Jump to
S1C2
Energy calculated at TPSSh/3-21G*
| | hartrees |
| Energy at 0K | -5202.020843 |
| Energy at 298.15K | |
| HF Energy | -5202.020843 |
| Nuclear repulsion energy | 416.091952 |
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 TPSSh/3-21G*
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Ag |
3120 |
3013 |
0.00 |
139.76 |
0.07 |
0.13 |
| 2 |
Ag |
1534 |
1481 |
0.00 |
20.10 |
0.75 |
0.86 |
| 3 |
Ag |
1303 |
1258 |
0.00 |
26.96 |
0.46 |
0.63 |
| 4 |
Ag |
1030 |
994 |
0.00 |
13.14 |
0.71 |
0.83 |
| 5 |
Ag |
668 |
645 |
0.00 |
93.12 |
0.29 |
0.45 |
| 6 |
Ag |
189 |
183 |
0.00 |
4.06 |
0.33 |
0.49 |
| 7 |
Au |
3208 |
3098 |
1.35 |
0.00 |
0.00 |
0.00 |
| 8 |
Au |
1129 |
1090 |
3.58 |
0.00 |
0.00 |
0.00 |
| 9 |
Au |
774 |
748 |
7.40 |
0.00 |
0.00 |
0.00 |
| 10 |
Au |
107 |
104 |
3.97 |
0.00 |
0.00 |
0.00 |
| 11 |
Bg |
3182 |
3072 |
0.00 |
92.44 |
0.75 |
0.86 |
| 12 |
Bg |
1324 |
1279 |
0.00 |
9.54 |
0.75 |
0.86 |
| 13 |
Bg |
946 |
914 |
0.00 |
9.64 |
0.75 |
0.86 |
| 14 |
Bu |
3129 |
3021 |
6.33 |
0.00 |
0.00 |
0.00 |
| 15 |
Bu |
1533 |
1480 |
10.52 |
0.00 |
0.00 |
0.00 |
| 16 |
Bu |
1238 |
1195 |
45.63 |
0.00 |
0.00 |
0.00 |
| 17 |
Bu |
611 |
590 |
73.57 |
0.00 |
0.00 |
0.00 |
| 18 |
Bu |
175 |
169 |
7.90 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 12599.0 cm
-1
Scaled (by 0.9657) Zero Point Vibrational Energy (zpe) 12166.9 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 TPSSh/3-21G*
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.506 |
0.568 |
0.000 |
| C2 |
-0.506 |
-0.568 |
0.000 |
| Br3 |
-0.506 |
2.263 |
0.000 |
| Br4 |
0.506 |
-2.263 |
0.000 |
| H5 |
1.122 |
0.564 |
0.899 |
| H6 |
1.122 |
0.564 |
-0.899 |
| H7 |
-1.122 |
-0.564 |
0.899 |
| H8 |
-1.122 |
-0.564 |
-0.899 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5216 | 1.9736 | 2.8316 | 1.0900 | 1.0900 | 2.1777 | 2.1777 |
C2 | 1.5216 | | 2.8316 | 1.9736 | 2.1777 | 2.1777 | 1.0900 | 1.0900 | Br3 | 1.9736 | 2.8316 | | 4.6379 | 2.5188 | 2.5188 | 3.0304 | 3.0304 | Br4 | 2.8316 | 1.9736 | 4.6379 | | 3.0304 | 3.0304 | 2.5188 | 2.5188 | H5 | 1.0900 | 2.1777 | 2.5188 | 3.0304 | | 1.7976 | 2.5128 | 3.0895 | H6 | 1.0900 | 2.1777 | 2.5188 | 3.0304 | 1.7976 | | 3.0895 | 2.5128 | H7 | 2.1777 | 1.0900 | 3.0304 | 2.5188 | 2.5128 | 3.0895 | | 1.7976 | H8 | 2.1777 | 1.0900 | 3.0304 | 2.5188 | 3.0895 | 2.5128 | 1.7976 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
107.512 |
|
C1 |
C2 |
H7 |
111.923 |
| C1 |
C2 |
H8 |
111.923 |
|
C2 |
C1 |
Br3 |
107.512 |
| C2 |
C1 |
H5 |
111.923 |
|
C2 |
C1 |
H6 |
111.923 |
| Br3 |
C1 |
H5 |
107.041 |
|
Br3 |
C1 |
H6 |
107.041 |
| Br4 |
C2 |
H7 |
107.041 |
|
Br4 |
C2 |
H8 |
107.041 |
| H5 |
C1 |
H6 |
111.085 |
|
H7 |
C2 |
H8 |
111.085 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at TPSSh/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.471 |
|
|
|
| 2 |
C |
-0.471 |
|
|
|
| 3 |
Br |
-0.071 |
|
|
|
| 4 |
Br |
-0.071 |
|
|
|
| 5 |
H |
0.271 |
|
|
|
| 6 |
H |
0.271 |
|
|
|
| 7 |
H |
0.271 |
|
|
|
| 8 |
H |
0.271 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.243 |
-2.007 |
0.000 |
| y |
-2.007 |
11.728 |
0.000 |
| z |
0.000 |
0.000 |
5.240 |
<r2> (average value of r
2) Å
2
| <r2> |
424.330 |
| (<r2>)1/2 |
20.599 |
Jump to
S1C1
