Jump to
S1C2
Energy calculated at HF/6-311G**
| hartrees |
Energy at 0K | -3109.964962 |
Energy at 298.15K | |
HF Energy | -3109.964962 |
Nuclear repulsion energy | 288.572862 |
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' |
3273 |
2974 |
17.19 |
11.23 |
0.09 |
0.17 |
2 |
A' |
3267 |
2968 |
1.46 |
147.90 |
0.09 |
0.16 |
3 |
A' |
1617 |
1469 |
0.12 |
13.31 |
0.69 |
0.82 |
4 |
A' |
1609 |
1461 |
6.97 |
0.40 |
0.66 |
0.80 |
5 |
A' |
1458 |
1325 |
2.51 |
16.80 |
0.58 |
0.74 |
6 |
A' |
1354 |
1230 |
79.08 |
3.05 |
0.49 |
0.66 |
7 |
A' |
1131 |
1028 |
1.21 |
8.17 |
0.73 |
0.85 |
8 |
A' |
797 |
725 |
35.23 |
55.18 |
0.31 |
0.47 |
9 |
A' |
684 |
622 |
92.91 |
13.26 |
0.27 |
0.43 |
10 |
A' |
265 |
241 |
0.92 |
6.70 |
0.36 |
0.53 |
11 |
A' |
212 |
192 |
8.33 |
0.25 |
0.32 |
0.48 |
12 |
A" |
3350 |
3043 |
4.49 |
2.65 |
0.75 |
0.86 |
13 |
A" |
3327 |
3022 |
0.53 |
95.63 |
0.75 |
0.86 |
14 |
A" |
1406 |
1277 |
0.17 |
6.10 |
0.75 |
0.86 |
15 |
A" |
1236 |
1123 |
3.16 |
0.05 |
0.75 |
0.86 |
16 |
A" |
1069 |
971 |
0.19 |
5.37 |
0.75 |
0.86 |
17 |
A" |
823 |
747 |
3.23 |
0.02 |
0.75 |
0.86 |
18 |
A" |
119 |
108 |
7.47 |
0.01 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13497.7 cm
-1
Scaled (by 0.9085) Zero Point Vibrational Energy (zpe) 12262.7 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/6-311G**
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.639 |
0.000 |
C2 |
1.239 |
-0.229 |
0.000 |
Br3 |
-1.594 |
-0.493 |
0.000 |
Cl4 |
2.698 |
0.821 |
0.000 |
H5 |
-0.060 |
1.253 |
0.883 |
H6 |
-0.060 |
1.253 |
-0.883 |
H7 |
1.294 |
-0.845 |
0.882 |
H8 |
1.294 |
-0.845 |
-0.882 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5125 | 1.9545 | 2.7046 | 1.0771 | 1.0771 | 2.1574 | 2.1574 |
C2 | 1.5125 | | 2.8444 | 1.7983 | 2.1589 | 2.1589 | 1.0774 | 1.0774 | Br3 | 1.9545 | 2.8444 | | 4.4885 | 2.4856 | 2.4856 | 3.0399 | 3.0399 | Cl4 | 2.7046 | 1.7983 | 4.4885 | | 2.9281 | 2.9281 | 2.3507 | 2.3507 | H5 | 1.0771 | 2.1589 | 2.4856 | 2.9281 | | 1.7665 | 2.4962 | 3.0576 | H6 | 1.0771 | 2.1589 | 2.4856 | 2.9281 | 1.7665 | | 3.0576 | 2.4962 | H7 | 2.1574 | 1.0774 | 3.0399 | 2.3507 | 2.4962 | 3.0576 | | 1.7649 | H8 | 2.1574 | 1.0774 | 3.0399 | 2.3507 | 3.0576 | 2.4962 | 1.7649 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
109.245 |
|
C1 |
C2 |
H7 |
111.720 |
C1 |
C2 |
H8 |
111.720 |
|
C2 |
C1 |
Br3 |
109.598 |
C2 |
C1 |
Cl4 |
38.886 |
|
C2 |
C1 |
H6 |
111.862 |
Br3 |
C1 |
H5 |
106.530 |
|
Br3 |
C1 |
H6 |
106.530 |
Cl4 |
C2 |
H7 |
106.971 |
|
Cl4 |
C2 |
H8 |
106.971 |
H5 |
C1 |
H6 |
110.178 |
|
H7 |
C2 |
H8 |
109.985 |
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 |
-0.231 |
|
|
|
2 |
C |
-0.194 |
|
|
|
3 |
Br |
-0.104 |
|
|
|
4 |
Cl |
-0.142 |
|
|
|
5 |
H |
0.169 |
|
|
|
6 |
H |
0.169 |
|
|
|
7 |
H |
0.167 |
|
|
|
8 |
H |
0.167 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.139 |
-0.046 |
0.000 |
0.147 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-52.460 |
-2.842 |
0.000 |
y |
-2.842 |
-44.080 |
0.000 |
z |
0.000 |
0.000 |
-44.147 |
|
Traceless |
| x | y | z |
x |
-8.346 |
-2.842 |
0.000 |
y |
-2.842 |
4.223 |
0.000 |
z |
0.000 |
0.000 |
4.123 |
|
Polar |
3z2-r2 | 8.246 |
x2-y2 | -8.380 |
xy | -2.842 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
10.003 |
2.266 |
0.000 |
y |
2.266 |
6.262 |
0.000 |
z |
0.000 |
0.000 |
4.698 |
<r2> (average value of r
2) Å
2
<r2> |
284.919 |
(<r2>)1/2 |
16.880 |
Jump to
S1C1
