Jump to
S1C2
Energy calculated at HF/6-311+G(3df,2p)
| hartrees |
Energy at 0K | -5222.845958 |
Energy at 298.15K | |
HF Energy | -5222.845958 |
Nuclear repulsion energy | 417.748280 |
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 HF/6-311+G(3df,2p)
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 |
3262 |
2964 |
0.00 |
133.74 |
0.04 |
0.08 |
2 |
Ag |
1616 |
1468 |
0.00 |
7.02 |
0.64 |
0.78 |
3 |
Ag |
1418 |
1288 |
0.00 |
51.57 |
0.29 |
0.45 |
4 |
Ag |
1126 |
1023 |
0.00 |
6.62 |
0.74 |
0.85 |
5 |
Ag |
726 |
659 |
0.00 |
94.28 |
0.26 |
0.41 |
6 |
Ag |
203 |
185 |
0.00 |
6.74 |
0.23 |
0.37 |
7 |
Au |
3345 |
3039 |
0.22 |
0.00 |
0.00 |
0.00 |
8 |
Au |
1204 |
1094 |
1.98 |
0.00 |
0.00 |
0.00 |
9 |
Au |
810 |
736 |
2.83 |
0.00 |
0.44 |
0.00 |
10 |
Au |
109 |
99 |
5.89 |
0.00 |
0.56 |
0.72 |
11 |
Bg |
3321 |
3017 |
0.00 |
68.13 |
0.75 |
0.86 |
12 |
Bg |
1397 |
1269 |
0.00 |
2.28 |
0.75 |
0.86 |
13 |
Bg |
1035 |
940 |
0.00 |
0.98 |
0.75 |
0.86 |
14 |
Bu |
3267 |
2969 |
10.81 |
0.00 |
0.00 |
0.00 |
15 |
Bu |
1608 |
1461 |
9.40 |
0.00 |
0.00 |
0.00 |
16 |
Bu |
1327 |
1206 |
85.84 |
0.00 |
0.00 |
0.00 |
17 |
Bu |
637 |
579 |
100.46 |
0.00 |
0.00 |
0.00 |
18 |
Bu |
196 |
178 |
6.92 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 13302.6 cm
-1
Scaled (by 0.9086) Zero Point Vibrational Energy (zpe) 12086.7 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 HF/6-311+G(3df,2p)
Point Group is C2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.490 |
0.574 |
0.000 |
C2 |
-0.490 |
-0.574 |
0.000 |
Br3 |
-0.490 |
2.265 |
0.000 |
Br4 |
0.490 |
-2.265 |
0.000 |
H5 |
1.105 |
0.581 |
0.882 |
H6 |
1.105 |
0.581 |
-0.882 |
H7 |
-1.105 |
-0.581 |
0.882 |
H8 |
-1.105 |
-0.581 |
-0.882 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5084 | 1.9548 | 2.8389 | 1.0750 | 1.0750 | 2.1571 | 2.1571 |
C2 | 1.5084 | | 2.8389 | 1.9548 | 2.1571 | 2.1571 | 1.0750 | 1.0750 | Br3 | 1.9548 | 2.8389 | | 4.6352 | 2.4810 | 2.4810 | 3.0428 | 3.0428 | Br4 | 2.8389 | 1.9548 | 4.6352 | | 3.0428 | 3.0428 | 2.4810 | 2.4810 | H5 | 1.0750 | 2.1571 | 2.4810 | 3.0428 | | 1.7635 | 2.4964 | 3.0565 | H6 | 1.0750 | 2.1571 | 2.4810 | 3.0428 | 1.7635 | | 3.0565 | 2.4964 | H7 | 2.1571 | 1.0750 | 3.0428 | 2.4810 | 2.4964 | 3.0565 | | 1.7635 | H8 | 2.1571 | 1.0750 | 3.0428 | 2.4810 | 3.0565 | 2.4964 | 1.7635 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Br4 |
109.437 |
|
C1 |
C2 |
H7 |
112.140 |
C1 |
C2 |
H8 |
112.140 |
|
C2 |
C1 |
Br3 |
109.437 |
C2 |
C1 |
H5 |
112.140 |
|
C2 |
C1 |
H6 |
112.140 |
Br3 |
C1 |
H5 |
106.283 |
|
Br3 |
C1 |
H6 |
106.283 |
Br4 |
C2 |
H7 |
106.283 |
|
Br4 |
C2 |
H8 |
106.283 |
H5 |
C1 |
H6 |
110.218 |
|
H7 |
C2 |
H8 |
110.218 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311+G(3df,2p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.210 |
|
|
|
2 |
C |
-0.210 |
|
|
|
3 |
Br |
-0.135 |
|
|
|
4 |
Br |
-0.135 |
|
|
|
5 |
H |
0.172 |
|
|
|
6 |
H |
0.172 |
|
|
|
7 |
H |
0.172 |
|
|
|
8 |
H |
0.172 |
|
|
|
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 |
-49.365 |
1.857 |
0.000 |
y |
1.857 |
-57.760 |
0.000 |
z |
0.000 |
0.000 |
-49.981 |
|
Traceless |
| x | y | z |
x |
4.506 |
1.857 |
0.000 |
y |
1.857 |
-8.087 |
0.000 |
z |
0.000 |
0.000 |
3.581 |
|
Polar |
3z2-r2 | 7.163 |
x2-y2 | 8.395 |
xy | 1.857 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
8.664 |
-1.752 |
0.000 |
y |
-1.752 |
13.714 |
0.000 |
z |
0.000 |
0.000 |
7.826 |
<r2> (average value of r
2) Å
2
<r2> |
424.871 |
(<r2>)1/2 |
20.612 |
Jump to
S1C1
