Jump to
S1C2
Energy calculated at B97D3/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -2780.558699 |
| Energy at 298.15K | -2780.562592 |
| HF Energy | -2780.558699 |
| Nuclear repulsion energy | 225.137622 |
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/aug-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' |
1789 |
1762 |
425.75 |
|
|
|
| 2 |
A' |
821 |
809 |
116.77 |
|
|
|
| 3 |
A' |
551 |
543 |
116.05 |
|
|
|
| 4 |
A' |
342 |
337 |
69.03 |
|
|
|
| 5 |
A' |
202 |
199 |
0.29 |
|
|
|
| 6 |
A" |
164 |
161 |
0.09 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1935.0 cm
-1
Scaled (by 0.9847) Zero Point Vibrational Energy (zpe) 1905.4 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/aug-cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Br1 |
-0.771 |
-0.784 |
0.000 |
| O2 |
0.000 |
0.884 |
0.000 |
| N3 |
1.572 |
0.787 |
0.000 |
| O4 |
1.999 |
1.856 |
0.000 |
Atom - Atom Distances (Å)
| |
Br1 |
O2 |
N3 |
O4 |
| Br1 | | 1.8372 | 2.8205 | 3.8263 |
O2 | 1.8372 | | 1.5746 | 2.2227 | N3 | 2.8205 | 1.5746 | | 1.1513 | O4 | 3.8263 | 2.2227 | 1.1513 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br1 |
O2 |
N3 |
111.286 |
|
O2 |
N3 |
O4 |
108.249 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Br |
0.297 |
|
|
|
| 2 |
O |
-0.431 |
|
|
|
| 3 |
N |
0.332 |
|
|
|
| 4 |
O |
-0.198 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.444 |
-0.484 |
0.000 |
0.657 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.833 |
1.914 |
0.000 |
| y |
1.914 |
-33.403 |
0.000 |
| z |
0.000 |
0.000 |
-33.618 |
|
| Traceless |
| | x | y | z |
| x |
0.677 |
1.914 |
0.000 |
| y |
1.914 |
-0.178 |
0.000 |
| z |
0.000 |
0.000 |
-0.499 |
|
| Polar |
| 3z2-r2 | -0.998 |
| x2-y2 | 0.570 |
| xy | 1.914 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
8.683 |
2.842 |
0.000 |
| y |
2.842 |
7.704 |
0.000 |
| z |
0.000 |
0.000 |
4.661 |
<r2> (average value of r
2) Å
2
| <r2> |
150.490 |
| (<r2>)1/2 |
12.267 |
Jump to
S1C1
Energy calculated at B97D3/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -2780.570136 |
| Energy at 298.15K | -2780.574376 |
| HF Energy | -2780.570136 |
| Nuclear repulsion energy | 229.029735 |
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/aug-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' |
1627 |
1602 |
305.85 |
|
|
|
| 2 |
A' |
990 |
975 |
77.45 |
|
|
|
| 3 |
A' |
768 |
757 |
98.83 |
|
|
|
| 4 |
A' |
287 |
282 |
62.15 |
|
|
|
| 5 |
A' |
140 |
138 |
7.17 |
|
|
|
| 6 |
A" |
469 |
462 |
1.54 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2140.7 cm
-1
Scaled (by 0.9847) Zero Point Vibrational Energy (zpe) 2107.9 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/aug-cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Br1 |
0.000 |
1.001 |
0.000 |
| O2 |
-0.899 |
-0.865 |
0.000 |
| N3 |
-0.152 |
-1.884 |
0.000 |
| O4 |
1.032 |
-1.868 |
0.000 |
Atom - Atom Distances (Å)
| |
Br1 |
O2 |
N3 |
O4 |
| Br1 | | 2.0715 | 2.8894 | 3.0492 |
O2 | 2.0715 | | 1.2635 | 2.1760 | N3 | 2.8894 | 1.2635 | | 1.1844 | O4 | 3.0492 | 2.1760 | 1.1844 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br1 |
O2 |
N3 |
118.049 |
|
O2 |
N3 |
O4 |
125.448 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Br |
0.045 |
|
|
|
| 2 |
O |
-0.186 |
|
|
|
| 3 |
N |
0.390 |
|
|
|
| 4 |
O |
-0.249 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.183 |
-0.347 |
0.000 |
0.393 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-35.450 |
1.344 |
0.000 |
| y |
1.344 |
-32.430 |
0.000 |
| z |
0.000 |
0.000 |
-33.588 |
|
| Traceless |
| | x | y | z |
| x |
-2.441 |
1.344 |
0.000 |
| y |
1.344 |
2.089 |
0.000 |
| z |
0.000 |
0.000 |
0.352 |
|
| Polar |
| 3z2-r2 | 0.704 |
| x2-y2 | -3.020 |
| xy | 1.344 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.104 |
-0.500 |
0.000 |
| y |
-0.500 |
11.568 |
0.000 |
| z |
0.000 |
0.000 |
4.744 |
<r2> (average value of r
2) Å
2
| <r2> |
130.113 |
| (<r2>)1/2 |
11.407 |