Jump to
S1C2
Energy calculated at B1B95/6-31+G**
| | hartrees |
| Energy at 0K | -5222.669814 |
| Energy at 298.15K | -5222.680028 |
| HF Energy | -5222.669814 |
| Nuclear repulsion energy | 419.727807 |
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 B1B95/6-31+G**
| 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 |
3145 |
3009 |
0.00 |
|
|
|
| 2 |
Ag |
1496 |
1431 |
0.00 |
|
|
|
| 3 |
Ag |
1309 |
1252 |
0.00 |
|
|
|
| 4 |
Ag |
1093 |
1045 |
0.00 |
|
|
|
| 5 |
Ag |
688 |
658 |
0.00 |
|
|
|
| 6 |
Ag |
194 |
185 |
0.00 |
|
|
|
| 7 |
Au |
3233 |
3093 |
0.00 |
|
|
|
| 8 |
Au |
1126 |
1077 |
4.14 |
|
|
|
| 9 |
Au |
767 |
733 |
4.14 |
|
|
|
| 10 |
Au |
130 |
124 |
4.64 |
|
|
|
| 11 |
Bg |
3211 |
3072 |
0.00 |
|
|
|
| 12 |
Bg |
1298 |
1241 |
0.00 |
|
|
|
| 13 |
Bg |
964 |
922 |
0.00 |
|
|
|
| 14 |
Bu |
3153 |
3016 |
5.08 |
|
|
|
| 15 |
Bu |
1490 |
1425 |
8.37 |
|
|
|
| 16 |
Bu |
1227 |
1174 |
59.72 |
|
|
|
| 17 |
Bu |
618 |
591 |
71.88 |
|
|
|
| 18 |
Bu |
171 |
163 |
7.30 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 12654.7 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 12105.5 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 B1B95/6-31+G**
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.488 |
0.571 |
0.000 |
| C2 |
-0.488 |
-0.571 |
0.000 |
| Br3 |
-0.488 |
2.251 |
0.000 |
| Br4 |
0.488 |
-2.251 |
0.000 |
| H5 |
1.113 |
0.574 |
0.889 |
| H6 |
1.113 |
0.574 |
-0.889 |
| H7 |
-1.113 |
-0.574 |
0.889 |
| H8 |
-1.113 |
-0.574 |
-0.889 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5030 | 1.9433 | 2.8223 | 1.0870 | 1.0870 | 2.1606 | 2.1606 |
C2 | 1.5030 | | 2.8223 | 1.9433 | 2.1606 | 2.1606 | 1.0870 | 1.0870 | Br3 | 1.9433 | 2.8223 | | 4.6070 | 2.4839 | 2.4839 | 3.0270 | 3.0270 | Br4 | 2.8223 | 1.9433 | 4.6070 | | 3.0270 | 3.0270 | 2.4839 | 2.4839 | H5 | 1.0870 | 2.1606 | 2.4839 | 3.0270 | | 1.7787 | 2.5053 | 3.0725 | H6 | 1.0870 | 2.1606 | 2.4839 | 3.0270 | 1.7787 | | 3.0725 | 2.5053 | H7 | 2.1606 | 1.0870 | 3.0270 | 2.4839 | 2.5053 | 3.0725 | | 1.7787 | H8 | 2.1606 | 1.0870 | 3.0270 | 2.4839 | 3.0725 | 2.5053 | 1.7787 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
109.296 |
|
C1 |
C2 |
H7 |
112.062 |
| C1 |
C2 |
H8 |
112.062 |
|
C2 |
C1 |
Br3 |
109.296 |
| C2 |
C1 |
H5 |
112.062 |
|
C2 |
C1 |
H6 |
112.062 |
| Br3 |
C1 |
H5 |
106.667 |
|
Br3 |
C1 |
H6 |
106.667 |
| Br4 |
C2 |
H7 |
106.667 |
|
Br4 |
C2 |
H8 |
106.667 |
| H5 |
C1 |
H6 |
109.800 |
|
H7 |
C2 |
H8 |
109.800 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.298 |
|
|
|
| 2 |
C |
-0.298 |
|
|
|
| 3 |
Br |
-0.128 |
|
|
|
| 4 |
Br |
-0.128 |
|
|
|
| 5 |
H |
0.213 |
|
|
|
| 6 |
H |
0.213 |
|
|
|
| 7 |
H |
0.213 |
|
|
|
| 8 |
H |
0.213 |
|
|
|
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 |
-48.951 |
1.313 |
0.000 |
| y |
1.313 |
-55.968 |
0.000 |
| z |
0.000 |
0.000 |
-49.701 |
|
| Traceless |
| | x | y | z |
| x |
3.884 |
1.313 |
0.000 |
| y |
1.313 |
-6.642 |
0.000 |
| z |
0.000 |
0.000 |
2.758 |
|
| Polar |
| 3z2-r2 | 5.516 |
| x2-y2 | 7.017 |
| xy | 1.313 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.949 |
-1.744 |
0.000 |
| y |
-1.744 |
13.231 |
0.000 |
| z |
0.000 |
0.000 |
7.147 |
<r2> (average value of r
2) Å
2
| <r2> |
419.839 |
| (<r2>)1/2 |
20.490 |
Jump to
S1C1
Energy calculated at B1B95/6-31+G**
| | hartrees |
| Energy at 0K | -5222.667170 |
| Energy at 298.15K | |
| HF Energy | -5222.667170 |
