Jump to
S1C2
Energy calculated at wB97X-D/cc-pVTZ
| | hartrees |
| Energy at 0K | -2779.320722 |
| Energy at 298.15K | -2779.324890 |
| HF Energy | -2779.320722 |
| Nuclear repulsion energy | 231.626572 |
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-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' |
1850 |
1768 |
306.73 |
|
|
|
| 2 |
A' |
911 |
871 |
169.09 |
|
|
|
| 3 |
A' |
680 |
650 |
344.51 |
|
|
|
| 4 |
A' |
444 |
425 |
32.41 |
|
|
|
| 5 |
A' |
250 |
239 |
0.01 |
|
|
|
| 6 |
A" |
170 |
162 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2151.9 cm
-1
Scaled (by 0.956) Zero Point Vibrational Energy (zpe) 2057.3 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-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Br1 |
-0.697 |
-0.810 |
0.000 |
| O2 |
0.000 |
0.874 |
0.000 |
| N3 |
1.410 |
0.845 |
0.000 |
| O4 |
1.815 |
1.930 |
0.000 |
Atom - Atom Distances (Å)
| |
Br1 |
O2 |
N3 |
O4 |
| Br1 | | 1.8220 | 2.6794 | 3.7169 |
O2 | 1.8220 | | 1.4105 | 2.1000 | N3 | 2.6794 | 1.4105 | | 1.1577 | O4 | 3.7169 | 2.1000 | 1.1577 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br1 |
O2 |
N3 |
111.332 |
|
O2 |
N3 |
O4 |
109.310 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Br |
0.153 |
|
|
|
| 2 |
O |
-0.253 |
|
|
|
| 3 |
N |
0.167 |
|
|
|
| 4 |
O |
-0.068 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.111 |
-0.944 |
0.000 |
0.950 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-33.839 |
1.224 |
0.000 |
| y |
1.224 |
-33.538 |
0.000 |
| z |
0.000 |
0.000 |
-33.309 |
|
| Traceless |
| | x | y | z |
| x |
-0.415 |
1.224 |
0.000 |
| y |
1.224 |
0.035 |
0.000 |
| z |
0.000 |
0.000 |
0.380 |
|
| Polar |
| 3z2-r2 | 0.759 |
| x2-y2 | -0.300 |
| xy | 1.224 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.262 |
2.540 |
0.000 |
| y |
2.540 |
6.250 |
0.000 |
| z |
0.000 |
0.000 |
3.147 |
<r2> (average value of r
2) Å
2
| <r2> |
142.597 |
| (<r2>)1/2 |
11.941 |
Jump to
S1C1
Energy calculated at wB97X-D/cc-pVTZ
| | hartrees |
| Energy at 0K | -2779.328107 |
| Energy at 298.15K | -2779.332578 |
| HF Energy | -2779.328107 |
| Nuclear repulsion energy | 242.084015 |
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-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' |
1766 |
1688 |
293.00 |
|
|
|
| 2 |
A' |
891 |
852 |
0.85 |
|
|
|
| 3 |
A' |
715 |
684 |
122.69 |
|
|
|
| 4 |
A' |
505 |
483 |
10.60 |
|
|
|
| 5 |
A' |
218 |
208 |
0.01 |
|
|
|
| 6 |
A" |
399 |
382 |
1.33 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2246.6 cm
-1
Scaled (by 0.956) Zero Point Vibrational Energy (zpe) 2147.8 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-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Br1 |
0.000 |
0.928 |
0.000 |
| O2 |
-0.891 |
-0.701 |
0.000 |
| N3 |
-0.143 |
-1.832 |
0.000 |
| O4 |
1.016 |
-1.756 |
0.000 |
Atom - Atom Distances (Å)
| |
Br1 |
O2 |
N3 |
O4 |
| Br1 | | 1.8568 | 2.7637 | 2.8702 |
O2 | 1.8568 | | 1.3563 | 2.1803 | N3 | 2.7637 | 1.3563 | | 1.1619 | O4 | 2.8702 | 2.1803 | 1.1619 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br1 |
O2 |
N3 |
117.819 |
|
O2 |
N3 |
O4 |
119.750 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Br |
0.111 |
|
|
|
| 2 |
O |
-0.193 |
|
|
|
| 3 |
N |
0.211 |
|
|
|
| 4 |
O |
-0.129 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.178 |
0.721 |
0.000 |
0.743 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-35.535 |
1.145 |
0.000 |
| y |
1.145 |
-32.600 |
0.000 |
| z |
0.000 |
0.000 |
-33.278 |
|
| Traceless |
| | x | y | z |
| x |
-2.595 |
1.145 |
0.000 |
| y |
1.145 |
1.806 |
0.000 |
| z |
0.000 |
0.000 |
0.789 |
|
| Polar |
| 3z2-r2 | 1.579 |
| x2-y2 | -2.934 |
| xy | 1.145 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.568 |
-0.329 |
0.000 |
| y |
-0.329 |
8.093 |
0.000 |
| z |
0.000 |
0.000 |
3.125 |
<r2> (average value of r
2) Å
2
| <r2> |
116.714 |
| (<r2>)1/2 |
10.803 |