Jump to
S1C2
Energy calculated at B97D3/daug-cc-pVTZ
| | hartrees |
| Energy at 0K | -3114.377235 |
| Energy at 298.15K | |
| HF Energy | -3114.377235 |
| Nuclear repulsion energy | 286.358328 |
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 B97D3/daug-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' |
3064 |
3064 |
7.45 |
37.00 |
0.03 |
0.05 |
| 2 |
A' |
3050 |
3050 |
2.83 |
143.66 |
0.03 |
0.05 |
| 3 |
A' |
1462 |
1462 |
2.52 |
3.58 |
0.75 |
0.85 |
| 4 |
A' |
1457 |
1457 |
3.22 |
2.63 |
0.75 |
0.86 |
| 5 |
A' |
1276 |
1276 |
1.96 |
24.86 |
0.31 |
0.47 |
| 6 |
A' |
1196 |
1196 |
38.47 |
4.95 |
0.23 |
0.38 |
| 7 |
A' |
1041 |
1041 |
0.85 |
5.75 |
0.74 |
0.85 |
| 8 |
A' |
683 |
683 |
28.45 |
77.05 |
0.25 |
0.40 |
| 9 |
A' |
594 |
594 |
72.44 |
17.75 |
0.22 |
0.36 |
| 10 |
A' |
237 |
237 |
0.93 |
6.25 |
0.20 |
0.34 |
| 11 |
A' |
189 |
189 |
7.42 |
0.45 |
0.18 |
0.30 |
| 12 |
A" |
3137 |
3137 |
1.37 |
8.08 |
0.75 |
0.86 |
| 13 |
A" |
3108 |
3108 |
0.53 |
72.53 |
0.75 |
0.86 |
| 14 |
A" |
1265 |
1265 |
0.02 |
2.12 |
0.75 |
0.86 |
| 15 |
A" |
1096 |
1096 |
1.55 |
0.03 |
0.75 |
0.86 |
| 16 |
A" |
951 |
951 |
0.13 |
0.87 |
0.75 |
0.86 |
| 17 |
A" |
756 |
756 |
2.78 |
0.00 |
0.75 |
0.86 |
| 18 |
A" |
108 |
108 |
5.33 |
0.01 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12334.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 12334.9 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 B97D3/daug-cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.653 |
0.000 |
| C2 |
1.239 |
-0.210 |
0.000 |
| Br3 |
-1.594 |
-0.526 |
0.000 |
| Cl4 |
2.701 |
0.874 |
0.000 |
| H5 |
-0.077 |
1.268 |
0.895 |
| H6 |
-0.077 |
1.268 |
-0.895 |
| H7 |
1.305 |
-0.831 |
0.892 |
| H8 |
1.305 |
-0.831 |
-0.892 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5096 | 1.9825 | 2.7100 | 1.0884 | 1.0884 | 2.1679 | 2.1679 |
C2 | 1.5096 | | 2.8513 | 1.8196 | 2.1714 | 2.1714 | 1.0894 | 1.0894 | Br3 | 1.9825 | 2.8513 | | 4.5178 | 2.5136 | 2.5136 | 3.0490 | 3.0490 | Cl4 | 2.7100 | 1.8196 | 4.5178 | | 2.9449 | 2.9449 | 2.3775 | 2.3775 | H5 | 1.0884 | 2.1714 | 2.5136 | 2.9449 | | 1.7892 | 2.5127 | 3.0834 | H6 | 1.0884 | 2.1714 | 2.5136 | 2.9449 | 1.7892 | | 3.0834 | 2.5127 | H7 | 2.1679 | 1.0894 | 3.0490 | 2.3775 | 2.5127 | 3.0834 | | 1.7849 | H8 | 2.1679 | 1.0894 | 3.0490 | 2.3775 | 3.0834 | 2.5127 | 1.7849 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
108.623 |
|
C1 |
C2 |
H7 |
112.036 |
| C1 |
C2 |
H8 |
112.036 |
|
C2 |
C1 |
Br3 |
108.717 |
| C2 |
C1 |
Cl4 |
39.515 |
|
C2 |
C1 |
H6 |
112.386 |
| Br3 |
C1 |
H5 |
106.193 |
|
Br3 |
C1 |
H6 |
106.193 |
| Cl4 |
C2 |
H7 |
106.931 |
|
Cl4 |
C2 |
H8 |
106.931 |
| H5 |
C1 |
H6 |
110.562 |
|
H7 |
C2 |
H8 |
110.011 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/daug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.120 |
|
|
|
| 2 |
C |
0.580 |
|
|
|
| 3 |
Br |
-0.778 |
|
|
|
| 4 |
Cl |
-0.914 |
|
|
|
| 5 |
H |
0.158 |
|
|
|
| 6 |
H |
0.158 |
|
|
|
| 7 |
H |
0.338 |
|
|
|
| 8 |
H |
0.338 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.046 |
-0.014 |
0.000 |
0.049 |
| 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 |
13.284 |
1.875 |
0.000 |
| y |
1.875 |
9.091 |
0.000 |
| z |
0.000 |
0.000 |
7.906 |
<r2> (average value of r
2) Å
2
| <r2> |
287.509 |
| (<r2>)1/2 |
16.956 |
