Jump to
S1C2
Energy calculated at HF/6-31G(2df,p)
| hartrees |
Energy at 0K | -3107.632588 |
Energy at 298.15K | |
HF Energy | -3107.632588 |
Nuclear repulsion energy | 290.461012 |
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/6-31G(2df,p)
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' |
3268 |
2959 |
15.92 |
5.34 |
0.10 |
0.18 |
2 |
A' |
3261 |
2953 |
0.82 |
123.92 |
0.08 |
0.14 |
3 |
A' |
1614 |
1462 |
0.84 |
10.74 |
0.74 |
0.85 |
4 |
A' |
1608 |
1456 |
6.57 |
1.80 |
0.74 |
0.85 |
5 |
A' |
1447 |
1310 |
2.72 |
13.19 |
0.42 |
0.59 |
6 |
A' |
1344 |
1217 |
58.90 |
1.92 |
0.31 |
0.48 |
7 |
A' |
1127 |
1020 |
1.28 |
5.39 |
0.60 |
0.75 |
8 |
A' |
803 |
727 |
32.80 |
46.26 |
0.28 |
0.44 |
9 |
A' |
703 |
636 |
80.75 |
8.93 |
0.22 |
0.36 |
10 |
A' |
269 |
243 |
0.80 |
5.83 |
0.27 |
0.42 |
11 |
A' |
214 |
194 |
7.43 |
0.20 |
0.20 |
0.33 |
12 |
A" |
3344 |
3028 |
2.41 |
0.84 |
0.75 |
0.86 |
13 |
A" |
3321 |
3007 |
0.17 |
84.71 |
0.75 |
0.86 |
14 |
A" |
1400 |
1267 |
0.06 |
6.58 |
0.75 |
0.86 |
15 |
A" |
1226 |
1110 |
1.35 |
0.15 |
0.75 |
0.86 |
16 |
A" |
1065 |
964 |
0.13 |
3.71 |
0.75 |
0.86 |
17 |
A" |
819 |
741 |
2.21 |
0.00 |
0.75 |
0.86 |
18 |
A" |
119 |
108 |
6.83 |
0.01 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13475.3 cm
-1
Scaled (by 0.9055) Zero Point Vibrational Energy (zpe) 12201.9 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/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.638 |
0.000 |
C2 |
1.220 |
-0.258 |
0.000 |
Br3 |
-1.591 |
-0.452 |
0.000 |
Cl4 |
2.702 |
0.751 |
0.000 |
H5 |
-0.036 |
1.257 |
0.881 |
H6 |
-0.036 |
1.257 |
-0.881 |
H7 |
1.256 |
-0.878 |
0.881 |
H8 |
1.256 |
-0.878 |
-0.881 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5132 | 1.9285 | 2.7046 | 1.0780 | 1.0780 | 2.1568 | 2.1568 |
C2 | 1.5132 | | 2.8180 | 1.7930 | 2.1564 | 2.1564 | 1.0782 | 1.0782 | Br3 | 1.9285 | 2.8180 | | 4.4588 | 2.4731 | 2.4731 | 3.0113 | 3.0113 | Cl4 | 2.7046 | 1.7930 | 4.4588 | | 2.9209 | 2.9209 | 2.3496 | 2.3496 | H5 | 1.0780 | 2.1564 | 2.4731 | 2.9209 | | 1.7626 | 2.4959 | 3.0556 | H6 | 1.0780 | 2.1564 | 2.4731 | 2.9209 | 1.7626 | | 3.0556 | 2.4959 | H7 | 2.1568 | 1.0782 | 3.0113 | 2.3496 | 2.4959 | 3.0556 | | 1.7626 | H8 | 2.1568 | 1.0782 | 3.0113 | 2.3496 | 3.0556 | 2.4959 | 1.7626 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
109.485 |
|
C1 |
C2 |
H7 |
111.566 |
C1 |
C2 |
H8 |
111.566 |
|
C2 |
C1 |
Br3 |
109.331 |
C2 |
C1 |
Cl4 |
38.681 |
|
C2 |
C1 |
H6 |
111.542 |
Br3 |
C1 |
H5 |
107.281 |
|
Br3 |
C1 |
H6 |
107.281 |
Cl4 |
C2 |
H7 |
107.195 |
|
Cl4 |
C2 |
H8 |
107.195 |
H5 |
C1 |
H6 |
109.679 |
|
H7 |
C2 |
H8 |
109.643 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31G(2df,p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.352 |
|
|
|
2 |
C |
-0.212 |
|
|
|
3 |
Br |
-0.057 |
|
|
|
4 |
Cl |
-0.174 |
|
|
|
5 |
H |
0.201 |
|
|
|
6 |
H |
0.201 |
|
|
|
7 |
H |
0.196 |
|
|
|
8 |
H |
0.196 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.163 |
-0.045 |
0.000 |
0.169 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-51.211 |
-2.447 |
0.000 |
y |
-2.447 |
-43.243 |
0.000 |
z |
0.000 |
0.000 |
-43.439 |
|
Traceless |
| x | y | z |
x |
-7.870 |
-2.447 |
0.000 |
y |
-2.447 |
4.083 |
0.000 |
z |
0.000 |
0.000 |
3.788 |
|
Polar |
3z2-r2 | 7.575 |
x2-y2 | -7.969 |
xy | -2.447 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
10.283 |
1.663 |
0.000 |
y |
1.663 |
6.946 |
0.000 |
z |
0.000 |
0.000 |
5.989 |
<r2> (average value of r
2) Å
2
<r2> |
280.943 |
(<r2>)1/2 |
16.761 |
Jump to
S1C1
