Jump to
S1C2
Energy calculated at B3PW91/6-311G**
| hartrees |
Energy at 0K | -3112.920735 |
Energy at 298.15K | |
HF Energy | -3112.920735 |
Nuclear repulsion energy | 288.130314 |
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 B3PW91/6-311G**
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' |
3117 |
3002 |
9.20 |
20.63 |
0.06 |
0.11 |
2 |
A' |
3107 |
2992 |
2.17 |
148.62 |
0.06 |
0.12 |
3 |
A' |
1484 |
1429 |
0.33 |
13.09 |
0.74 |
0.85 |
4 |
A' |
1479 |
1425 |
7.33 |
0.53 |
0.74 |
0.85 |
5 |
A' |
1324 |
1275 |
2.89 |
14.90 |
0.63 |
0.77 |
6 |
A' |
1236 |
1190 |
44.23 |
2.96 |
0.51 |
0.68 |
7 |
A' |
1075 |
1036 |
1.04 |
9.60 |
0.73 |
0.84 |
8 |
A' |
741 |
714 |
31.13 |
56.28 |
0.29 |
0.46 |
9 |
A' |
646 |
622 |
61.84 |
14.04 |
0.25 |
0.40 |
10 |
A' |
248 |
239 |
0.88 |
4.36 |
0.39 |
0.56 |
11 |
A' |
192 |
185 |
8.03 |
0.16 |
0.32 |
0.48 |
12 |
A" |
3192 |
3074 |
1.82 |
5.18 |
0.75 |
0.86 |
13 |
A" |
3167 |
3050 |
0.53 |
93.59 |
0.75 |
0.86 |
14 |
A" |
1294 |
1246 |
0.21 |
4.93 |
0.75 |
0.86 |
15 |
A" |
1135 |
1093 |
3.92 |
0.07 |
0.75 |
0.86 |
16 |
A" |
979 |
943 |
0.12 |
5.74 |
0.75 |
0.86 |
17 |
A" |
769 |
741 |
5.55 |
0.02 |
0.75 |
0.86 |
18 |
A" |
113 |
109 |
5.62 |
0.02 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12648.3 cm
-1
Scaled (by 0.9631) Zero Point Vibrational Energy (zpe) 12181.6 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 B3PW91/6-311G**
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.643 |
0.000 |
C2 |
1.235 |
-0.224 |
0.000 |
Br3 |
-1.592 |
-0.498 |
0.000 |
Cl4 |
2.698 |
0.829 |
0.000 |
H5 |
-0.063 |
1.263 |
0.892 |
H6 |
-0.063 |
1.263 |
-0.892 |
H7 |
1.290 |
-0.848 |
0.890 |
H8 |
1.290 |
-0.848 |
-0.890 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5087 | 1.9591 | 2.7049 | 1.0880 | 1.0880 | 2.1631 | 2.1631 |
C2 | 1.5087 | | 2.8406 | 1.8031 | 2.1658 | 2.1658 | 1.0886 | 1.0886 | Br3 | 1.9591 | 2.8406 | | 4.4916 | 2.4974 | 2.4974 | 3.0371 | 3.0371 | Cl4 | 2.7049 | 1.8031 | 4.4916 | | 2.9341 | 2.9341 | 2.3640 | 2.3640 | H5 | 1.0880 | 2.1658 | 2.4974 | 2.9341 | | 1.7834 | 2.5072 | 3.0760 | H6 | 1.0880 | 2.1658 | 2.4974 | 2.9341 | 1.7834 | | 3.0760 | 2.5072 | H7 | 2.1631 | 1.0886 | 3.0371 | 2.3640 | 2.5072 | 3.0760 | | 1.7809 | H8 | 2.1631 | 1.0886 | 3.0371 | 2.3640 | 3.0760 | 2.5072 | 1.7809 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
109.194 |
|
C1 |
C2 |
H7 |
111.760 |
C1 |
C2 |
H8 |
111.760 |
|
C2 |
C1 |
Br3 |
109.308 |
C2 |
C1 |
Cl4 |
39.018 |
|
C2 |
C1 |
H6 |
112.016 |
Br3 |
C1 |
H5 |
106.560 |
|
Br3 |
C1 |
H6 |
106.560 |
Cl4 |
C2 |
H7 |
107.069 |
|
Cl4 |
C2 |
H8 |
107.069 |
H5 |
C1 |
H6 |
110.084 |
|
H7 |
C2 |
H8 |
109.767 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.334 |
|
|
|
2 |
C |
-0.322 |
|
|
|
3 |
Br |
-0.058 |
|
|
|
4 |
Cl |
-0.093 |
|
|
|
5 |
H |
0.201 |
|
|
|
6 |
H |
0.201 |
|
|
|
7 |
H |
0.203 |
|
|
|
8 |
H |
0.203 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.189 |
-0.061 |
0.000 |
0.199 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-50.673 |
-2.340 |
0.000 |
y |
-2.340 |
-43.555 |
0.000 |
z |
0.000 |
0.000 |
-43.727 |
|
Traceless |
| x | y | z |
x |
-7.032 |
-2.340 |
0.000 |
y |
-2.340 |
3.645 |
0.000 |
z |
0.000 |
0.000 |
3.388 |
|
Polar |
3z2-r2 | 6.775 |
x2-y2 | -7.118 |
xy | -2.340 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
10.713 |
2.242 |
0.000 |
y |
2.242 |
6.492 |
0.000 |
z |
0.000 |
0.000 |
4.901 |
<r2> (average value of r
2) Å
2
<r2> |
284.717 |
(<r2>)1/2 |
16.874 |
Jump to
S1C1
