Jump to
S1C2
Energy calculated at B1B95/6-31G*
| | hartrees |
| Energy at 0K | -3110.842092 |
| Energy at 298.15K | |
| HF Energy | -3110.842092 |
| Nuclear repulsion energy | 289.730778 |
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 B1B95/6-31G*
| 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' |
3161 |
3001 |
6.99 |
36.04 |
0.07 |
0.13 |
| 2 |
A' |
3147 |
2988 |
3.23 |
114.05 |
0.08 |
0.14 |
| 3 |
A' |
1517 |
1440 |
1.11 |
15.36 |
0.75 |
0.86 |
| 4 |
A' |
1512 |
1435 |
6.46 |
2.11 |
0.74 |
0.85 |
| 5 |
A' |
1343 |
1275 |
3.25 |
13.77 |
0.59 |
0.74 |
| 6 |
A' |
1245 |
1182 |
42.87 |
2.55 |
0.44 |
0.61 |
| 7 |
A' |
1093 |
1037 |
1.46 |
7.73 |
0.75 |
0.86 |
| 8 |
A' |
761 |
722 |
34.53 |
45.72 |
0.30 |
0.46 |
| 9 |
A' |
660 |
626 |
55.27 |
12.72 |
0.25 |
0.40 |
| 10 |
A' |
251 |
238 |
0.86 |
4.46 |
0.34 |
0.51 |
| 11 |
A' |
191 |
182 |
8.00 |
0.12 |
0.28 |
0.44 |
| 12 |
A" |
3239 |
3075 |
1.35 |
12.68 |
0.75 |
0.86 |
| 13 |
A" |
3211 |
3048 |
0.69 |
86.04 |
0.75 |
0.86 |
| 14 |
A" |
1310 |
1244 |
0.10 |
9.84 |
0.75 |
0.86 |
| 15 |
A" |
1146 |
1088 |
2.55 |
0.34 |
0.75 |
0.86 |
| 16 |
A" |
985 |
935 |
0.11 |
8.27 |
0.75 |
0.86 |
| 17 |
A" |
772 |
732 |
4.15 |
0.04 |
0.75 |
0.86 |
| 18 |
A" |
114 |
108 |
5.87 |
0.03 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12828.7 cm
-1
Scaled (by 0.9493) Zero Point Vibrational Energy (zpe) 12178.3 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 B1B95/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.652 |
0.000 |
| C2 |
1.220 |
-0.233 |
0.000 |
| Br3 |
-1.586 |
-0.478 |
0.000 |
| Cl4 |
2.694 |
0.787 |
0.000 |
| H5 |
-0.054 |
1.272 |
0.891 |
| H6 |
-0.054 |
1.272 |
-0.891 |
| H7 |
1.253 |
-0.862 |
0.888 |
| H8 |
1.253 |
-0.862 |
-0.888 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5073 | 1.9472 | 2.6972 | 1.0871 | 1.0871 | 2.1568 | 2.1568 |
C2 | 1.5073 | | 2.8168 | 1.7924 | 2.1641 | 2.1641 | 1.0885 | 1.0885 | Br3 | 1.9472 | 2.8168 | | 4.4628 | 2.4907 | 2.4907 | 2.9999 | 2.9999 | Cl4 | 2.6972 | 1.7924 | 4.4628 | | 2.9291 | 2.9291 | 2.3627 | 2.3627 | H5 | 1.0871 | 2.1641 | 2.4907 | 2.9291 | | 1.7824 | 2.5030 | 3.0708 | H6 | 1.0871 | 2.1641 | 2.4907 | 2.9291 | 1.7824 | | 3.0708 | 2.5030 | H7 | 2.1568 | 1.0885 | 2.9999 | 2.3627 | 2.5030 | 3.0708 | | 1.7755 | H8 | 2.1568 | 1.0885 | 2.9999 | 2.3627 | 3.0708 | 2.5030 | 1.7755 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