Energy calculated at HF/6-311G**
| hartrees |
Energy at 0K | -3109.961514 |
Energy at 298.15K | |
HF Energy | -3109.961514 |
Nuclear repulsion energy | 303.643253 |
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 |
3326 |
3021 |
4.73 |
32.31 |
0.75 |
0.86 |
2 |
A |
3310 |
3007 |
2.17 |
92.24 |
0.75 |
0.86 |
3 |
A |
3255 |
2957 |
25.79 |
176.17 |
0.04 |
0.07 |
4 |
A |
3240 |
2943 |
8.77 |
67.25 |
0.37 |
0.54 |
5 |
A |
1601 |
1454 |
0.65 |
6.08 |
0.62 |
0.76 |
6 |
A |
1590 |
1445 |
8.21 |
12.32 |
0.73 |
0.84 |
7 |
A |
1467 |
1333 |
35.77 |
1.61 |
0.72 |
0.83 |
8 |
A |
1421 |
1291 |
74.96 |
3.01 |
0.53 |
0.69 |
9 |
A |
1327 |
1206 |
4.07 |
10.91 |
0.74 |
0.85 |
10 |
A |
1249 |
1135 |
2.84 |
4.65 |
0.73 |
0.84 |
11 |
A |
1119 |
1017 |
1.20 |
3.05 |
0.67 |
0.80 |
12 |
A |
1012 |
919 |
11.97 |
6.47 |
0.45 |
0.62 |
13 |
A |
951 |
864 |
23.59 |
2.37 |
0.73 |
0.84 |
14 |
A |
721 |
655 |
37.65 |
15.49 |
0.44 |
0.62 |
15 |
A |
611 |
555 |
21.93 |
24.10 |
0.23 |
0.37 |
16 |
A |
413 |
375 |
9.26 |
2.99 |
0.69 |
0.82 |
17 |
A |
259 |
235 |
1.42 |
1.50 |
0.49 |
0.66 |
18 |
A |
105 |
96 |
0.81 |
2.13 |
0.73 |
0.85 |
Unscaled Zero Point Vibrational Energy (zpe) 13487.6 cm
-1
Scaled (by 0.9085) Zero Point Vibrational Energy (zpe) 12253.5 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 HF/6-311G**
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.012 |
1.083 |
-0.389 |
C2 |
1.282 |
0.889 |
0.408 |
Br3 |
-1.371 |
-0.223 |
0.036 |
Cl4 |
2.201 |
-0.566 |
-0.086 |
H5 |
-0.414 |
2.047 |
-0.155 |
H6 |
0.189 |
1.008 |
-1.449 |
H7 |
1.935 |
1.733 |
0.237 |
H8 |
1.082 |
0.795 |
1.463 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5121 | 1.9487 | 2.7565 | 1.0797 | 1.0776 | 2.1243 | 2.1585 |
C2 | 1.5121 | | 2.9005 | 1.7899 | 2.1296 | 2.1585 | 1.0808 | 1.0779 | Br3 | 1.9487 | 2.9005 | | 3.5897 | 2.4705 | 2.4807 | 3.8464 | 3.0154 | Cl4 | 2.7565 | 1.7899 | 3.5897 | | 3.6968 | 2.8948 | 2.3362 | 2.3461 | H5 | 1.0797 | 2.1296 | 2.4705 | 3.6968 | | 1.7659 | 2.4023 | 2.5346 | H6 | 1.0776 | 2.1585 | 2.4807 | 2.8948 | 1.7659 | | 2.5330 | 3.0539 | H7 | 2.1243 | 1.0808 | 3.8464 | 2.3362 | 2.4023 | 2.5330 | | 1.7637 | H8 | 2.1585 | 1.0779 | 3.0154 | 2.3461 | 2.5346 | 3.0539 | 1.7637 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
112.922 |
|
C1 |
C2 |
H7 |
108.884 |
C1 |
C2 |
H8 |
111.806 |
|
C2 |
C1 |
Br3 |
113.279 |
C2 |
C1 |
Cl4 |
36.731 |
|
C2 |
C1 |
H6 |
111.828 |
Br3 |
C1 |
H5 |
105.722 |
|
Br3 |
C1 |
H6 |
106.539 |
Cl4 |
C2 |
H7 |
106.302 |
|
Cl4 |
C2 |
H8 |
107.167 |
H5 |
C1 |
H6 |
109.880 |
|
H7 |
C2 |
H8 |
109.580 |
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 |
-0.235 |
|
|
|
2 |
C |
-0.192 |
|
|
|
3 |
Br |
-0.089 |
|
|
|
4 |
Cl |
-0.127 |
|
|
|
5 |
H |
0.154 |
|
|
|
6 |
H |
0.170 |
|
|
|
7 |
H |
0.152 |
|
|
|
8 |
H |
0.167 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.330 |
3.083 |
0.121 |
3.103 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-49.308 |
3.096 |
0.526 |
y |
3.096 |
-41.108 |
-0.124 |
z |
0.526 |
-0.124 |
-43.704 |
|
Traceless |
| x | y | z |
x |
-6.902 |
3.096 |
0.526 |
y |
3.096 |
5.398 |
-0.124 |
z |
0.526 |
-0.124 |
1.504 |
|
Polar |
3z2-r2 | 3.008 |
x2-y2 | -8.200 |
xy | 3.096 |
xz | 0.526 |
yz | -0.124 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
8.022 |
0.295 |
-0.402 |
y |
0.295 |
7.122 |
0.069 |
z |
-0.402 |
0.069 |
5.030 |
<r2> (average value of r
2) Å
2
<r2> |
225.188 |
(<r2>)1/2 |
15.006 |