Jump to
S1C2
Energy calculated at HF/LANL2DZ
| | hartrees |
| Energy at 0K | -51.889095 |
| Energy at 298.15K | -51.892858 |
| HF Energy | -51.889095 |
| Nuclear repulsion energy | 20.535573 |
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 HF/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' |
3353 |
3017 |
16.18 |
|
|
|
| 2 |
A' |
1474 |
1326 |
47.77 |
|
|
|
| 3 |
A' |
642 |
578 |
20.08 |
|
|
|
| 4 |
A' |
255 |
229 |
96.41 |
|
|
|
| 5 |
A" |
3533 |
3180 |
2.14 |
|
|
|
| 6 |
A" |
989 |
890 |
2.99 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5122.6 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 4609.9 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 HF/LANL2DZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.005 |
1.555 |
0.000 |
| Br2 |
-0.005 |
-0.383 |
0.000 |
| H3 |
0.103 |
2.037 |
0.948 |
| H4 |
0.103 |
2.037 |
-0.948 |
Atom - Atom Distances (Å)
| |
C1 |
Br2 |
H3 |
H4 |
| C1 | | 1.9378 | 1.0692 | 1.0692 |
Br2 | 1.9378 | | 2.6015 | 2.6015 | H3 | 1.0692 | 2.6015 | | 1.8961 | H4 | 1.0692 | 2.6015 | 1.8961 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br2 |
C1 |
H3 |
116.818 |
|
Br2 |
C1 |
H4 |
116.818 |
| H3 |
C1 |
H4 |
124.917 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.460 |
|
|
|
| 2 |
Br |
-0.014 |
|
|
|
| 3 |
H |
0.237 |
|
|
|
| 4 |
H |
0.237 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.234 |
1.850 |
0.000 |
1.865 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.622 |
0.482 |
0.000 |
| y |
0.482 |
-18.433 |
0.000 |
| z |
0.000 |
0.000 |
-21.447 |
|
| Traceless |
| | x | y | z |
| x |
-3.682 |
0.482 |
0.000 |
| y |
0.482 |
4.102 |
0.000 |
| z |
0.000 |
0.000 |
-0.420 |
|
| Polar |
| 3z2-r2 | -0.841 |
| x2-y2 | -5.189 |
| xy | 0.482 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.853 |
0.050 |
0.000 |
| y |
0.050 |
5.283 |
0.000 |
| z |
0.000 |
0.000 |
1.715 |
<r2> (average value of r
2) Å
2
| <r2> |
38.871 |
| (<r2>)1/2 |
6.235 |
Jump to
S1C1
Energy calculated at HF/LANL2DZ
| | hartrees |
| Energy at 0K | -51.889074 |
| Energy at 298.15K | |
| HF Energy | -51.889074 |
| Nuclear repulsion energy | 20.548090 |
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 HF/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 |
A1 |
3355 |
3019 |
15.45 |
149.68 |
0.12 |
0.22 |
| 2 |
A1 |
1471 |
1324 |
49.35 |
0.70 |
0.47 |
0.64 |
| 3 |
A1 |
643 |
579 |
19.02 |
28.71 |
0.35 |
0.52 |
| 4 |
B1 |
181i |
163i |
109.38 |
0.08 |
0.75 |
0.86 |
| 5 |
B2 |
3539 |
3185 |
1.64 |
51.92 |
0.75 |
0.86 |
| 6 |
B2 |
985 |
886 |
3.18 |
6.46 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4906.1 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 4415.0 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 HF/LANL2DZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.553 |
| Br2 |
0.000 |
0.000 |
0.383 |
| H3 |
0.000 |
0.950 |
-2.042 |
| H4 |
0.000 |
-0.950 |
-2.042 |
Atom - Atom Distances (Å)
| |
C1 |
Br2 |
H3 |
H4 |
| C1 | | 1.9354 | 1.0688 | 1.0688 |
Br2 | 1.9354 | | 2.6041 | 2.6041 | H3 | 1.0688 | 2.6041 | | 1.9007 | H4 | 1.0688 | 2.6041 | 1.9007 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br2 |
C1 |
H3 |
117.231 |
|
Br2 |
C1 |
H4 |
117.231 |
| H3 |
C1 |
H4 |
125.538 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.468 |
|
|
|
| 2 |
Br |
-0.011 |
|
|
|
| 3 |
H |
0.239 |
|
|
|
| 4 |
H |
0.239 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
-1.841 |
1.841 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.658 |
0.000 |
0.000 |
| y |
0.000 |
-21.424 |
0.000 |
| z |
0.000 |
0.000 |
-18.389 |
|
| Traceless |
| | x | y | z |
| x |
-3.752 |
0.000 |
0.000 |
| y |
0.000 |
-0.400 |
0.000 |
| z |
0.000 |
0.000 |
4.152 |
|
| Polar |
| 3z2-r2 | 8.304 |
| x2-y2 | -2.234 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.842 |
0.000 |
0.000 |
| y |
0.000 |
1.715 |
0.000 |
| z |
0.000 |
0.000 |
5.266 |
<r2> (average value of r
2) Å
2
| <r2> |
38.847 |
| (<r2>)1/2 |
6.233 |