Jump to
S1C2
Energy calculated at QCISD/6-31G*
| | hartrees |
| Energy at 0K | -3107.986825 |
| Energy at 298.15K | |
| HF Energy | -3107.438448 |
| Nuclear repulsion energy | 287.718776 |
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 QCISD/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' |
202 |
192 |
7.16 |
|
|
|
| 2 |
A' |
255 |
243 |
0.81 |
|
|
|
| 3 |
A' |
660 |
628 |
45.62 |
|
|
|
| 4 |
A' |
786 |
749 |
25.46 |
|
|
|
| 5 |
A' |
1102 |
1049 |
1.30 |
|
|
|
| 6 |
A' |
1270 |
1209 |
43.69 |
|
|
|
| 7 |
A' |
1380 |
1315 |
3.02 |
|
|
|
| 8 |
A' |
1537 |
1464 |
6.01 |
|
|
|
| 9 |
A' |
1541 |
1467 |
1.17 |
|
|
|
| 10 |
A' |
3140 |
2991 |
4.03 |
|
|
|
| 11 |
A' |
3151 |
3001 |
8.02 |
|
|
|
| 12 |
A" |
116 |
111 |
6.09 |
|
|
|
| 13 |
A" |
783 |
746 |
3.04 |
|
|
|
| 14 |
A" |
1009 |
961 |
0.19 |
|
|
|
| 15 |
A" |
1169 |
1113 |
2.29 |
|
|
|
| 16 |
A" |
1331 |
1268 |
0.09 |
|
|
|
| 17 |
A" |
3200 |
3047 |
1.01 |
|
|
|
| 18 |
A" |
3225 |
3071 |
2.60 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 12928.2 cm
-1
Scaled (by 0.9523) Zero Point Vibrational Energy (zpe) 12311.5 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 QCISD/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.656 |
0.000 |
| C2 |
1.239 |
-0.218 |
0.000 |
| Br3 |
-1.594 |
-0.499 |
0.000 |
| Cl4 |
2.701 |
0.823 |
0.000 |
| H5 |
-0.062 |
1.278 |
0.895 |
| H6 |
-0.062 |
1.278 |
-0.895 |
| H7 |
1.276 |
-0.849 |
0.891 |
| H8 |
1.276 |
-0.849 |
-0.891 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5162 | 1.9684 | 2.7061 | 1.0909 | 1.0909 | 2.1646 | 2.1646 |
C2 | 1.5162 | | 2.8461 | 1.7948 | 2.1746 | 2.1746 | 1.0919 | 1.0919 | Br3 | 1.9684 | 2.8461 | | 4.4933 | 2.5105 | 2.5105 | 3.0246 | 3.0246 | Cl4 | 2.7061 | 1.7948 | 4.4933 | | 2.9397 | 2.9397 | 2.3702 | 2.3702 | H5 | 1.0909 | 2.1746 | 2.5105 | 2.9397 | | 1.7891 | 2.5120 | 3.0818 | H6 | 1.0909 | 2.1746 | 2.5105 | 2.9397 | 1.7891 | | 3.0818 | 2.5120 | H7 | 2.1646 | 1.0919 | 3.0246 | 2.3702 | 2.5120 | 3.0818 | | 1.7814 | H8 | 2.1646 | 1.0919 | 3.0246 | 2.3702 | 3.0818 | 2.5120 | 1.7814 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
109.342 |
|
C1 |
C2 |
H7 |
111.146 |
| C1 |
C2 |
H8 |
111.146 |
|
C2 |
C1 |
Br3 |
108.832 |
| C2 |
C1 |
Cl4 |
38.742 |
|
C2 |
C1 |
H6 |
112.020 |
| Br3 |
C1 |
H5 |
106.753 |
|
Br3 |
C1 |
H6 |
106.753 |
| Cl4 |
C2 |
H7 |
107.888 |
|
Cl4 |
C2 |
H8 |
107.888 |
| H5 |
C1 |
H6 |
110.173 |
|
H7 |
C2 |
H8 |
109.320 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at QCISD/6-31G*
