Jump to
S1C2
Energy calculated at B1B95/cc-pVDZ
| | hartrees |
| Energy at 0K | -3113.318255 |
| Energy at 298.15K | |
| HF Energy | -3113.318255 |
| Nuclear repulsion energy | 289.258313 |
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 B1B95/cc-pVDZ
| 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' |
3138 |
3016 |
6.62 |
42.73 |
0.06 |
0.10 |
| 2 |
A' |
3127 |
3006 |
2.96 |
140.06 |
0.06 |
0.11 |
| 3 |
A' |
1469 |
1412 |
0.39 |
13.31 |
0.74 |
0.85 |
| 4 |
A' |
1460 |
1403 |
6.19 |
0.94 |
0.74 |
0.85 |
| 5 |
A' |
1297 |
1247 |
1.09 |
15.49 |
0.65 |
0.79 |
| 6 |
A' |
1204 |
1157 |
40.71 |
1.80 |
0.50 |
0.67 |
| 7 |
A' |
1094 |
1051 |
1.17 |
7.47 |
0.75 |
0.86 |
| 8 |
A' |
756 |
727 |
30.38 |
39.93 |
0.29 |
0.45 |
| 9 |
A' |
659 |
633 |
55.89 |
12.68 |
0.26 |
0.41 |
| 10 |
A' |
250 |
240 |
0.77 |
4.55 |
0.36 |
0.53 |
| 11 |
A' |
190 |
183 |
7.25 |
0.15 |
0.40 |
0.57 |
| 12 |
A" |
3219 |
3094 |
0.86 |
8.36 |
0.75 |
0.86 |
| 13 |
A" |
3194 |
3070 |
0.49 |
98.60 |
0.75 |
0.86 |
| 14 |
A" |
1277 |
1227 |
0.02 |
5.95 |
0.75 |
0.86 |
| 15 |
A" |
1109 |
1066 |
2.32 |
0.11 |
0.75 |
0.86 |
| 16 |
A" |
962 |
924 |
0.23 |
7.60 |
0.75 |
0.86 |
| 17 |
A" |
765 |
736 |
4.31 |
0.03 |
0.75 |
0.86 |
| 18 |
A" |
112 |
107 |
5.24 |
0.00 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12640.0 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 12149.5 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 B1B95/cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.640 |
0.000 |
| C2 |
1.230 |
-0.230 |
0.000 |
| Br3 |
-1.587 |
-0.489 |
0.000 |
| Cl4 |
2.689 |
0.815 |
0.000 |
| H5 |
-0.058 |
1.266 |
0.895 |
| H6 |
-0.058 |
1.266 |
-0.895 |
| H7 |
1.279 |
-0.860 |
0.893 |
| H8 |
1.279 |
-0.860 |
-0.893 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5061 | 1.9474 | 2.6944 | 1.0938 | 1.0938 | 2.1642 | 2.1642 |
C2 | 1.5061 | | 2.8282 | 1.7942 | 2.1668 | 2.1668 | 1.0945 | 1.0945 | Br3 | 1.9474 | 2.8282 | | 4.4697 | 2.4940 | 2.4940 | 3.0244 | 3.0244 | Cl4 | 2.6944 | 1.7942 | 4.4697 | | 2.9236 | 2.9236 | 2.3643 | 2.3643 | H5 | 1.0938 | 2.1668 | 2.4940 | 2.9236 | | 1.7900 | 2.5113 | 3.0830 | H6 | 1.0938 | 2.1668 | 2.4940 | 2.9236 | 1.7900 | | 3.0830 | 2.5113 | H7 | 2.1642 | 1.0945 | 3.0244 | 2.3643 | 2.5113 | 3.0830 | | 1.7868 | H8 | 2.1642 | 1.0945 | 3.0244 | 2.3643 | 3.0830 | 2.5113 | 1.7868 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