| Nuclear repulsion energy | 454.590952 |
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 B1B95/6-31+G**
| 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 |
3194 |
3055 |
0.00 |
94.33 |
0.75 |
0.86 |
| 2 |
A |
3126 |
2991 |
13.29 |
226.89 |
0.02 |
0.04 |
| 3 |
A |
1479 |
1415 |
0.78 |
4.50 |
0.75 |
0.85 |
| 4 |
A |
1329 |
1271 |
23.38 |
5.99 |
0.40 |
0.57 |
| 5 |
A |
1214 |
1161 |
1.75 |
11.33 |
0.74 |
0.85 |
| 6 |
A |
1062 |
1016 |
0.22 |
2.82 |
0.65 |
0.79 |
| 7 |
A |
926 |
885 |
7.87 |
6.97 |
0.23 |
0.37 |
| 8 |
A |
575 |
550 |
8.77 |
20.60 |
0.06 |
0.12 |
| 9 |
A |
241 |
230 |
1.10 |
1.41 |
0.18 |
0.31 |
| 10 |
A |
71 |
68 |
0.21 |
0.65 |
0.72 |
0.84 |
| 11 |
B |
3206 |
3067 |
0.20 |
29.21 |
0.75 |
0.86 |
| 12 |
B |
3119 |
2983 |
2.06 |
45.90 |
0.75 |
0.86 |
| 13 |
B |
1472 |
1408 |
15.29 |
13.34 |
0.75 |
0.86 |
| 14 |
B |
1292 |
1236 |
68.37 |
1.19 |
0.75 |
0.86 |
| 15 |
B |
1141 |
1091 |
2.73 |
2.82 |
0.75 |
0.86 |
| 16 |
B |
863 |
826 |
19.51 |
1.01 |
0.75 |
0.86 |
| 17 |
B |
606 |
580 |
16.30 |
9.28 |
0.75 |
0.86 |
| 18 |
B |
369 |
353 |
6.41 |
2.09 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12641.2 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 12092.5 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 B1B95/6-31+G**
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.316 |
0.681 |
1.175 |
| C2 |
-0.316 |
-0.681 |
1.175 |
| Br3 |
-0.316 |
1.783 |
-0.292 |
| Br4 |
0.316 |
-1.783 |
-0.292 |
| H5 |
0.045 |
1.213 |
2.086 |
| H6 |
1.399 |
0.628 |
1.089 |
| H7 |
-0.045 |
-1.213 |
2.086 |
| H8 |
-1.399 |
-0.628 |
1.089 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5027 | 1.9405 | 2.8681 | 1.0900 | 1.0875 | 2.1337 | 2.1601 |
C2 | 1.5027 | | 2.8681 | 1.9405 | 2.1337 | 2.1601 | 1.0900 | 1.0875 | Br3 | 1.9405 | 2.8681 | | 3.6224 | 2.4725 | 2.4869 | 3.8355 | 2.9821 | Br4 | 2.8681 | 1.9405 | 3.6224 | | 3.8355 | 2.9821 | 2.4725 | 2.4869 | H5 | 1.0900 | 2.1337 | 2.4725 | 3.8355 | | 1.7811 | 2.4282 | 2.5441 | H6 | 1.0875 | 2.1601 | 2.4869 | 2.9821 | 1.7811 | | 2.5441 | 3.0675 | H7 | 2.1337 | 1.0900 | 3.8355 | 2.4725 | 2.4282 | 2.5441 | | 1.7811 | H8 | 2.1601 | 1.0875 | 2.9821 | 2.4869 | 2.5441 | 3.0675 | 1.7811 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
112.187 |
|
C1 |
C2 |
H7 |
109.734 |
| C1 |
C2 |
H8 |
112.011 |
|
C2 |
C1 |
Br3 |
112.187 |
| C2 |
C1 |
H5 |
109.734 |
|
C2 |
C1 |
H6 |
112.011 |
| Br3 |
C1 |
H5 |
105.907 |
|
Br3 |
C1 |
H6 |
107.032 |
| Br4 |
C2 |
H7 |
105.907 |
|
Br4 |
C2 |
H8 |
107.032 |
| H5 |
C1 |
H6 |
109.754 |
|
H7 |
C2 |
H8 |
109.754 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.290 |
|
|
|
| 2 |
C |
-0.290 |
|
|
|
| 3 |
Br |
-0.123 |
|
|
|
| 4 |
Br |
-0.123 |
|
|
|
| 5 |
H |
0.199 |
|
|
|
| 6 |
H |
0.213 |
|
|
|
| 7 |
H |
0.199 |
|
|
|
| 8 |
H |
0.213 |
|
|
|
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 |
2.721 |
2.721 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-49.387 |
0.970 |
0.000 |
| y |
0.970 |
-54.205 |
0.000 |
| z |
0.000 |
0.000 |
-44.949 |
|
| Traceless |
| | x | y | z |
| x |
0.190 |
0.970 |
0.000 |
| y |
0.970 |
-7.037 |
0.000 |
| z |
0.000 |
0.000 |
6.847 |
|
| Polar |
| 3z2-r2 | 13.694 |
| x2-y2 | 4.818 |
| xy | 0.970 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.518 |
-0.744 |
0.000 |
| y |
-0.744 |
10.438 |
0.000 |
| z |
0.000 |
0.000 |
9.044 |
<r2> (average value of r
2) Å
2
| <r2> |
308.591 |
| (<r2>)1/2 |
17.567 |