Jump to
S1C2
Energy calculated at B3LYP/cc-pVTZ-PP
| | hartrees |
| Energy at 0K | -912.499655 |
| Energy at 298.15K | |
| HF Energy | -912.499655 |
| Nuclear repulsion energy | 276.604970 |
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 B3LYP/cc-pVTZ-PP
| 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 |
3108 |
3108 |
0.00 |
157.53 |
0.04 |
0.07 |
| 2 |
Ag |
1492 |
1492 |
0.00 |
8.24 |
0.75 |
0.86 |
| 3 |
Ag |
1274 |
1274 |
0.00 |
44.60 |
0.43 |
0.60 |
| 4 |
Ag |
1064 |
1064 |
0.00 |
15.86 |
0.66 |
0.79 |
| 5 |
Ag |
647 |
647 |
0.00 |
108.16 |
0.27 |
0.43 |
| 6 |
Ag |
184 |
184 |
0.00 |
5.61 |
0.28 |
0.43 |
| 7 |
Au |
3189 |
3189 |
0.31 |
0.00 |
0.00 |
0.00 |
| 8 |
Au |
1094 |
1094 |
3.07 |
0.00 |
0.00 |
0.00 |
| 9 |
Au |
762 |
762 |
4.05 |
0.00 |
0.00 |
0.00 |
| 10 |
Au |
100 |
100 |
4.09 |
0.00 |
0.00 |
0.00 |
| 11 |
Bg |
3165 |
3165 |
0.00 |
79.46 |
0.75 |
0.86 |
| 12 |
Bg |
1286 |
1286 |
0.00 |
2.11 |
0.75 |
0.86 |
| 13 |
Bg |
939 |
939 |
0.00 |
3.62 |
0.75 |
0.86 |
| 14 |
Bu |
3117 |
3117 |
5.33 |
0.00 |
0.00 |
0.00 |
| 15 |
Bu |
1488 |
1488 |
6.98 |
0.00 |
0.00 |
0.00 |
| 16 |
Bu |
1206 |
1206 |
55.47 |
0.00 |
0.00 |
0.00 |
| 17 |
Bu |
574 |
574 |
76.30 |
0.00 |
0.00 |
0.00 |
| 18 |
Bu |
176 |
176 |
6.53 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 12432.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 12432.9 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 B3LYP/cc-pVTZ-PP
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.494 |
0.566 |
0.000 |
| C2 |
-0.494 |
-0.566 |
0.000 |
| Br3 |
-0.494 |
2.284 |
0.000 |
| Br4 |
0.494 |
-2.284 |
0.000 |
| H5 |
1.113 |
0.580 |
0.890 |
| H6 |
1.113 |
0.580 |
-0.890 |
| H7 |
-1.113 |
-0.580 |
0.890 |
| H8 |
-1.113 |
-0.580 |
-0.890 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5027 | 1.9816 | 2.8502 | 1.0839 | 1.0839 | 2.1648 | 2.1648 |
C2 | 1.5027 | | 2.8502 | 1.9816 | 2.1648 | 2.1648 | 1.0839 | 1.0839 | Br3 | 1.9816 | 2.8502 | | 4.6736 | 2.5054 | 2.5054 | 3.0621 | 3.0621 | Br4 | 2.8502 | 1.9816 | 4.6736 | | 3.0621 | 3.0621 | 2.5054 | 2.5054 | H5 | 1.0839 | 2.1648 | 2.5054 | 3.0621 | | 1.7797 | 2.5094 | 3.0764 | H6 | 1.0839 | 2.1648 | 2.5054 | 3.0621 | 1.7797 | | 3.0764 | 2.5094 | H7 | 2.1648 | 1.0839 | 3.0621 | 2.5054 | 2.5094 | 3.0764 | | 1.7797 | H8 | 2.1648 | 1.0839 | 3.0621 | 2.5054 | 3.0764 | 2.5094 | 1.7797 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
