Jump to
S1C2
Energy calculated at B2PLYP=FULLultrafine/6-311G**
| hartrees |
Energy at 0K | -5226.166604 |
Energy at 298.15K | |
HF Energy | -5225.742100 |
Nuclear repulsion energy | 415.709255 |
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 B2PLYP=FULLultrafine/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 |
3133 |
3133 |
0.00 |
155.25 |
0.07 |
0.12 |
2 |
Ag |
1503 |
1503 |
0.00 |
12.90 |
0.73 |
0.84 |
3 |
Ag |
1313 |
1313 |
0.00 |
32.78 |
0.51 |
0.68 |
4 |
Ag |
1077 |
1077 |
0.00 |
15.63 |
0.68 |
0.81 |
5 |
Ag |
676 |
676 |
0.00 |
92.52 |
0.28 |
0.44 |
6 |
Ag |
191 |
191 |
0.00 |
4.63 |
0.34 |
0.51 |
7 |
Au |
3217 |
3217 |
1.23 |
0.00 |
0.71 |
0.83 |
8 |
Au |
1124 |
1124 |
4.96 |
0.00 |
0.00 |
0.00 |
9 |
Au |
772 |
772 |
4.90 |
0.00 |
0.00 |
0.00 |
10 |
Au |
107 |
107 |
4.30 |
0.00 |
0.00 |
0.00 |
11 |
Bg |
3196 |
3196 |
0.00 |
91.97 |
0.75 |
0.86 |
12 |
Bg |
1305 |
1305 |
0.00 |
3.91 |
0.75 |
0.86 |
13 |
Bg |
964 |
964 |
0.00 |
6.15 |
0.75 |
0.86 |
14 |
Bu |
3140 |
3140 |
7.85 |
0.00 |
0.00 |
0.00 |
15 |
Bu |
1497 |
1497 |
6.76 |
0.00 |
0.00 |
0.00 |
16 |
Bu |
1235 |
1235 |
65.18 |
0.00 |
0.00 |
0.00 |
17 |
Bu |
600 |
600 |
69.54 |
0.00 |
0.00 |
0.00 |
18 |
Bu |
182 |
182 |
6.75 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 12616.2 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 12616.2 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 B2PLYP=FULLultrafine/6-311G**
Point Group is C2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.493 |
0.571 |
0.000 |
C2 |
-0.493 |
-0.571 |
0.000 |
Br3 |
-0.493 |
2.275 |
0.000 |
Br4 |
0.493 |
-2.275 |
0.000 |
H5 |
1.114 |
0.575 |
0.891 |
H6 |
1.114 |
0.575 |
-0.891 |
H7 |
-1.114 |
-0.575 |
0.891 |
H8 |
-1.114 |
-0.575 |
-0.891 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5092 | 1.9684 | 2.8457 | 1.0859 | 1.0859 | 2.1659 | 2.1659 |
C2 | 1.5092 | | 2.8457 | 1.9684 | 2.1659 | 2.1659 | 1.0859 | 1.0859 | Br3 | 1.9684 | 2.8457 | | 4.6548 | 2.5029 | 2.5029 | 3.0497 | 3.0497 | Br4 | 2.8457 | 1.9684 | 4.6548 | | 3.0497 | 3.0497 | 2.5029 | 2.5029 | H5 | 1.0859 | 2.1659 | 2.5029 | 3.0497 | | 1.7820 | 2.5075 | 3.0762 | H6 | 1.0859 | 2.1659 | 2.5029 | 3.0497 | 1.7820 | | 3.0762 | 2.5075 | H7 | 2.1659 | 1.0859 | 3.0497 | 2.5029 | 2.5075 | 3.0762 | | 1.7820 | H8 | 2.1659 | 1.0859 | 3.0497 | 2.5029 | 3.0762 | 2.5075 | 1.7820 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Br4 |
109.113 |
|
C1 |
C2 |
H7 |
112.115 |
C1 |
C2 |
H8 |
112.115 |
|
C2 |
C1 |
Br3 |
109.113 |
C2 |
C1 |
H5 |
112.115 |
|
C2 |
C1 |
H6 |
112.115 |
Br3 |
C1 |
H5 |
106.452 |
|
Br3 |
C1 |
H6 |
106.452 |
Br4 |
C2 |
H7 |
106.452 |
|
Br4 |
C2 |
H8 |
106.452 |
H5 |
C1 |
H6 |
110.268 |
|
H7 |
C2 |
H8 |
110.268 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at B2PLYP=FULLultrafine/6-311G**
| hartrees |
Energy at 0K | -5226.162810 |
Energy at 298.15K | |
HF Energy | -5225.738079 |
Nuclear repulsion energy | 449.087753 |
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 B2PLYP=FULLultrafine/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 |
3175 |
0.10 |
101.26 |
0.75 |
0.86 |
2 |
A |
3114 |
