Jump to
S1C2
Energy calculated at TPSSh/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -3110.590510 |
| Energy at 298.15K | |
| HF Energy | -3110.590510 |
| Nuclear repulsion energy | 289.499501 |
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 TPSSh/6-31G(2df,p)
| 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' |
3110 |
3001 |
9.69 |
7.72 |
0.07 |
0.13 |
| 2 |
A' |
3102 |
2993 |
0.80 |
134.14 |
0.06 |
0.11 |
| 3 |
A' |
1495 |
1443 |
1.35 |
8.90 |
0.75 |
0.85 |
| 4 |
A' |
1493 |
1440 |
3.09 |
4.16 |
0.74 |
0.85 |
| 5 |
A' |
1303 |
1257 |
2.85 |
12.95 |
0.46 |
0.63 |
| 6 |
A' |
1218 |
1176 |
42.12 |
1.72 |
0.28 |
0.44 |
| 7 |
A' |
1061 |
1024 |
1.14 |
5.46 |
0.73 |
0.84 |
| 8 |
A' |
728 |
702 |
33.90 |
51.92 |
0.27 |
0.43 |
| 9 |
A' |
650 |
627 |
60.32 |
10.66 |
0.20 |
0.33 |
| 10 |
A' |
246 |
238 |
0.78 |
4.22 |
0.27 |
0.43 |
| 11 |
A' |
187 |
181 |
7.99 |
0.08 |
0.17 |
0.29 |
| 12 |
A" |
3186 |
3075 |
2.05 |
1.13 |
0.75 |
0.86 |
| 13 |
A" |
3162 |
3052 |
0.14 |
87.45 |
0.75 |
0.86 |
| 14 |
A" |
1289 |
1243 |
0.06 |
6.17 |
0.75 |
0.86 |
| 15 |
A" |
1114 |
1075 |
1.82 |
0.20 |
0.75 |
0.86 |
| 16 |
A" |
971 |
937 |
0.09 |
4.50 |
0.75 |
0.86 |
| 17 |
A" |
759 |
733 |
2.70 |
0.00 |
0.75 |
0.86 |
| 18 |
A" |
111 |
107 |
5.76 |
0.03 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12592.9 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 12152.2 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 TPSSh/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.651 |
0.000 |
| C2 |
1.210 |
-0.261 |
0.000 |
| Br3 |
-1.592 |
-0.454 |
0.000 |
| Cl4 |
2.709 |
0.750 |
0.000 |
| H5 |
-0.038 |
1.275 |
0.892 |
| H6 |
-0.038 |
1.275 |
-0.892 |
| H7 |
1.246 |
-0.885 |
0.892 |
| H8 |
1.246 |
-0.885 |
-0.892 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5151 | 1.9382 | 2.7112 | 1.0890 | 1.0890 | 2.1699 | 2.1699 |
C2 | 1.5151 | | 2.8087 | 1.8089 | 2.1705 | 2.1705 | 1.0894 | 1.0894 | Br3 | 1.9382 | 2.8087 | | 4.4671 | 2.4898 | 2.4898 | 3.0062 | 3.0062 | Cl4 | 2.7112 | 1.8089 | 4.4671 | | 2.9358 | 2.9358 | 2.3692 | 2.3692 | H5 | 1.0890 | 2.1705 | 2.4898 | 2.9358 | | 1.7840 | 2.5127 | 3.0817 | H6 | 1.0890 | 2.1705 | 2.4898 | 2.9358 | 1.7840 | | 3.0817 | 2.5127 | H7 | 2.1699 | 1.0894 | 3.0062 | 2.3692 | 2.5127 | 3.0817 | | 1.7842 | H8 | 2.1699 | 1.0894 | 3.0062 | 2.3692 | 3.0817 | 2.5127 | 1.7842 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
108.984 |
|
C1 |
C2 |
H7 |
111.805 |
| C1 |
C2 |
H8 |
111.805 |
|
C2 |
C1 |
Br3 |
108.222 |
| C2 |
C1 |
Cl4 |
39.116 |
|
C2 |
C1 |
H6 |
111.877 |
| Br3 |
C1 |
H5 |
107.323 |
|
Br3 |
C1 |
H6 |
107.323 |
| Cl4 |
C2 |
H7 |
107.030 |
|
Cl4 |
C2 |
H8 |
107.030 |
| H5 |
C1 |
H6 |
109.991 |
|
H7 |
C2 |
H8 |
109.952 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at TPSSh/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.352 |
|
|
|
| 2 |
C |
-0.219 |
|
|
|
| 3 |
Br |
-0.036 |
|
|
|
| 4 |
Cl |
-0.165 |
|
|
|
| 5 |
H |
0.194 |
|
|
|
| 6 |
H |
0.194 |
|
|
|
| 7 |
H |
0.192 |
|
|
|
| 8 |
H |
0.192 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.225 |
-0.059 |
0.000 |
0.233 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
11.151 |
1.691 |
0.000 |
| y |
1.691 |
7.184 |
0.000 |
| z |
0.000 |
0.000 |
6.212 |
<r2> (average value of r
2) Å
2
| <r2> |
281.326 |
| (<r2>)1/2 |
16.773 |
Jump to
S1C1
Energy calculated at TPSSh/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -3110.587482 |
| Energy at 298.15K | |
| HF Energy | -3110.587482 |
| Nuclear repulsion energy | 306.238997 |
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 TPSSh/6-31G(2df,p)
| 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 |
3161 |
3050 |
3.21 |
28.46 |
0.74 |
0.85 |
| 2 |
A |
3145 |
3035 |
0.88 |
90.87 |
0.75 |
0.86 |
| 3 |
A |
3086 |
2978 |
16.39 |
172.78 |
0.03 |
0.05 |
| 4 |
A |
3074 |
2967 |
6.09 |
73.45 |
0.38 |
0.55 |
| 5 |
A |
1477 |
1425 |
1.98 |
7.11 |
0.70 |
0.82 |
| 6 |
A |
1470 |
1418 |
6.19 |
11.94 |
0.75 |
0.86 |
| 7 |
A |
1324 |
1278 |
22.55 |
2.59 |
0.73 |
0.84 |
| 8 |
A |
1287 |
1242 |
47.36 |
1.43 |
0.31 |
0.47 |
| 9 |
A |
1199 |
1157 |
2.15 |
10.89 |
0.73 |
0.84 |
| 10 |
A |
1136 |
1097 |
0.90 |
3.74 |
0.73 |
0.84 |
| 11 |
A |
1033 |
997 |
1.91 |
2.50 |
0.75 |
0.86 |
| 12 |
A |
932 |
900 |
8.47 |
4.13 |
0.38 |
0.55 |
| 13 |
A |
867 |
836 |
18.20 |
0.95 |
0.73 |
0.84 |
| 14 |
A |
673 |
650 |
21.93 |
8.75 |
0.35 |
0.51 |
| 15 |
A |
590 |
570 |
10.53 |
14.35 |
0.14 |
0.25 |
| 16 |
A |
380 |
366 |
7.59 |
1.85 |
0.71 |
0.83 |
| 17 |
A |
235 |
227 |
1.18 |
0.87 |
0.25 |
0.40 |
| 18 |
A |
96 |
93 |
0.58 |
0.94 |
0.70 |
0.82 |
Unscaled Zero Point Vibrational Energy (zpe) 12582.2 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 12141.9 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 TPSSh/6-31G(2df,p)
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.010 |
1.108 |
-0.384 |
| C2 |
1.270 |
0.911 |
0.403 |
| Br3 |
-1.338 |
-0.228 |
0.036 |
| Cl4 |
2.149 |
-0.578 |
-0.088 |
| H5 |
-0.448 |
2.075 |
-0.129 |
| H6 |
0.167 |
1.058 |
-1.458 |
| H7 |
1.949 |
1.747 |
0.214 |
| H8 |
1.076 |
0.828 |
1.472 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5156 | 1.9309 | 2.7557 | 1.0921 | 1.0895 | 2.1460 | 2.1687 |
C2 | 1.5156 | | 2.8705 | 1.7977 | 2.1425 | 2.1679 | 1.0928 | 1.0900 | Br3 | 1.9309 | 2.8705 | | 3.5074 | 2.4754 | 2.4811 | 3.8397 | 3.0013 | Cl4 | 2.7557 | 1.7977 | 3.5074 | | 3.7134 | 2.9126 | 2.3531 | 2.3581 | H5 | 1.0921 | 2.1425 | 2.4754 | 3.7134 | | 1.7834 | 2.4441 | 2.5380 | H6 | 1.0895 | 2.1679 | 2.4811 | 2.9126 | 1.7834 | | 2.5391 | 3.0762 | H7 | 2.1460 | 1.0928 | 3.8397 | 2.3531 | 2.4441 | 2.5391 | | 1.7854 | H8 | 2.1687 | 1.0900 | 3.0013 | 2.3581 | 2.5380 | 3.0762 | 1.7854 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
112.272 |
|
C1 |
C2 |
H7 |
109.650 |
| C1 |
C2 |
H8 |
111.637 |
|
C2 |
C1 |
Br3 |
112.231 |
| C2 |
C1 |
Cl4 |
37.134 |
|
C2 |
C1 |
H6 |
111.605 |
| Br3 |
C1 |
H5 |
106.619 |
|
Br3 |
C1 |
H6 |
107.146 |
| Cl4 |
C2 |
H7 |
106.427 |
|
Cl4 |
C2 |
H8 |
106.926 |
| H5 |
C1 |
H6 |
109.668 |
|
H7 |
C2 |
H8 |
109.758 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at TPSSh/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.360 |
|
|
|
| 2 |
C |
-0.222 |
|
|
|
| 3 |
Br |
-0.022 |
|
|
|
| 4 |
Cl |
-0.147 |
|
|
|
| 5 |
H |
0.185 |
|
|
|
| 6 |
H |
0.194 |
|
|
|
| 7 |
H |
0.179 |
|
|
|
| 8 |
H |
0.191 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.278 |
2.692 |
0.116 |
2.708 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
9.206 |
0.107 |
-0.202 |
| y |
0.107 |
7.972 |
0.057 |
| z |
-0.202 |
0.057 |
6.364 |
<r2> (average value of r
2) Å
2
| <r2> |
218.454 |
| (<r2>)1/2 |
14.780 |