Jump to
S1C2
Energy calculated at HF/6-311G*
| hartrees |
Energy at 0K | -5222.822466 |
Energy at 298.15K | -5222.832804 |
HF Energy | -5222.822466 |
Nuclear repulsion energy | 417.029466 |
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/6-311G*
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 |
3292 |
2978 |
0.00 |
|
|
|
2 |
Ag |
1628 |
1473 |
0.00 |
|
|
|
3 |
Ag |
1438 |
1301 |
0.00 |
|
|
|
4 |
Ag |
1131 |
1023 |
0.00 |
|
|
|
5 |
Ag |
725 |
656 |
0.00 |
|
|
|
6 |
Ag |
203 |
184 |
0.00 |
|
|
|
7 |
Au |
3376 |
3053 |
4.40 |
|
|
|
8 |
Au |
1224 |
1107 |
4.92 |
|
|
|
9 |
Au |
816 |
738 |
4.16 |
|
|
|
10 |
Au |
111 |
101 |
6.03 |
|
|
|
11 |
Bg |
3353 |
3033 |
0.00 |
|
|
|
12 |
Bg |
1413 |
1278 |
0.00 |
|
|
|
13 |
Bg |
1046 |
946 |
0.00 |
|
|
|
14 |
Bu |
3298 |
2983 |
18.08 |
|
|
|
15 |
Bu |
1620 |
1465 |
8.54 |
|
|
|
16 |
Bu |
1346 |
1218 |
105.74 |
|
|
|
17 |
Bu |
634 |
573 |
106.43 |
|
|
|
18 |
Bu |
197 |
178 |
7.53 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13425.5 cm
-1
Scaled (by 0.9044) Zero Point Vibrational Energy (zpe) 12142.0 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/6-311G*
Point Group is C2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.491 |
0.574 |
0.000 |
C2 |
-0.491 |
-0.574 |
0.000 |
Br3 |
-0.491 |
2.269 |
0.000 |
Br4 |
0.491 |
-2.269 |
0.000 |
H5 |
1.107 |
0.581 |
0.882 |
H6 |
1.107 |
0.581 |
-0.882 |
H7 |
-1.107 |
-0.581 |
0.882 |
H8 |
-1.107 |
-0.581 |
-0.882 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5103 | 1.9588 | 2.8431 | 1.0758 | 1.0758 | 2.1600 | 2.1600 |
C2 | 1.5103 | | 2.8431 | 1.9588 | 2.1600 | 2.1600 | 1.0758 | 1.0758 | Br3 | 1.9588 | 2.8431 | | 4.6433 | 2.4859 | 2.4859 | 3.0468 | 3.0468 | Br4 | 2.8431 | 1.9588 | 4.6433 | | 3.0468 | 3.0468 | 2.4859 | 2.4859 | H5 | 1.0758 | 2.1600 | 2.4859 | 3.0468 | | 1.7631 | 2.5013 | 3.0603 | H6 | 1.0758 | 2.1600 | 2.4859 | 3.0468 | 1.7631 | | 3.0603 | 2.5013 | H7 | 2.1600 | 1.0758 | 3.0468 | 2.4859 | 2.5013 | 3.0603 | | 1.7631 | H8 | 2.1600 | 1.0758 | 3.0468 | 2.4859 | 3.0603 | 2.5013 | 1.7631 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Br4 |
109.401 |
|
C1 |
C2 |
H7 |
112.191 |
C1 |
C2 |
H8 |
112.191 |
|
C2 |
C1 |
Br3 |
109.401 |
C2 |
C1 |
H5 |
112.191 |
|
C2 |
C1 |
H6 |
112.191 |
Br3 |
C1 |
H5 |
106.333 |
|
Br3 |
C1 |
H6 |
106.333 |
Br4 |
C2 |
H7 |
106.333 |
|
Br4 |
C2 |
H8 |
106.333 |
H5 |
C1 |
H6 |
110.053 |
|
H7 |
C2 |
H8 |
110.053 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.473 |
|
|
|
2 |
C |
-0.473 |
|
|
|
3 |
Br |
-0.085 |
|
|
|
4 |
Br |
-0.085 |
|
|
|
5 |
H |
0.279 |
|
|
|
6 |
H |
0.279 |
|
|
|
7 |
H |
0.279 |
|
|
|
8 |
H |
0.279 |
|
|
|
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 |
-49.377 |
1.705 |
0.000 |
y |
1.705 |
-57.968 |
0.000 |
z |
0.000 |
0.000 |
-50.013 |
|
Traceless |
| x | y | z |
x |
4.614 |
1.705 |
0.000 |
y |
1.705 |
-8.274 |
0.000 |
z |
0.000 |
0.000 |
3.659 |
|
Polar |
3z2-r2 | 7.319 |
x2-y2 | 8.592 |
xy | 1.705 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
6.457 |
-2.208 |
0.000 |
y |
-2.208 |
11.961 |
0.000 |
z |
0.000 |
0.000 |
5.202 |
<r2> (average value of r
2) Å
2
<r2> |
426.268 |
(<r2>)1/2 |
20.646 |
Jump to
S1C1
Energy calculated at HF/6-311G*
| hartrees |
Energy at 0K | -5222.818121 |
Energy at 298.15K | |
HF Energy | -5222.818121 |
Nuclear repulsion energy | 448.693876 |
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/6-311G*
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 |
3333 |
3015 |
0.35 |
102.19 |
0.75 |
0.86 |
2 |
A |
3274 |
2961 |
33.12 |
197.83 |
0.04 |
0.07 |
3 |
A |
1613 |
1459 |
0.10 |
5.96 |
0.57 |
0.72 |
4 |
A |
1451 |
1312 |
38.71 |
3.60 |
0.42 |
0.59 |
5 |
A |
1320 |
1194 |
3.21 |
12.02 |
0.75 |
0.86 |
6 |
A |
1112 |
1006 |
0.20 |
3.01 |
0.72 |
0.84 |
7 |
A |
989 |
894 |
10.59 |
8.06 |
0.44 |
0.61 |
8 |
A |
592 |
535 |
16.47 |
26.51 |
0.09 |
0.16 |
9 |
A |
244 |
220 |
1.38 |
1.75 |
0.45 |
0.62 |
10 |
A |
84 |
76 |
0.40 |
1.69 |
0.72 |
0.84 |
11 |
B |
3346 |
3026 |
5.94 |
23.91 |
0.75 |
0.86 |
12 |
B |
3261 |
2949 |
4.45 |
47.44 |
0.75 |
0.86 |
13 |
B |
1604 |
1451 |
9.70 |
14.13 |
0.75 |
0.86 |
14 |
B |
1419 |
1283 |
105.35 |
3.51 |
0.75 |
0.86 |
15 |
B |
1237 |
1119 |
4.40 |
5.15 |
0.75 |
0.86 |
16 |
B |
932 |
843 |
21.28 |
1.86 |
0.75 |
0.86 |
17 |
B |
630 |
570 |
28.69 |
19.11 |
0.75 |
0.86 |
18 |
B |
382 |
346 |
8.33 |
3.26 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13411.1 cm
-1
Scaled (by 0.9044) Zero Point Vibrational Energy (zpe) 12129.0 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/6-311G*
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.315 |
0.687 |
1.160 |
C2 |
-0.315 |
-0.687 |
1.160 |
Br3 |
-0.315 |
1.830 |
-0.289 |
Br4 |
0.315 |
-1.830 |
-0.289 |
H5 |
0.050 |
1.201 |
2.071 |
H6 |
1.387 |
0.642 |
1.072 |
H7 |
-0.050 |
-1.201 |
2.071 |
H8 |
-1.387 |
-0.642 |
1.072 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5121 | 1.9491 | 2.9037 | 1.0794 | 1.0764 | 2.1283 | 2.1611 |
C2 | 1.5121 | | 2.9037 | 1.9491 | 2.1283 | 2.1611 | 1.0794 | 1.0764 | Br3 | 1.9491 | 2.9037 | | 3.7131 | 2.4691 | 2.4818 | 3.8500 | 3.0177 | Br4 | 2.9037 | 1.9491 | 3.7131 | | 3.8500 | 3.0177 | 2.4691 | 2.4818 | H5 | 1.0794 | 2.1283 | 2.4691 | 3.8500 | | 1.7602 | 2.4040 | 2.5413 | H6 | 1.0764 | 2.1611 | 2.4818 | 3.0177 | 1.7602 | | 2.5413 | 3.0562 | H7 | 2.1283 | 1.0794 | 3.8500 | 2.4691 | 2.4040 | 2.5413 | | 1.7602 | H8 | 2.1611 | 1.0764 | 3.0177 | 2.4818 | 2.5413 | 3.0562 | 1.7602 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Br4 |
113.456 |
|
C1 |
C2 |
H7 |
109.288 |
C1 |
C2 |
H8 |
112.103 |
|
C2 |
C1 |
Br3 |
113.456 |
C2 |
C1 |
H5 |
109.288 |
|
C2 |
C1 |
H6 |
112.103 |
Br3 |
C1 |
H5 |
105.616 |
|
Br3 |
C1 |
H6 |
106.644 |
Br4 |
C2 |
H7 |
105.616 |
|
Br4 |
C2 |
H8 |
106.644 |
H5 |
C1 |
H6 |
109.476 |
|
H7 |
C2 |
H8 |
109.476 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.477 |
|
|
|
2 |
C |
-0.477 |
|
|
|
3 |
Br |
-0.069 |
|
|
|
4 |
Br |
-0.069 |
|
|
|
5 |
H |
0.267 |
|
|
|
6 |
H |
0.279 |
|
|
|
7 |
H |
0.267 |
|
|
|
8 |
H |
0.279 |
|
|
|
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 |
3.002 |
3.002 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-49.740 |
1.087 |
0.000 |
y |
1.087 |
-55.259 |
0.000 |
z |
0.000 |
0.000 |
-45.443 |
|
Traceless |
| x | y | z |
x |
0.611 |
1.087 |
0.000 |
y |
1.087 |
-7.668 |
0.000 |
z |
0.000 |
0.000 |
7.057 |
|
Polar |
3z2-r2 | 14.114 |
x2-y2 | 5.519 |
xy | 1.087 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.712 |
-0.929 |
0.000 |
y |
-0.929 |
8.818 |
0.000 |
z |
0.000 |
0.000 |
7.885 |
<r2> (average value of r
2) Å
2
<r2> |
319.851 |
(<r2>)1/2 |
17.884 |