Jump to
S1C2
Energy calculated at TPSSh/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -5222.139855 |
| Energy at 298.15K | |
| HF Energy | -5222.139855 |
| Nuclear repulsion energy | 420.342163 |
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/6-31G(2df,p)
| 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 |
3103 |
2995 |
0.00 |
130.36 |
0.04 |
0.08 |
| 2 |
Ag |
1492 |
1440 |
0.00 |
11.34 |
0.75 |
0.85 |
| 3 |
Ag |
1277 |
1232 |
0.00 |
24.85 |
0.35 |
0.52 |
| 4 |
Ag |
1061 |
1024 |
0.00 |
7.02 |
0.75 |
0.85 |
| 5 |
Ag |
671 |
648 |
0.00 |
81.32 |
0.25 |
0.40 |
| 6 |
Ag |
191 |
185 |
0.00 |
3.68 |
0.24 |
0.38 |
| 7 |
Au |
3187 |
3076 |
1.01 |
0.00 |
0.00 |
0.00 |
| 8 |
Au |
1096 |
1058 |
2.74 |
0.00 |
0.00 |
0.00 |
| 9 |
Au |
752 |
725 |
3.06 |
0.00 |
0.00 |
0.00 |
| 10 |
Au |
103 |
99 |
4.31 |
0.00 |
0.00 |
0.00 |
| 11 |
Bg |
3163 |
3053 |
0.00 |
80.03 |
0.75 |
0.86 |
| 12 |
Bg |
1286 |
1241 |
0.00 |
4.83 |
0.75 |
0.86 |
| 13 |
Bg |
946 |
912 |
0.00 |
3.51 |
0.75 |
0.86 |
| 14 |
Bu |
3111 |
3002 |
7.55 |
0.00 |
0.00 |
0.00 |
| 15 |
Bu |
1489 |
1437 |
4.39 |
0.00 |
0.00 |
0.00 |
| 16 |
Bu |
1202 |
1160 |
51.68 |
0.00 |
0.00 |
0.00 |
| 17 |
Bu |
611 |
590 |
71.60 |
0.00 |
0.00 |
0.00 |
| 18 |
Bu |
176 |
169 |
7.09 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 12458.6 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 12022.6 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 TPSSh/6-31G(2df,p)
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.495 |
0.572 |
0.000 |
| C2 |
-0.495 |
-0.572 |
0.000 |
| Br3 |
-0.495 |
2.243 |
0.000 |
| Br4 |
0.495 |
-2.243 |
0.000 |
| H5 |
1.120 |
0.570 |
0.892 |
| H6 |
1.120 |
0.570 |
-0.892 |
| H7 |
-1.120 |
-0.570 |
0.892 |
| H8 |
-1.120 |
-0.570 |
-0.892 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5128 | 1.9415 | 2.8150 | 1.0890 | 1.0890 | 2.1694 | 2.1694 |
C2 | 1.5128 | | 2.8150 | 1.9415 | 2.1694 | 2.1694 | 1.0890 | 1.0890 | Br3 | 1.9415 | 2.8150 | | 4.5933 | 2.4901 | 2.4901 | 3.0161 | 3.0161 | Br4 | 2.8150 | 1.9415 | 4.5933 | | 3.0161 | 3.0161 | 2.4901 | 2.4901 | H5 | 1.0890 | 2.1694 | 2.4901 | 3.0161 | | 1.7832 | 2.5132 | 3.0816 | H6 | 1.0890 | 2.1694 | 2.4901 | 3.0161 | 1.7832 | | 3.0816 | 2.5132 | H7 | 2.1694 | 1.0890 | 3.0161 | 2.4901 | 2.5132 | 3.0816 | | 1.7832 | H8 | 2.1694 | 1.0890 | 3.0161 | 2.4901 | 3.0816 | 2.5132 | 1.7832 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
108.526 |
|
C1 |
C2 |
H7 |
111.951 |
| C1 |
C2 |
H8 |
111.951 |
|
C2 |
C1 |
Br3 |
108.526 |
| C2 |
C1 |
H5 |
111.951 |
|
C2 |
C1 |
H6 |
111.951 |
| Br3 |
C1 |
H5 |
107.127 |
|
Br3 |
C1 |
H6 |
107.127 |
| Br4 |
C2 |
H7 |
107.127 |
|
Br4 |
C2 |
H8 |
107.127 |
| H5 |
C1 |
H6 |
109.912 |
|
H7 |
C2 |
H8 |
109.912 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at TPSSh/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.352 |
|
|
|
| 2 |
C |
-0.352 |
|
|
|
| 3 |
Br |
-0.036 |
|
|
|
| 4 |
Br |
-0.036 |
|
|
|
| 5 |
H |
0.194 |
|
|
|
| 6 |
H |
0.194 |
|
|
|
| 7 |
H |
0.194 |
|
|
|
| 8 |
H |
0.194 |
|
|
|
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 |
8.030 |
-1.639 |
0.000 |
| y |
-1.639 |
13.294 |
0.000 |
| z |
0.000 |
0.000 |
7.215 |
<r2> (average value of r
2) Å
2
| <r2> |
417.104 |
| (<r2>)1/2 |
20.423 |
Jump to
S1C1
