Jump to
S1C2
Energy calculated at PBE1PBE/6-311G*
| hartrees |
Energy at 0K | -3112.421347 |
Energy at 298.15K | |
HF Energy | -3112.421347 |
Nuclear repulsion energy | 289.227035 |
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/6-311G*
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' |
3135 |
3005 |
12.04 |
17.57 |
0.07 |
0.12 |
2 |
A' |
3125 |
2996 |
2.30 |
144.79 |
0.07 |
0.13 |
3 |
A' |
1500 |
1437 |
0.94 |
13.10 |
0.73 |
0.85 |
4 |
A' |
1497 |
1435 |
7.94 |
1.64 |
0.73 |
0.84 |
5 |
A' |
1346 |
1290 |
2.86 |
14.30 |
0.65 |
0.79 |
6 |
A' |
1254 |
1202 |
44.95 |
2.83 |
0.53 |
0.70 |
7 |
A' |
1091 |
1046 |
1.15 |
8.76 |
0.73 |
0.85 |
8 |
A' |
759 |
727 |
31.81 |
51.62 |
0.29 |
0.45 |
9 |
A' |
662 |
634 |
59.09 |
14.22 |
0.25 |
0.40 |
10 |
A' |
252 |
241 |
0.84 |
4.02 |
0.39 |
0.56 |
11 |
A' |
194 |
186 |
7.96 |
0.13 |
0.31 |
0.47 |
12 |
A" |
3211 |
3077 |
3.16 |
4.04 |
0.75 |
0.86 |
13 |
A" |
3185 |
3053 |
0.57 |
96.72 |
0.75 |
0.86 |
14 |
A" |
1314 |
1259 |
0.23 |
5.72 |
0.75 |
0.86 |
15 |
A" |
1157 |
1109 |
4.83 |
0.06 |
0.75 |
0.86 |
16 |
A" |
993 |
952 |
0.18 |
6.13 |
0.75 |
0.86 |
17 |
A" |
774 |
742 |
5.77 |
0.03 |
0.75 |
0.86 |
18 |
A" |
117 |
112 |
5.73 |
0.02 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12782.1 cm
-1
Scaled (by 0.9585) Zero Point Vibrational Energy (zpe) 12251.6 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 PBE1PBE/6-311G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.641 |
0.000 |
C2 |
1.230 |
-0.228 |
0.000 |
Br3 |
-1.587 |
-0.491 |
0.000 |
Cl4 |
2.689 |
0.817 |
0.000 |
H5 |
-0.057 |
1.265 |
0.890 |
H6 |
-0.057 |
1.265 |
-0.890 |
H7 |
1.281 |
-0.854 |
0.889 |
H8 |
1.281 |
-0.854 |
-0.889 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5061 | 1.9496 | 2.6950 | 1.0881 | 1.0881 | 2.1602 | 2.1602 |
C2 | 1.5061 | | 2.8295 | 1.7948 | 2.1622 | 2.1622 | 1.0886 | 1.0886 | Br3 | 1.9496 | 2.8295 | | 4.4720 | 2.4936 | 2.4936 | 3.0242 | 3.0242 | Cl4 | 2.6950 | 1.7948 | 4.4720 | | 2.9208 | 2.9208 | 2.3597 | 2.3597 | H5 | 1.0881 | 2.1622 | 2.4936 | 2.9208 | | 1.7799 | 2.5056 | 3.0728 | H6 | 1.0881 | 2.1622 | 2.4936 | 2.9208 | 1.7799 | | 3.0728 | 2.5056 | H7 | 2.1602 | 1.0886 | 3.0242 | 2.3597 | 2.5056 | 3.0728 | | 1.7780 | H8 | 2.1602 | 1.0886 | 3.0242 | 2.3597 | 3.0728 | 2.5056 | 1.7780 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
109.145 |
|
C1 |
C2 |
H7 |
111.707 |
C1 |
C2 |
H8 |
111.707 |
|
C2 |
C1 |
Br3 |
109.252 |
C2 |
C1 |
Cl4 |
38.987 |
|
C2 |
C1 |
H6 |
111.905 |
Br3 |
C1 |
H5 |
106.894 |
|
Br3 |
C1 |
H6 |
106.894 |
Cl4 |
C2 |
H7 |
107.297 |
|
Cl4 |
C2 |
H8 |
107.297 |
H5 |
C1 |
H6 |
109.739 |
|
H7 |
C2 |
H8 |
109.493 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.544 |
|
|
|
2 |
C |
-0.520 |
|
|
|
3 |
Br |
-0.033 |
|
|
|
4 |
Cl |
-0.074 |
|
|
|
5 |
H |
0.293 |
|
|
|
6 |
H |
0.293 |
|
|
|
7 |
H |
0.292 |
|
|
|
8 |
H |
0.292 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.196 |
-0.060 |
0.000 |
0.205 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-50.835 |
-2.282 |
0.000 |
y |
-2.282 |
-43.644 |
0.000 |
z |
0.000 |
0.000 |
-43.809 |
|
Traceless |
| x | y | z |
x |
-7.109 |
-2.282 |
0.000 |
y |
-2.282 |
3.679 |
0.000 |
z |
0.000 |
0.000 |
3.430 |
|
Polar |
3z2-r2 | 6.860 |
x2-y2 | -7.191 |
xy | -2.282 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
10.487 |
2.179 |
0.000 |
y |
2.179 |
6.397 |
0.000 |
z |
0.000 |
0.000 |
4.856 |
<r2> (average value of r
2) Å
2
<r2> |
282.657 |
(<r2>)1/2 |
16.812 |
Jump to
