Jump to
S1C2
Energy calculated at B2PLYP/6-31G
| hartrees |
Energy at 0K | -3109.528640 |
Energy at 298.15K | |
HF Energy | -3109.439912 |
Nuclear repulsion energy | 281.549719 |
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 B2PLYP/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' |
3175 |
3175 |
6.78 |
8.48 |
0.07 |
0.12 |
2 |
A' |
3167 |
3167 |
0.42 |
154.35 |
0.08 |
0.15 |
3 |
A' |
1549 |
1549 |
3.61 |
14.46 |
0.75 |
0.86 |
4 |
A' |
1544 |
1544 |
8.30 |
7.36 |
0.75 |
0.86 |
5 |
A' |
1350 |
1350 |
2.69 |
34.84 |
0.50 |
0.67 |
6 |
A' |
1272 |
1272 |
43.12 |
3.47 |
0.45 |
0.62 |
7 |
A' |
1098 |
1098 |
1.35 |
25.62 |
0.66 |
0.80 |
8 |
A' |
680 |
680 |
20.44 |
88.60 |
0.31 |
0.48 |
9 |
A' |
602 |
602 |
74.00 |
5.72 |
0.34 |
0.51 |
10 |
A' |
237 |
237 |
1.04 |
9.90 |
0.38 |
0.55 |
11 |
A' |
190 |
190 |
9.57 |
0.33 |
0.55 |
0.71 |
12 |
A" |
3263 |
3263 |
2.61 |
2.41 |
0.75 |
0.86 |
13 |
A" |
3240 |
3240 |
0.18 |
98.66 |
0.75 |
0.86 |
14 |
A" |
1335 |
1335 |
0.01 |
11.10 |
0.75 |
0.86 |
15 |
A" |
1144 |
1144 |
1.68 |
0.22 |
0.75 |
0.86 |
16 |
A" |
980 |
980 |
0.09 |
17.76 |
0.75 |
0.86 |
17 |
A" |
792 |
792 |
5.44 |
0.20 |
0.75 |
0.86 |
18 |
A" |
108 |
108 |
7.70 |
0.01 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12863.2 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 12863.2 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 B2PLYP/6-31G
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.676 |
0.000 |
C2 |
1.217 |
-0.216 |
0.000 |
Br3 |
-1.623 |
-0.530 |
0.000 |
Cl4 |
2.769 |
0.876 |
0.000 |
H5 |
-0.082 |
1.284 |
0.897 |
H6 |
-0.082 |
1.284 |
-0.897 |
H7 |
1.290 |
-0.829 |
0.895 |
H8 |
1.290 |
-0.829 |
-0.895 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5092 | 2.0219 | 2.7764 | 1.0868 | 1.0868 | 2.1746 | 2.1746 |
C2 | 1.5092 | | 2.8574 | 1.8974 | 2.1777 | 2.1777 | 1.0872 | 1.0872 | Br3 | 2.0219 | 2.8574 | | 4.6115 | 2.5440 | 2.5440 | 3.0616 | 3.0616 | Cl4 | 2.7764 | 1.8974 | 4.6115 | | 3.0162 | 3.0162 | 2.4281 | 2.4281 | H5 | 1.0868 | 2.1777 | 2.5440 | 3.0162 | | 1.7936 | 2.5191 | 3.0914 | H6 | 1.0868 | 2.1777 | 2.5440 | 3.0162 | 1.7936 | | 3.0914 | 2.5191 | H7 | 2.1746 | 1.0872 | 3.0616 | 2.4281 | 2.5191 | 3.0914 | | 1.7903 | H8 | 2.1746 | 1.0872 | 3.0616 | 2.4281 | 3.0914 | 2.5191 | 1.7903 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
108.638 |
|
C1 |
C2 |
H7 |
112.759 |
C1 |
C2 |
H8 |
112.759 |
|
C2 |
C1 |
Br3 |
107.148 |
C2 |
C1 |
Cl4 |
40.360 |
|
C2 |
C1 |
H6 |
113.042 |
Br3 |
C1 |
H5 |
105.887 |
|
Br3 |
C1 |
H6 |
105.887 |
Cl4 |
C2 |
H7 |
105.656 |
|
Cl4 |
C2 |
H8 |
105.656 |
H5 |
C1 |
H6 |
111.216 |
|
H7 |
C2 |
H8 |
110.843 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-31G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.459 |
|
|
|
2 |
C |
-0.380 |
|
|
|
3 |
Br |
0.008 |
|
|
|
4 |
Cl |
-0.057 |
|
|
|
5 |
H |
0.225 |
|
|
|
6 |
H |
0.225 |
|
|
|
7 |
H |
0.219 |
|
|
|
8 |
H |
0.219 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.467 |
-0.190 |
0.000 |
0.504 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-53.197 |
-3.519 |
-0.013 |
y |
-3.519 |
-43.992 |
-0.005 |
z |
-0.013 |
-0.005 |
-43.794 |
|
Traceless |
| x | y | z |
x |
-9.304 |
-3.519 |
-0.013 |
y |
-3.519 |
4.504 |
-0.005 |
z |
-0.013 |
-0.005 |
4.801 |
|
Polar |
3z2-r2 | 9.601 |
x2-y2 | -9.205 |
xy | -3.519 |
xz | -0.013 |
yz | -0.005 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
9.928 |
2.901 |
0.000 |
y |
2.901 |
5.601 |
0.000 |
z |
0.000 |
0.000 |
3.782 |
<r2> (average value of r
2) Å
2
<r2> |
297.893 |
(<r2>)1/2 |
17.260 |
