Jump to
S1C2
Energy calculated at B97D3/cc-pVTZ
| | hartrees |
| Energy at 0K | -2780.553424 |
| Energy at 298.15K | -2780.557329 |
| HF Energy | -2780.553424 |
| Nuclear repulsion energy | 225.190779 |
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/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' |
1795 |
1770 |
404.37 |
|
|
|
| 2 |
A' |
827 |
815 |
120.88 |
|
|
|
| 3 |
A' |
556 |
548 |
106.78 |
|
|
|
| 4 |
A' |
346 |
341 |
60.26 |
|
|
|
| 5 |
A' |
203 |
200 |
0.21 |
|
|
|
| 6 |
A" |
166 |
164 |
0.08 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1946.0 cm
-1
Scaled (by 0.986) Zero Point Vibrational Energy (zpe) 1918.8 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 B97D3/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Br1 |
-0.769 |
-0.785 |
0.000 |
| O2 |
0.000 |
0.885 |
0.000 |
| N3 |
1.569 |
0.789 |
0.000 |
| O4 |
1.992 |
1.860 |
0.000 |
Atom - Atom Distances (Å)
| |
Br1 |
O2 |
N3 |
O4 |
| Br1 | | 1.8383 | 2.8183 | 3.8240 |
O2 | 1.8383 | | 1.5717 | 2.2183 | N3 | 2.8183 | 1.5717 | | 1.1522 | O4 | 3.8240 | 2.2183 | 1.1522 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br1 |
O2 |
N3 |
112.903 |
|
O2 |
N3 |
O4 |
109.084 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Br |
0.138 |
|
|
|
| 2 |
O |
-0.271 |
|
|
|
| 3 |
N |
0.143 |
|
|
|
| 4 |
O |
-0.010 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.444 |
-0.514 |
0.000 |
0.679 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.603 |
1.885 |
0.000 |
| y |
1.885 |
-32.909 |
0.000 |
| z |
0.000 |
0.000 |
-33.321 |
|
| Traceless |
| | x | y | z |
| x |
0.512 |
1.885 |
0.000 |
| y |
1.885 |
0.053 |
0.000 |
| z |
0.000 |
0.000 |
-0.565 |
|
| Polar |
| 3z2-r2 | -1.130 |
| x2-y2 | 0.306 |
| xy | 1.885 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.399 |
3.045 |
0.000 |
| y |
3.045 |
6.556 |
0.000 |
| z |
0.000 |
0.000 |
3.198 |
<r2> (average value of r
2) Å
2
| <r2> |
150.134 |
| (<r2>)1/2 |
12.253 |
Jump to
S1C1
Energy calculated at B97D3/cc-pVTZ
| | hartrees |
| Energy at 0K | -2780.566253 |
| Energy at 298.15K | -2780.570498 |
| HF Energy | -2780.566253 |
| Nuclear repulsion energy | 228.187536 |
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/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' |
1642 |
1619 |
295.89 |
|
|
|
| 2 |
A' |
1023 |
1009 |
92.91 |
|
|
|
| 3 |
A' |
771 |
761 |
107.32 |
|
|
|
| 4 |
A' |
284 |
280 |
65.18 |
|
|
|
| 5 |
A' |
140 |
138 |
7.27 |
|
|
|
| 6 |
A" |
473 |
466 |
1.84 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2166.4 cm
-1
Scaled (by 0.986) Zero Point Vibrational Energy (zpe) 2136.1 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/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Br1 |
0.000 |
1.007 |
0.000 |
| O2 |
-0.901 |
-0.878 |
0.000 |
| N3 |
-0.151 |
-1.887 |
0.000 |
| O4 |
1.033 |
-1.876 |
0.000 |
Atom - Atom Distances (Å)
| |
Br1 |
O2 |
N3 |
O4 |
| Br1 | | 2.0897 | 2.8978 | 3.0625 |
O2 | 2.0897 | | 1.2569 | 2.1764 | N3 | 2.8978 | 1.2569 | | 1.1842 | O4 | 3.0625 | 2.1764 | 1.1842 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br1 |
O2 |
N3 |
119.616 |
|
O2 |
N3 |
O4 |
123.325 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Br |
-0.049 |
|
|
|
| 2 |
O |
-0.101 |
|
|
|
| 3 |
N |
0.260 |
|
|
|
| 4 |
O |
-0.109 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.187 |
-0.571 |
0.000 |
0.601 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-35.196 |
1.434 |
0.000 |
| y |
1.434 |
-31.968 |
0.000 |
| z |
0.000 |
0.000 |
-33.365 |
|
| Traceless |
| | x | y | z |
| x |
-2.530 |
1.434 |
0.000 |
| y |
1.434 |
2.312 |
0.000 |
| z |
0.000 |
0.000 |
0.217 |
|
| Polar |
| 3z2-r2 | 0.435 |
| x2-y2 | -3.228 |
| xy | 1.434 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.801 |
-0.448 |
0.000 |
| y |
-0.448 |
10.576 |
0.000 |
| z |
0.000 |
0.000 |
3.210 |
<r2> (average value of r
2) Å
2
| <r2> |
130.865 |
| (<r2>)1/2 |
11.440 |