Jump to
S1C2
Energy calculated at B1B95/6-311G*
| hartrees |
Energy at 0K | -5227.531256 |
Energy at 298.15K | -5227.541428 |
HF Energy | -5227.531256 |
Nuclear repulsion energy | 418.732299 |
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 B1B95/6-311G*
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 |
3141 |
3011 |
0.00 |
|
|
|
2 |
Ag |
1502 |
1440 |
0.00 |
|
|
|
3 |
Ag |
1308 |
1254 |
0.00 |
|
|
|
4 |
Ag |
1091 |
1046 |
0.00 |
|
|
|
5 |
Ag |
678 |
650 |
0.00 |
|
|
|
6 |
Ag |
191 |
183 |
0.00 |
|
|
|
7 |
Au |
3226 |
3092 |
1.99 |
|
|
|
8 |
Au |
1129 |
1083 |
5.90 |
|
|
|
9 |
Au |
764 |
733 |
6.27 |
|
|
|
10 |
Au |
108 |
103 |
4.34 |
|
|
|
11 |
Bg |
3203 |
3070 |
0.00 |
|
|
|
12 |
Bg |
1306 |
1252 |
0.00 |
|
|
|
13 |
Bg |
961 |
921 |
0.00 |
|
|
|
14 |
Bu |
3149 |
3018 |
9.52 |
|
|
|
15 |
Bu |
1496 |
1435 |
8.81 |
|
|
|
16 |
Bu |
1231 |
1180 |
60.38 |
|
|
|
17 |
Bu |
609 |
583 |
73.94 |
|
|
|
18 |
Bu |
177 |
169 |
7.50 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 12633.5 cm
-1
Scaled (by 0.9586) Zero Point Vibrational Energy (zpe) 12110.5 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 B1B95/6-311G*
Point Group is C2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.491 |
0.568 |
0.000 |
C2 |
-0.491 |
-0.568 |
0.000 |
Br3 |
-0.491 |
2.256 |
0.000 |
Br4 |
0.491 |
-2.256 |
0.000 |
H5 |
1.114 |
0.571 |
0.888 |
H6 |
1.114 |
0.571 |
-0.888 |
H7 |
-1.114 |
-0.571 |
0.888 |
H8 |
-1.114 |
-0.571 |
-0.888 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5009 | 1.9530 | 2.8240 | 1.0849 | 1.0849 | 2.1590 | 2.1590 |
C2 | 1.5009 | | 2.8240 | 1.9530 | 2.1590 | 2.1590 | 1.0849 | 1.0849 | Br3 | 1.9530 | 2.8240 | | 4.6179 | 2.4907 | 2.4907 | 3.0283 | 3.0283 | Br4 | 2.8240 | 1.9530 | 4.6179 | | 3.0283 | 3.0283 | 2.4907 | 2.4907 | H5 | 1.0849 | 2.1590 | 2.4907 | 3.0283 | | 1.7759 | 2.5040 | 3.0698 | H6 | 1.0849 | 2.1590 | 2.4907 | 3.0283 | 1.7759 | | 3.0698 | 2.5040 | H7 | 2.1590 | 1.0849 | 3.0283 | 2.4907 | 2.5040 | 3.0698 | | 1.7759 | H8 | 2.1590 | 1.0849 | 3.0283 | 2.4907 | 3.0698 | 2.5040 | 1.7759 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Br4 |
108.992 |
|
C1 |
C2 |
H7 |
112.214 |
C1 |
C2 |
H8 |
112.214 |
|
C2 |
C1 |
Br3 |
108.992 |
C2 |
C1 |
H5 |
112.214 |
|
C2 |
C1 |
H6 |
112.214 |
Br3 |
C1 |
H5 |
106.624 |
|
Br3 |
C1 |
H6 |
106.624 |
Br4 |
C2 |
H7 |
106.624 |
|
Br4 |
C2 |
H8 |
106.624 |
H5 |
C1 |
H6 |
109.860 |
|
H7 |
C2 |
H8 |
109.860 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.539 |
|
|
|
2 |
C |
-0.539 |
|
|
|
3 |
Br |
-0.036 |
|
|
|
4 |
Br |
-0.036 |
|
|
|
5 |
H |
0.288 |
|
|
|
6 |
H |
0.288 |
|
|
|
7 |
H |
0.288 |
|
|
|
8 |
H |
0.288 |
|
|
|
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 |
-48.736 |
1.219 |
0.000 |
y |
1.219 |
-55.602 |
0.000 |
z |
0.000 |
0.000 |
-49.406 |
|
Traceless |
| x | y | z |
x |
3.769 |
1.219 |
0.000 |
y |
1.219 |
-6.531 |
0.000 |
z |
0.000 |
0.000 |
2.763 |
|
Polar |
3z2-r2 | 5.525 |
x2-y2 | 6.866 |
xy | 1.219 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
6.660 |
-2.076 |
0.000 |
y |
-2.076 |
12.624 |
0.000 |
z |
0.000 |
0.000 |
5.408 |
<r2> (average value of r
2) Å
2
<r2> |
421.383 |
(<r2>)1/2 |
20.528 |
Jump to
S1C1
Energy calculated at B1B95/6-311G*
| hartrees |
Energy at 0K | -5227.527675 |
Energy at 298.15K | |
HF Energy | -5227.527675 |