Energy calculated at TPSSh/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -5222.137030 |
| Energy at 298.15K | |
| HF Energy | -5222.137030 |
| Nuclear repulsion energy | 458.764729 |
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/6-31G(2df,p)
| 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 |
3146 |
3035 |
0.26 |
88.74 |
0.75 |
0.86 |
| 2 |
A |
3085 |
2977 |
17.84 |
202.39 |
0.02 |
0.04 |
| 3 |
A |
1473 |
1422 |
0.05 |
4.74 |
0.70 |
0.82 |
| 4 |
A |
1305 |
1259 |
18.64 |
2.99 |
0.41 |
0.58 |
| 5 |
A |
1182 |
1141 |
1.72 |
9.81 |
0.74 |
0.85 |
| 6 |
A |
1025 |
989 |
0.91 |
2.18 |
0.73 |
0.85 |
| 7 |
A |
916 |
884 |
6.35 |
4.06 |
0.38 |
0.55 |
| 8 |
A |
577 |
557 |
7.98 |
17.86 |
0.06 |
0.11 |
| 9 |
A |
222 |
214 |
1.01 |
0.84 |
0.23 |
0.38 |
| 10 |
A |
81 |
78 |
0.20 |
0.66 |
0.63 |
0.77 |
| 11 |
B |
3160 |
3050 |
2.52 |
29.12 |
0.75 |
0.86 |
| 12 |
B |
3076 |
2968 |
2.46 |
48.83 |
0.75 |
0.86 |
| 13 |
B |
1468 |
1416 |
8.31 |
13.78 |
0.75 |
0.86 |
| 14 |
B |
1272 |
1227 |
55.22 |
0.78 |
0.75 |
0.86 |
| 15 |
B |
1118 |
1079 |
1.34 |
3.07 |
0.75 |
0.86 |
| 16 |
B |
846 |
816 |
15.17 |
0.60 |
0.75 |
0.86 |
| 17 |
B |
607 |
586 |
11.75 |
6.61 |
0.75 |
0.86 |
| 18 |
B |
354 |
342 |
6.25 |
1.82 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12455.3 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 12019.4 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 TPSSh/6-31G(2df,p)
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.304 |
0.694 |
1.201 |
| C2 |
-0.304 |
-0.694 |
1.201 |
| Br3 |
-0.304 |
1.747 |
-0.299 |
| Br4 |
0.304 |
-1.747 |
-0.299 |
| H5 |
-0.000 |
1.231 |
2.103 |
| H6 |
1.391 |
0.657 |
1.145 |
| H7 |
0.000 |
-1.231 |
2.103 |
| H8 |
-1.391 |
-0.657 |
1.145 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5149 | 1.9313 | 2.8653 | 1.0924 | 1.0896 | 2.1470 | 2.1682 |
C2 | 1.5149 | | 2.8653 | 1.9313 | 2.1470 | 2.1682 | 1.0924 | 1.0896 | Br3 | 1.9313 | 2.8653 | | 3.5473 | 2.4750 | 2.4794 | 3.8381 | 3.0078 | Br4 | 2.8653 | 1.9313 | 3.5473 | | 3.8381 | 3.0078 | 2.4750 | 2.4794 | H5 | 1.0924 | 2.1470 | 2.4750 | 3.8381 | | 1.7842 | 2.4621 | 2.5331 | H6 | 1.0896 | 2.1682 | 2.4794 | 3.0078 | 1.7842 | | 2.5331 | 3.0771 | H7 | 2.1470 | 1.0924 | 3.8381 | 2.4750 | 2.4621 | 2.5331 | | 1.7842 | H8 | 2.1682 | 1.0896 | 3.0078 | 2.4794 | 2.5331 | 3.0771 | 1.7842 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
111.933 |
|
C1 |
C2 |
H7 |
109.807 |
| C1 |
C2 |
H8 |
111.666 |
|
C2 |
C1 |
Br3 |
111.933 |
| C2 |
C1 |
H5 |
109.807 |
|
C2 |
C1 |
H6 |
111.666 |
| Br3 |
C1 |
H5 |
106.558 |
|
Br3 |
C1 |
H6 |
106.999 |
| Br4 |
C2 |
H7 |
106.558 |
|
Br4 |
C2 |
H8 |
106.999 |
| H5 |
C1 |
H6 |
109.710 |
|
H7 |
C2 |
H8 |
109.710 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at TPSSh/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.356 |
|
|
|
| 2 |
C |
-0.356 |
|
|
|
| 3 |
Br |
-0.020 |
|
|
|
| 4 |
Br |
-0.020 |
|
|
|
| 5 |
H |
0.183 |
|
|
|
| 6 |
H |
0.193 |
|
|
|
| 7 |
H |
0.183 |
|
|
|
| 8 |
H |
0.193 |
|
|
|
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 |
2.585 |
2.585 |
| 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 |
7.435 |
-0.651 |
0.000 |
| y |
-0.651 |
10.489 |
0.000 |
| z |
0.000 |
0.000 |
9.097 |
<r2> (average value of r
2) Å
2
| <r2> |
300.154 |
| (<r2>)1/2 |
17.325 |