108.995 |
|
C1 |
C2 |
H7 |
112.629 |
| C1 |
C2 |
H8 |
112.629 |
|
C2 |
C1 |
Br3 |
108.995 |
| C2 |
C1 |
H5 |
112.629 |
|
C2 |
C1 |
H6 |
112.629 |
| Br3 |
C1 |
H5 |
105.881 |
|
Br3 |
C1 |
H6 |
105.881 |
| Br4 |
C2 |
H7 |
105.881 |
|
Br4 |
C2 |
H8 |
105.881 |
| H5 |
C1 |
H6 |
110.366 |
|
H7 |
C2 |
H8 |
110.366 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/cc-pVTZ-PP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.186 |
|
|
|
| 2 |
C |
-0.186 |
|
|
|
| 3 |
Br |
-0.105 |
|
|
|
| 4 |
Br |
-0.105 |
|
|
|
| 5 |
H |
0.145 |
|
|
|
| 6 |
H |
0.145 |
|
|
|
| 7 |
H |
0.145 |
|
|
|
| 8 |
H |
0.145 |
|
|
|
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
| Primitive |
| | x | y | z |
| x |
-48.486 |
1.260 |
0.000 |
| y |
1.260 |
-55.140 |
0.000 |
| z |
0.000 |
0.000 |
-49.072 |
|
| Traceless |
| | x | y | z |
| x |
3.620 |
1.260 |
0.000 |
| y |
1.260 |
-6.361 |
0.000 |
| z |
0.000 |
0.000 |
2.741 |
|
| Polar |
| 3z2-r2 | 5.482 |
| x2-y2 | 6.654 |
| xy | 1.260 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.951 |
-1.926 |
0.000 |
| y |
-1.926 |
14.162 |
0.000 |
| z |
0.000 |
0.000 |
6.878 |
<r2> (average value of r
2) Å
2
| <r2> |
321.057 |
| (<r2>)1/2 |
17.918 |
Jump to
S1C1
Energy calculated at B3LYP/cc-pVTZ-PP
| | hartrees |
| Energy at 0K | -912.495627 |
| Energy at 298.15K | |
| HF Energy | -912.495627 |
| Nuclear repulsion energy | 292.641452 |
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 B3LYP/cc-pVTZ-PP
| 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 |
3143 |
3143 |
0.00 |
89.87 |
0.74 |
0.85 |
| 2 |
A |
3085 |
3085 |
14.44 |
250.82 |
0.02 |
0.04 |
| 3 |
A |
1468 |
1468 |
0.59 |
3.16 |
0.74 |
0.85 |
| 4 |
A |
1304 |
1304 |
20.45 |
3.54 |
0.35 |
0.52 |
| 5 |
A |
1184 |
1184 |
1.80 |
9.33 |
0.75 |
0.86 |
| 6 |
A |
1031 |
1031 |
1.51 |
2.04 |
0.57 |
0.72 |
| 7 |
A |
900 |
900 |
8.07 |
6.60 |
0.36 |
0.53 |
| 8 |
A |
544 |
544 |
7.88 |
20.12 |
0.06 |
0.11 |
| 9 |
A |
224 |
224 |
1.19 |
1.78 |
0.31 |
0.47 |
| 10 |
A |
75 |
75 |
0.22 |
1.15 |
0.69 |
0.82 |
| 11 |
B |
3157 |
3157 |
1.15 |
24.81 |
0.75 |
0.86 |
| 12 |
B |
3077 |
3077 |
1.93 |
51.66 |
0.75 |
0.86 |
| 13 |
B |
1465 |
1465 |
11.58 |
10.77 |
0.75 |
0.86 |
| 14 |
B |
1274 |
1274 |
71.32 |
4.17 |
0.75 |
0.86 |
| 15 |
B |
1117 |
1117 |
1.86 |
3.19 |
0.75 |
0.86 |
| 16 |
B |
845 |
845 |
19.03 |
1.04 |
0.75 |
0.86 |
| 17 |
B |
578 |
578 |
17.23 |
9.69 |
0.75 |
0.86 |
| 18 |
B |
