Jump to
S1C2
Energy calculated at HF/Def2TZVPP
| | hartrees |
| Energy at 0K | -2776.506550 |
| Energy at 298.15K | -2776.510920 |
| HF Energy | -2776.506550 |
| Nuclear repulsion energy | 237.201269 |
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/Def2TZVPP
| 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' |
2026 |
1836 |
299.75 |
|
|
|
| 2 |
A' |
1013 |
918 |
205.03 |
|
|
|
| 3 |
A' |
900 |
816 |
501.51 |
|
|
|
| 4 |
A' |
521 |
472 |
1.51 |
|
|
|
| 5 |
A' |
295 |
268 |
0.49 |
|
|
|
| 6 |
A" |
163 |
148 |
0.13 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2458.9 cm
-1
Scaled (by 0.9064) Zero Point Vibrational Energy (zpe) 2228.8 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 HF/Def2TZVPP
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Br1 |
-0.684 |
-0.789 |
0.000 |
| O2 |
0.000 |
0.854 |
0.000 |
| N3 |
1.374 |
0.823 |
0.000 |
| O4 |
1.792 |
1.878 |
0.000 |
Atom - Atom Distances (Å)
| |
Br1 |
O2 |
N3 |
O4 |
| Br1 | | 1.7798 | 2.6144 | 3.6396 |
O2 | 1.7798 | | 1.3742 | 2.0642 | N3 | 2.6144 | 1.3742 | | 1.1351 | O4 | 3.6396 | 2.0642 | 1.1351 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br1 |
O2 |
N3 |
111.321 |
|
O2 |
N3 |
O4 |
110.331 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/Def2TZVPP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Br |
0.162 |
|
|
|
| 2 |
O |
-0.235 |
|
|
|
| 3 |
N |
0.329 |
|
|
|
| 4 |
O |
-0.256 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.467 |
-1.397 |
0.000 |
1.473 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-34.839 |
0.618 |
0.000 |
| y |
0.618 |
-34.539 |
0.000 |
| z |
0.000 |
0.000 |
-33.388 |
|
| Traceless |
| | x | y | z |
| x |
-0.876 |
0.618 |
0.000 |
| y |
0.618 |
-0.425 |
0.000 |
| z |
0.000 |
0.000 |
1.301 |
|
| Polar |
| 3z2-r2 | 2.601 |
| x2-y2 | -0.301 |
| xy | 0.618 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.508 |
2.177 |
0.000 |
| y |
2.177 |
6.192 |
0.000 |
| z |
0.000 |
0.000 |
3.240 |
<r2> (average value of r
2) Å
2
| <r2> |
137.834 |
| (<r2>)1/2 |
11.740 |
Jump to
S1C1
Energy calculated at HF/Def2TZVPP
| | hartrees |
| Energy at 0K | -2776.509767 |
| Energy at 298.15K | -2776.514398 |
| HF Energy | -2776.509767 |
| Nuclear repulsion energy | 247.158581 |
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/Def2TZVPP
| 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' |
1978 |
1793 |
303.84 |
|
|
|
| 2 |
A' |
1014 |
919 |
155.00 |
|
|
|
| 3 |
A' |
871 |
789 |
197.96 |
|
|
|
| 4 |
A' |
650 |
589 |
2.66 |
|
|
|
| 5 |
A' |
255 |
231 |
0.48 |
|
|
|
| 6 |
A" |
344 |
312 |
2.02 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2555.7 cm
-1
Scaled (by 0.9064) Zero Point Vibrational Energy (zpe) 2316.5 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/Def2TZVPP
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Br1 |
0.000 |
0.903 |
0.000 |
| O2 |
-0.863 |
-0.676 |
0.000 |
| N3 |
-0.145 |
-1.805 |
0.000 |
| O4 |
0.989 |
-1.697 |
0.000 |
Atom - Atom Distances (Å)
| |
Br1 |
O2 |
N3 |
O4 |
| Br1 | | 1.8000 | 2.7119 | 2.7821 |
O2 | 1.8000 | | 1.3373 | 2.1143 | N3 | 2.7119 | 1.3373 | | 1.1388 | O4 | 2.7821 | 2.1143 | 1.1388 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br1 |
O2 |
N3 |
118.889 |
|
O2 |
N3 |
O4 |
117.050 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/Def2TZVPP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Br |
0.146 |
|
|
|
| 2 |
O |
-0.226 |
|
|
|
| 3 |
N |
0.370 |
|
|
|
| 4 |
O |
-0.290 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.219 |
0.927 |
0.000 |
0.953 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-36.064 |
1.240 |
0.000 |
| y |
1.240 |
-32.913 |
0.000 |
| z |
0.000 |
0.000 |
-33.390 |
|
| Traceless |
| | x | y | z |
| x |
-2.912 |
1.240 |
0.000 |
| y |
1.240 |
1.813 |
0.000 |
| z |
0.000 |
0.000 |
1.099 |
|
| Polar |
| 3z2-r2 | 2.198 |
| x2-y2 | -3.151 |
| xy | 1.240 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.468 |
-0.104 |
0.000 |
| y |
-0.104 |
7.058 |
0.000 |
| z |
0.000 |
0.000 |
3.220 |
<r2> (average value of r
2) Å
2
| <r2> |
113.766 |
| (<r2>)1/2 |
10.666 |