109.146 |
|
C1 |
C2 |
H7 |
111.672 |
| C1 |
C2 |
H8 |
111.672 |
|
C2 |
C1 |
Br3 |
109.293 |
| C2 |
C1 |
Cl4 |
38.981 |
|
C2 |
C1 |
H6 |
111.930 |
| Br3 |
C1 |
H5 |
106.802 |
|
Br3 |
C1 |
H6 |
106.802 |
| Cl4 |
C2 |
H7 |
107.372 |
|
Cl4 |
C2 |
H8 |
107.372 |
| H5 |
C1 |
H6 |
109.821 |
|
H7 |
C2 |
H8 |
109.419 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.107 |
|
|
|
| 2 |
C |
-0.067 |
|
|
|
| 3 |
Br |
-0.095 |
|
|
|
| 4 |
Cl |
-0.124 |
|
|
|
| 5 |
H |
0.099 |
|
|
|
| 6 |
H |
0.099 |
|
|
|
| 7 |
H |
0.097 |
|
|
|
| 8 |
H |
0.097 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.109 |
-0.048 |
0.000 |
0.119 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-49.297 |
-2.051 |
0.000 |
| y |
-2.051 |
-42.794 |
0.000 |
| z |
0.000 |
0.000 |
-43.011 |
|
| Traceless |
| | x | y | z |
| x |
-6.395 |
-2.051 |
0.000 |
| y |
-2.051 |
3.360 |
0.000 |
| z |
0.000 |
0.000 |
3.035 |
|
| Polar |
| 3z2-r2 | 6.069 |
| x2-y2 | -6.503 |
| xy | -2.051 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
9.947 |
2.007 |
0.000 |
| y |
2.007 |
6.235 |
0.000 |
| z |
0.000 |
0.000 |
4.823 |
<r2> (average value of r
2) Å
2
| <r2> |
281.796 |
| (<r2>)1/2 |
16.787 |
Jump to
S1C1
Energy calculated at B1B95/cc-pVDZ
| | hartrees |
| Energy at 0K | -3113.315869 |
| Energy at 298.15K | |
| HF Energy | -3113.315869 |
| Nuclear repulsion energy | 305.873640 |
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 B1B95/cc-pVDZ
| 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 |
3197 |
3073 |
1.04 |
47.22 |
0.75 |
0.86 |
| 2 |
A |
3176 |
3053 |
1.14 |
95.14 |
0.75 |
0.86 |
| 3 |
A |
3120 |
2999 |
11.47 |
175.41 |
0.03 |
0.06 |
| 4 |
A |
3102 |
2982 |
8.34 |
107.99 |
0.20 |
0.34 |
| 5 |
A |
1445 |
1389 |
2.26 |
5.33 |
0.74 |
0.85 |
| 6 |
A |
1435 |
1379 |
10.19 |
13.09 |
0.75 |
0.86 |
| 7 |
A |
1319 |
1268 |
21.41 |
2.93 |
0.75 |
0.86 |
| 8 |
A |
1274 |
1225 |
49.34 |
1.68 |
0.57 |
0.72 |
| 9 |
A |
1206 |
1159 |
2.80 |
13.40 |
0.74 |
0.85 |
| 10 |
A |
1133 |
1089 |
1.30 |
5.54 |
0.74 |
0.85 |
| 11 |
A |
1055 |
1014 |
2.34 |
3.22 |
0.72 |
0.84 |
| 12 |
A |
932 |
896 |
9.06 |
6.15 |
0.48 |
0.65 |
| 13 |
A |
863 |
830 |
22.02 |
1.52 |
0.74 |
0.85 |
| 14 |
A |
692 |
665 |
19.68 |
8.86 |
0.38 |
0.55 |
| 15 |
A |
590 |
568 |
12.14 |
14.44 |
0.20 |
0.33 |
| 16 |
A |
387 |
372 |
7.44 |
2.82 |
0.73 |
0.84 |
| 17 |
A |
242 |
233 |
1.09 |
1.39 |
0.50 |
0.67 |
| 18 |
