Jump to
S1C2
Energy calculated at B3LYP/aug-cc-pVTZ
| hartrees |
Energy at 0K | -3113.123722 |
Energy at 298.15K | |
HF Energy | -3113.123722 |
Nuclear repulsion energy | 286.803847 |
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 B3LYP/aug-cc-pVTZ
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' |
3113 |
3012 |
5.99 |
28.65 |
0.03 |
0.06 |
2 |
A' |
3100 |
2999 |
1.85 |
140.63 |
0.03 |
0.06 |
3 |
A' |
1494 |
1445 |
3.26 |
3.52 |
0.73 |
0.85 |
4 |
A' |
1489 |
1440 |
3.93 |
2.91 |
0.74 |
0.85 |
5 |
A' |
1308 |
1266 |
1.67 |
25.81 |
0.31 |
0.48 |
6 |
A' |
1225 |
1185 |
40.08 |
4.62 |
0.24 |
0.39 |
7 |
A' |
1060 |
1026 |
0.91 |
5.68 |
0.74 |
0.85 |
8 |
A' |
714 |
691 |
25.89 |
67.10 |
0.25 |
0.40 |
9 |
A' |
622 |
601 |
68.03 |
14.88 |
0.22 |
0.36 |
10 |
A' |
243 |
235 |
0.87 |
6.07 |
0.21 |
0.35 |
11 |
A' |
192 |
186 |
7.10 |
0.36 |
0.18 |
0.31 |
12 |
A" |
3182 |
3079 |
0.29 |
6.24 |
0.75 |
0.86 |
13 |
A" |
3155 |
3052 |
0.25 |
69.63 |
0.75 |
0.86 |
14 |
A" |
1291 |
1250 |
0.01 |
2.21 |
0.75 |
0.86 |
15 |
A" |
1121 |
1084 |
1.41 |
0.03 |
0.75 |
0.86 |
16 |
A" |
971 |
940 |
0.13 |
0.94 |
0.75 |
0.86 |
17 |
A" |
769 |
744 |
2.88 |
0.00 |
0.75 |
0.86 |
18 |
A" |
108 |
104 |
5.56 |
0.01 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12577.3 cm
-1
Scaled (by 0.9675) Zero Point Vibrational Energy (zpe) 12168.6 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 B3LYP/aug-cc-pVTZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.646 |
0.000 |
C2 |
1.239 |
-0.213 |
0.000 |
Br3 |
-1.596 |
-0.518 |
0.000 |
Cl4 |
2.703 |
0.863 |
0.000 |
H5 |
-0.075 |
1.260 |
0.890 |
H6 |
-0.075 |
1.260 |
-0.890 |
H7 |
1.306 |
-0.832 |
0.888 |
H8 |
1.306 |
-0.832 |
-0.888 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5075 | 1.9751 | 2.7119 | 1.0839 | 1.0839 | 2.1631 | 2.1631 |
C2 | 1.5075 | | 2.8514 | 1.8167 | 2.1652 | 2.1652 | 1.0848 | 1.0848 | Br3 | 1.9751 | 2.8514 | | 4.5154 | 2.5035 | 2.5035 | 3.0512 | 3.0512 | Cl4 | 2.7119 | 1.8167 | 4.5154 | | 2.9439 | 2.9439 | 2.3693 | 2.3693 | H5 | 1.0839 | 2.1652 | 2.5035 | 2.9439 | | 1.7794 | 2.5071 | 3.0735 | H6 | 1.0839 | 2.1652 | 2.5035 | 2.9439 | 1.7794 | | 3.0735 | 2.5071 | H7 | 2.1631 | 1.0848 | 3.0512 | 2.3693 | 2.5071 | 3.0735 | | 1.7761 | H8 | 2.1631 | 1.0848 | 3.0512 | 2.3693 | 3.0735 | 2.5071 | 1.7761 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
108.978 |
|
C1 |
C2 |
H7 |
112.083 |
C1 |
C2 |
H8 |
112.083 |
|
C2 |
C1 |
Br3 |
109.187 |
C2 |
C1 |
Cl4 |
39.308 |
|
C2 |
C1 |
H6 |
112.311 |
Br3 |
C1 |
H5 |
106.159 |
|
Br3 |
C1 |
H6 |
106.159 |
Cl4 |
C2 |
H7 |
106.755 |
|
Cl4 |
C2 |
H8 |
106.755 |
H5 |
C1 |
H6 |
110.334 |
|
H7 |
C2 |
H8 |
109.900 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/aug-cc-pVTZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.362 |
|
|
|
2 |
C |
-0.148 |
|
|
|
3 |
Br |
-0.083 |
|
|
|
4 |
Cl |
-0.271 |
|
|
|
5 |
H |
0.215 |
|
|
|
6 |
H |
0.215 |
|
|
|
7 |
H |
0.217 |
|
|
|
8 |
H |
0.217 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.076 |
-0.031 |
0.000 |
0.082 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-50.716 |
-2.478 |
0.000 |
y |
-2.478 |
-43.955 |
0.000 |
z |
0.000 |
0.000 |
-43.942 |
|
Traceless |
| x | y | z |
x |
-6.767 |
-2.478 |
0.000 |
y |
-2.478 |
3.374 |
0.000 |
z |
0.000 |
0.000 |
3.393 |
|
Polar |
3z2-r2 | 6.786 |
x2-y2 | -6.761 |
xy | -2.478 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
12.832 |
1.848 |
0.000 |
y |
1.848 |
8.853 |
0.000 |
z |
0.000 |
0.000 |
7.688 |
<r2> (average value of r
2) Å
2
<r2> |
287.399 |
(<r2>)1/2 |
16.953 |
Jump to
S1C1
