Jump to
S1C2
Energy calculated at PBE1PBE/6-311G*
| hartrees |
Energy at 0K | -5226.183181 |
Energy at 298.15K | |
HF Energy | -5226.183181 |
Nuclear repulsion energy | 418.187023 |
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 PBE1PBE/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 |
Ag |
3132 |
3002 |
0.00 |
152.83 |
0.06 |
0.12 |
2 |
Ag |
1499 |
1436 |
0.00 |
12.97 |
0.73 |
0.85 |
3 |
Ag |
1311 |
1256 |
0.00 |
33.01 |
0.53 |
0.69 |
4 |
Ag |
1092 |
1046 |
0.00 |
14.15 |
0.66 |
0.80 |
5 |
Ag |
685 |
657 |
0.00 |
94.24 |
0.28 |
0.44 |
6 |
Ag |
193 |
185 |
0.00 |
3.76 |
0.35 |
0.52 |
7 |
Au |
3217 |
3084 |
1.57 |
0.00 |
0.00 |
0.00 |
8 |
Au |
1130 |
1084 |
5.86 |
0.00 |
0.00 |
0.00 |
9 |
Au |
766 |
734 |
6.59 |
0.00 |
0.00 |
0.00 |
10 |
Au |
108 |
104 |
4.40 |
0.00 |
0.00 |
0.00 |
11 |
Bg |
3194 |
3062 |
0.00 |
93.86 |
0.75 |
0.86 |
12 |
Bg |
1307 |
1253 |
0.00 |
4.44 |
0.75 |
0.86 |
13 |
Bg |
963 |
923 |
0.00 |
6.41 |
0.75 |
0.86 |
14 |
Bu |
3140 |
3010 |
9.09 |
0.00 |
0.00 |
0.00 |
15 |
Bu |
1493 |
1431 |
9.72 |
0.00 |
0.00 |
0.00 |
16 |
Bu |
1234 |
1183 |
58.10 |
0.00 |
0.00 |
0.00 |
17 |
Bu |
615 |
590 |
72.57 |
0.00 |
0.00 |
0.00 |
18 |
Bu |
181 |
173 |
7.40 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 12629.7 cm
-1
Scaled (by 0.9585) Zero Point Vibrational Energy (zpe) 12105.6 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 PBE1PBE/6-311G*
Point Group is C2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.491 |
0.569 |
0.000 |
C2 |
-0.491 |
-0.569 |
0.000 |
Br3 |
-0.491 |
2.259 |
0.000 |
Br4 |
0.491 |
-2.259 |
0.000 |
H5 |
1.116 |
0.573 |
0.890 |
H6 |
1.116 |
0.573 |
-0.890 |
H7 |
-1.116 |
-0.573 |
0.890 |
H8 |
-1.116 |
-0.573 |
-0.890 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5032 | 1.9547 | 2.8283 | 1.0878 | 1.0878 | 2.1631 | 2.1631 |
C2 | 1.5032 | | 2.8283 | 1.9547 | 2.1631 | 2.1631 | 1.0878 | 1.0878 | Br3 | 1.9547 | 2.8283 | | 4.6239 | 2.4941 | 2.4941 | 3.0335 | 3.0335 | Br4 | 2.8283 | 1.9547 | 4.6239 | | 3.0335 | 3.0335 | 2.4941 | 2.4941 | H5 | 1.0878 | 2.1631 | 2.4941 | 3.0335 | | 1.7803 | 2.5092 | 3.0766 | H6 | 1.0878 | 2.1631 | 2.4941 | 3.0335 | 1.7803 | | 3.0766 | 2.5092 | H7 | 2.1631 | 1.0878 | 3.0335 | 2.4941 | 2.5092 | 3.0766 | | 1.7803 | H8 | 2.1631 | 1.0878 | 3.0335 | 2.4941 | 3.0766 | 2.5092 | 1.7803 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Br4 |
109.054 |
|
C1 |
C2 |
H7 |
112.205 |
C1 |
C2 |
H8 |
112.205 |
|
C2 |
C1 |
Br3 |
109.054 |
C2 |
C1 |
H5 |
112.205 |
|
C2 |
C1 |
H6 |
112.205 |
Br3 |
C1 |
H5 |
106.623 |
|
Br3 |
C1 |
H6 |
106.623 |
Br4 |
C2 |
H7 |
106.623 |
|
Br4 |
C2 |
H8 |
106.623 |
H5 |
C1 |
H6 |
109.822 |
|
H7 |
C2 |
H8 |
109.822 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.547 |
|
|
|
2 |
C |
-0.547 |
|
|
|
3 |
Br |
-0.036 |
|
|
|
4 |
Br |
-0.036 |
|
|
|
5 |
H |
0.291 |
|
|
|
6 |
H |
0.291 |
|
|
|
7 |
H |
0.291 |
|
|
|
8 |
H |
0.291 |
|
|
|
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 |
-48.860 |
1.241 |
0.000 |
y |
1.241 |
-55.809 |
0.000 |
z |
0.000 |
0.000 |
-49.531 |
|
Traceless |
| x | y | z |
x |
3.810 |
1.241 |
0.000 |
y |
1.241 |
-6.614 |
0.000 |
z |
0.000 |
0.000 |
2.804 |
|
Polar |
3z2-r2 | 5.608 |
x2-y2 | 6.949 |
xy | 1.241 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
6.655 |
-2.062 |
0.000 |
y |
-2.062 |
12.609 |
0.000 |
z |
0.000 |
0.000 |
5.410 |
<r2> (average value of r
2) Å
2
<r2> |
422.498 |
(<r2>)1/2 |
20.555 |
Jump to
S1C1