Jump to
S1C1
Energy calculated at B97D3/daug-cc-pVTZ
| | hartrees |
| Energy at 0K | -3114.374388 |
| Energy at 298.15K | |
| HF Energy | -3114.374388 |
| Nuclear repulsion energy | 301.762138 |
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 B97D3/daug-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 |
3111 |
3111 |
2.05 |
38.82 |
0.75 |
0.85 |
| 2 |
A |
3085 |
3085 |
1.55 |
75.69 |
0.74 |
0.85 |
| 3 |
A |
3039 |
3039 |
13.37 |
192.77 |
0.03 |
0.06 |
| 4 |
A |
3017 |
3017 |
10.68 |
135.30 |
0.16 |
0.28 |
| 5 |
A |
1439 |
1439 |
3.95 |
5.03 |
0.74 |
0.85 |
| 6 |
A |
1432 |
1432 |
7.45 |
6.66 |
0.74 |
0.85 |
| 7 |
A |
1298 |
1298 |
18.32 |
2.48 |
0.29 |
0.45 |
| 8 |
A |
1257 |
1257 |
51.34 |
4.95 |
0.28 |
0.44 |
| 9 |
A |
1177 |
1177 |
2.41 |
5.75 |
0.74 |
0.85 |
| 10 |
A |
1117 |
1117 |
0.75 |
1.26 |
0.66 |
0.79 |
| 11 |
A |
1014 |
1014 |
2.29 |
0.90 |
0.68 |
0.81 |
| 12 |
A |
906 |
906 |
8.67 |
4.64 |
0.20 |
0.33 |
| 13 |
A |
848 |
848 |
19.86 |
1.01 |
0.74 |
0.85 |
| 14 |
A |
634 |
634 |
25.24 |
9.60 |
0.25 |
0.40 |
| 15 |
A |
538 |
538 |
12.63 |
19.07 |
0.11 |
0.20 |
| 16 |
A |
376 |
376 |
8.85 |
1.95 |
0.66 |
0.79 |
| 17 |
A |
238 |
238 |
1.48 |
1.74 |
0.18 |
0.30 |
| 18 |
A |
95 |
95 |
0.51 |
0.95 |
0.62 |
0.76 |
Unscaled Zero Point Vibrational Energy (zpe) 12309.6 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 12309.6 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 B97D3/daug-cc-pVTZ
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.022 |
1.105 |
-0.387 |
| C2 |
1.289 |
0.903 |
0.407 |
| Br3 |
-1.374 |
-0.225 |
0.036 |
| Cl4 |
2.200 |
-0.578 |
-0.086 |
| H5 |
-0.418 |
2.074 |
-0.143 |
| H6 |
0.192 |
1.031 |
-1.460 |
| H7 |
1.960 |
1.748 |
0.230 |
| H8 |
1.090 |
0.813 |
1.475 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5089 | 1.9740 | 2.7692 | 1.0917 | 1.0890 | 2.1339 | 2.1670 |
C2 | 1.5089 | | 2.9154 | 1.8074 | 2.1413 | 2.1690 | 1.0938 | 1.0902 | Br3 | 1.9740 | 2.9154 | | 3.5931 | 2.4966 | 2.5038 | 3.8793 | 3.0367 | Cl4 | 2.7692 | 1.8074 | 3.5931 | | 3.7268 | 2.9168 | 2.3593 | 2.3669 | H5 | 1.0917 | 2.1413 | 2.4966 | 3.7268 | | 1.7880 | 2.4295 | 2.5460 | H6 | 1.0890 | 2.1690 | 2.5038 | 2.9168 | 1.7880 | | 2.5491 | 3.0774 | H7 | 2.1339 | 1.0938 | 3.8793 | 2.3593 | 2.4295 | 2.5491 | | 1.7836 | H8 | 2.1670 | 1.0902 | 3.0367 | 2.3669 | 2.5460 | 3.0774 | 1.7836 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
112.926 |
|
C1 |
C2 |
H7 |
109.106 |
| C1 |
C2 |
H8 |
111.970 |
|
C2 |
C1 |
Br3 |
112.987 |
| C2 |
C1 |
Cl4 |
36.952 |
|
C2 |
C1 |
H6 |
112.201 |
| Br3 |
C1 |
H5 |
105.400 |
|
Br3 |
C1 |
H6 |
106.022 |
| Cl4 |
C2 |
H7 |
106.203 |
|
Cl4 |
C2 |
H8 |
106.921 |
| H5 |
C1 |
H6 |
110.146 |
|
H7 |
C2 |
H8 |
109.514 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/daug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.155 |
|
|
|
| 2 |
C |
0.712 |
|
|
|
| 3 |
Br |
-0.775 |
|
|
|
| 4 |
Cl |
-0.917 |
|
|
|
| 5 |
H |
0.250 |
|
|
|
| 6 |
H |
0.097 |
|
|
|
| 7 |
H |
0.170 |
|
|
|
| 8 |
H |
0.307 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.386 |
2.642 |
0.103 |
2.672 |
| 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 |
11.317 |
0.158 |
-0.123 |
| y |
0.158 |
9.540 |
0.035 |
| z |
-0.123 |
0.035 |
8.111 |
<r2> (average value of r
2) Å
2
| <r2> |
226.194 |
| (<r2>)1/2 |
15.040 |