Energy calculated at HF/6-311+G(3df,2p)
| hartrees |
Energy at 0K | -5222.841900 |
Energy at 298.15K | |
HF Energy | -5222.841900 |
Nuclear repulsion energy | 449.682541 |
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 HF/6-311+G(3df,2p)
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 |
3302 |
3000 |
0.03 |
76.79 |
0.75 |
0.86 |
2 |
A |
3243 |
2947 |
21.95 |
203.18 |
0.03 |
0.06 |
3 |
A |
1598 |
1452 |
0.23 |
4.18 |
0.61 |
0.75 |
4 |
A |
1432 |
1301 |
27.32 |
5.54 |
0.10 |
0.18 |
5 |
A |
1303 |
1184 |
0.70 |
4.09 |
0.71 |
0.83 |
6 |
A |
1107 |
1006 |
0.75 |
1.54 |
0.68 |
0.81 |
7 |
A |
984 |
894 |
8.85 |
4.17 |
0.20 |
0.33 |
8 |
A |
595 |
540 |
13.65 |
30.45 |
0.06 |
0.11 |
9 |
A |
243 |
221 |
1.55 |
1.39 |
0.20 |
0.33 |
10 |
A |
83 |
76 |
0.39 |
0.96 |
0.61 |
0.76 |
11 |
B |
3315 |
3012 |
1.51 |
20.36 |
0.75 |
0.86 |
12 |
B |
3231 |
2936 |
3.41 |
31.10 |
0.75 |
0.86 |
13 |
B |
1592 |
1446 |
11.64 |
7.69 |
0.75 |
0.86 |
14 |
B |
1400 |
1272 |
92.73 |
5.42 |
0.75 |
0.86 |
15 |
B |
1222 |
1111 |
1.36 |
0.94 |
0.75 |
0.86 |
16 |
B |
927 |
842 |
17.34 |
1.13 |
0.75 |
0.86 |
17 |
B |
632 |
574 |
25.62 |
13.59 |
0.75 |
0.86 |
18 |
B |
382 |
347 |
8.11 |
2.22 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13294.5 cm
-1
Scaled (by 0.9086) Zero Point Vibrational Energy (zpe) 12079.4 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 HF/6-311+G(3df,2p)
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.315 |
0.686 |
1.157 |
C2 |
-0.315 |
-0.686 |
1.157 |
Br3 |
-0.315 |
1.825 |
-0.288 |
Br4 |
0.315 |
-1.825 |
-0.288 |
H5 |
0.049 |
1.200 |
2.066 |
H6 |
1.386 |
0.640 |
1.066 |
H7 |
-0.049 |
-1.200 |
2.066 |
H8 |
-1.386 |
-0.640 |
1.066 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5101 | 1.9446 | 2.8971 | 1.0784 | 1.0757 | 2.1256 | 2.1589 |
C2 | 1.5101 | | 2.8971 | 1.9446 | 2.1256 | 2.1589 | 1.0784 | 1.0757 | Br3 | 1.9446 | 2.8971 | | 3.7047 | 2.4628 | 2.4763 | 3.8428 | 3.0093 | Br4 | 2.8971 | 1.9446 | 3.7047 | | 3.8428 | 3.0093 | 2.4628 | 2.4763 | H5 | 1.0784 | 2.1256 | 2.4628 | 3.8428 | | 1.7616 | 2.4024 | 2.5389 | H6 | 1.0757 | 2.1589 | 2.4763 | 3.0093 | 1.7616 | | 2.5389 | 3.0533 | H7 | 2.1256 | 1.0784 | 3.8428 | 2.4628 | 2.4024 | 2.5389 | | 1.7616 | H8 | 2.1589 | 1.0757 | 3.0093 | 2.4763 | 2.5389 | 3.0533 | 1.7616 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Br4 |
113.388 |
|
C1 |
C2 |
H7 |
109.271 |
C1 |
C2 |
H8 |
112.126 |
|
C2 |
C1 |
Br3 |
113.388 |
C2 |
C1 |
H5 |
109.271 |
|
C2 |
C1 |
H6 |
112.126 |
Br3 |
C1 |
H5 |
105.500 |
|
Br3 |
C1 |
H6 |
106.575 |
Br4 |
C2 |
H7 |
105.500 |
|
Br4 |
C2 |
H8 |
106.575 |
H5 |
C1 |
H6 |
109.727 |
|
H7 |
C2 |
H8 |
109.727 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311+G(3df,2p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.177 |
|
|
|
2 |
C |
-0.177 |
|
|
|
3 |
Br |
-0.140 |
|
|
|
4 |
Br |
-0.140 |
|
|
|
5 |
H |
0.155 |
|
|
|
6 |
H |
0.162 |
|
|
|
7 |
H |
0.155 |
|
|
|
8 |
H |
0.162 |
|
|
|
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 |
2.906 |
2.906 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-49.730 |
1.238 |
0.000 |
y |
1.238 |
-55.266 |
0.000 |
z |
0.000 |
0.000 |
-45.505 |
|
Traceless |
| x | y | z |
x |
0.655 |
1.238 |
0.000 |
y |
1.238 |
-7.648 |
0.000 |
z |
0.000 |
0.000 |
6.993 |
|
Polar |
3z2-r2 | 13.987 |
x2-y2 | 5.536 |
xy | 1.238 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
8.124 |
-0.759 |
0.000 |
y |
-0.759 |
11.151 |
0.000 |
z |
0.000 |
0.000 |
9.605 |
<r2> (average value of r
2) Å
2
<r2> |
318.564 |
(<r2>)1/2 |
17.848 |