF Energy | -3112.116326 |
| Nuclear repulsion energy | 287.556380 |
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/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' |
3136 |
3136 |
10.93 |
11.45 |
0.07 |
0.13 |
| 2 |
A' |
3127 |
3127 |
1.39 |
152.47 |
0.07 |
0.13 |
| 3 |
A' |
1504 |
1504 |
0.19 |
13.94 |
0.72 |
0.84 |
| 4 |
A' |
1500 |
1500 |
5.74 |
0.54 |
0.73 |
0.84 |
| 5 |
A' |
1349 |
1349 |
3.49 |
14.21 |
0.62 |
0.76 |
| 6 |
A' |
1256 |
1256 |
50.86 |
3.11 |
0.51 |
0.68 |
| 7 |
A' |
1077 |
1077 |
0.99 |
9.60 |
0.74 |
0.85 |
| 8 |
A' |
747 |
747 |
28.20 |
54.41 |
0.30 |
0.46 |
| 9 |
A' |
647 |
647 |
59.25 |
12.72 |
0.25 |
0.40 |
| 10 |
A' |
250 |
250 |
0.82 |
4.96 |
0.38 |
0.55 |
| 11 |
A' |
196 |
196 |
7.33 |
0.19 |
0.32 |
0.48 |
| 12 |
A" |
3211 |
3211 |
2.59 |
3.18 |
0.75 |
0.86 |
| 13 |
A" |
3187 |
3187 |
0.43 |
94.55 |
0.75 |
0.86 |
| 14 |
A" |
1312 |
1312 |
0.20 |
5.06 |
0.75 |
0.86 |
| 15 |
A" |
1152 |
1152 |
4.08 |
0.09 |
0.75 |
0.86 |
| 16 |
A" |
995 |
995 |
0.16 |
5.93 |
0.75 |
0.86 |
| 17 |
A" |
781 |
781 |
4.24 |
0.03 |
0.75 |
0.86 |
| 18 |
A" |
116 |
116 |
5.59 |
0.02 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12770.0 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 12770.0 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/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.644 |
0.000 |
| C2 |
1.239 |
-0.223 |
0.000 |
| Br3 |
-1.595 |
-0.504 |
0.000 |
| Cl4 |
2.701 |
0.839 |
0.000 |
| H5 |
-0.061 |
1.262 |
0.891 |
| H6 |
-0.061 |
1.262 |
-0.891 |
| H7 |
1.294 |
-0.844 |
0.890 |
| H8 |
1.294 |
-0.844 |
-0.890 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5122 | 1.9648 | 2.7083 | 1.0863 | 1.0863 | 2.1633 | 2.1633 |
C2 | 1.5122 | | 2.8481 | 1.8069 | 2.1657 | 2.1657 | 1.0866 | 1.0866 | Br3 | 1.9648 | 2.8481 | | 4.5011 | 2.5030 | 2.5030 | 3.0420 | 3.0420 | Cl4 | 2.7083 | 1.8069 | 4.5011 | | 2.9331 | 2.9331 | 2.3676 | 2.3676 | H5 | 1.0863 | 2.1657 | 2.5030 | 2.9331 | | 1.7816 | 2.5047 | 3.0731 | H6 | 1.0863 | 2.1657 | 2.5030 | 2.9331 | 1.7816 | | 3.0731 | 2.5047 | H7 | 2.1633 | 1.0866 | 3.0420 | 2.3676 | 2.5047 | 3.0731 | | 1.7797 | H8 | 2.1633 | 1.0866 | 3.0420 | 2.3676 | 3.0731 | 2.5047 | 1.7797 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
109.040 |
|
C1 |
C2 |
H7 |
111.648 |
| C1 |
C2 |
H8 |
111.648 |
|
C2 |
C1 |
Br3 |
109.308 |
| C2 |
C1 |
Cl4 |
39.102 |
|
C2 |
C1 |
H6 |
111.870 |
| Br3 |
C1 |
H5 |
106.670 |
|
Br3 |
C1 |
H6 |
106.670 |
| Cl4 |
C2 |
H7 |
107.174 |
|
Cl4 |
C2 |
H8 |
107.174 |
| H5 |
C1 |
H6 |
110.180 |
|
H7 |
C2 |
H8 |
109.948 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.286 |
|
|
|
| 2 |
C |
-0.268 |
|
|
|
| 3 |
Br |
-0.064 |
|
|
|
| 4 |
Cl |
-0.099 |
|
|
|
| 5 |
H |
0.179 |
|
|
|
| 6 |
H |
0.179 |
|
|
|
| 7 |
H |
0.180 |
|
|
|
| 8 |
H |
0.180 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.188 |
-0.069 |
0.000 |
0.200 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-51.160 |
-2.338 |
-0.009 |
| y |
-2.338 |
-44.062 |
-0.003 |
| z |
-0.009 |
-0.003 |
-44.180 |
|
| Traceless |
| | x | y | z |
| x |
-7.039 |
-2.338 |
-0.009 |
| y |
-2.338 |
3.608 |
-0.003 |
| z |
-0.009 |
-0.003 |
3.432 |
|
| Polar |
| 3z2-r2 | 6.863 |
| x2-y2 | -7.098 |
| xy | -2.338 |
| xz | -0.009 |
| yz | -0.003 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
10.557 |
2.270 |
0.000 |
| y |
2.270 |
6.480 |
0.000 |
| z |
0.000 |
0.000 |
4.877 |
<r2> (average value of r
2) Å
2
| <r2> |
286.088 |
| (<r2>)1/2 |
16.914 |
Jump to
S1C1
Energy calculated at B2PLYP/6-311G**
| | hartrees |
