Jump to
S1C2
Energy calculated at B3LYP/LANL2DZ
| | hartrees |
| Energy at 0K | -106.718866 |
| Energy at 298.15K | |
| HF Energy | -106.718866 |
| Nuclear repulsion energy | 85.948211 |
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/LANL2DZ
| 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' |
3153 |
3031 |
15.85 |
1.42 |
0.30 |
0.46 |
| 2 |
A' |
3146 |
3024 |
0.11 |
207.97 |
0.05 |
0.09 |
| 3 |
A' |
1509 |
1450 |
1.51 |
13.36 |
0.75 |
0.86 |
| 4 |
A' |
1502 |
1444 |
11.98 |
2.19 |
0.72 |
0.84 |
| 5 |
A' |
1324 |
1272 |
1.07 |
32.79 |
0.45 |
0.62 |
| 6 |
A' |
1257 |
1208 |
33.64 |
3.91 |
0.55 |
0.71 |
| 7 |
A' |
1083 |
1041 |
1.33 |
28.69 |
0.70 |
0.83 |
| 8 |
A' |
669 |
643 |
18.93 |
90.98 |
0.29 |
0.44 |
| 9 |
A' |
584 |
561 |
74.11 |
9.54 |
0.32 |
0.48 |
| 10 |
A' |
229 |
220 |
1.22 |
11.55 |
0.41 |
0.58 |
| 11 |
A' |
186 |
178 |
9.74 |
0.54 |
0.55 |
0.71 |
| 12 |
A" |
3249 |
3122 |
10.48 |
0.65 |
0.75 |
0.86 |
| 13 |
A" |
3225 |
3100 |
0.18 |
90.53 |
0.75 |
0.86 |
| 14 |
A" |
1294 |
1243 |
0.01 |
10.47 |
0.75 |
0.86 |
| 15 |
A" |
1121 |
1077 |
1.06 |
0.42 |
0.75 |
0.86 |
| 16 |
A" |
975 |
937 |
0.31 |
11.67 |
0.75 |
0.86 |
| 17 |
A" |
794 |
764 |
9.66 |
0.16 |
0.75 |
0.86 |
| 18 |
A" |
106 |
101 |
7.13 |
0.03 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12702.0 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 12209.2 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 B3LYP/LANL2DZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.664 |
0.000 |
| C2 |
1.257 |
-0.189 |
0.000 |
| Br3 |
-1.624 |
-0.583 |
0.000 |
| Cl4 |
2.752 |
0.978 |
0.000 |
| H5 |
-0.100 |
1.271 |
0.899 |
| H6 |
-0.100 |
1.271 |
-0.899 |
| H7 |
1.358 |
-0.797 |
0.899 |
| H8 |
1.358 |
-0.797 |
-0.899 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5187 | 2.0476 | 2.7702 | 1.0897 | 1.0897 | 2.1877 | 2.1877 |
C2 | 1.5187 | | 2.9077 | 1.8972 | 2.1865 | 2.1865 | 1.0897 | 1.0897 | Br3 | 2.0476 | 2.9077 | | 4.6467 | 2.5636 | 2.5636 | 3.1224 | 3.1224 | Cl4 | 2.7702 | 1.8972 | 4.6467 | | 3.0046 | 3.0046 | 2.4291 | 2.4291 | H5 | 1.0897 | 2.1865 | 2.5636 | 3.0046 | | 1.7978 | 2.5305 | 3.1040 | H6 | 1.0897 | 2.1865 | 2.5636 | 3.0046 | 1.7978 | | 3.1040 | 2.5305 | H7 | 2.1877 | 1.0897 | 3.1224 | 2.4291 | 2.5305 | 3.1040 | | 1.7976 | H8 | 2.1877 | 1.0897 | 3.1224 | 2.4291 | 3.1040 | 2.5305 | 1.7976 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
107.872 |
|
C1 |
C2 |
H7 |
112.978 |
| C1 |
C2 |
H8 |
112.978 |
|
C2 |
C1 |
Br3 |
108.325 |
| C2 |
C1 |
Cl4 |
40.677 |
|
C2 |
C1 |
H6 |
112.884 |
| Br3 |
C1 |
H5 |
105.494 |
|
Br3 |
C1 |
H6 |
105.494 |
| Cl4 |
C2 |
H7 |
105.632 |
|
Cl4 |
C2 |
H8 |
105.632 |
| H5 |
C1 |
H6 |
111.164 |
|
H7 |
C2 |
H8 |
111.141 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.524 |
|
|
|
| 2 |
C |
-0.448 |
|
|
|
| 3 |
Br |
-0.038 |
|
|
|
| 4 |
Cl |
-0.088 |
|
|
|
| 5 |
H |
0.280 |
|
|
|
| 6 |
H |
0.280 |
|
|
|
| 7 |
H |
0.269 |
|
|
|
| 8 |
H |
0.269 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.251 |
-0.177 |
0.000 |
0.307 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-48.519 |
-3.522 |
0.000 |
| y |
-3.522 |
-39.715 |
0.000 |
| z |
0.000 |
0.000 |
-39.482 |
|
| Traceless |
| | x | y | z |
| x |
-8.921 |
-3.522 |
0.000 |
| y |
-3.522 |
4.285 |
0.000 |
| z |
0.000 |
0.000 |
4.635 |
|
| Polar |
| 3z2-r2 | 9.271 |
| x2-y2 | -8.804 |
| xy | -3.522 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
9.726 |
3.321 |
0.000 |
| y |
3.321 |
5.633 |
0.000 |
| z |
0.000 |
0.000 |
3.280 |
<r2> (average value of r
2) Å
2
| <r2> |
130.935 |
| (<r2>)1/2 |
11.443 |
Jump to