Energy calculated at PBE1PBE/6-311G*
| hartrees |
Energy at 0K | -5226.179457 |
Energy at 298.15K | |
HF Energy | -5226.179457 |
Nuclear repulsion energy | 451.773293 |
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 PBE1PBE/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 |
3175 |
3043 |
0.11 |
102.83 |
0.75 |
0.86 |
2 |
A |
3114 |
2985 |
18.53 |
227.26 |
0.02 |
0.03 |
3 |
A |
1479 |
1417 |
1.58 |
4.22 |
0.66 |
0.79 |
4 |
A |
1333 |
1278 |
24.67 |
4.72 |
0.64 |
0.78 |
5 |
A |
1218 |
1167 |
2.87 |
15.26 |
0.75 |
0.86 |
6 |
A |
1057 |
1013 |
0.34 |
2.86 |
0.58 |
0.74 |
7 |
A |
922 |
884 |
9.48 |
8.48 |
0.43 |
0.60 |
8 |
A |
574 |
550 |
8.20 |
16.23 |
0.08 |
0.14 |
9 |
A |
232 |
223 |
1.11 |
1.61 |
0.49 |
0.66 |
10 |
A |
81 |
77 |
0.22 |
1.35 |
0.73 |
0.85 |
11 |
B |
3189 |
3056 |
2.55 |
29.66 |
0.75 |
0.86 |
12 |
B |
3105 |
2976 |
2.81 |
53.72 |
0.75 |
0.86 |
13 |
B |
1472 |
1411 |
15.29 |
14.44 |
0.75 |
0.86 |
14 |
B |
1301 |
1247 |
66.32 |
1.58 |
0.75 |
0.86 |
15 |
B |
1145 |
1097 |
4.03 |
5.74 |
0.75 |
0.86 |
16 |
B |
858 |
823 |
23.87 |
1.65 |
0.75 |
0.86 |
17 |
B |
608 |
582 |
15.60 |
10.24 |
0.75 |
0.86 |
18 |
B |
361 |
346 |
6.39 |
2.47 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12610.6 cm
-1
Scaled (by 0.9585) Zero Point Vibrational Energy (zpe) 12087.3 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 PBE1PBE/6-311G*
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.307 |
0.687 |
1.177 |
C2 |
-0.307 |
-0.687 |
1.177 |
Br3 |
-0.307 |
1.803 |
-0.293 |
Br4 |
0.307 |
-1.803 |
-0.293 |
H5 |
0.023 |
1.212 |
2.090 |
H6 |
1.393 |
0.647 |
1.107 |
H7 |
-0.023 |
-1.212 |
2.090 |
H8 |
-1.393 |
-0.647 |
1.107 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5045 | 1.9447 | 2.8907 | 1.0913 | 1.0885 | 2.1326 | 2.1619 |
C2 | 1.5045 | | 2.8907 | 1.9447 | 2.1326 | 2.1619 | 1.0913 | 1.0885 | Br3 | 1.9447 | 2.8907 | | 3.6571 | 2.4774 | 2.4868 | 3.8531 | 3.0236 | Br4 | 2.8907 | 1.9447 | 3.6571 | | 3.8531 | 3.0236 | 2.4774 | 2.4868 | H5 | 1.0913 | 2.1326 | 2.4774 | 3.8531 | | 1.7776 | 2.4239 | 2.5352 | H6 | 1.0885 | 2.1619 | 2.4868 | 3.0236 | 1.7776 | | 2.5352 | 3.0716 | H7 | 2.1326 | 1.0913 | 3.8531 | 2.4774 | 2.4239 | 2.5352 | | 1.7776 | H8 | 2.1619 | 1.0885 | 3.0236 | 2.4868 | 2.5352 | 3.0716 | 1.7776 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Br4 |
113.260 |
|
C1 |
C2 |
H7 |
109.452 |
C1 |
C2 |
H8 |
111.976 |
|
C2 |
C1 |
Br3 |
113.260 |
C2 |
C1 |
H5 |
109.452 |
|
C2 |
C1 |
H6 |
111.976 |
Br3 |
C1 |
H5 |
105.927 |
|
Br3 |
C1 |
H6 |
106.710 |
Br4 |
C2 |
H7 |
105.927 |
|
Br4 |
C2 |
H8 |
106.710 |
H5 |
C1 |
H6 |
109.271 |
|
H7 |
C2 |
H8 |
109.271 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.546 |
|
|
|
2 |
C |
-0.546 |
|
|
|
3 |
Br |
-0.023 |
|
|
|
4 |
Br |
-0.023 |
|
|
|
5 |
H |
0.279 |
|
|
|
6 |
H |
0.290 |
|
|
|
7 |
H |
0.279 |
|
|
|
8 |
H |
0.290 |
|
|
|
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 |
2.693 |
2.693 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-49.277 |
0.841 |
0.000 |
y |
0.841 |
-53.833 |
0.000 |
z |
0.000 |
0.000 |
-44.975 |
|
Traceless |
| x | y | z |
x |
0.127 |
0.841 |
0.000 |
y |
0.841 |
-6.706 |
0.000 |
z |
0.000 |
0.000 |
6.580 |
|
Polar |
3z2-r2 | 13.159 |
x2-y2 | 4.556 |
xy | 0.841 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.891 |
-0.803 |
0.000 |
y |
-0.803 |
9.215 |
0.000 |
z |
0.000 |
0.000 |
8.113 |
<r2> (average value of r
2) Å
2
<r2> |
313.140 |
(<r2>)1/2 |
17.696 |