Jump to
S1C2
Energy calculated at HF/LANL2DZ
| | hartrees |
| Energy at 0K | -105.665430 |
| Energy at 298.15K | |
| HF Energy | -105.665430 |
| Nuclear repulsion energy | 86.711426 |
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/LANL2DZ
| 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' |
3346 |
3011 |
17.84 |
36.65 |
0.07 |
0.12 |
| 2 |
A' |
3339 |
3005 |
3.96 |
193.36 |
0.05 |
0.10 |
| 3 |
A' |
1645 |
1480 |
1.03 |
15.14 |
0.73 |
0.84 |
| 4 |
A' |
1634 |
1470 |
11.71 |
2.33 |
0.67 |
0.80 |
| 5 |
A' |
1458 |
1312 |
1.83 |
38.01 |
0.44 |
0.62 |
| 6 |
A' |
1378 |
1240 |
73.55 |
5.08 |
0.54 |
0.70 |
| 7 |
A' |
1156 |
1041 |
1.75 |
24.84 |
0.75 |
0.85 |
| 8 |
A' |
726 |
653 |
20.95 |
92.77 |
0.31 |
0.47 |
| 9 |
A' |
623 |
561 |
115.04 |
7.89 |
0.35 |
0.52 |
| 10 |
A' |
248 |
223 |
1.69 |
16.65 |
0.38 |
0.55 |
| 11 |
A' |
204 |
184 |
11.07 |
0.82 |
0.51 |
0.68 |
| 12 |
A" |
3441 |
3097 |
8.44 |
1.27 |
0.75 |
0.86 |
| 13 |
A" |
3423 |
3080 |
0.04 |
99.21 |
0.75 |
0.86 |
| 14 |
A" |
1413 |
1272 |
0.03 |
13.94 |
0.75 |
0.86 |
| 15 |
A" |
1233 |
1109 |
0.97 |
0.38 |
0.75 |
0.86 |
| 16 |
A" |
1072 |
965 |
0.61 |
13.54 |
0.75 |
0.86 |
| 17 |
A" |
854 |
769 |
5.38 |
0.20 |
0.75 |
0.86 |
| 18 |
A" |
112 |
101 |
10.84 |
0.05 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13651.9 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 12285.4 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/LANL2DZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.654 |
0.000 |
| C2 |
1.253 |
-0.195 |
0.000 |
| Br3 |
-1.616 |
-0.567 |
0.000 |
| Cl4 |
2.737 |
0.951 |
0.000 |
| H5 |
-0.092 |
1.256 |
0.885 |
| H6 |
-0.092 |
1.256 |
-0.885 |
| H7 |
1.351 |
-0.795 |
0.885 |
| H8 |
1.351 |
-0.795 |
-0.885 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5145 | 2.0259 | 2.7532 | 1.0738 | 1.0738 | 2.1704 | 2.1704 |
C2 | 1.5145 | | 2.8937 | 1.8751 | 2.1679 | 2.1679 | 1.0735 | 1.0735 | Br3 | 2.0259 | 2.8937 | | 4.6105 | 2.5353 | 2.5353 | 3.1052 | 3.1052 | Cl4 | 2.7532 | 1.8751 | 4.6105 | | 2.9801 | 2.9801 | 2.3985 | 2.3985 | H5 | 1.0738 | 2.1679 | 2.5353 | 2.9801 | | 1.7698 | 2.5078 | 3.0696 | H6 | 1.0738 | 2.1679 | 2.5353 | 2.9801 | 1.7698 | | 3.0696 | 2.5078 | H7 | 2.1704 | 1.0735 | 3.1052 | 2.3985 | 2.5078 | 3.0696 | | 1.7703 | H8 | 2.1704 | 1.0735 | 3.1052 | 2.3985 | 3.0696 | 2.5078 | 1.7703 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
108.164 |
|
C1 |
C2 |
H7 |
112.883 |
| C1 |
C2 |
H8 |
112.883 |
|
C2 |
C1 |
Br3 |
108.781 |
| C2 |
C1 |
Cl4 |
40.325 |
|
C2 |
C1 |
H6 |
112.664 |
| Br3 |
C1 |
H5 |
105.608 |
|
Br3 |
C1 |
H6 |
105.608 |
| Cl4 |
C2 |
H7 |
105.625 |
|
Cl4 |
C2 |
H8 |
105.625 |
| H5 |
C1 |
H6 |
110.990 |
|
H7 |
C2 |
H8 |
111.082 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.473 |
|
|
|
| 2 |
C |
-0.356 |
|
|
|
| 3 |
Br |
-0.051 |
|
|
|
| 4 |
Cl |
-0.139 |
|
|
|
| 5 |
H |
0.260 |
|
|
|
| 6 |
H |
0.260 |
|
|
|
| 7 |
H |
0.249 |
|
|
|
| 8 |
H |
0.249 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.301 |
-0.235 |
0.000 |
0.382 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-51.599 |
-4.762 |
0.000 |
| y |
-4.762 |
-40.591 |
0.000 |
| z |
0.000 |
0.000 |
-39.860 |
|
| Traceless |
| | x | y | z |
| x |
-11.373 |
-4.762 |
0.000 |
| y |
-4.762 |
5.138 |
0.000 |
| z |
0.000 |
0.000 |
6.235 |
|
| Polar |
| 3z2-r2 | 12.470 |
| x2-y2 | -11.007 |
| xy | -4.762 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
9.135 |
3.445 |
0.000 |
| y |
3.445 |
5.513 |
0.000 |
| z |
0.000 |
0.000 |
3.125 |
<r2> (average value of r
2) Å
2
| <r2> |
130.251 |
| (<r2>)1/2 |
11.413 |
Jump to
