Jump to
S1C2
Energy calculated at B1B95/6-311G*
| | hartrees |
| Energy at 0K | -3113.327721 |
| Energy at 298.15K | |
| HF Energy | -3113.327721 |
| Nuclear repulsion energy | 289.607993 |
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 B1B95/6-311G*
| 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' |
3143 |
3013 |
12.31 |
18.25 |
0.07 |
0.13 |
| 2 |
A' |
3133 |
3003 |
2.41 |
144.85 |
0.07 |
0.13 |
| 3 |
A' |
1503 |
1440 |
0.76 |
13.29 |
0.73 |
0.85 |
| 4 |
A' |
1500 |
1438 |
7.29 |
1.48 |
0.73 |
0.85 |
| 5 |
A' |
1343 |
1288 |
3.10 |
14.55 |
0.65 |
0.79 |
| 6 |
A' |
1251 |
1199 |
46.61 |
2.94 |
0.53 |
0.69 |
| 7 |
A' |
1091 |
1045 |
1.15 |
8.99 |
0.73 |
0.85 |
| 8 |
A' |
753 |
721 |
33.07 |
52.52 |
0.29 |
0.45 |
| 9 |
A' |
658 |
630 |
59.87 |
14.73 |
0.25 |
0.40 |
| 10 |
A' |
250 |
239 |
0.81 |
4.15 |
0.39 |
0.56 |
| 11 |
A' |
190 |
183 |
8.08 |
0.12 |
0.31 |
0.47 |
| 12 |
A" |
3218 |
3085 |
3.58 |
4.30 |
0.75 |
0.86 |
| 13 |
A" |
3193 |
3061 |
0.61 |
97.47 |
0.75 |
0.86 |
| 14 |
A" |
1313 |
1259 |
0.24 |
5.78 |
0.75 |
0.86 |
| 15 |
A" |
1155 |
1108 |
4.81 |
0.07 |
0.75 |
0.86 |
| 16 |
A" |
991 |
950 |
0.18 |
6.21 |
0.75 |
0.86 |
| 17 |
A" |
773 |
741 |
5.44 |
0.03 |
0.75 |
0.86 |
| 18 |
A" |
116 |
111 |
5.72 |
0.02 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12786.5 cm
-1
Scaled (by 0.9586) Zero Point Vibrational Energy (zpe) 12257.2 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 B1B95/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.642 |
0.000 |
| C2 |
1.227 |
-0.227 |
0.000 |
| Br3 |
-1.584 |
-0.492 |
0.000 |
| Cl4 |
2.685 |
0.818 |
0.000 |
| H5 |
-0.057 |
1.263 |
0.888 |
| H6 |
-0.057 |
1.263 |
-0.888 |
| H7 |
1.278 |
-0.851 |
0.887 |
| H8 |
1.278 |
-0.851 |
-0.887 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5037 | 1.9482 | 2.6910 | 1.0852 | 1.0852 | 2.1561 | 2.1561 |
C2 | 1.5037 | | 2.8239 | 1.7942 | 2.1583 | 2.1583 | 1.0857 | 1.0857 | Br3 | 1.9482 | 2.8239 | | 4.4661 | 2.4903 | 2.4903 | 3.0178 | 3.0178 | Cl4 | 2.6910 | 1.7942 | 4.4661 | | 2.9165 | 2.9165 | 2.3569 | 2.3569 | H5 | 1.0852 | 2.1583 | 2.4903 | 2.9165 | | 1.7758 | 2.5004 | 3.0663 | H6 | 1.0852 | 2.1583 | 2.4903 | 2.9165 | 1.7758 | | 3.0663 | 2.5004 | H7 | 2.1561 | 1.0857 | 3.0178 | 2.3569 | 2.5004 | 3.0663 | | 1.7739 | H8 | 2.1561 | 1.0857 | 3.0178 | 2.3569 | 3.0663 | 2.5004 | 1.7739 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