| Energy at 0K | -3112.299441 |
| Energy at 298.15K | |
| HF Energy | -3112.113112 |
| Nuclear repulsion energy | 303.341172 |
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/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 |
3185 |
3185 |
2.88 |
37.14 |
0.75 |
0.86 |
| 2 |
A |
3168 |
3168 |
1.61 |
92.30 |
0.75 |
0.86 |
| 3 |
A |
3114 |
3114 |
14.86 |
171.49 |
0.03 |
0.07 |
| 4 |
A |
3099 |
3099 |
9.25 |
96.04 |
0.24 |
0.39 |
| 5 |
A |
1485 |
1485 |
1.30 |
5.57 |
0.68 |
0.81 |
| 6 |
A |
1477 |
1477 |
9.60 |
12.73 |
0.74 |
0.85 |
| 7 |
A |
1363 |
1363 |
27.64 |
2.92 |
0.75 |
0.86 |
| 8 |
A |
1319 |
1319 |
51.20 |
1.98 |
0.57 |
0.73 |
| 9 |
A |
1230 |
1230 |
4.82 |
12.87 |
0.74 |
0.85 |
| 10 |
A |
1165 |
1165 |
2.77 |
5.24 |
0.74 |
0.85 |
| 11 |
A |
1056 |
1056 |
1.36 |
2.49 |
0.74 |
0.85 |
| 12 |
A |
950 |
950 |
9.54 |
6.76 |
0.44 |
0.61 |
| 13 |
A |
885 |
885 |
22.30 |
2.01 |
0.74 |
0.85 |
| 14 |
A |
684 |
684 |
23.00 |
10.42 |
0.43 |
0.60 |
| 15 |
A |
579 |
579 |
11.97 |
15.77 |
0.21 |
0.34 |
| 16 |
A |
390 |
390 |
7.14 |
2.68 |
0.71 |
0.83 |
| 17 |
A |
246 |
246 |
1.15 |
1.52 |
0.53 |
0.69 |
| 18 |
A |
102 |
102 |
0.52 |
1.95 |
0.73 |
0.85 |
Unscaled Zero Point Vibrational Energy (zpe) 12747.1 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 12747.1 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/6-311G**
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.014 |
1.101 |
-0.385 |
| C2 |
1.288 |
0.901 |
0.404 |
| Br3 |
-1.365 |
-0.225 |
0.036 |
| Cl4 |
2.184 |
-0.577 |
-0.086 |
| H5 |
-0.417 |
2.070 |
-0.138 |
| H6 |
0.190 |
1.037 |
-1.455 |
| H7 |
1.954 |
1.744 |
0.220 |
| H8 |
1.090 |
0.819 |
1.470 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5121 | 1.9583 | 2.7598 | 1.0891 | 1.0869 | 2.1317 | 2.1626 |
C2 | 1.5121 | | 2.9052 | 1.7963 | 2.1378 | 2.1640 | 1.0904 | 1.0874 | Br3 | 1.9583 | 2.9052 | | 3.5686 | 2.4889 | 2.4962 | 3.8633 | 3.0284 | Cl4 | 2.7598 | 1.7963 | 3.5686 | | 3.7120 | 2.9082 | 2.3526 | 2.3601 | H5 | 1.0891 | 2.1378 | 2.4889 | 3.7120 | | 1.7812 | 2.4203 | 2.5338 | H6 | 1.0869 | 2.1640 | 2.4962 | 2.9082 | 1.7812 | | 2.5340 | 3.0684 | H7 | 2.1317 | 1.0904 | 3.8633 | 2.3526 | 2.4203 | 2.5340 | | 1.7790 | H8 | 2.1626 | 1.0874 | 3.0284 | 2.3601 | 2.5338 | 3.0684 | 1.7790 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
112.779 |
|
C1 |
C2 |
H7 |
108.914 |
| C1 |
C2 |
H8 |
111.553 |
|
C2 |
C1 |
Br3 |
113.049 |
| C2 |
C1 |
Cl4 |
36.879 |
|
C2 |
C1 |
H6 |
111.692 |
| Br3 |
C1 |
H5 |
105.968 |
|
Br3 |
C1 |
H6 |
106.579 |
| Cl4 |
C2 |
H7 |
106.600 |
|
Cl4 |
C2 |
H8 |
107.292 |
| H5 |
C1 |
H6 |
109.886 |
|
H7 |
C2 |
H8 |
109.552 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.288 |
|
|
|
| 2 |
C |
-0.264 |
|
|
|
| 3 |
Br |
-0.051 |
|
|
|
| 4 |
Cl |
-0.085 |
|
|
|
| 5 |
H |
0.164 |
|
|
|
| 6 |
H |
0.179 |
|
|
|
| 7 |
H |
0.166 |
|
|
|
| 8 |
H |
0.178 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.270 |
2.744 |
0.113 |
2.760 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-48.498 |
2.876 |
0.407 |
| y |
2.876 |
-41.177 |
-0.087 |
| z |
0.407 |
-0.087 |
-43.813 |
|
| Traceless |
| | x | y | z |
| x |
-6.003 |
2.876 |
0.407 |
| y |
2.876 |
4.978 |
-0.087 |
| z |
0.407 |
-0.087 |
1.025 |
|
| Polar |
| 3z2-r2 | 2.050 |
| x2-y2 | -7.321 |
| xy | 2.876 |
| xz | 0.407 |
| yz | -0.087 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
8.338 |
0.261 |
-0.318 |
| y |
0.261 |
7.381 |
0.076 |
| z |
-0.318 |
0.076 |
5.229 |
<r2> (average value of r
2) Å
2
| <r2> |
224.290 |
| (<r2>)1/2 |
14.976 |