Jump to
S1C2
Energy calculated at B3PW91/STO-3G
| | hartrees |
| Energy at 0K | -2584.782895 |
| Energy at 298.15K | -2584.786843 |
| HF Energy | -2584.782895 |
| Nuclear repulsion energy | 80.287998 |
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 B3PW91/STO-3G
| 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' |
3386 |
2997 |
0.75 |
|
|
|
| 2 |
A' |
1548 |
1370 |
22.80 |
|
|
|
| 3 |
A' |
814 |
721 |
22.53 |
|
|
|
| 4 |
A' |
431 |
381 |
32.17 |
|
|
|
| 5 |
A" |
3574 |
3163 |
0.07 |
|
|
|
| 6 |
A" |
1020 |
902 |
0.94 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5386.3 cm
-1
Scaled (by 0.885) Zero Point Vibrational Energy (zpe) 4766.9 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 B3PW91/STO-3G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.010 |
1.489 |
0.000 |
| Br2 |
-0.010 |
-0.370 |
0.000 |
| H3 |
0.197 |
2.006 |
0.944 |
| H4 |
0.197 |
2.006 |
-0.944 |
Atom - Atom Distances (Å)
| |
C1 |
Br2 |
H3 |
H4 |
| C1 | | 1.8593 | 1.0954 | 1.0954 |
Br2 | 1.8593 | | 2.5647 | 2.5647 | H3 | 1.0954 | 2.5647 | | 1.8874 | H4 | 1.0954 | 2.5647 | 1.8874 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br2 |
C1 |
H3 |
118.135 |
|
Br2 |
C1 |
H4 |
118.135 |
| H3 |
C1 |
H4 |
118.974 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.218 |
|
|
|
| 2 |
Br |
0.044 |
|
|
|
| 3 |
H |
0.087 |
|
|
|
| 4 |
H |
0.087 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.274 |
0.772 |
0.000 |
0.819 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.046 |
0.508 |
0.000 |
| y |
0.508 |
-21.245 |
0.000 |
| z |
0.000 |
0.000 |
-22.203 |
|
| Traceless |
| | x | y | z |
| x |
-1.322 |
0.508 |
0.000 |
| y |
0.508 |
1.380 |
0.000 |
| z |
0.000 |
0.000 |
-0.057 |
|
| Polar |
| 3z2-r2 | -0.115 |
| x2-y2 | -1.801 |
| xy | 0.508 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.437 |
0.072 |
0.000 |
| y |
0.072 |
2.947 |
0.000 |
| z |
0.000 |
0.000 |
0.899 |
<r2> (average value of r
2) Å
2
| <r2> |
41.853 |
| (<r2>)1/2 |
6.469 |
Jump to
S1C1
Energy calculated at B3PW91/STO-3G
| | hartrees |
| Energy at 0K | -2584.782645 |
| Energy at 298.15K | |
| HF Energy | -2584.782645 |
| Nuclear repulsion energy | 80.411337 |
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 B3PW91/STO-3G
| 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 |
3403 |
3012 |
0.96 |
36.39 |
0.13 |
0.23 |
| 2 |
A1 |
1539 |
1362 |
25.52 |
7.70 |
0.75 |
0.86 |
| 3 |
A1 |
806 |
713 |
21.44 |
6.05 |
0.34 |
0.51 |
| 4 |
B1 |
316i |
280i |
46.92 |
0.19 |
0.75 |
0.86 |
| 5 |
B2 |
3595 |
3181 |
0.02 |
27.98 |
0.75 |
0.86 |
| 6 |
B2 |
1000 |
885 |
0.78 |
4.52 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 5013.4 cm
-1
Scaled (by 0.885) Zero Point Vibrational Energy (zpe) 4436.9 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 B3PW91/STO-3G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.484 |
| Br2 |
0.000 |
0.000 |
0.370 |
| H3 |
0.000 |
0.950 |
-2.024 |
| H4 |
0.000 |
-0.950 |
-2.024 |
Atom - Atom Distances (Å)
| |
C1 |
Br2 |
H3 |
H4 |
| C1 | | 1.8539 | 1.0931 | 1.0931 |
Br2 | 1.8539 | | 2.5757 | 2.5757 | H3 | 1.0931 | 2.5757 | | 1.9006 | H4 | 1.0931 | 2.5757 | 1.9006 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br2 |
C1 |
H3 |
119.609 |
|
Br2 |
C1 |
H4 |
119.609 |
| H3 |
C1 |
H4 |
120.782 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.225 |
|
|
|
| 2 |
Br |
0.048 |
|
|
|
| 3 |
H |
0.088 |
|
|
|
| 4 |
H |
0.088 |
|
|
|
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 |
-0.775 |
0.775 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.110 |
0.000 |
0.000 |
| y |
0.000 |
-22.151 |
0.000 |
| z |
0.000 |
0.000 |
-21.145 |
|
| Traceless |
| | x | y | z |
| x |
-1.462 |
0.000 |
0.000 |
| y |
0.000 |
-0.024 |
0.000 |
| z |
0.000 |
0.000 |
1.486 |
|
| Polar |
| 3z2-r2 | 2.971 |
| x2-y2 | -0.959 |
| 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 |
0.421 |
0.000 |
0.000 |
| y |
0.000 |
0.896 |
0.000 |
| z |
0.000 |
0.000 |
2.915 |
<r2> (average value of r
2) Å
2
| <r2> |
41.828 |
| (<r2>)1/2 |
6.467 |