Nuclear repulsion energy | 453.518605 |
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 B1B95/6-311G*
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 |
3181 |
3050 |
0.17 |
104.15 |
0.75 |
0.86 |
2 |
A |
3121 |
2992 |
19.33 |
228.19 |
0.02 |
0.03 |
3 |
A |
1482 |
1420 |
1.20 |
4.24 |
0.66 |
0.80 |
4 |
A |
1332 |
1277 |
24.75 |
4.63 |
0.64 |
0.78 |
5 |
A |
1216 |
1165 |
2.94 |
15.43 |
0.75 |
0.86 |
6 |
A |
1055 |
1011 |
0.32 |
2.91 |
0.61 |
0.76 |
7 |
A |
922 |
883 |
9.28 |
8.37 |
0.44 |
0.61 |
8 |
A |
572 |
549 |
8.61 |
17.09 |
0.08 |
0.14 |
9 |
A |
229 |
220 |
1.05 |
1.56 |
0.51 |
0.68 |
10 |
A |
78 |
75 |
0.20 |
1.33 |
0.73 |
0.84 |
11 |
B |
3195 |
3063 |
3.04 |
30.58 |
0.75 |
0.86 |
12 |
B |
3112 |
2983 |
2.88 |
55.00 |
0.75 |
0.86 |
13 |
B |
1475 |
1414 |
13.98 |
14.53 |
0.75 |
0.86 |
14 |
B |
1300 |
1246 |
66.92 |
1.58 |
0.75 |
0.86 |
15 |
B |
1144 |
1096 |
4.05 |
5.76 |
0.75 |
0.86 |
16 |
B |
856 |
821 |
23.24 |
1.61 |
0.75 |
0.86 |
17 |
B |
605 |
580 |
15.63 |
10.54 |
0.75 |
0.86 |
18 |
B |
357 |
343 |
6.37 |
2.54 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12615.7 cm
-1
Scaled (by 0.9586) Zero Point Vibrational Energy (zpe) 12093.4 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 B1B95/6-311G*
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.306 |
0.686 |
1.182 |
C2 |
-0.306 |
-0.686 |
1.182 |
Br3 |
-0.306 |
1.790 |
-0.294 |
Br4 |
0.306 |
-1.790 |
-0.294 |
H5 |
0.020 |
1.214 |
2.090 |
H6 |
1.389 |
0.648 |
1.115 |
H7 |
-0.020 |
-1.214 |
2.090 |
H8 |
-1.389 |
-0.648 |
1.115 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5023 | 1.9427 | 2.8825 | 1.0884 | 1.0856 | 2.1305 | 2.1580 |
C2 | 1.5023 | | 2.8825 | 1.9427 | 2.1305 | 2.1580 | 1.0884 | 1.0856 | Br3 | 1.9427 | 2.8825 | | 3.6313 | 2.4743 | 2.4829 | 3.8455 | 3.0163 | Br4 | 2.8825 | 1.9427 | 3.6313 | | 3.8455 | 3.0163 | 2.4743 | 2.4829 | H5 | 1.0884 | 2.1305 | 2.4743 | 3.8455 | | 1.7739 | 2.4282 | 2.5299 | H6 | 1.0856 | 2.1580 | 2.4829 | 3.0163 | 1.7739 | | 2.5299 | 3.0652 | H7 | 2.1305 | 1.0884 | 3.8455 | 2.4743 | 2.4282 | 2.5299 | | 1.7739 | H8 | 2.1580 | 1.0856 | 3.0163 | 2.4829 | 2.5299 | 3.0652 | 1.7739 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Br4 |
112.966 |
|
C1 |
C2 |
H7 |
109.611 |
C1 |
C2 |
H8 |
111.990 |
|
C2 |
C1 |
Br3 |
112.966 |
C2 |
C1 |
H5 |
109.611 |
|
C2 |
C1 |
H6 |
111.990 |
Br3 |
C1 |
H5 |
105.968 |
|
Br3 |
C1 |
H6 |
106.702 |
Br4 |
C2 |
H7 |
105.968 |
|
Br4 |
C2 |
H8 |
106.702 |
H5 |
C1 |
H6 |
109.367 |
|
H7 |
C2 |
H8 |
109.367 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.538 |
|
|
|
2 |
C |
-0.538 |
|
|
|
3 |
Br |
-0.023 |
|
|
|
4 |
Br |
-0.023 |
|
|
|
5 |
H |
0.275 |
|
|
|
6 |
H |
0.287 |
|
|
|
7 |
H |
0.275 |
|
|
|
8 |
H |
0.287 |
|
|
|
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 |
2.679 |
2.679 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-49.158 |
0.830 |
0.000 |
y |
0.830 |
-53.635 |
0.000 |
z |
0.000 |
0.000 |
-44.828 |
|
Traceless |
| x | y | z |
x |
0.073 |
0.830 |
0.000 |
y |
0.830 |
-6.642 |
0.000 |
z |
0.000 |
0.000 |
6.569 |
|
Polar |
3z2-r2 | 13.138 |
x2-y2 | 4.477 |
xy | 0.830 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.890 |
-0.801 |
0.000 |
y |
-0.801 |
9.183 |
0.000 |
z |
0.000 |
0.000 |
8.145 |
<r2> (average value of r
2) Å
2
<r2> |
309.976 |
(<r2>)1/2 |
17.606 |