109.346 |
|
C1 |
C2 |
H7 |
111.359 |
| C1 |
C2 |
H8 |
111.359 |
|
C2 |
C1 |
Br3 |
108.579 |
| C2 |
C1 |
Cl4 |
38.831 |
|
C2 |
C1 |
H6 |
112.037 |
| Br3 |
C1 |
H5 |
106.891 |
|
Br3 |
C1 |
H6 |
106.891 |
| Cl4 |
C2 |
H7 |
107.673 |
|
Cl4 |
C2 |
H8 |
107.673 |
| H5 |
C1 |
H6 |
110.124 |
|
H7 |
C2 |
H8 |
109.291 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.335 |
|
|
|
| 2 |
C |
-0.417 |
|
|
|
| 3 |
Br |
-0.119 |
|
|
|
| 4 |
Cl |
-0.059 |
|
|
|
| 5 |
H |
0.231 |
|
|
|
| 6 |
H |
0.231 |
|
|
|
| 7 |
H |
0.234 |
|
|
|
| 8 |
H |
0.234 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.206 |
-0.058 |
0.000 |
0.214 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-49.794 |
-2.184 |
0.000 |
| y |
-2.184 |
-42.691 |
0.000 |
| z |
0.000 |
0.000 |
-42.970 |
|
| Traceless |
| | x | y | z |
| x |
-6.963 |
-2.184 |
0.000 |
| y |
-2.184 |
3.691 |
0.000 |
| z |
0.000 |
0.000 |
3.272 |
|
| Polar |
| 3z2-r2 | 6.544 |
| x2-y2 | -7.103 |
| xy | -2.184 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
9.889 |
1.885 |
0.000 |
| y |
1.885 |
6.236 |
0.000 |
| z |
0.000 |
0.000 |
5.110 |
<r2> (average value of r
2) Å
2
| <r2> |
280.971 |
| (<r2>)1/2 |
16.762 |
Jump to
S1C1
Energy calculated at B1B95/6-31G*
| | hartrees |
| Energy at 0K | -3110.839568 |
| Energy at 298.15K | |
| HF Energy | -3110.839568 |
| Nuclear repulsion energy | 307.064065 |
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 B1B95/6-31G*
| 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 |
3216 |
3053 |
1.57 |
45.56 |
0.75 |
0.86 |
| 2 |
A |
3191 |
3030 |
1.70 |
84.40 |
0.75 |
0.86 |
| 3 |
A |
3141 |
2982 |
10.31 |
138.04 |
0.06 |
0.10 |
| 4 |
A |
3121 |
2963 |
9.83 |
108.99 |
0.20 |
0.34 |
| 5 |
A |
1499 |
1423 |
1.76 |
7.55 |
0.69 |
0.82 |
| 6 |
A |
1490 |
1415 |
10.61 |
16.48 |
0.75 |
0.86 |
| 7 |
A |
1360 |
1291 |
25.98 |
4.55 |
0.75 |
0.86 |
| 8 |
A |
1312 |
1246 |
46.52 |
1.51 |
0.54 |
0.70 |
| 9 |
A |
1232 |
1170 |
3.51 |
17.40 |
0.75 |
0.85 |
| 10 |
A |
1164 |
1105 |
1.69 |
6.20 |
0.73 |
0.85 |
| 11 |
A |
1060 |
1007 |
1.86 |
3.94 |
0.73 |
0.84 |
| 12 |
A |
951 |
903 |
9.14 |
6.19 |
0.45 |
0.62 |
| 13 |
A |
879 |
835 |
21.67 |
1.54 |
0.72 |
0.84 |
| 14 |
A |
698 |
663 |
19.33 |
9.29 |
0.39 |
0.56 |
| 15 |
A |
592 |
562 |
11.95 |
14.78 |
0.20 |
0.34 |
| 16 |
A |
390 |
370 |
7.99 |
2.42 |
0.71 |
0.83 |
| 17 |
A |
242 |
229 |
1.16 |
0.94 |
0.35 |
0.52 |
| 18 |
A |