| | hartrees |
| Energy at 0K | -3107.984273 |
| Energy at 298.15K | |
| HF Energy | -3107.435079 |
| Nuclear repulsion energy | 304.581333 |
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 QCISD/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 |
3206 |
3053 |
2.38 |
|
|
|
| 2 |
A |
3182 |
3030 |
2.52 |
|
|
|
| 3 |
A |
3134 |
2984 |
11.92 |
|
|
|
| 4 |
A |
3114 |
2965 |
10.45 |
|
|
|
| 5 |
A |
1526 |
1454 |
1.66 |
|
|
|
| 6 |
A |
1519 |
1446 |
9.26 |
|
|
|
| 7 |
A |
1391 |
1325 |
25.67 |
|
|
|
| 8 |
A |
1339 |
1275 |
43.37 |
|
|
|
| 9 |
A |
1252 |
1192 |
3.47 |
|
|
|
| 10 |
A |
1182 |
1125 |
1.68 |
|
|
|
| 11 |
A |
1078 |
1027 |
1.26 |
|
|
|
| 12 |
A |
971 |
925 |
7.41 |
|
|
|
| 13 |
A |
902 |
859 |
16.51 |
|
|
|
| 14 |
A |
710 |
676 |
15.57 |
|
|
|
| 15 |
A |
585 |
557 |
11.01 |
|
|
|
| 16 |
A |
397 |
378 |
7.18 |
|
|
|
| 17 |
A |
248 |
236 |
1.14 |
|
|
|
| 18 |
A |
106 |
101 |
0.58 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 12920.5 cm
-1
Scaled (by 0.9523) Zero Point Vibrational Energy (zpe) 12304.2 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 QCISD/6-31G*
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.016 |
1.120 |
-0.384 |
| C2 |
1.291 |
0.902 |
0.405 |
| Br3 |
-1.350 |
-0.226 |
0.036 |
| Cl4 |
2.152 |
-0.585 |
-0.088 |
| H5 |
-0.422 |
2.088 |
-0.127 |
| H6 |
0.189 |
1.064 |
-1.461 |
| H7 |
1.971 |
1.742 |
0.230 |
| H8 |
1.081 |
0.826 |
1.475 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5157 | 1.9633 | 2.7490 | 1.0931 | 1.0913 | 2.1414 | 2.1625 |
C2 | 1.5157 | | 2.8954 | 1.7872 | 2.1510 | 2.1732 | 1.0953 | 1.0924 | Br3 | 1.9633 | 2.8954 | | 3.5220 | 2.4983 | 2.5039 | 3.8651 | 3.0142 | Cl4 | 2.7490 | 1.7872 | 3.5220 | | 3.7111 | 2.9077 | 2.3561 | 2.3623 | H5 | 1.0931 | 2.1510 | 2.4983 | 3.7111 | | 1.7891 | 2.4441 | 2.5332 | H6 | 1.0913 | 2.1732 | 2.5039 | 2.9077 | 1.7891 | | 2.5483 | 3.0769 | H7 | 2.1414 | 1.0953 | 3.8651 | 2.3561 | 2.4441 | 2.5483 | | 1.7836 | H8 | 2.1625 | 1.0924 | 3.0142 | 2.3623 | 2.5332 | 3.0769 | 1.7836 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
112.407 |
|
C1 |
C2 |
H7 |
109.134 |
| C1 |
C2 |
H8 |
110.976 |
|
C2 |
C1 |
Br3 |
112.013 |
| C2 |
C1 |
Cl4 |
36.946 |
|
C2 |
C1 |
H6 |
111.910 |
| Br3 |
C1 |
H5 |
106.121 |
|
Br3 |
C1 |
H6 |
106.592 |
| Cl4 |
C2 |
H7 |
107.197 |
|
Cl4 |
C2 |
H8 |
107.788 |
| H5 |
C1 |
H6 |
109.973 |
|
H7 |
C2 |
H8 |
109.227 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability