Jump to
S1C2
Energy calculated at PBE1PBE/6-31G*
| hartrees |
Energy at 0K | -3109.934088 |
Energy at 298.15K | |
HF Energy | -3109.934088 |
Nuclear repulsion energy | 289.351828 |
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 PBE1PBE/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' |
3155 |
2998 |
6.72 |
35.45 |
0.07 |
0.13 |
2 |
A' |
3141 |
2985 |
3.07 |
114.59 |
0.08 |
0.14 |
3 |
A' |
1515 |
1440 |
1.24 |
15.30 |
0.75 |
0.85 |
4 |
A' |
1510 |
1435 |
7.21 |
2.04 |
0.74 |
0.85 |
5 |
A' |
1347 |
1280 |
3.00 |
13.63 |
0.59 |
0.74 |
6 |
A' |
1248 |
1186 |
40.67 |
2.51 |
0.44 |
0.61 |
7 |
A' |
1094 |
1039 |
1.45 |
7.55 |
0.75 |
0.85 |
8 |
A' |
767 |
729 |
33.59 |
45.47 |
0.30 |
0.46 |
9 |
A' |
664 |
631 |
54.72 |
12.41 |
0.25 |
0.40 |
10 |
A' |
253 |
241 |
0.90 |
4.34 |
0.34 |
0.50 |
11 |
A' |
195 |
186 |
7.91 |
0.13 |
0.27 |
0.43 |
12 |
A" |
3232 |
3071 |
1.04 |
12.28 |
0.75 |
0.86 |
13 |
A" |
3204 |
3045 |
0.59 |
86.19 |
0.75 |
0.86 |
14 |
A" |
1312 |
1247 |
0.09 |
9.74 |
0.75 |
0.86 |
15 |
A" |
1149 |
1092 |
2.56 |
0.33 |
0.75 |
0.86 |
16 |
A" |
988 |
939 |
0.10 |
8.12 |
0.75 |
0.86 |
17 |
A" |
773 |
735 |
4.49 |
0.03 |
0.75 |
0.86 |
18 |
A" |
115 |
109 |
5.90 |
0.03 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12830.2 cm
-1
Scaled (by 0.9503) Zero Point Vibrational Energy (zpe) 12192.5 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 PBE1PBE/6-31G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.652 |
0.000 |
C2 |
1.223 |
-0.233 |
0.000 |
Br3 |
-1.588 |
-0.478 |
0.000 |
Cl4 |
2.697 |
0.788 |
0.000 |
H5 |
-0.054 |
1.274 |
0.893 |
H6 |
-0.054 |
1.274 |
-0.893 |
H7 |
1.257 |
-0.864 |
0.890 |
H8 |
1.257 |
-0.864 |
-0.890 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5097 | 1.9490 | 2.7006 | 1.0898 | 1.0898 | 2.1608 | 2.1608 |
C2 | 1.5097 | | 2.8222 | 1.7932 | 2.1678 | 2.1678 | 1.0911 | 1.0911 | Br3 | 1.9490 | 2.8222 | | 4.4686 | 2.4941 | 2.4941 | 3.0063 | 3.0063 | Cl4 | 2.7006 | 1.7932 | 4.4686 | | 2.9328 | 2.9328 | 2.3652 | 2.3652 | H5 | 1.0898 | 2.1678 | 2.4941 | 2.9328 | | 1.7862 | 2.5077 | 3.0769 | H6 | 1.0898 | 2.1678 | 2.4941 | 2.9328 | 1.7862 | | 3.0769 | 2.5077 | H7 | 2.1608 | 1.0911 | 3.0063 | 2.3652 | 2.5077 | 3.0769 | | 1.7794 | H8 | 2.1608 | 1.0911 | 3.0063 | 2.3652 | 3.0769 | 2.5077 | 1.7794 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
109.400 |
|
C1 |
C2 |
H7 |
111.350 |
C1 |
C2 |
H8 |
111.350 |
|
C2 |
C1 |
Br3 |
108.703 |
C2 |
C1 |
Cl4 |
38.778 |
|
C2 |
C1 |
H6 |
112.001 |
Br3 |
C1 |
H5 |
106.894 |
|
Br3 |
C1 |
H6 |
106.894 |
Cl4 |
C2 |
H7 |
107.674 |
|
Cl4 |
C2 |
H8 |
107.674 |
H5 |
C1 |
H6 |
110.075 |
|
H7 |
C2 |
H8 |
109.255 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/6-31G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.355 |
|
|
|
2 |
C |
-0.440 |
|
|
|
3 |
Br |
-0.116 |
|
|
|
4 |
Cl |
-0.054 |
|
|
|
5 |
H |
0.239 |
|
|
|
6 |
H |
0.239 |
|
|
|
7 |
H |
0.243 |
|
|
|
8 |
H |
0.243 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.198 |
-0.055 |
0.000 |
0.206 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-49.995 |
-2.205 |
0.000 |
y |
-2.205 |
-42.826 |
0.000 |
z |
0.000 |
0.000 |
-43.105 |
|
Traceless |
| x | y | z |
x |
-7.029 |
-2.205 |
0.000 |
y |
-2.205 |
3.724 |
0.000 |
z |
0.000 |
0.000 |
3.305 |
|
Polar |
3z2-r2 | 6.610 |
x2-y2 | -7.169 |
xy | -2.205 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
9.897 |
1.879 |
0.000 |
y |
1.879 |
6.240 |
0.000 |
z |
0.000 |
0.000 |
5.119 |
<r2> (average value of r
2) Å
2
<r2> |
281.751 |
(<r2>)1/2 |
16.785 |
Jump to
S1C1
Energy calculated at PBE1PBE/6-31G*
| hartrees |
Energy at 0K | -3109.931457 |
Energy at 298.15K | |
HF Energy | -3109.931457 |
Nuclear repulsion energy | 306.144064 |
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 PBE1PBE/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 |
3210 |
3051 |
1.22 |
45.03 |
0.75 |
0.86 |
2 |
A |
3185 |
3027 |
1.45 |
84.01 |
0.75 |
0.86 |
3 |
A |
3135 |
2979 |
9.91 |
138.12 |
0.05 |
0.10 |
4 |
A |
3114 |
2959 |
9.47 |
108.80 |
0.20 |
0.34 |
5 |
A |
1497 |
1422 |
2.17 |
7.58 |
0.69 |
0.82 |
6 |
A |
1488 |
1414 |
11.78 |
16.26 |
0.75 |
0.86 |
7 |
A |
1362 |
1294 |
25.39 |
4.56 |
0.75 |
0.86 |
8 |
A |
1314 |
1249 |
45.60 |
1.51 |
0.54 |
0.70 |
9 |
A |
1235 |
1174 |
3.43 |
17.32 |
0.75 |
0.85 |
10 |
A |
1167 |
1109 |
1.70 |
6.10 |
0.73 |
0.85 |
11 |
A |
1063 |
1011 |
1.89 |
3.77 |
0.72 |
0.84 |
12 |
A |
952 |
905 |
9.53 |
6.30 |
0.43 |
0.60 |
13 |
A |
883 |
839 |
22.69 |
1.62 |
0.72 |
0.84 |
14 |
A |
700 |
666 |
18.84 |
9.00 |
0.40 |
0.57 |
15 |
A |
594 |
564 |
11.65 |
14.38 |
0.20 |
0.34 |
16 |
A |
393 |
374 |
7.91 |
2.35 |
0.71 |
0.83 |
17 |
A |
245 |
233 |
1.24 |
0.99 |
0.33 |
0.50 |
18 |
A |
103 |
98 |
0.56 |
1.20 |
0.73 |
0.85 |
Unscaled Zero Point Vibrational Energy (zpe) 12819.9 cm
-1
Scaled (by 0.9503) Zero Point Vibrational Energy (zpe) 12182.8 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 PBE1PBE/6-31G*
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.004 |
1.113 |
-0.379 |
C2 |
1.280 |
0.903 |
0.398 |
Br3 |
-1.341 |
-0.227 |
0.036 |
Cl4 |
2.145 |
-0.581 |
-0.087 |
H5 |
-0.433 |
2.078 |
-0.116 |
H6 |
0.171 |
1.066 |
-1.455 |
H7 |
1.957 |
1.743 |
0.213 |
H8 |
1.082 |
0.833 |
1.469 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5086 | 1.9432 | 2.7454 | 1.0922 | 1.0902 | 2.1358 | 2.1577 |
C2 | 1.5086 | | 2.8772 | 1.7846 | 2.1402 | 2.1656 | 1.0944 | 1.0916 | Br3 | 1.9432 | 2.8772 | | 3.5058 | 2.4821 | 2.4862 | 3.8456 | 3.0079 | Cl4 | 2.7454 | 1.7846 | 3.5058 | | 3.7039 | 2.9117 | 2.3506 | 2.3555 | H5 | 1.0922 | 2.1402 | 2.4821 | 3.7039 | | 1.7851 | 2.4360 | 2.5215 | H6 | 1.0902 | 2.1656 | 2.4862 | 2.9117 | 1.7851 | | 2.5358 | 3.0717 | H7 | 2.1358 | 1.0944 | 3.8456 | 2.3506 | 2.4360 | 2.5358 | | 1.7810 | H8 | 2.1577 | 1.0916 | 3.0079 | 2.3555 | 2.5215 | 3.0717 | 1.7810 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
112.682 |
|
C1 |
C2 |
H7 |
109.240 |
C1 |
C2 |
H8 |
111.146 |
|
C2 |
C1 |
Br3 |
112.315 |
C2 |
C1 |
Cl4 |
36.853 |
|
C2 |
C1 |
H6 |
111.869 |
Br3 |
C1 |
H5 |
106.304 |
|
Br3 |
C1 |
H6 |
106.686 |
Cl4 |
C2 |
H7 |
107.012 |
|
Cl4 |
C2 |
H8 |
107.503 |
H5 |
C1 |
H6 |
109.759 |
|
H7 |
C2 |
H8 |
109.119 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/6-31G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.360 |
|
|
|
2 |
C |
-0.436 |
|
|
|
3 |
Br |
-0.103 |
|
|
|
4 |
Cl |
-0.043 |
|
|
|
5 |
H |
0.229 |
|
|
|
6 |
H |
0.240 |
|
|
|
7 |
H |
0.231 |
|
|
|
8 |
H |
0.243 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.305 |
2.777 |
0.123 |
2.797 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-47.152 |
2.890 |
0.445 |
y |
2.890 |
-39.993 |
-0.125 |
z |
0.445 |
-0.125 |
-42.713 |
|
Traceless |
| x | y | z |
x |
-5.800 |
2.890 |
0.445 |
y |
2.890 |
4.940 |
-0.125 |
z |
0.445 |
-0.125 |
0.860 |
|
Polar |
3z2-r2 | 1.720 |
x2-y2 | -7.160 |
xy | 2.890 |
xz | 0.445 |
yz | -0.125 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
7.993 |
0.192 |
-0.286 |
y |
0.192 |
7.137 |
0.082 |
z |
-0.286 |
0.082 |
5.301 |
<r2> (average value of r
2) Å
2
<r2> |
218.593 |
(<r2>)1/2 |
14.785 |