Energy calculated at B3PW91/6-311G**
| hartrees |
Energy at 0K | -3112.917864 |
Energy at 298.15K | |
HF Energy | -3112.917864 |
Nuclear repulsion energy | 303.619608 |
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 B3PW91/6-311G**
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 |
3168 |
3051 |
1.99 |
40.43 |
0.75 |
0.86 |
2 |
A |
3148 |
3032 |
1.50 |
90.78 |
0.75 |
0.86 |
3 |
A |
3097 |
2983 |
12.27 |
170.63 |
0.04 |
0.07 |
4 |
A |
3080 |
2966 |
9.73 |
112.13 |
0.21 |
0.34 |
5 |
A |
1462 |
1408 |
2.23 |
5.25 |
0.71 |
0.83 |
6 |
A |
1455 |
1402 |
11.79 |
12.60 |
0.74 |
0.85 |
7 |
A |
1340 |
1291 |
24.56 |
3.74 |
0.75 |
0.86 |
8 |
A |
1297 |
1249 |
48.57 |
1.95 |
0.56 |
0.72 |
9 |
A |
1216 |
1171 |
4.36 |
13.44 |
0.75 |
0.85 |
10 |
A |
1151 |
1108 |
2.59 |
5.17 |
0.74 |
0.85 |
11 |
A |
1049 |
1010 |
1.67 |
2.48 |
0.67 |
0.80 |
12 |
A |
936 |
902 |
10.83 |
6.99 |
0.42 |
0.59 |
13 |
A |
872 |
840 |
26.14 |
1.99 |
0.75 |
0.86 |
14 |
A |
679 |
654 |
23.55 |
9.39 |
0.43 |
0.60 |
15 |
A |
578 |
557 |
12.18 |
14.82 |
0.20 |
0.34 |
16 |
A |
386 |
371 |
7.65 |
2.54 |
0.71 |
0.83 |
17 |
A |
243 |
234 |
1.28 |
1.54 |
0.52 |
0.69 |
18 |
A |
99 |
95 |
0.53 |
1.90 |
0.74 |
0.85 |
Unscaled Zero Point Vibrational Energy (zpe) 12627.6 cm
-1
Scaled (by 0.9631) Zero Point Vibrational Energy (zpe) 12161.6 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 B3PW91/6-311G**
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.012 |
1.096 |
-0.382 |
C2 |
1.285 |
0.897 |
0.401 |
Br3 |
-1.365 |
-0.225 |
0.036 |
Cl4 |
2.187 |
-0.574 |
-0.086 |
H5 |
-0.420 |
2.066 |
-0.134 |
H6 |
0.183 |
1.034 |
-1.455 |
H7 |
1.951 |
1.743 |
0.218 |
H8 |
1.091 |
0.816 |
1.470 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5075 | 1.9534 | 2.7580 | 1.0907 | 1.0886 | 2.1300 | 2.1620 |
C2 | 1.5075 | | 2.9004 | 1.7932 | 2.1358 | 2.1634 | 1.0923 | 1.0892 | Br3 | 1.9534 | 2.9004 | | 3.5708 | 2.4838 | 2.4907 | 3.8600 | 3.0287 | Cl4 | 2.7580 | 1.7932 | 3.5708 | | 3.7111 | 2.9118 | 2.3492 | 2.3563 | H5 | 1.0907 | 2.1358 | 2.4838 | 3.7111 | | 1.7818 | 2.4190 | 2.5345 | H6 | 1.0886 | 2.1634 | 2.4907 | 2.9118 | 1.7818 | | 2.5356 | 3.0711 | H7 | 2.1300 | 1.0923 | 3.8600 | 2.3492 | 2.4190 | 2.5356 | | 1.7794 | H8 | 2.1620 | 1.0892 | 3.0287 | 2.3563 | 2.5345 | 3.0711 | 1.7794 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
113.072 |
|
C1 |
C2 |
H7 |
108.979 |
C1 |
C2 |
H8 |
111.717 |
|
C2 |
C1 |
Br3 |
113.237 |
C2 |
C1 |
Cl4 |
36.738 |
|
C2 |
C1 |
H6 |
111.870 |
Br3 |
C1 |
H5 |
105.850 |
|
Br3 |
C1 |
H6 |
106.430 |
Cl4 |
C2 |
H7 |
106.460 |
|
Cl4 |
C2 |
H8 |
107.126 |
H5 |
C1 |
H6 |
109.694 |
|
H7 |
C2 |
H8 |
109.304 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.334 |
|
|
|
2 |
C |
-0.314 |
|
|
|
3 |
Br |
-0.047 |
|
|
|
4 |
Cl |
-0.080 |
|
|
|
5 |
H |
0.186 |
|
|
|
6 |
H |
0.201 |
|
|
|
7 |
H |
0.188 |
|
|
|
8 |
H |
0.201 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.276 |
2.786 |
0.113 |
2.802 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-48.054 |
2.881 |
0.429 |
y |
2.881 |
-40.660 |
-0.105 |
z |
0.429 |
-0.105 |
-43.333 |
|
Traceless |
| x | y | z |
x |
-6.058 |
2.881 |
0.429 |
y |
2.881 |
5.034 |
-0.105 |
z |
0.429 |
-0.105 |
1.024 |
|
Polar |
3z2-r2 | 2.048 |
x2-y2 | -7.394 |
xy | 2.881 |
xz | 0.429 |
yz | -0.105 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
8.459 |
0.251 |
-0.291 |
y |
0.251 |
7.387 |
0.075 |
z |
-0.291 |
0.075 |
5.257 |
<r2> (average value of r
2) Å
2
<r2> |
223.905 |
(<r2>)1/2 |
14.963 |