Jump to
S1C2
Energy calculated at wB97X-D/cc-pVDZ
| | hartrees |
| Energy at 0K | -2776.730159 |
| Energy at 298.15K | -2776.734359 |
| HF Energy | -2776.730159 |
| Nuclear repulsion energy | 230.324898 |
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 wB97X-D/cc-pVDZ
| 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' |
1847 |
1760 |
295.60 |
|
|
|
| 2 |
A' |
913 |
869 |
221.63 |
|
|
|
| 3 |
A' |
707 |
674 |
317.63 |
|
|
|
| 4 |
A' |
441 |
420 |
13.82 |
|
|
|
| 5 |
A' |
243 |
232 |
0.00 |
|
|
|
| 6 |
A" |
193 |
184 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2171.7 cm
-1
Scaled (by 0.9526) Zero Point Vibrational Energy (zpe) 2068.7 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 wB97X-D/cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Br1 |
-0.690 |
-0.830 |
0.000 |
| O2 |
0.000 |
0.872 |
0.000 |
| N3 |
1.412 |
0.881 |
0.000 |
| O4 |
1.784 |
1.987 |
0.000 |
Atom - Atom Distances (Å)
| |
Br1 |
O2 |
N3 |
O4 |
| Br1 | | 1.8364 | 2.7098 | 3.7493 |
O2 | 1.8364 | | 1.4115 | 2.1040 | N3 | 2.7098 | 1.4115 | | 1.1674 | O4 | 3.7493 | 2.1040 | 1.1674 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br1 |
O2 |
N3 |
112.434 |
|
O2 |
N3 |
O4 |
108.973 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Br |
0.165 |
|
|
|
| 2 |
O |
-0.122 |
|
|
|
| 3 |
N |
-0.084 |
|
|
|
| 4 |
O |
0.041 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.307 |
-1.208 |
0.000 |
1.246 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-34.462 |
1.153 |
0.000 |
| y |
1.153 |
-34.210 |
0.000 |
| z |
0.000 |
0.000 |
-33.707 |
|
| Traceless |
| | x | y | z |
| x |
-0.503 |
1.153 |
0.000 |
| y |
1.153 |
-0.126 |
0.000 |
| z |
0.000 |
0.000 |
0.629 |
|
| Polar |
| 3z2-r2 | 1.258 |
| x2-y2 | -0.252 |
| xy | 1.153 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.508 |
2.561 |
0.000 |
| y |
2.561 |
6.851 |
0.000 |
| z |
0.000 |
0.000 |
3.574 |
<r2> (average value of r
2) Å
2
| <r2> |
144.452 |
| (<r2>)1/2 |
12.019 |
Jump to
S1C1
Energy calculated at wB97X-D/cc-pVDZ
| | hartrees |
| Energy at 0K | -2776.737926 |
| Energy at 298.15K | -2776.742432 |
| HF Energy | -2776.737926 |
| Nuclear repulsion energy | 240.906595 |
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 wB97X-D/cc-pVDZ
| 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' |
1774 |
1690 |
310.10 |
|
|
|
| 2 |
A' |
886 |
844 |
1.11 |
|
|
|
| 3 |
A' |
771 |
734 |
126.09 |
|
|
|
| 4 |
A' |
510 |
486 |
5.08 |
|
|
|
| 5 |
A' |
219 |
208 |
0.10 |
|
|
|
| 6 |
A" |
413 |
394 |
1.61 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2286.2 cm
-1
Scaled (by 0.9526) Zero Point Vibrational Energy (zpe) 2177.8 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 wB97X-D/cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Br1 |
0.000 |
0.934 |
0.000 |
| O2 |
-0.894 |
-0.708 |
0.000 |
| N3 |
-0.146 |
-1.844 |
0.000 |
| O4 |
1.022 |
-1.766 |
0.000 |
Atom - Atom Distances (Å)
| |
Br1 |
O2 |
N3 |
O4 |
| Br1 | | 1.8700 | 2.7816 | 2.8870 |
O2 | 1.8700 | | 1.3593 | 2.1886 | N3 | 2.7816 | 1.3593 | | 1.1711 | O4 | 2.8870 | 2.1886 | 1.1711 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br1 |
O2 |
N3 |
118.076 |
|
O2 |
N3 |
O4 |
119.558 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Br |
0.137 |
|
|
|
| 2 |
O |
-0.008 |
|
|
|
| 3 |
N |
-0.124 |
|
|
|
| 4 |
O |
-0.006 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.163 |
0.874 |
0.000 |
0.889 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-36.086 |
1.217 |
0.000 |
| y |
1.217 |
-33.009 |
0.000 |
| z |
0.000 |
0.000 |
-33.654 |
|
| Traceless |
| | x | y | z |
| x |
-2.755 |
1.217 |
0.000 |
| y |
1.217 |
1.861 |
0.000 |
| z |
0.000 |
0.000 |
0.894 |
|
| Polar |
| 3z2-r2 | 1.788 |
| x2-y2 | -3.077 |
| xy | 1.217 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.972 |
-0.328 |
0.000 |
| y |
-0.328 |
8.546 |
0.000 |
| z |
0.000 |
0.000 |
3.557 |
<r2> (average value of r
2) Å
2
| <r2> |
117.742 |
| (<r2>)1/2 |
10.851 |