Jump to
S1C2
Energy calculated at PBEPBE/6-311+G(3df,2p)
| hartrees |
Energy at 0K | -5226.018216 |
Energy at 298.15K | |
HF Energy | -5226.018216 |
Nuclear repulsion energy | 415.112447 |
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 PBEPBE/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 |
3032 |
3007 |
0.00 |
159.70 |
0.02 |
0.04 |
2 |
Ag |
1435 |
1423 |
0.00 |
5.73 |
0.74 |
0.85 |
3 |
Ag |
1222 |
1212 |
0.00 |
52.07 |
0.29 |
0.45 |
4 |
Ag |
1048 |
1040 |
0.00 |
10.62 |
0.68 |
0.81 |
5 |
Ag |
637 |
632 |
0.00 |
131.58 |
0.26 |
0.41 |
6 |
Ag |
183 |
181 |
0.00 |
4.41 |
0.21 |
0.34 |
7 |
Au |
3115 |
3090 |
0.00 |
0.00 |
0.00 |
0.00 |
8 |
Au |
1056 |
1048 |
2.55 |
0.00 |
0.00 |
0.00 |
9 |
Au |
735 |
729 |
3.77 |
0.00 |
0.00 |
0.00 |
10 |
Au |
99 |
99 |
4.03 |
0.00 |
0.00 |
0.00 |
11 |
Bg |
3090 |
3065 |
0.00 |
74.54 |
0.75 |
0.86 |
12 |
Bg |
1239 |
1229 |
0.00 |
1.75 |
0.75 |
0.86 |
13 |
Bg |
908 |
901 |
0.00 |
0.87 |
0.75 |
0.86 |
14 |
Bu |
3041 |
3016 |
3.42 |
0.00 |
0.00 |
0.00 |
15 |
Bu |
1431 |
1419 |
7.61 |
0.00 |
0.00 |
0.00 |
16 |
Bu |
1157 |
1147 |
41.77 |
0.00 |
0.00 |
0.00 |
17 |
Bu |
575 |
570 |
75.60 |
0.00 |
0.00 |
0.00 |
18 |
Bu |
171 |
169 |
7.27 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 12087.0 cm
-1
Scaled (by 0.9918) Zero Point Vibrational Energy (zpe) 11987.9 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 PBEPBE/6-311+G(3df,2p)
Point Group is C2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.496 |
0.567 |
0.000 |
C2 |
-0.496 |
-0.567 |
0.000 |
Br3 |
-0.496 |
2.275 |
0.000 |
Br4 |
0.496 |
-2.275 |
0.000 |
H5 |
1.121 |
0.578 |
0.897 |
H6 |
1.121 |
0.578 |
-0.897 |
H7 |
-1.121 |
-0.578 |
0.897 |
H8 |
-1.121 |
-0.578 |
-0.897 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5064 | 1.9754 | 2.8421 | 1.0935 | 1.0935 | 2.1749 | 2.1749 |
C2 | 1.5064 | | 2.8421 | 1.9754 | 2.1749 | 2.1749 | 1.0935 | 1.0935 | Br3 | 1.9754 | 2.8421 | | 4.6573 | 2.5099 | 2.5099 | 3.0556 | 3.0556 | Br4 | 2.8421 | 1.9754 | 4.6573 | | 3.0556 | 3.0556 | 2.5099 | 2.5099 | H5 | 1.0935 | 2.1749 | 2.5099 | 3.0556 | | 1.7944 | 2.5224 | 3.0955 | H6 | 1.0935 | 2.1749 | 2.5099 | 3.0556 | 1.7944 | | 3.0955 | 2.5224 | H7 | 2.1749 | 1.0935 | 3.0556 | 2.5099 | 2.5224 | 3.0955 | | 1.7944 | H8 | 2.1749 | 1.0935 | 3.0556 | 2.5099 | 3.0955 | 2.5224 | 1.7944 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Br4 |
108.680 |
|
C1 |
C2 |
H7 |
112.583 |
C1 |
C2 |
H8 |
112.583 |
|
C2 |
C1 |
Br3 |
108.680 |
C2 |
C1 |
H5 |
112.583 |
|
C2 |
C1 |
H6 |
112.583 |
Br3 |
C1 |
H5 |
106.150 |
|
Br3 |
C1 |
H6 |
106.150 |
Br4 |
C2 |
H7 |
106.150 |
|
Br4 |
C2 |
H8 |
106.150 |
H5 |
C1 |
H6 |
110.269 |
|
H7 |
C2 |
H8 |
110.269 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/6-311+G(3df,2p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.262 |
|
|
|
2 |
C |
-0.262 |
|
|
|
3 |
Br |
-0.096 |
|
|
|
4 |
Br |
-0.096 |
|
|
|
5 |
H |
0.179 |
|
|
|
6 |
H |
0.179 |
|
|
|
7 |
H |
0.179 |
|
|
|
8 |
H |
0.179 |
|
|
|
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 |
-49.265 |
1.333 |
0.000 |
y |
1.333 |
-55.934 |
0.000 |
z |
0.000 |
0.000 |
-49.914 |
|
Traceless |
| x | y | z |
x |
3.659 |
1.333 |
0.000 |
y |
1.333 |
-6.344 |
0.000 |
z |
0.000 |
0.000 |
2.685 |
|
Polar |
3z2-r2 | 5.371 |
x2-y2 | 6.668 |
xy | 1.333 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
9.408 |
-1.733 |
0.000 |
y |
-1.733 |
15.663 |
0.000 |
z |
0.000 |
0.000 |
8.549 |
<r2> (average value of r
2) Å
2
<r2> |
428.270 |
(<r2>)1/2 |
20.695 |
Jump to
S1C1
