Jump to
S1C2
Energy calculated at B97D3/3-21G
| | hartrees |
| Energy at 0K | -2766.912999 |
| Energy at 298.15K | -2766.916902 |
| HF Energy | -2766.912999 |
| Nuclear repulsion energy | |
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 B97D3/3-21G
| 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' |
1414 |
1390 |
188.73 |
|
|
|
| 2 |
A' |
801 |
788 |
143.15 |
|
|
|
| 3 |
A' |
636 |
625 |
17.30 |
|
|
|
| 4 |
A' |
355 |
349 |
6.72 |
|
|
|
| 5 |
A' |
186 |
183 |
0.17 |
|
|
|
| 6 |
A" |
160 |
157 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1776.2 cm
-1
Scaled (by 0.983) Zero Point Vibrational Energy (zpe) 1746.0 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 B97D3/3-21G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Br1 |
-0.794 |
-0.801 |
0.000 |
| O2 |
0.000 |
0.927 |
0.000 |
| N3 |
1.604 |
0.775 |
0.000 |
| O4 |
2.068 |
1.899 |
0.000 |
Atom - Atom Distances (Å)
| |
Br1 |
O2 |
N3 |
O4 |
| Br1 | | 1.9016 | 2.8693 | 3.9343 |
O2 | 1.9016 | | 1.6114 | 2.2852 | N3 | 2.8693 | 1.6114 | | 1.2158 | O4 | 3.9343 | 2.2852 | 1.2158 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br1 |
O2 |
N3 |
113.642 |
|
O2 |
N3 |
O4 |
109.840 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Br |
0.222 |
|
|
|
| 2 |
O |
-0.315 |
|
|
|
| 3 |
N |
0.294 |
|
|
|
| 4 |
O |
-0.200 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.090 |
-1.079 |
0.000 |
1.082 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.894 |
0.961 |
0.000 |
| y |
0.961 |
-33.374 |
0.000 |
| z |
0.000 |
0.000 |
-32.629 |
|
| Traceless |
| | x | y | z |
| x |
0.108 |
0.961 |
0.000 |
| y |
0.961 |
-0.613 |
0.000 |
| z |
0.000 |
0.000 |
0.505 |
|
| Polar |
| 3z2-r2 | 1.010 |
| x2-y2 | 0.480 |
| xy | 0.961 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.676 |
3.398 |
0.000 |
| y |
3.398 |
5.237 |
0.000 |
| z |
0.000 |
0.000 |
1.101 |
<r2> (average value of r
2) Å
2
| <r2> |
157.244 |
| (<r2>)1/2 |
12.540 |
Jump to
S1C1
Energy calculated at B97D3/3-21G
| | hartrees |
| Energy at 0K | -2766.923884 |
| Energy at 298.15K | -2766.928029 |
| HF Energy | -2766.923884 |
| Nuclear repulsion energy | |
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 B97D3/3-21G
| 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' |
1353 |
1330 |
178.62 |
|
|
|
| 2 |
A' |
751 |
738 |
1.53 |
|
|
|
| 3 |
A' |
552 |
542 |
24.37 |
|
|
|
| 4 |
A' |
444 |
437 |
14.08 |
|
|
|
| 5 |
A' |
155 |
152 |
0.42 |
|
|
|
| 6 |
A" |
372 |
365 |
1.44 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1813.1 cm
-1
Scaled (by 0.983) Zero Point Vibrational Energy (zpe) 1782.2 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 B97D3/3-21G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Br1 |
0.000 |
0.968 |
0.000 |
| O2 |
-0.962 |
-0.710 |
0.000 |
| N3 |
-0.137 |
-1.956 |
0.000 |
| O4 |
1.082 |
-1.812 |
0.000 |
Atom - Atom Distances (Å)
| |
Br1 |
O2 |
N3 |
O4 |
| Br1 | | 1.9340 | 2.9266 | 2.9832 |
O2 | 1.9340 | | 1.4937 | 2.3223 | N3 | 2.9266 | 1.4937 | | 1.2280 | O4 | 2.9832 | 2.3223 | 1.2280 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br1 |
O2 |
N3 |
120.639 |
|
O2 |
N3 |
O4 |
124.454 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Br |
0.181 |
|
|
|
| 2 |
O |
-0.279 |
|
|
|
| 3 |
N |
0.312 |
|
|
|
| 4 |
O |
-0.214 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.404 |
0.627 |
0.000 |
0.746 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-35.237 |
0.789 |
0.000 |
| y |
0.789 |
-32.040 |
0.000 |
| z |
0.000 |
0.000 |
-32.655 |
|
| Traceless |
| | x | y | z |
| x |
-2.890 |
0.789 |
0.000 |
| y |
0.789 |
1.906 |
0.000 |
| z |
0.000 |
0.000 |
0.984 |
|
| Polar |
| 3z2-r2 | 1.967 |
| x2-y2 | -3.198 |
| xy | 0.789 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.133 |
-0.284 |
0.000 |
| y |
-0.284 |
7.380 |
0.000 |
| z |
0.000 |
0.000 |
1.099 |
<r2> (average value of r
2) Å
2
| <r2> |
127.567 |
| (<r2>)1/2 |
11.295 |