Jump to
S1C2
Energy calculated at B3LYP/6-311G*
| hartrees |
Energy at 0K | -3113.016354 |
Energy at 298.15K | |
HF Energy | -3113.016354 |
Nuclear repulsion energy | 286.074528 |
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/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' |
3120 |
3015 |
12.51 |
14.73 |
0.07 |
0.13 |
2 |
A' |
3110 |
3005 |
1.92 |
145.70 |
0.07 |
0.14 |
3 |
A' |
1504 |
1453 |
1.59 |
11.69 |
0.73 |
0.84 |
4 |
A' |
1502 |
1451 |
6.04 |
3.23 |
0.73 |
0.85 |
5 |
A' |
1336 |
1291 |
3.54 |
18.16 |
0.60 |
0.75 |
6 |
A' |
1249 |
1207 |
49.99 |
3.82 |
0.51 |
0.67 |
7 |
A' |
1064 |
1028 |
0.95 |
10.98 |
0.72 |
0.84 |
8 |
A' |
714 |
690 |
29.05 |
68.62 |
0.30 |
0.46 |
9 |
A' |
621 |
600 |
71.72 |
13.04 |
0.25 |
0.40 |
10 |
A' |
243 |
235 |
0.92 |
5.58 |
0.38 |
0.55 |
11 |
A' |
193 |
186 |
7.99 |
0.23 |
0.32 |
0.49 |
12 |
A" |
3192 |
3084 |
4.37 |
3.84 |
0.75 |
0.86 |
13 |
A" |
3167 |
3060 |
0.58 |
97.86 |
0.75 |
0.86 |
14 |
A" |
1309 |
1265 |
0.20 |
5.21 |
0.75 |
0.86 |
15 |
A" |
1146 |
1107 |
4.59 |
0.10 |
0.75 |
0.86 |
16 |
A" |
985 |
952 |
0.16 |
6.55 |
0.75 |
0.86 |
17 |
A" |
776 |
749 |
5.30 |
0.03 |
0.75 |
0.86 |
18 |
A" |
112 |
109 |
5.94 |
0.02 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12670.4 cm
-1
Scaled (by 0.9663) Zero Point Vibrational Energy (zpe) 12243.4 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/6-311G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.647 |
0.000 |
C2 |
1.241 |
-0.214 |
0.000 |
Br3 |
-1.601 |
-0.517 |
0.000 |
Cl4 |
2.712 |
0.861 |
0.000 |
H5 |
-0.072 |
1.266 |
0.891 |
H6 |
-0.072 |
1.266 |
-0.891 |
H7 |
1.308 |
-0.836 |
0.890 |
H8 |
1.308 |
-0.836 |
-0.890 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5110 | 1.9794 | 2.7204 | 1.0866 | 1.0866 | 2.1680 | 2.1680 |
C2 | 1.5110 | | 2.8582 | 1.8219 | 2.1697 | 2.1697 | 1.0871 | 1.0871 | Br3 | 1.9794 | 2.8582 | | 4.5276 | 2.5119 | 2.5119 | 3.0580 | 3.0580 | Cl4 | 2.7204 | 1.8219 | 4.5276 | | 2.9503 | 2.9503 | 2.3755 | 2.3755 | H5 | 1.0866 | 2.1697 | 2.5119 | 2.9503 | | 1.7810 | 2.5136 | 3.0801 | H6 | 1.0866 | 2.1697 | 2.5119 | 2.9503 | 1.7810 | | 3.0801 | 2.5136 | H7 | 2.1680 | 1.0871 | 3.0580 | 2.3755 | 2.5136 | 3.0801 | | 1.7791 | H8 | 2.1680 | 1.0871 | 3.0580 | 2.3755 | 3.0801 | 2.5136 | 1.7791 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
109.058 |
|
C1 |
C2 |
H7 |
112.082 |
C1 |
C2 |
H8 |
112.082 |
|
C2 |
C1 |
Br3 |
109.209 |
C2 |
C1 |
Cl4 |
39.273 |
|
C2 |
C1 |
H6 |
112.250 |
Br3 |
C1 |
H5 |
106.354 |
|
Br3 |
C1 |
H6 |
106.354 |
Cl4 |
C2 |
H7 |
106.754 |
|
Cl4 |
C2 |
H8 |
106.754 |
H5 |
C1 |
H6 |
110.077 |
|
H7 |
C2 |
H8 |
109.826 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.491 |
|
|
|
2 |
C |
-0.471 |
|
|
|
3 |
Br |
-0.047 |
|
|
|
4 |
Cl |
-0.090 |
|
|
|
5 |
H |
0.275 |
|
|
|
6 |
H |
0.275 |
|
|
|
7 |
H |
0.275 |
|
|
|
8 |
H |
0.275 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.225 |
-0.079 |
0.000 |
0.239 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-51.380 |
-2.517 |
0.000 |
y |
-2.517 |
-44.038 |
0.000 |
z |
0.000 |
0.000 |
-44.096 |
|
Traceless |
| x | y | z |
x |
-7.313 |
-2.517 |
0.000 |
y |
-2.517 |
3.700 |
0.000 |
z |
0.000 |
0.000 |
3.613 |
|
Polar |
3z2-r2 | 7.226 |
x2-y2 | -7.342 |
xy | -2.517 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
10.879 |
2.384 |
0.000 |
y |
2.384 |
6.546 |
0.000 |
z |
0.000 |
0.000 |
4.889 |
<r2> (average value of r
2) Å
2
<r2> |
288.956 |
(<r2>)1/2 |
16.999 |
Jump to
S1C1