3114 |
16.96 |
226.79 |
0.02 |
0.03 |
3 |
A |
1482 |
1482 |
0.63 |
4.49 |
0.62 |
0.76 |
4 |
A |
1333 |
1333 |
25.32 |
3.66 |
0.60 |
0.75 |
5 |
A |
1210 |
1210 |
2.80 |
13.49 |
0.75 |
0.86 |
6 |
A |
1048 |
1048 |
0.48 |
2.48 |
0.68 |
0.81 |
7 |
A |
923 |
923 |
8.16 |
8.33 |
0.44 |
0.61 |
8 |
A |
561 |
561 |
8.58 |
17.50 |
0.08 |
0.15 |
9 |
A |
232 |
232 |
1.07 |
1.72 |
0.48 |
0.65 |
10 |
A |
81 |
81 |
0.22 |
1.48 |
0.73 |
0.84 |
11 |
B |
3188 |
3188 |
2.09 |
28.77 |
0.75 |
0.86 |
12 |
B |
3106 |
3106 |
2.56 |
51.70 |
0.75 |
0.86 |
13 |
B |
1476 |
1476 |
10.92 |
13.64 |
0.75 |
0.86 |
14 |
B |
1304 |
1304 |
73.04 |
2.24 |
0.75 |
0.86 |
15 |
B |
1140 |
1140 |
3.46 |
5.47 |
0.75 |
0.86 |
16 |
B |
860 |
860 |
19.45 |
1.55 |
0.75 |
0.86 |
17 |
B |
597 |
597 |
15.80 |
11.32 |
0.75 |
0.86 |
18 |
B |
359 |
359 |
6.32 |
2.78 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12594.3 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 12594.3 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 B2PLYP=FULLultrafine/6-311G**
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.311 |
0.689 |
1.181 |
C2 |
-0.311 |
-0.689 |
1.181 |
Br3 |
-0.311 |
1.816 |
-0.294 |
Br4 |
0.311 |
-1.816 |
-0.294 |
H5 |
0.026 |
1.212 |
2.093 |
H6 |
1.394 |
0.646 |
1.104 |
H7 |
-0.026 |
-1.212 |
2.093 |
H8 |
-1.394 |
-0.646 |
1.104 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5111 | 1.9573 | 2.9066 | 1.0895 | 1.0867 | 2.1355 | 2.1660 |
C2 | 1.5111 | | 2.9066 | 1.9573 | 2.1355 | 2.1660 | 1.0895 | 1.0867 | Br3 | 1.9573 | 2.9066 | | 3.6846 | 2.4849 | 2.4955 | 3.8664 | 3.0308 | Br4 | 2.9066 | 1.9573 | 3.6846 | | 3.8664 | 3.0308 | 2.4849 | 2.4955 | H5 | 1.0895 | 2.1355 | 2.4849 | 3.8664 | | 1.7803 | 2.4256 | 2.5393 | H6 | 1.0867 | 2.1660 | 2.4955 | 3.0308 | 1.7803 | | 2.5393 | 3.0721 | H7 | 2.1355 | 1.0895 | 3.8664 | 2.4849 | 2.4256 | 2.5393 | | 1.7803 | H8 | 2.1660 | 1.0867 | 3.0308 | 2.4955 | 2.5393 | 3.0721 | 1.7803 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Br4 |
113.231 |
|
C1 |
C2 |
H7 |
109.326 |
C1 |
C2 |
H8 |
111.938 |
|
C2 |
C1 |
Br3 |
113.231 |
C2 |
C1 |
H5 |
109.326 |
|
C2 |
C1 |
H6 |
111.938 |
Br3 |
C1 |
H5 |
105.731 |
|
Br3 |
C1 |
H6 |
106.604 |
Br4 |
C2 |
H7 |
105.731 |
|
Br4 |
C2 |
H8 |
106.604 |
H5 |
C1 |
H6 |
109.784 |
|
H7 |
C2 |
H8 |
109.784 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.287 |
|
|
|
2 |
C |
-0.287 |
|
|
|
3 |
Br |
-0.053 |
|
|
|
4 |
Br |
-0.053 |
|
|
|
5 |
H |
0.164 |
|
|
|
6 |
H |
0.176 |
|
|
|
7 |
H |
0.164 |
|
|
|
8 |
H |
0.176 |
|
|
|
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 |
2.638 |
2.638 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-49.667 |
0.850 |
0.000 |
y |
0.850 |
-54.236 |
0.000 |
z |
0.000 |
0.000 |
-45.446 |
|
Traceless |
| x | y | z |
x |
0.174 |
0.850 |
0.000 |
y |
0.850 |
-6.679 |
0.000 |
z |
0.000 |
0.000 |
6.505 |
|
Polar |
3z2-r2 | 13.010 |
x2-y2 | 4.569 |
xy | 0.850 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.912 |
-0.833 |
0.000 |
y |
-0.833 |
9.220 |
0.000 |
z |
0.000 |
0.000 |
8.167 |
<r2> (average value of r
2) Å
2
<r2> |
317.163 |
(<r2>)1/2 |
17.809 |