Energy calculated at TPSSh/3-21G*
| | hartrees |
| Energy at 0K | -5202.017209 |
| Energy at 298.15K | |
| HF Energy | -5202.017209 |
| Nuclear repulsion energy | 458.568232 |
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 TPSSh/3-21G*
| 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 |
3159 |
3051 |
0.12 |
99.80 |
0.75 |
0.86 |
| 2 |
A |
3097 |
2991 |
16.57 |
205.51 |
0.02 |
0.04 |
| 3 |
A |
1515 |
1463 |
0.12 |
7.95 |
0.67 |
0.80 |
| 4 |
A |
1336 |
1290 |
19.33 |
4.83 |
0.70 |
0.82 |
| 5 |
A |
1200 |
1159 |
2.39 |
20.94 |
0.75 |
0.86 |
| 6 |
A |
1005 |
970 |
1.23 |
3.29 |
0.75 |
0.86 |
| 7 |
A |
921 |
890 |
10.00 |
7.80 |
0.54 |
0.70 |
| 8 |
A |
578 |
558 |
8.66 |
17.44 |
0.09 |
0.17 |
| 9 |
A |
218 |
211 |
0.93 |
0.85 |
0.38 |
0.55 |
| 10 |
A |
82 |
79 |
0.14 |
0.82 |
0.73 |
0.84 |
| 11 |
B |
3176 |
3067 |
2.70 |
31.47 |
0.75 |
0.86 |
| 12 |
B |
3088 |
2982 |
2.20 |
62.48 |
0.75 |
0.86 |
| 13 |
B |
1516 |
1464 |
13.35 |
21.38 |
0.75 |
0.86 |
| 14 |
B |
1314 |
1269 |
42.95 |
0.51 |
0.75 |
0.86 |
| 15 |
B |
1154 |
1115 |
2.57 |
7.52 |
0.75 |
0.86 |
| 16 |
B |
852 |
823 |
20.92 |
0.73 |
0.75 |
0.86 |
| 17 |
B |
609 |
588 |
9.62 |
9.45 |
0.75 |
0.86 |
| 18 |
B |
353 |
341 |
6.35 |
3.00 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12586.7 cm
-1
Scaled (by 0.9657) Zero Point Vibrational Energy (zpe) 12155.0 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 TPSSh/3-21G*
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.306 |
0.698 |
1.246 |
| C2 |
-0.306 |
-0.698 |
1.246 |
| Br3 |
-0.306 |
1.724 |
-0.308 |
| Br4 |
0.306 |
-1.724 |
-0.308 |
| H5 |
-0.015 |
1.255 |
2.131 |
| H6 |
1.395 |
0.658 |
1.190 |
| H7 |
0.015 |
-1.255 |
2.131 |
| H8 |
-1.395 |
-0.658 |
1.190 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5249 | 1.9599 | 2.8779 | 1.0940 | 1.0908 | 2.1641 | 2.1762 |
C2 | 1.5249 | | 2.8779 | 1.9599 | 2.1641 | 2.1762 | 1.0940 | 1.0908 | Br3 | 1.9599 | 2.8779 | | 3.5018 | 2.5011 | 2.5046 | 3.8635 | 3.0174 | Br4 | 2.8779 | 1.9599 | 3.5018 | | 3.8635 | 3.0174 | 2.5011 | 2.5046 | H5 | 1.0940 | 2.1641 | 2.5011 | 3.8635 | | 1.7971 | 2.5097 | 2.5392 | H6 | 1.0908 | 2.1762 | 2.5046 | 3.0174 | 1.7971 | | 2.5392 | 3.0843 | H7 | 2.1641 | 1.0940 | 3.8635 | 2.5011 | 2.5097 | 2.5392 | | 1.7971 | H8 | 2.1762 | 1.0908 | 3.0174 | 2.5046 | 2.5392 | 3.0843 | 1.7971 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
110.727 |
|
C1 |
C2 |
H7 |
110.361 |
| C1 |
C2 |
H8 |
111.525 |
|
C2 |
C1 |
Br3 |
110.727 |
| C2 |
C1 |
H5 |
110.361 |
|
C2 |
C1 |
H6 |
111.525 |
| Br3 |
C1 |
H5 |
106.486 |
|
Br3 |
C1 |
H6 |
106.888 |
| Br4 |
C2 |
H7 |
106.486 |
|
Br4 |
C2 |
H8 |
106.888 |
| H5 |
C1 |
H6 |
110.682 |
|
H7 |
C2 |
H8 |
110.682 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at TPSSh/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.474 |
|
|
|
| 2 |
C |
-0.474 |
|
|
|
| 3 |
Br |
-0.055 |
|
|
|
| 4 |
Br |
-0.055 |
|
|
|
| 5 |
H |
0.260 |
|
|
|
| 6 |
H |
0.270 |
|
|
|
| 7 |
H |
0.260 |
|
|
|
| 8 |
H |
0.270 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
2.565 |
2.565 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.569 |
-0.748 |
0.000 |
| y |
-0.748 |
8.294 |
0.000 |
| z |
0.000 |
0.000 |
7.767 |
<r2> (average value of r
2) Å
2
| <r2> |
296.745 |
| (<r2>)1/2 |
17.226 |