109.052 |
|
C1 |
C2 |
H7 |
111.734 |
| C1 |
C2 |
H8 |
111.734 |
|
C2 |
C1 |
Br3 |
109.102 |
| C2 |
C1 |
Cl4 |
39.066 |
|
C2 |
C1 |
H6 |
111.944 |
| Br3 |
C1 |
H5 |
106.889 |
|
Br3 |
C1 |
H6 |
106.889 |
| Cl4 |
C2 |
H7 |
107.280 |
|
Cl4 |
C2 |
H8 |
107.280 |
| H5 |
C1 |
H6 |
109.816 |
|
H7 |
C2 |
H8 |
109.561 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.536 |
|
|
|
| 2 |
C |
-0.513 |
|
|
|
| 3 |
Br |
-0.033 |
|
|
|
| 4 |
Cl |
-0.075 |
|
|
|
| 5 |
H |
0.290 |
|
|
|
| 6 |
H |
0.290 |
|
|
|
| 7 |
H |
0.289 |
|
|
|
| 8 |
H |
0.289 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.211 |
-0.067 |
0.000 |
0.222 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-50.693 |
-2.282 |
0.000 |
| y |
-2.282 |
-43.528 |
0.000 |
| z |
0.000 |
0.000 |
-43.691 |
|
| Traceless |
| | x | y | z |
| x |
-7.083 |
-2.282 |
0.000 |
| y |
-2.282 |
3.664 |
0.000 |
| z |
0.000 |
0.000 |
3.420 |
|
| Polar |
| 3z2-r2 | 6.840 |
| x2-y2 | -7.165 |
| xy | -2.282 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
10.497 |
2.192 |
0.000 |
| y |
2.192 |
6.407 |
0.000 |
| z |
0.000 |
0.000 |
4.856 |
<r2> (average value of r
2) Å
2
| <r2> |
281.876 |
| (<r2>)1/2 |
16.789 |
Jump to
S1C1
Energy calculated at B1B95/6-311G*
| | hartrees |
| Energy at 0K | -3113.324855 |
| Energy at 298.15K | |
| HF Energy | -3113.324855 |
| Nuclear repulsion energy | 305.865575 |
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 B1B95/6-311G*
| 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 |
3194 |
3062 |
3.79 |
39.96 |
0.75 |
0.86 |
| 2 |
A |
3174 |
3043 |
2.20 |
94.60 |
0.75 |
0.86 |
| 3 |
A |
3123 |
2993 |
15.98 |
166.61 |
0.04 |
0.07 |
| 4 |
A |
3106 |
2977 |
11.14 |
104.44 |
0.23 |
0.38 |
| 5 |
A |
1484 |
1423 |
2.40 |
5.78 |
0.71 |
0.83 |
| 6 |
A |
1476 |
1415 |
12.11 |
13.06 |
0.74 |
0.85 |
| 7 |
A |
1360 |
1303 |
25.82 |
4.13 |
0.75 |
0.85 |
| 8 |
A |
1316 |
1261 |
47.49 |
1.65 |
0.57 |
0.72 |
| 9 |
A |
1236 |
1184 |
5.04 |
14.34 |
0.75 |
0.85 |
| 10 |
A |
1168 |
1120 |
3.34 |
5.59 |
0.74 |
0.85 |
| 11 |
A |
1062 |
1018 |
1.36 |
2.73 |
0.70 |
0.82 |
| 12 |
A |
948 |
909 |
10.84 |
6.81 |
0.43 |
0.60 |
| 13 |
A |
881 |
845 |
26.59 |
2.01 |
0.75 |
0.86 |
| 14 |
A |
690 |
662 |
22.79 |
9.31 |
0.42 |
0.59 |
| 15 |
A |
589 |
565 |
12.20 |
15.09 |
0.20 |
0.34 |
| 16 |
A |
387 |
371 |
7.33 |
2.46 |
0.71 |
0.83 |
| 17 |
A |
243 |
233 |
1.15 |
1.39 |
0.56 |
0.72 |
| 18 |
A |