Energy calculated at B3LYP/6-311G*
| hartrees |
Energy at 0K | -3113.013005 |
Energy at 298.15K | |
HF Energy | -3113.013005 |
Nuclear repulsion energy | 301.320448 |
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/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 |
3165 |
3058 |
4.47 |
37.23 |
0.75 |
0.86 |
2 |
A |
3145 |
3039 |
2.05 |
95.04 |
0.75 |
0.86 |
3 |
A |
3096 |
2991 |
16.69 |
170.92 |
0.04 |
0.07 |
4 |
A |
3078 |
2974 |
10.48 |
108.91 |
0.25 |
0.41 |
5 |
A |
1484 |
1434 |
2.36 |
6.09 |
0.71 |
0.83 |
6 |
A |
1478 |
1428 |
10.98 |
13.16 |
0.74 |
0.85 |
7 |
A |
1353 |
1308 |
28.34 |
4.06 |
0.75 |
0.86 |
8 |
A |
1311 |
1267 |
54.18 |
2.25 |
0.56 |
0.71 |
9 |
A |
1225 |
1184 |
5.51 |
14.83 |
0.75 |
0.86 |
10 |
A |
1160 |
1121 |
3.15 |
5.74 |
0.74 |
0.85 |
11 |
A |
1043 |
1008 |
1.28 |
2.60 |
0.71 |
0.83 |
12 |
A |
936 |
904 |
11.17 |
7.80 |
0.42 |
0.60 |
13 |
A |
875 |
846 |
25.88 |
1.94 |
0.74 |
0.85 |
14 |
A |
657 |
635 |
27.48 |
10.91 |
0.44 |
0.61 |
15 |
A |
559 |
540 |
13.57 |
16.41 |
0.20 |
0.34 |
16 |
A |
383 |
370 |
8.29 |
2.97 |
0.71 |
0.83 |
17 |
A |
242 |
234 |
1.35 |
1.68 |
0.50 |
0.67 |
18 |
A |
97 |
94 |
0.57 |
2.05 |
0.73 |
0.85 |
Unscaled Zero Point Vibrational Energy (zpe) 12643.4 cm
-1
Scaled (by 0.9663) Zero Point Vibrational Energy (zpe) 12217.3 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/6-311G*
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.018 |
1.101 |
-0.386 |
C2 |
1.290 |
0.903 |
0.405 |
Br3 |
-1.378 |
-0.226 |
0.036 |
Cl4 |
2.210 |
-0.576 |
-0.086 |
H5 |
-0.416 |
2.071 |
-0.145 |
H6 |
0.190 |
1.034 |
-1.458 |
H7 |
1.957 |
1.748 |
0.228 |
H8 |
1.096 |
0.817 |
1.472 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5105 | 1.9718 | 2.7756 | 1.0897 | 1.0873 | 2.1341 | 2.1669 |
C2 | 1.5105 | | 2.9204 | 1.8099 | 2.1392 | 2.1675 | 1.0913 | 1.0879 | Br3 | 1.9718 | 2.9204 | | 3.6069 | 2.4964 | 2.5050 | 3.8803 | 3.0450 | Cl4 | 2.7756 | 1.8099 | 3.6069 | | 3.7288 | 2.9250 | 2.3594 | 2.3681 | H5 | 1.0897 | 2.1392 | 2.4964 | 3.7288 | | 1.7788 | 2.4236 | 2.5447 | H6 | 1.0873 | 2.1675 | 2.5050 | 2.9250 | 1.7788 | | 2.5447 | 3.0747 | H7 | 2.1341 | 1.0913 | 3.8803 | 2.3594 | 2.4236 | 2.5447 | | 1.7767 | H8 | 2.1669 | 1.0879 | 3.0450 | 2.3681 | 2.5447 | 3.0747 | 1.7767 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
113.116 |
|
C1 |
C2 |
H7 |
109.150 |
C1 |
C2 |
H8 |
111.987 |
|
C2 |
C1 |
Br3 |
113.327 |
C2 |
C1 |
Cl4 |
36.850 |
|
C2 |
C1 |
H6 |
112.073 |
Br3 |
C1 |
H5 |
105.611 |
|
Br3 |
C1 |
H6 |
106.324 |
Cl4 |
C2 |
H7 |
106.171 |
|
Cl4 |
C2 |
H8 |
106.959 |
H5 |
C1 |
H6 |
109.591 |
|
H7 |
C2 |
H8 |
109.237 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.494 |
|
|
|
2 |
C |
-0.467 |
|
|
|
3 |
Br |
-0.035 |
|
|
|
4 |
Cl |
-0.076 |
|
|
|
5 |
H |
0.261 |
|
|
|
6 |
H |
0.276 |
|
|
|
7 |
H |
0.262 |
|
|
|
8 |
H |
0.274 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.253 |
2.840 |
0.118 |
2.854 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-48.654 |
2.978 |
0.419 |
y |
2.978 |
-41.028 |
-0.099 |
z |
0.419 |
-0.099 |
-43.718 |
|
Traceless |
| x | y | z |
x |
-6.281 |
2.978 |
0.419 |
y |
2.978 |
5.158 |
-0.099 |
z |
0.419 |
-0.099 |
1.123 |
|
Polar |
3z2-r2 | 2.246 |
x2-y2 | -7.626 |
xy | 2.978 |
xz | 0.419 |
yz | -0.099 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
8.537 |
0.254 |
-0.319 |
y |
0.254 |
7.418 |
0.079 |
z |
-0.319 |
0.079 |
5.245 |
<r2> (average value of r
2) Å
2
<r2> |
227.558 |
(<r2>)1/2 |
15.085 |