Energy calculated at B3LYP/aug-cc-pVTZ
| hartrees |
Energy at 0K | -3113.120571 |
Energy at 298.15K | |
HF Energy | -3113.120571 |
Nuclear repulsion energy | 302.059253 |
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 B3LYP/aug-cc-pVTZ
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 |
3156 |
3054 |
0.83 |
34.75 |
0.75 |
0.85 |
2 |
A |
3134 |
3032 |
0.79 |
71.91 |
0.74 |
0.85 |
3 |
A |
3089 |
2989 |
11.16 |
182.53 |
0.03 |
0.06 |
4 |
A |
3070 |
2970 |
8.10 |
113.41 |
0.17 |
0.29 |
5 |
A |
1472 |
1424 |
4.91 |
5.11 |
0.75 |
0.86 |
6 |
A |
1465 |
1417 |
7.93 |
6.14 |
0.74 |
0.85 |
7 |
A |
1328 |
1285 |
19.18 |
2.07 |
0.27 |
0.43 |
8 |
A |
1290 |
1248 |
51.87 |
5.23 |
0.32 |
0.48 |
9 |
A |
1205 |
1166 |
1.78 |
5.23 |
0.73 |
0.84 |
10 |
A |
1142 |
1105 |
0.70 |
1.23 |
0.66 |
0.80 |
11 |
A |
1036 |
1003 |
2.20 |
0.91 |
0.73 |
0.84 |
12 |
A |
927 |
897 |
8.62 |
4.33 |
0.19 |
0.32 |
13 |
A |
869 |
840 |
19.55 |
1.14 |
0.73 |
0.84 |
14 |
A |
656 |
635 |
23.53 |
10.17 |
0.28 |
0.44 |
15 |
A |
560 |
542 |
12.19 |
19.70 |
0.12 |
0.22 |
16 |
A |
381 |
369 |
8.09 |
1.87 |
0.68 |
0.81 |
17 |
A |
239 |
232 |
1.40 |
1.54 |
0.19 |
0.32 |
18 |
A |
93 |
90 |
0.57 |
1.00 |
0.63 |
0.77 |
Unscaled Zero Point Vibrational Energy (zpe) 12555.7 cm
-1
Scaled (by 0.9675) Zero Point Vibrational Energy (zpe) 12147.6 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 B3LYP/aug-cc-pVTZ
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.020 |
1.097 |
-0.387 |
C2 |
1.286 |
0.900 |
0.406 |
Br3 |
-1.375 |
-0.225 |
0.036 |
Cl4 |
2.205 |
-0.574 |
-0.086 |
H5 |
-0.417 |
2.064 |
-0.148 |
H6 |
0.191 |
1.023 |
-1.455 |
H7 |
1.952 |
1.744 |
0.231 |
H8 |
1.090 |
0.809 |
1.470 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5069 | 1.9676 | 2.7674 | 1.0870 | 1.0846 | 2.1295 | 2.1623 |
C2 | 1.5069 | | 2.9127 | 1.8053 | 2.1355 | 2.1631 | 1.0888 | 1.0855 | Br3 | 1.9676 | 2.9127 | | 3.5991 | 2.4876 | 2.4963 | 3.8708 | 3.0336 | Cl4 | 2.7674 | 1.8053 | 3.5991 | | 3.7195 | 2.9124 | 2.3527 | 2.3614 | H5 | 1.0870 | 2.1355 | 2.4876 | 3.7195 | | 1.7780 | 2.4205 | 2.5419 | H6 | 1.0846 | 2.1631 | 2.4963 | 2.9124 | 1.7780 | | 2.5431 | 3.0676 | H7 | 2.1295 | 1.0888 | 3.8708 | 2.3527 | 2.4205 | 2.5431 | | 1.7746 | H8 | 2.1623 | 1.0855 | 3.0336 | 2.3614 | 2.5419 | 3.0676 | 1.7746 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
113.030 |
|
C1 |
C2 |
H7 |
109.183 |
C1 |
C2 |
H8 |
112.013 |
|
C2 |
C1 |
Br3 |
113.258 |
C2 |
C1 |
Cl4 |
36.896 |
|
C2 |
C1 |
H6 |
112.133 |
Br3 |
C1 |
H5 |
105.390 |
|
Br3 |
C1 |
H6 |
106.098 |
Cl4 |
C2 |
H7 |
106.107 |
|
Cl4 |
C2 |
H8 |
106.887 |
H5 |
C1 |
H6 |
109.922 |
|
H7 |
C2 |
H8 |
109.404 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/aug-cc-pVTZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.371 |
|
|
|
2 |
C |
-0.156 |
|
|
|
3 |
Br |
-0.059 |
|
|
|
4 |
Cl |
-0.236 |
|
|
|
5 |
H |
0.189 |
|
|
|
6 |
H |
0.218 |
|
|
|
7 |
H |
0.187 |
|
|
|
8 |
H |
0.228 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.359 |
2.670 |
0.105 |
2.696 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-48.424 |
2.733 |
0.493 |
y |
2.733 |
-40.964 |
-0.094 |
z |
0.493 |
-0.094 |
-43.599 |
|
Traceless |
| x | y | z |
x |
-6.142 |
2.733 |
0.493 |
y |
2.733 |
5.047 |
-0.094 |
z |
0.493 |
-0.094 |
1.096 |
|
Polar |
3z2-r2 | 2.191 |
x2-y2 | -7.459 |
xy | 2.733 |
xz | 0.493 |
yz | -0.094 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
11.008 |
0.161 |
-0.158 |
y |
0.161 |
9.318 |
0.035 |
z |
-0.158 |
0.035 |
7.883 |
<r2> (average value of r
2) Å
2
<r2> |
226.517 |
(<r2>)1/2 |
15.050 |