S1C1
Energy calculated at B3LYP/LANL2DZ
| | hartrees |
| Energy at 0K | -106.714902 |
| Energy at 298.15K | |
| HF Energy | -106.714902 |
| Nuclear repulsion energy | 86.917847 |
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/LANL2DZ
| 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 |
3213 |
3088 |
9.62 |
26.34 |
0.75 |
0.85 |
| 2 |
A |
3199 |
3075 |
1.61 |
97.94 |
0.74 |
0.85 |
| 3 |
A |
3122 |
3001 |
27.24 |
268.60 |
0.01 |
0.02 |
| 4 |
A |
3111 |
2990 |
4.80 |
62.58 |
0.58 |
0.73 |
| 5 |
A |
1486 |
1428 |
6.83 |
10.01 |
0.73 |
0.85 |
| 6 |
A |
1478 |
1420 |
11.98 |
13.93 |
0.75 |
0.85 |
| 7 |
A |
1342 |
1290 |
17.88 |
5.59 |
0.62 |
0.77 |
| 8 |
A |
1311 |
1260 |
40.99 |
3.88 |
0.62 |
0.77 |
| 9 |
A |
1207 |
1160 |
0.52 |
21.94 |
0.75 |
0.86 |
| 10 |
A |
1143 |
1099 |
1.40 |
7.20 |
0.75 |
0.86 |
| 11 |
A |
1064 |
1022 |
2.61 |
4.38 |
0.72 |
0.84 |
| 12 |
A |
942 |
905 |
9.73 |
11.63 |
0.39 |
0.56 |
| 13 |
A |
881 |
847 |
28.33 |
1.64 |
0.70 |
0.82 |
| 14 |
A |
616 |
592 |
24.09 |
20.91 |
0.46 |
0.63 |
| 15 |
A |
529 |
508 |
12.59 |
23.41 |
0.26 |
0.41 |
| 16 |
A |
370 |
356 |
11.05 |
6.51 |
0.75 |
0.85 |
| 17 |
A |
238 |
229 |
1.91 |
3.16 |
0.47 |
0.64 |
| 18 |
A |
90 |
87 |
0.81 |
3.87 |
0.74 |
0.85 |
Unscaled Zero Point Vibrational Energy (zpe) 12670.4 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 12178.8 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/LANL2DZ
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.038 |
1.131 |
-0.404 |
| C2 |
1.298 |
0.942 |
0.422 |
| Br3 |
-1.406 |
-0.231 |
0.036 |
| Cl4 |
2.253 |
-0.594 |
-0.086 |
| H5 |
-0.418 |
2.100 |
-0.181 |
| H6 |
0.221 |
1.033 |
-1.474 |
| H7 |
1.988 |
1.774 |
0.251 |
| H8 |
1.092 |
0.832 |
1.487 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5183 | 2.0331 | 2.8258 | 1.0938 | 1.0904 | 2.1549 | 2.1855 |
C2 | 1.5183 | | 2.9724 | 1.8787 | 2.1562 | 2.1827 | 1.0942 | 1.0904 | Br3 | 2.0331 | 2.9724 | | 3.6790 | 2.5413 | 2.5543 | 3.9475 | 3.0783 | Cl4 | 2.8258 | 1.8787 | 3.6790 | | 3.7951 | 2.9505 | 2.4066 | 2.4197 | H5 | 1.0938 | 2.1562 | 2.5413 | 3.7951 | | 1.7943 | 2.4657 | 2.5830 | H6 | 1.0904 | 2.1827 | 2.5543 | 2.9505 | 1.7943 | | 2.5784 | 3.0935 | H7 | 2.1549 | 1.0942 | 3.9475 | 2.4066 | 2.4657 | 2.5784 | | 1.7935 | H8 | 2.1855 | 1.0904 | 3.0783 | 2.4197 | 2.5830 | 3.0935 | 1.7935 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
112.144 |
|
C1 |
C2 |
H7 |
110.088 |
| C1 |
C2 |
H8 |
112.784 |
|
C2 |
C1 |
Br3 |
112.840 |
| C2 |
C1 |
Cl4 |
38.010 |
|
C2 |
C1 |
H6 |
112.549 |
| Br3 |
C1 |
H5 |
104.697 |
|
Br3 |
C1 |
H6 |
105.723 |
| Cl4 |
C2 |
H7 |
105.013 |
|
Cl4 |
C2 |
H8 |
106.105 |
| H5 |
C1 |
H6 |
110.465 |
|
H7 |
C2 |
H8 |
110.372 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.524 |
|
|
|
| 2 |
C |
-0.448 |
|
|
|
| 3 |
Br |
-0.025 |
|
|
|
| 4 |
Cl |
-0.070 |
|
|
|
| 5 |
H |
0.260 |
|
|
|
| 6 |
H |
0.281 |
|
|
|
| 7 |
H |
0.255 |
|
|
|
| 8 |
H |
0.271 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.281 |
3.282 |
0.176 |
3.299 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-44.888 |
3.475 |
0.493 |
| y |
3.475 |
-36.342 |
-0.134 |
| z |
0.493 |
-0.134 |
-38.990 |
|
| Traceless |
| | x | y | z |
| x |
-7.221 |
3.475 |
0.493 |
| y |
3.475 |
5.597 |
-0.134 |
| z |
0.493 |
-0.134 |
1.625 |
|
| Polar |
| 3z2-r2 | 3.249 |
| x2-y2 | -8.546 |
| xy | 3.475 |
| xz | 0.493 |
| yz | -0.134 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.175 |
0.668 |
-0.654 |
| y |
0.668 |
6.509 |
0.006 |
| z |
-0.654 |
0.006 |
3.680 |
<r2> (average value of r
2) Å
2
| <r2> |
121.639 |
| (<r2>)1/2 |
11.029 |