S1C1
Energy calculated at HF/LANL2DZ
| | hartrees |
| Energy at 0K | -105.661321 |
| Energy at 298.15K | |
| HF Energy | -105.661321 |
| Nuclear repulsion energy | 87.664215 |
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/LANL2DZ
| 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 |
3409 |
3067 |
8.47 |
28.23 |
0.75 |
0.86 |
| 2 |
A |
3399 |
3058 |
0.96 |
103.83 |
0.74 |
0.85 |
| 3 |
A |
3319 |
2987 |
39.60 |
271.79 |
0.02 |
0.04 |
| 4 |
A |
3308 |
2977 |
6.95 |
48.16 |
0.62 |
0.76 |
| 5 |
A |
1625 |
1463 |
4.45 |
11.32 |
0.75 |
0.86 |
| 6 |
A |
1614 |
1453 |
8.13 |
15.41 |
0.73 |
0.84 |
| 7 |
A |
1471 |
1323 |
31.41 |
3.94 |
0.48 |
0.65 |
| 8 |
A |
1438 |
1294 |
69.22 |
5.57 |
0.54 |
0.70 |
| 9 |
A |
1325 |
1192 |
1.37 |
21.60 |
0.75 |
0.86 |
| 10 |
A |
1253 |
1128 |
1.47 |
7.91 |
0.74 |
0.85 |
| 11 |
A |
1141 |
1026 |
2.16 |
6.38 |
0.67 |
0.80 |
| 12 |
A |
1026 |
924 |
9.35 |
11.33 |
0.45 |
0.62 |
| 13 |
A |
965 |
868 |
25.95 |
2.19 |
0.69 |
0.82 |
| 14 |
A |
655 |
589 |
44.13 |
31.03 |
0.46 |
0.63 |
| 15 |
A |
565 |
508 |
22.07 |
40.38 |
0.25 |
0.40 |
| 16 |
A |
401 |
361 |
14.12 |
7.80 |
0.73 |
0.84 |
| 17 |
A |
257 |
231 |
2.16 |
3.24 |
0.49 |
0.65 |
| 18 |
A |
97 |
87 |
1.40 |
4.42 |
0.74 |
0.85 |
Unscaled Zero Point Vibrational Energy (zpe) 13633.3 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 12268.6 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/LANL2DZ
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.036 |
1.113 |
-0.406 |
| C2 |
1.289 |
0.927 |
0.425 |
| Br3 |
-1.400 |
-0.228 |
0.036 |
| Cl4 |
2.246 |
-0.583 |
-0.086 |
| H5 |
-0.408 |
2.072 |
-0.197 |
| H6 |
0.222 |
1.007 |
-1.459 |
| H7 |
1.964 |
1.752 |
0.267 |
| H8 |
1.082 |
0.808 |
1.472 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5149 | 2.0135 | 2.8037 | 1.0772 | 1.0745 | 2.1391 | 2.1713 |
C2 | 1.5149 | | 2.9522 | 1.8594 | 2.1396 | 2.1668 | 1.0770 | 1.0741 | Br3 | 2.0135 | 2.9522 | | 3.6649 | 2.5149 | 2.5278 | 3.9095 | 3.0488 | Cl4 | 2.8037 | 1.8594 | 3.6649 | | 3.7555 | 2.9172 | 2.3783 | 2.3912 | H5 | 1.0772 | 2.1396 | 2.5149 | 3.7555 | | 1.7669 | 2.4379 | 2.5701 | H6 | 1.0745 | 2.1668 | 2.5278 | 2.9172 | 1.7669 | | 2.5626 | 3.0614 | H7 | 2.1391 | 1.0770 | 3.9095 | 2.3783 | 2.4379 | 2.5626 | | 1.7665 | H8 | 2.1713 | 1.0741 | 3.0488 | 2.3912 | 2.5701 | 3.0614 | 1.7665 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
111.982 |
|
C1 |
C2 |
H7 |
110.096 |
| C1 |
C2 |
H8 |
112.894 |
|
C2 |
C1 |
Br3 |
112.821 |
| C2 |
C1 |
Cl4 |
37.950 |
|
C2 |
C1 |
H6 |
112.496 |
| Br3 |
C1 |
H5 |
104.823 |
|
Br3 |
C1 |
H6 |
105.837 |
| Cl4 |
C2 |
H7 |
105.031 |
|
Cl4 |
C2 |
H8 |
106.082 |
| H5 |
C1 |
H6 |
110.403 |
|
H7 |
C2 |
H8 |
110.412 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.483 |
|
|
|
| 2 |
C |
-0.363 |
|
|
|
| 3 |
Br |
-0.033 |
|
|
|
| 4 |
Cl |
-0.120 |
|
|
|
| 5 |
H |
0.244 |
|
|
|
| 6 |
H |
0.263 |
|
|
|
| 7 |
H |
0.239 |
|
|
|
| 8 |
H |
0.252 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.290 |
3.811 |
0.223 |
3.829 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-46.873 |
3.912 |
0.802 |
| y |
3.912 |
-37.080 |
-0.157 |
| z |
0.802 |
-0.157 |
-39.353 |
|
| Traceless |
| | x | y | z |
| x |
-8.657 |
3.912 |
0.802 |
| y |
3.912 |
6.033 |
-0.157 |
| z |
0.802 |
-0.157 |
2.623 |
|
| Polar |
| 3z2-r2 | 5.247 |
| x2-y2 | -9.793 |
| xy | 3.912 |
| xz | 0.802 |
| yz | -0.157 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.920 |
0.734 |
-0.813 |
| y |
0.734 |
6.400 |
0.005 |
| z |
-0.813 |
0.005 |
3.506 |
<r2> (average value of r
2) Å
2
| <r2> |
120.816 |
| (<r2>)1/2 |
10.992 |