Jump to
S1C1
Energy calculated at B2PLYP/6-31G
| hartrees |
Energy at 0K | -3109.524807 |
Energy at 298.15K | |
HF Energy | -3109.435941 |
Nuclear repulsion energy | 298.327634 |
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 B2PLYP/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 |
3232 |
3232 |
2.20 |
32.28 |
0.75 |
0.85 |
2 |
A |
3218 |
3218 |
0.42 |
103.32 |
0.75 |
0.86 |
3 |
A |
3147 |
3147 |
12.82 |
197.81 |
0.02 |
0.04 |
4 |
A |
3138 |
3138 |
3.27 |
68.68 |
0.54 |
0.71 |
5 |
A |
1531 |
1531 |
6.32 |
14.62 |
0.72 |
0.84 |
6 |
A |
1522 |
1522 |
8.72 |
16.41 |
0.74 |
0.85 |
7 |
A |
1369 |
1369 |
25.87 |
5.31 |
0.69 |
0.82 |
8 |
A |
1337 |
1337 |
48.27 |
2.54 |
0.63 |
0.78 |
9 |
A |
1231 |
1231 |
1.88 |
28.13 |
0.75 |
0.86 |
10 |
A |
1167 |
1167 |
1.39 |
10.62 |
0.74 |
0.85 |
11 |
A |
1076 |
1076 |
2.70 |
4.74 |
0.71 |
0.83 |
12 |
A |
953 |
953 |
8.49 |
13.61 |
0.54 |
0.70 |
13 |
A |
881 |
881 |
21.93 |
3.03 |
0.66 |
0.79 |
14 |
A |
619 |
619 |
26.49 |
19.12 |
0.47 |
0.64 |
15 |
A |
545 |
545 |
13.26 |
19.96 |
0.22 |
0.36 |
16 |
A |
379 |
379 |
10.35 |
5.02 |
0.74 |
0.85 |
17 |
A |
241 |
241 |
1.55 |
1.91 |
0.43 |
0.60 |
18 |
A |
91 |
91 |
0.82 |
2.71 |
0.74 |
0.85 |
Unscaled Zero Point Vibrational Energy (zpe) 12838.2 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 12838.2 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 B2PLYP/6-31G
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.017 |
1.148 |
-0.400 |
C2 |
1.270 |
0.955 |
0.418 |
Br3 |
-1.374 |
-0.236 |
0.036 |
Cl4 |
2.211 |
-0.596 |
-0.086 |
H5 |
-0.449 |
2.104 |
-0.161 |
H6 |
0.195 |
1.064 |
-1.470 |
H7 |
1.969 |
1.775 |
0.250 |
H8 |
1.062 |
0.843 |
1.480 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5091 | 2.0100 | 2.8208 | 1.0904 | 1.0875 | 2.1514 | 2.1731 |
C2 | 1.5091 | | 2.9248 | 1.8835 | 2.1474 | 2.1754 | 1.0907 | 1.0879 | Br3 | 2.0100 | 2.9248 | | 3.6052 | 2.5245 | 2.5339 | 3.9073 | 3.0305 | Cl4 | 2.8208 | 1.8835 | 3.6052 | | 3.7917 | 2.9561 | 2.4073 | 2.4177 | H5 | 1.0904 | 2.1474 | 2.5245 | 3.7917 | | 1.7914 | 2.4750 | 2.5631 | H6 | 1.0875 | 2.1754 | 2.5339 | 2.9561 | 1.7914 | | 2.5713 | 3.0829 | H7 | 2.1514 | 1.0907 | 3.9073 | 2.4073 | 2.4750 | 2.5713 | | 1.7902 | H8 | 2.1731 | 1.0879 | 3.0305 | 2.4177 | 2.5631 | 3.0829 | 1.7902 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
112.025 |
|
C1 |
C2 |
H7 |
110.660 |
C1 |
C2 |
H8 |
112.587 |
|
C2 |
C1 |
Br3 |
111.638 |
C2 |
C1 |
Cl4 |
38.243 |
|
C2 |
C1 |
H6 |
112.804 |
Br3 |
C1 |
H5 |
105.127 |
|
Br3 |
C1 |
H6 |
105.899 |
Cl4 |
C2 |
H7 |
104.919 |
|
Cl4 |
C2 |
H8 |
105.771 |
H5 |
C1 |
H6 |
110.674 |
|
H7 |
C2 |
H8 |
110.516 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-31G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.468 |
|
|
|
2 |
C |
-0.386 |
|
|
|
3 |
Br |
0.024 |
|
|
|
4 |
Cl |
-0.038 |
|
|
|
5 |
H |
0.214 |
|
|
|
6 |
H |
0.226 |
|
|
|
7 |
H |
0.209 |
|
|
|
8 |
H |
0.218 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.130 |
3.273 |
0.186 |
3.281 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-49.081 |
3.305 |
0.686 |
y |
3.305 |
-40.869 |
-0.103 |
z |
0.686 |
-0.103 |
-43.340 |
|
Traceless |
| x | y | z |
x |
-6.976 |
3.305 |
0.686 |
y |
3.305 |
5.341 |
-0.103 |
z |
0.686 |
-0.103 |
1.635 |
|
Polar |
3z2-r2 | 3.270 |
x2-y2 | -8.212 |
xy | 3.305 |
xz | 0.686 |
yz | -0.103 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
7.287 |
0.395 |
-0.569 |
y |
0.395 |
6.721 |
0.039 |
z |
-0.569 |
0.039 |
4.076 |
<r2> (average value of r
2) Å
2
<r2> |
229.281 |
(<r2>)1/2 |
15.142 |