105 |
100 |
0.53 |
1.18 |
0.73 |
0.84 |
Unscaled Zero Point Vibrational Energy (zpe) 12822.4 cm
-1
Scaled (by 0.9493) Zero Point Vibrational Energy (zpe) 12172.3 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 B1B95/6-31G*
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.003 |
1.118 |
-0.378 |
| C2 |
1.278 |
0.907 |
0.396 |
| Br3 |
-1.333 |
-0.227 |
0.036 |
| Cl4 |
2.129 |
-0.584 |
-0.087 |
| H5 |
-0.436 |
2.079 |
-0.111 |
| H6 |
0.169 |
1.074 |
-1.452 |
| H7 |
1.959 |
1.739 |
0.207 |
| H8 |
1.083 |
0.840 |
1.465 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5066 | 1.9409 | 2.7397 | 1.0896 | 1.0876 | 2.1338 | 2.1539 |
C2 | 1.5066 | | 2.8697 | 1.7835 | 2.1379 | 2.1619 | 1.0917 | 1.0890 | Br3 | 1.9409 | 2.8697 | | 3.4833 | 2.4792 | 2.4824 | 3.8385 | 3.0029 | Cl4 | 2.7397 | 1.7835 | 3.4833 | | 3.6982 | 2.9083 | 2.3483 | 2.3525 | H5 | 1.0896 | 2.1379 | 2.4792 | 3.6982 | | 1.7813 | 2.4397 | 2.5152 | H6 | 1.0876 | 2.1619 | 2.4824 | 2.9083 | 1.7813 | | 2.5298 | 3.0658 | H7 | 2.1338 | 1.0917 | 3.8385 | 2.3483 | 2.4397 | 2.5298 | | 1.7773 | H8 | 2.1539 | 1.0890 | 3.0029 | 2.3525 | 2.5152 | 3.0658 | 1.7773 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
112.480 |
|
C1 |
C2 |
H7 |
109.377 |
| C1 |
C2 |
H8 |
111.137 |
|
C2 |
C1 |
Br3 |
112.079 |
| C2 |
C1 |
Cl4 |
36.980 |
|
C2 |
C1 |
H6 |
111.875 |
| Br3 |
C1 |
H5 |
106.373 |
|
Br3 |
C1 |
H6 |
106.687 |
| Cl4 |
C2 |
H7 |
107.049 |
|
Cl4 |
C2 |
H8 |
107.489 |
| H5 |
C1 |
H6 |
109.805 |
|
H7 |
C2 |
H8 |
109.175 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.340 |
|
|
|
| 2 |
C |
-0.412 |
|
|
|
| 3 |
Br |
-0.107 |
|
|
|
| 4 |
Cl |
-0.048 |
|
|
|
| 5 |
H |
0.220 |
|
|
|
| 6 |
H |
0.231 |
|
|
|
| 7 |
H |
0.222 |
|
|
|
| 8 |
H |
0.234 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.303 |
2.766 |
0.123 |
2.786 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-46.920 |
2.885 |
0.444 |
| y |
2.885 |
-39.847 |
-0.125 |
| z |
0.444 |
-0.125 |
-42.588 |
|
| Traceless |
| | x | y | z |
| x |
-5.702 |
2.885 |
0.444 |
| y |
2.885 |
4.907 |
-0.125 |
| z |
0.444 |
-0.125 |
0.796 |
|
| Polar |
| 3z2-r2 | 1.591 |
| x2-y2 | -7.073 |
| xy | 2.885 |
| xz | 0.444 |
| yz | -0.125 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.963 |
0.200 |
-0.284 |
| y |
0.200 |
7.149 |
0.081 |
| z |
-0.284 |
0.081 |
5.292 |
<r2> (average value of r
2) Å
2
| <r2> |
216.802 |
| (<r2>)1/2 |
14.724 |