A |
101 |
97 |
0.48 |
1.68 |
0.72 |
0.84 |
Unscaled Zero Point Vibrational Energy (zpe) 12635.1 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 12144.9 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 B1B95/cc-pVDZ
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.006 |
1.107 |
-0.377 |
| C2 |
1.282 |
0.903 |
0.395 |
| Br3 |
-1.345 |
-0.226 |
0.036 |
| Cl4 |
2.149 |
-0.581 |
-0.086 |
| H5 |
-0.433 |
2.077 |
-0.118 |
| H6 |
0.174 |
1.057 |
-1.457 |
| H7 |
1.960 |
1.744 |
0.199 |
| H8 |
1.095 |
0.837 |
1.472 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5048 | 1.9420 | 2.7432 | 1.0961 | 1.0944 | 2.1343 | 2.1625 |
C2 | 1.5048 | | 2.8815 | 1.7853 | 2.1405 | 2.1637 | 1.0977 | 1.0951 | Br3 | 1.9420 | 2.8815 | | 3.5139 | 2.4815 | 2.4859 | 3.8508 | 3.0238 | Cl4 | 2.7432 | 1.7853 | 3.5139 | | 3.7060 | 2.9092 | 2.3502 | 2.3556 | H5 | 1.0961 | 2.1405 | 2.4815 | 3.7060 | | 1.7897 | 2.4369 | 2.5302 | H6 | 1.0944 | 2.1637 | 2.4859 | 2.9092 | 1.7897 | | 2.5311 | 3.0784 | H7 | 2.1343 | 1.0977 | 3.8508 | 2.3502 | 2.4369 | 2.5311 | | 1.7866 | H8 | 2.1625 | 1.0951 | 3.0238 | 2.3556 | 2.5302 | 3.0784 | 1.7866 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
112.701 |
|
C1 |
C2 |
H7 |
109.190 |
| C1 |
C2 |
H8 |
111.591 |
|
C2 |
C1 |
Br3 |
112.829 |
| C2 |
C1 |
Cl4 |
36.898 |
|
C2 |
C1 |
H6 |
111.733 |
| Br3 |
C1 |
H5 |
106.163 |
|
Br3 |
C1 |
H6 |
106.552 |
| Cl4 |
C2 |
H7 |
106.777 |
|
Cl4 |
C2 |
H8 |
107.291 |
| H5 |
C1 |
H6 |
109.579 |
|
H7 |
C2 |
H8 |
109.124 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.109 |
|
|
|
| 2 |
C |
-0.068 |
|
|
|
| 3 |
Br |
-0.086 |
|
|
|
| 4 |
Cl |
-0.113 |
|
|
|
| 5 |
H |
0.091 |
|
|
|
| 6 |
H |
0.099 |
|
|
|
| 7 |
H |
0.090 |
|
|
|
| 8 |
H |
0.097 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.328 |
2.624 |
0.109 |
2.647 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-46.766 |
2.688 |
0.371 |
| y |
2.688 |
-40.036 |
-0.097 |
| z |
0.371 |
-0.097 |
-42.664 |
|
| Traceless |
| | x | y | z |
| x |
-5.417 |
2.688 |
0.371 |
| y |
2.688 |
4.679 |
-0.097 |
| z |
0.371 |
-0.097 |
0.738 |
|
| Polar |
| 3z2-r2 | 1.475 |
| x2-y2 | -6.731 |
| xy | 2.688 |
| xz | 0.371 |
| yz | -0.097 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.948 |
0.326 |
-0.264 |
| y |
0.326 |
7.124 |
0.045 |
| z |
-0.264 |
0.045 |
5.130 |
<r2> (average value of r
2) Å
2
| <r2> |
219.124 |
| (<r2>)1/2 |
14.803 |