350 |
350 |
6.36 |
2.53 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12410.3 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 12410.3 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 B3LYP/cc-pVTZ-PP
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.313 |
0.685 |
1.179 |
| C2 |
-0.313 |
-0.685 |
1.179 |
| Br3 |
-0.313 |
1.830 |
-0.293 |
| Br4 |
0.313 |
-1.830 |
-0.293 |
| H5 |
0.036 |
1.213 |
2.089 |
| H6 |
1.393 |
0.646 |
1.093 |
| H7 |
-0.036 |
-1.213 |
2.089 |
| H8 |
-1.393 |
-0.646 |
1.093 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5058 | 1.9676 | 2.9146 | 1.0879 | 1.0847 | 2.1334 | 2.1651 |
C2 | 1.5058 | | 2.9146 | 1.9676 | 2.1334 | 2.1651 | 1.0879 | 1.0847 | Br3 | 1.9676 | 2.9146 | | 3.7139 | 2.4854 | 2.4972 | 3.8749 | 3.0363 | Br4 | 2.9146 | 1.9676 | 3.7139 | | 3.8749 | 3.0363 | 2.4854 | 2.4972 | H5 | 1.0879 | 2.1334 | 2.4854 | 3.8749 | | 1.7770 | 2.4273 | 2.5472 | H6 | 1.0847 | 2.1651 | 2.4972 | 3.0363 | 1.7770 | | 2.5472 | 3.0711 | H7 | 2.1334 | 1.0879 | 3.8749 | 2.4854 | 2.4273 | 2.5472 | | 1.7770 | H8 | 2.1651 | 1.0847 | 3.0363 | 2.4972 | 2.5472 | 3.0711 | 1.7770 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
113.428 |
|
C1 |
C2 |
H7 |
109.626 |
| C1 |
C2 |
H8 |
112.381 |
|
C2 |
C1 |
Br3 |
113.428 |
| C2 |
C1 |
H5 |
109.626 |
|
C2 |
C1 |
H6 |
112.381 |
| Br3 |
C1 |
H5 |
105.192 |
|
Br3 |
C1 |
H6 |
106.154 |
| Br4 |
C2 |
H7 |
105.192 |
|
Br4 |
C2 |
H8 |
106.154 |
| H5 |
C1 |
H6 |
109.754 |
|
H7 |
C2 |
H8 |
109.754 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/cc-pVTZ-PP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.193 |
|
|
|
| 2 |
C |
-0.193 |
|
|
|
| 3 |
Br |
-0.087 |
|
|
|
| 4 |
Br |
-0.087 |
|
|
|
| 5 |
H |
0.139 |
|
|
|
| 6 |
H |
0.141 |
|
|
|
| 7 |
H |
0.139 |
|
|
|
| 8 |
H |
0.141 |
|
|
|
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 |
2.527 |
2.527 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-48.840 |
0.857 |
0.000 |
| y |
0.857 |
-53.287 |
0.000 |
| z |
0.000 |
0.000 |
-44.769 |
|
| Traceless |
| | x | y | z |
| x |
0.188 |
0.857 |
0.000 |
| y |
0.857 |
-6.483 |
0.000 |
| z |
0.000 |
0.000 |
6.294 |
|
| Polar |
| 3z2-r2 | 12.588 |
| x2-y2 | 4.447 |
| xy | 0.857 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.276 |
-0.762 |
0.000 |
| y |
-0.762 |
10.812 |
0.000 |
| z |
0.000 |
0.000 |
9.213 |
<r2> (average value of r
2) Å
2
| <r2> |
249.566 |
| (<r2>)1/2 |
15.798 |