Energy calculated at HF/6-31G(2df,p)
| hartrees |
Energy at 0K | -3107.629383 |
Energy at 298.15K | |
HF Energy | -3107.629383 |
Nuclear repulsion energy | 306.087661 |
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/6-31G(2df,p)
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 |
3321 |
3007 |
3.77 |
23.71 |
0.75 |
0.86 |
2 |
A |
3306 |
2994 |
1.14 |
85.01 |
0.75 |
0.86 |
3 |
A |
3250 |
2943 |
23.74 |
150.67 |
0.04 |
0.07 |
4 |
A |
3235 |
2930 |
6.47 |
53.13 |
0.45 |
0.62 |
5 |
A |
1601 |
1450 |
2.05 |
6.74 |
0.75 |
0.86 |
6 |
A |
1591 |
1441 |
7.32 |
10.72 |
0.74 |
0.85 |
7 |
A |
1455 |
1317 |
30.66 |
0.93 |
0.64 |
0.78 |
8 |
A |
1414 |
1280 |
59.19 |
2.16 |
0.35 |
0.52 |
9 |
A |
1318 |
1194 |
1.35 |
8.61 |
0.71 |
0.83 |
10 |
A |
1241 |
1124 |
0.87 |
2.98 |
0.72 |
0.84 |
11 |
A |
1115 |
1009 |
1.62 |
3.08 |
0.63 |
0.77 |
12 |
A |
1012 |
917 |
10.44 |
4.04 |
0.39 |
0.56 |
13 |
A |
950 |
860 |
18.25 |
1.40 |
0.70 |
0.83 |
14 |
A |
726 |
657 |
31.39 |
12.57 |
0.39 |
0.56 |
15 |
A |
628 |
569 |
16.29 |
20.61 |
0.16 |
0.28 |
16 |
A |
416 |
377 |
8.70 |
2.05 |
0.69 |
0.82 |
17 |
A |
259 |
235 |
1.30 |
0.93 |
0.24 |
0.39 |
18 |
A |
106 |
96 |
0.80 |
1.11 |
0.70 |
0.82 |
Unscaled Zero Point Vibrational Energy (zpe) 13471.6 cm
-1
Scaled (by 0.9055) Zero Point Vibrational Energy (zpe) 12198.5 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/6-31G(2df,p)
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.005 |
1.083 |
-0.387 |
C2 |
1.270 |
0.892 |
0.405 |
Br3 |
-1.352 |
-0.225 |
0.036 |
Cl4 |
2.176 |
-0.565 |
-0.087 |
H5 |
-0.430 |
2.047 |
-0.148 |
H6 |
0.177 |
1.023 |
-1.448 |
H7 |
1.925 |
1.735 |
0.232 |
H8 |
1.070 |
0.804 |
1.462 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5131 | 1.9237 | 2.7500 | 1.0806 | 1.0783 | 2.1292 | 2.1566 |
C2 | 1.5131 | | 2.8735 | 1.7848 | 2.1280 | 2.1552 | 1.0814 | 1.0786 | Br3 | 1.9237 | 2.8735 | | 3.5466 | 2.4589 | 2.4690 | 3.8229 | 2.9931 | Cl4 | 2.7500 | 1.7848 | 3.5466 | | 3.6899 | 2.8931 | 2.3353 | 2.3437 | H5 | 1.0806 | 2.1280 | 2.4589 | 3.6899 | | 1.7624 | 2.4049 | 2.5272 | H6 | 1.0783 | 2.1552 | 2.4690 | 2.8931 | 1.7624 | | 2.5264 | 3.0513 | H7 | 2.1292 | 1.0814 | 3.8229 | 2.3353 | 2.4049 | 2.5264 | | 1.7631 | H8 | 2.1566 | 1.0786 | 2.9931 | 2.3437 | 2.5272 | 3.0513 | 1.7631 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
112.734 |
|
C1 |
C2 |
H7 |
109.165 |
C1 |
C2 |
H8 |
111.538 |
|
C2 |
C1 |
Br3 |
112.919 |
C2 |
C1 |
Cl4 |
36.770 |
|
C2 |
C1 |
H6 |
111.441 |
Br3 |
C1 |
H5 |
106.464 |
|
Br3 |
C1 |
H6 |
107.286 |
Cl4 |
C2 |
H7 |
106.535 |
|
Cl4 |
C2 |
H8 |
107.283 |
H5 |
C1 |
H6 |
109.445 |
|
H7 |
C2 |
H8 |
109.423 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31G(2df,p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.355 |
|
|
|
2 |
C |
-0.212 |
|
|
|
3 |
Br |
-0.047 |
|
|
|
4 |
Cl |
-0.162 |
|
|
|
5 |
H |
0.193 |
|
|
|
6 |
H |
0.202 |
|
|
|
7 |
H |
0.186 |
|
|
|
8 |
H |
0.195 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.309 |
2.873 |
0.115 |
2.892 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-48.266 |
2.825 |
0.520 |
y |
2.825 |
-40.473 |
-0.094 |
z |
0.520 |
-0.094 |
-43.034 |
|
Traceless |
| x | y | z |
x |
-6.512 |
2.825 |
0.520 |
y |
2.825 |
5.177 |
-0.094 |
z |
0.520 |
-0.094 |
1.335 |
|
Polar |
3z2-r2 | 2.670 |
x2-y2 | -7.793 |
xy | 2.825 |
xz | 0.520 |
yz | -0.094 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
8.722 |
0.145 |
-0.284 |
y |
0.145 |
7.673 |
0.054 |
z |
-0.284 |
0.054 |
6.130 |
<r2> (average value of r
2) Å
2
<r2> |
220.906 |
(<r2>)1/2 |
14.863 |