101 |
97 |
0.51 |
1.77 |
0.74 |
0.85 |
Unscaled Zero Point Vibrational Energy (zpe) 12769.1 cm
-1
Scaled (by 0.9586) Zero Point Vibrational Energy (zpe) 12240.5 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 B1B95/6-311G*
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.009 |
1.101 |
-0.380 |
| C2 |
1.279 |
0.899 |
0.399 |
| Br3 |
-1.348 |
-0.225 |
0.036 |
| Cl4 |
2.156 |
-0.577 |
-0.086 |
| H5 |
-0.424 |
2.068 |
-0.131 |
| H6 |
0.182 |
1.046 |
-1.450 |
| H7 |
1.950 |
1.737 |
0.215 |
| H8 |
1.087 |
0.825 |
1.466 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5030 | 1.9427 | 2.7410 | 1.0877 | 1.0858 | 2.1267 | 2.1549 |
C2 | 1.5030 | | 2.8803 | 1.7847 | 2.1319 | 2.1556 | 1.0893 | 1.0863 | Br3 | 1.9427 | 2.8803 | | 3.5243 | 2.4773 | 2.4829 | 3.8416 | 3.0126 | Cl4 | 2.7410 | 1.7847 | 3.5243 | | 3.6951 | 2.8979 | 2.3428 | 2.3489 | H5 | 1.0877 | 2.1319 | 2.4773 | 3.6951 | | 1.7747 | 2.4213 | 2.5253 | H6 | 1.0858 | 2.1556 | 2.4829 | 2.8979 | 1.7747 | | 2.5251 | 3.0616 | H7 | 2.1267 | 1.0893 | 3.8416 | 2.3428 | 2.4213 | 2.5251 | | 1.7729 | H8 | 2.1549 | 1.0863 | 3.0126 | 2.3489 | 2.5253 | 3.0616 | 1.7729 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
112.682 |
|
C1 |
C2 |
H7 |
109.210 |
| C1 |
C2 |
H8 |
111.644 |
|
C2 |
C1 |
Br3 |
112.803 |
| C2 |
C1 |
Cl4 |
36.924 |
|
C2 |
C1 |
H6 |
111.737 |
| Br3 |
C1 |
H5 |
106.215 |
|
Br3 |
C1 |
H6 |
106.696 |
| Cl4 |
C2 |
H7 |
106.699 |
|
Cl4 |
C2 |
H8 |
107.284 |
| H5 |
C1 |
H6 |
109.470 |
|
H7 |
C2 |
H8 |
109.150 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.538 |
|
|
|
| 2 |
C |
-0.508 |
|
|
|
| 3 |
Br |
-0.021 |
|
|
|
| 4 |
Cl |
-0.061 |
|
|
|
| 5 |
H |
0.275 |
|
|
|
| 6 |
H |
0.290 |
|
|
|
| 7 |
H |
0.275 |
|
|
|
| 8 |
H |
0.288 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.268 |
2.797 |
0.115 |
2.812 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-47.990 |
2.912 |
0.401 |
| y |
2.912 |
-40.599 |
-0.104 |
| z |
0.401 |
-0.104 |
-43.336 |
|
| Traceless |
| | x | y | z |
| x |
-6.022 |
2.912 |
0.401 |
| y |
2.912 |
5.064 |
-0.104 |
| z |
0.401 |
-0.104 |
0.958 |
|
| Polar |
| 3z2-r2 | 1.916 |
| x2-y2 | -7.390 |
| xy | 2.912 |
| xz | 0.401 |
| yz | -0.104 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
8.274 |
0.260 |
-0.293 |
| y |
0.260 |
7.332 |
0.075 |
| z |
-0.293 |
0.075 |
5.202 |
<r2> (average value of r
2) Å
2
| <r2> |
220.072 |
| (<r2>)1/2 |
14.835 |