S1C1
Energy calculated at PBE1PBE/6-311G*
| hartrees |
Energy at 0K | -3112.418438 |
Energy at 298.15K | |
HF Energy | -3112.418438 |
Nuclear repulsion energy | 304.947623 |
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/6-311G*
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 |
3187 |
3054 |
3.31 |
39.02 |
0.75 |
0.86 |
2 |
A |
3167 |
3036 |
1.99 |
93.62 |
0.75 |
0.86 |
3 |
A |
3116 |
2986 |
15.58 |
166.67 |
0.04 |
0.07 |
4 |
A |
3099 |
2970 |
10.77 |
102.63 |
0.23 |
0.38 |
5 |
A |
1481 |
1419 |
2.89 |
5.82 |
0.71 |
0.83 |
6 |
A |
1473 |
1412 |
13.21 |
12.90 |
0.74 |
0.85 |
7 |
A |
1361 |
1304 |
25.49 |
4.18 |
0.75 |
0.86 |
8 |
A |
1317 |
1262 |
47.03 |
1.65 |
0.56 |
0.72 |
9 |
A |
1238 |
1186 |
4.97 |
14.24 |
0.75 |
0.85 |
10 |
A |
1169 |
1121 |
3.31 |
5.55 |
0.74 |
0.85 |
11 |
A |
1064 |
1020 |
1.38 |
2.64 |
0.68 |
0.81 |
12 |
A |
949 |
910 |
11.10 |
6.95 |
0.42 |
0.59 |
13 |
A |
884 |
847 |
27.34 |
2.07 |
0.75 |
0.86 |
14 |
A |
693 |
664 |
22.17 |
8.93 |
0.43 |
0.60 |
15 |
A |
591 |
566 |
11.86 |
14.51 |
0.20 |
0.34 |
16 |
A |
390 |
374 |
7.29 |
2.39 |
0.71 |
0.83 |
17 |
A |
246 |
236 |
1.21 |
1.43 |
0.54 |
0.70 |
18 |
A |
101 |
97 |
0.53 |
1.81 |
0.74 |
0.85 |
Unscaled Zero Point Vibrational Energy (zpe) 12762.1 cm
-1
Scaled (by 0.9585) Zero Point Vibrational Energy (zpe) 12232.5 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/6-311G*
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.010 |
1.096 |
-0.381 |
C2 |
1.281 |
0.895 |
0.400 |
Br3 |
-1.356 |
-0.224 |
0.036 |
Cl4 |
2.172 |
-0.574 |
-0.086 |
H5 |
-0.421 |
2.067 |
-0.135 |
H6 |
0.183 |
1.039 |
-1.454 |
H7 |
1.948 |
1.741 |
0.218 |
H8 |
1.088 |
0.818 |
1.469 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5051 | 1.9446 | 2.7472 | 1.0907 | 1.0887 | 2.1288 | 2.1589 |
C2 | 1.5051 | | 2.8880 | 1.7858 | 2.1342 | 2.1595 | 1.0922 | 1.0892 | Br3 | 1.9446 | 2.8880 | | 3.5471 | 2.4803 | 2.4868 | 3.8488 | 3.0190 | Cl4 | 2.7472 | 1.7858 | 3.5471 | | 3.7011 | 2.9029 | 2.3455 | 2.3523 | H5 | 1.0907 | 2.1342 | 2.4803 | 3.7011 | | 1.7785 | 2.4174 | 2.5311 | H6 | 1.0887 | 2.1595 | 2.4868 | 2.9029 | 1.7785 | | 2.5306 | 3.0680 | H7 | 2.1288 | 1.0922 | 3.8488 | 2.3455 | 2.4174 | 2.5306 | | 1.7767 | H8 | 2.1589 | 1.0892 | 3.0190 | 2.3523 | 2.5311 | 3.0680 | 1.7767 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
112.913 |
|
C1 |
C2 |
H7 |
109.056 |
C1 |
C2 |
H8 |
111.641 |
|
C2 |
C1 |
Br3 |
113.072 |
C2 |
C1 |
Cl4 |
36.780 |
|
C2 |
C1 |
H6 |
111.728 |
Br3 |
C1 |
H5 |
106.163 |
|
Br3 |
C1 |
H6 |
106.712 |
Cl4 |
C2 |
H7 |
106.676 |
|
Cl4 |
C2 |
H8 |
107.314 |
H5 |
C1 |
H6 |
109.381 |
|
H7 |
C2 |
H8 |
109.064 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.546 |
|
|
|
2 |
C |
-0.515 |
|
|
|
3 |
Br |
-0.022 |
|
|
|
4 |
Cl |
-0.061 |
|
|
|
5 |
H |
0.280 |
|
|
|
6 |
H |
0.293 |
|
|
|
7 |
H |
0.280 |
|
|
|
8 |
H |
0.292 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.275 |
2.800 |
0.113 |
2.816 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-48.169 |
2.904 |
0.398 |
y |
2.904 |
-40.731 |
-0.105 |
z |
0.398 |
-0.105 |
-43.446 |
|
Traceless |
| x | y | z |
x |
-6.080 |
2.904 |
0.398 |
y |
2.904 |
5.076 |
-0.105 |
z |
0.398 |
-0.105 |
1.004 |
|
Polar |
3z2-r2 | 2.008 |
x2-y2 | -7.438 |
xy | 2.904 |
xz | 0.398 |
yz | -0.105 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
8.293 |
0.254 |
-0.294 |
y |
0.254 |
7.304 |
0.075 |
z |
-0.294 |
0.075 |
5.203 |
<r2> (average value of r
2) Å
2
<r2> |
221.887 |
(<r2>)1/2 |
14.896 |