Jump to
S1C2
Energy calculated at B97D3/6-31+G**
| | hartrees |
| Energy at 0K | -2777.984669 |
| Energy at 298.15K | -2777.988576 |
| HF Energy | -2777.984669 |
| Nuclear repulsion energy | 223.938242 |
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 B97D3/6-31+G**
| 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' |
1775 |
1744 |
377.45 |
|
|
|
| 2 |
A' |
830 |
816 |
134.69 |
|
|
|
| 3 |
A' |
541 |
532 |
110.14 |
|
|
|
| 4 |
A' |
342 |
336 |
58.61 |
|
|
|
| 5 |
A' |
196 |
193 |
0.17 |
|
|
|
| 6 |
A" |
189 |
186 |
0.11 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1936.2 cm
-1
Scaled (by 0.9828) Zero Point Vibrational Energy (zpe) 1902.9 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 B97D3/6-31+G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Br1 |
-0.746 |
-0.820 |
0.000 |
| O2 |
0.000 |
0.882 |
0.000 |
| N3 |
1.543 |
0.852 |
0.000 |
| O4 |
1.914 |
1.960 |
0.000 |
Atom - Atom Distances (Å)
| |
Br1 |
O2 |
N3 |
O4 |
| Br1 | | 1.8587 | 2.8348 | 3.8478 |
O2 | 1.8587 | | 1.5433 | 2.1964 | N3 | 2.8348 | 1.5433 | | 1.1687 | O4 | 3.8478 | 2.1964 | 1.1687 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br1 |
O2 |
N3 |
114.107 |
|
O2 |
N3 |
O4 |
108.925 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Br |
0.133 |
|
|
|
| 2 |
O |
-0.118 |
|
|
|
| 3 |
N |
-0.145 |
|
|
|
| 4 |
O |
0.130 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.176 |
-0.792 |
0.000 |
0.812 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-33.439 |
1.830 |
0.000 |
| y |
1.830 |
-33.573 |
0.000 |
| z |
0.000 |
0.000 |
-33.778 |
|
| Traceless |
| | x | y | z |
| x |
0.236 |
1.830 |
0.000 |
| y |
1.830 |
0.036 |
0.000 |
| z |
0.000 |
0.000 |
-0.272 |
|
| Polar |
| 3z2-r2 | -0.544 |
| x2-y2 | 0.134 |
| xy | 1.830 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.691 |
3.102 |
0.000 |
| y |
3.102 |
7.373 |
0.000 |
| z |
0.000 |
0.000 |
3.747 |
<r2> (average value of r
2) Å
2
| <r2> |
152.022 |
| (<r2>)1/2 |
12.330 |
Jump to
S1C1
Energy calculated at B97D3/6-31+G**
| | hartrees |
| Energy at 0K | -2777.997712 |
| Energy at 298.15K | -2778.001994 |
| HF Energy | -2777.997712 |
| Nuclear repulsion energy | 229.042265 |
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 B97D3/6-31+G**
| 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' |
1641 |
1613 |
311.41 |
|
|
|
| 2 |
A' |
982 |
965 |
84.79 |
|
|
|
| 3 |
A' |
775 |
761 |
84.90 |
|
|
|
| 4 |
A' |
321 |
315 |
60.57 |
|
|
|
| 5 |
A' |
145 |
143 |
4.12 |
|
|
|
| 6 |
A" |
471 |
463 |
2.03 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2167.4 cm
-1
Scaled (by 0.9828) Zero Point Vibrational Energy (zpe) 2130.1 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 B97D3/6-31+G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Br1 |
0.000 |
0.998 |
0.000 |
| O2 |
-0.902 |
-0.853 |
0.000 |
| N3 |
-0.156 |
-1.889 |
0.000 |
| O4 |
1.039 |
-1.859 |
0.000 |
Atom - Atom Distances (Å)
| |
Br1 |
O2 |
N3 |
O4 |
| Br1 | | 2.0587 | 2.8915 | 3.0400 |
O2 | 2.0587 | | 1.2772 | 2.1861 | N3 | 2.8915 | 1.2772 | | 1.1950 | O4 | 3.0400 | 2.1861 | 1.1950 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br1 |
O2 |
N3 |
119.865 |
|
O2 |
N3 |
O4 |
122.968 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Br |
0.007 |
|
|
|
| 2 |
O |
0.117 |
|
|
|
| 3 |
N |
-0.148 |
|
|
|
| 4 |
O |
0.024 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.124 |
-0.120 |
0.000 |
0.173 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-35.797 |
1.420 |
0.000 |
| y |
1.420 |
-32.536 |
0.000 |
| z |
0.000 |
0.000 |
-33.735 |
|
| Traceless |
| | x | y | z |
| x |
-2.662 |
1.420 |
0.000 |
| y |
1.420 |
2.230 |
0.000 |
| z |
0.000 |
0.000 |
0.432 |
|
| Polar |
| 3z2-r2 | 0.863 |
| x2-y2 | -3.261 |
| xy | 1.420 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.360 |
-0.476 |
0.000 |
| y |
-0.476 |
10.863 |
0.000 |
| z |
0.000 |
0.000 |
3.762 |
<r2> (average value of r
2) Å
2
| <r2> |
129.869 |
| (<r2>)1/2 |
11.396 |