Energy calculated at PBEPBE/6-311+G(3df,2p)
| hartrees |
Energy at 0K | -5226.014687 |
Energy at 298.15K | |
HF Energy | -5226.014687 |
Nuclear repulsion energy | 448.537484 |
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 PBEPBE/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 |
3069 |
3044 |
0.01 |
85.75 |
0.75 |
0.86 |
2 |
A |
3011 |
2986 |
11.70 |
274.10 |
0.02 |
0.04 |
3 |
A |
1409 |
1397 |
1.41 |
2.91 |
0.74 |
0.85 |
4 |
A |
1254 |
1244 |
15.29 |
6.25 |
0.17 |
0.29 |
5 |
A |
1144 |
1135 |
1.23 |
6.80 |
0.75 |
0.86 |
6 |
A |
1009 |
1001 |
1.72 |
2.05 |
0.34 |
0.51 |
7 |
A |
874 |
867 |
7.19 |
5.53 |
0.19 |
0.32 |
8 |
A |
543 |
539 |
6.37 |
21.19 |
0.04 |
0.09 |
9 |
A |
221 |
219 |
1.31 |
1.62 |
0.17 |
0.29 |
10 |
A |
75 |
74 |
0.19 |
0.70 |
0.61 |
0.76 |
11 |
B |
3084 |
3059 |
0.39 |
28.32 |
0.75 |
0.86 |
12 |
B |
3002 |
2978 |
1.67 |
47.22 |
0.75 |
0.86 |
13 |
B |
1406 |
1395 |
13.57 |
9.59 |
0.75 |
0.86 |
14 |
B |
1221 |
1211 |
59.45 |
3.53 |
0.75 |
0.86 |
15 |
B |
1081 |
1072 |
1.23 |
1.21 |
0.75 |
0.86 |
16 |
B |
815 |
809 |
20.26 |
0.88 |
0.75 |
0.86 |
17 |
B |
574 |
569 |
15.51 |
6.62 |
0.75 |
0.86 |
18 |
B |
344 |
341 |
6.29 |
1.79 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12068.1 cm
-1
Scaled (by 0.9918) Zero Point Vibrational Energy (zpe) 11969.1 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 PBEPBE/6-311+G(3df,2p)
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.310 |
0.687 |
1.186 |
C2 |
-0.310 |
-0.687 |
1.186 |
Br3 |
-0.310 |
1.816 |
-0.295 |
Br4 |
0.310 |
-1.816 |
-0.295 |
H5 |
0.023 |
1.221 |
2.101 |
H6 |
1.401 |
0.651 |
1.107 |
H7 |
-0.023 |
-1.221 |
2.101 |
H8 |
-1.401 |
-0.651 |
1.107 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5078 | 1.9625 | 2.9084 | 1.0974 | 1.0943 | 2.1421 | 2.1738 |
C2 | 1.5078 | | 2.9084 | 1.9625 | 2.1421 | 2.1738 | 1.0974 | 1.0943 | Br3 | 1.9625 | 2.9084 | | 3.6844 | 2.4906 | 2.4999 | 3.8788 | 3.0405 | Br4 | 2.9084 | 1.9625 | 3.6844 | | 3.8788 | 3.0405 | 2.4906 | 2.4999 | H5 | 1.0974 | 2.1421 | 2.4906 | 3.8788 | | 1.7919 | 2.4426 | 2.5533 | H6 | 1.0943 | 2.1738 | 2.4999 | 3.0405 | 1.7919 | | 2.5533 | 3.0899 | H7 | 2.1421 | 1.0974 | 3.8788 | 2.4906 | 2.4426 | 2.5533 | | 1.7919 | H8 | 2.1738 | 1.0943 | 3.0405 | 2.4999 | 2.5533 | 3.0899 | 1.7919 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Br4 |
113.225 |
|
C1 |
C2 |
H7 |
109.619 |
C1 |
C2 |
H8 |
112.346 |
|
C2 |
C1 |
Br3 |
113.225 |
C2 |
C1 |
H5 |
109.619 |
|
C2 |
C1 |
H6 |
112.346 |
Br3 |
C1 |
H5 |
105.448 |
|
Br3 |
C1 |
H6 |
106.232 |
Br4 |
C2 |
H7 |
105.448 |
|
Br4 |
C2 |
H8 |
106.232 |
H5 |
C1 |
H6 |
109.685 |
|
H7 |
C2 |
H8 |
109.685 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/6-311+G(3df,2p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.230 |
|
|
|
2 |
C |
-0.230 |
|
|
|
3 |
Br |
-0.099 |
|
|
|
4 |
Br |
-0.099 |
|
|
|
5 |
H |
0.160 |
|
|
|
6 |
H |
0.168 |
|
|
|
7 |
H |
0.160 |
|
|
|
8 |
H |
0.168 |
|
|
|
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 |
2.542 |
2.542 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-49.682 |
0.952 |
0.000 |
y |
0.952 |
-54.227 |
0.000 |
z |
0.000 |
0.000 |
-45.461 |
|
Traceless |
| x | y | z |
x |
0.162 |
0.952 |
0.000 |
y |
0.952 |
-6.656 |
0.000 |
z |
0.000 |
0.000 |
6.494 |
|
Polar |
3z2-r2 | 12.987 |
x2-y2 | 4.545 |
xy | 0.952 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
8.849 |
-0.684 |
0.000 |
y |
-0.684 |
12.462 |
0.000 |
z |
0.000 |
0.000 |
10.387 |
<r2> (average value of r
2) Å
2
<r2> |
317.480 |
(<r2>)1/2 |
17.818 |