Jump to
S1C2
S1C3
Energy calculated at wB97X-D/6-31+G**
| | hartrees |
| Energy at 0K | -280.133567 |
| Energy at 298.15K | |
| HF Energy | -280.133567 |
| Nuclear repulsion energy | 119.865634 |
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/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 |
A1 |
1229 |
1170 |
0.66 |
|
|
|
| 2 |
A1 |
986 |
939 |
21.29 |
|
|
|
| 3 |
A1 |
355 |
339 |
47.68 |
|
|
|
| 4 |
B1 |
805 |
766 |
12.60 |
|
|
|
| 5 |
B2 |
1333 |
1270 |
25.57 |
|
|
|
| 6 |
B2 |
294i |
280i |
11.86 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2206.9 cm
-1
Scaled (by 0.9523) Zero Point Vibrational Energy (zpe) 2101.6 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/6-31+G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
0.000 |
0.000 |
-0.091 |
| O2 |
0.000 |
0.000 |
1.255 |
| O3 |
0.000 |
1.092 |
-0.588 |
| O4 |
0.000 |
-1.092 |
-0.588 |
Atom - Atom Distances (Å)
| |
N1 |
O2 |
O3 |
O4 |
| N1 | | 1.3457 | 1.2001 | 1.2001 |
O2 | 1.3457 | | 2.1423 | 2.1423 | O3 | 1.2001 | 2.1423 | | 2.1845 | O4 | 1.2001 | 2.1423 | 2.1845 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O2 |
N1 |
O3 |
114.475 |
|
O2 |
N1 |
O4 |
114.475 |
| O3 |
N1 |
O4 |
131.050 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
0.093 |
|
|
|
| 2 |
O |
0.005 |
|
|
|
| 3 |
O |
-0.049 |
|
|
|
| 4 |
O |
-0.049 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
0.207 |
0.207 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.201 |
0.000 |
0.000 |
| y |
0.000 |
-23.054 |
0.000 |
| z |
0.000 |
0.000 |
-22.607 |
|
| Traceless |
| | x | y | z |
| x |
2.629 |
0.000 |
0.000 |
| y |
0.000 |
-1.650 |
0.000 |
| z |
0.000 |
0.000 |
-0.979 |
|
| Polar |
| 3z2-r2 | -1.958 |
| x2-y2 | 2.853 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.782 |
0.000 |
0.000 |
| y |
0.000 |
4.728 |
0.000 |
| z |
0.000 |
0.000 |
5.290 |
<r2> (average value of r
2) Å
2
| <r2> |
50.085 |
| (<r2>)1/2 |
7.077 |
Jump to
S1C1
S1C3
Energy calculated at wB97X-D/6-31+G**
| | hartrees |
| Energy at 0K | -280.133766 |
| Energy at 298.15K | -280.135622 |
| HF Energy | -280.133766 |
| Nuclear repulsion energy | 119.799114 |
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/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 |
A1 |
1524 |
1452 |
134.39 |
|
|
|
| 2 |
A1 |
1153 |
1098 |
3.58 |
|
|
|
| 3 |
A1 |
339 |
323 |
0.03 |
|
|
|
| 4 |
B1 |
799 |
761 |
13.13 |
|
|
|
| 5 |
B2 |
946 |
901 |
49.78 |
|
|
|
| 6 |
B2 |
390 |
372 |
71.87 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2575.7 cm
-1
Scaled (by 0.9523) Zero Point Vibrational Energy (zpe) 2452.9 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 wB97X-D/6-31+G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
0.000 |
0.000 |
0.068 |
| O2 |
0.000 |
0.000 |
1.268 |
| O3 |
0.000 |
1.024 |
-0.664 |
| O4 |
0.000 |
-1.024 |
-0.664 |
Atom - Atom Distances (Å)
| |
N1 |
O2 |
O3 |
O4 |
| N1 | | 1.2004 | 1.2583 | 1.2583 |
O2 | 1.2004 | | 2.1864 | 2.1864 | O3 | 1.2583 | 2.1864 | | 2.0480 | O4 | 1.2583 | 2.1864 | 2.0480 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O2 |
N1 |
O3 |
125.532 |
|
O2 |
N1 |
O4 |
125.532 |
| O3 |
N1 |
O4 |
108.936 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
0.099 |
|
|
|
| 2 |
O |
-0.071 |
|
|
|
| 3 |
O |
-0.014 |
|
|
|
| 4 |
O |
-0.014 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
-0.151 |
0.151 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.200 |
0.000 |
0.000 |
| y |
0.000 |
-22.452 |
0.000 |
| z |
0.000 |
0.000 |
-23.189 |
|
| Traceless |
| | x | y | z |
| x |
2.621 |
0.000 |
0.000 |
| y |
0.000 |
-0.758 |
0.000 |
| z |
0.000 |
0.000 |
-1.863 |
|
| Polar |
| 3z2-r2 | -3.726 |
| x2-y2 | 2.253 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.786 |
0.000 |
0.000 |
| y |
0.000 |
5.521 |
0.000 |
| z |
0.000 |
0.000 |
4.379 |
<r2> (average value of r
2) Å
2
| <r2> |
50.122 |
| (<r2>)1/2 |
7.080 |
Jump to
S1C1
S1C2
Energy calculated at wB97X-D/6-31+G**
| | hartrees |
| Energy at 0K | -280.133567 |
| Energy at 298.15K | |
| HF Energy | -280.133567 |
| Nuclear repulsion energy | 119.881058 |
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/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 |
A1 |
1227 |
1168 |
0.69 |
|
|
|
| 2 |
A1 |
991 |
944 |
20.99 |
|
|
|
| 3 |
A1 |
336 |
320 |
50.31 |
|
|
|
| 4 |
B1 |
805 |
766 |
12.60 |
|
|
|
| 5 |
B2 |
1326 |
1262 |
22.61 |
|
|
|
| 6 |
B2 |
297i |
283i |
12.99 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2193.4 cm
-1
Scaled (by 0.9523) Zero Point Vibrational Energy (zpe) 2088.8 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/6-31+G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
0.000 |
0.000 |
-0.091 |
| O2 |
0.000 |
0.000 |
1.252 |
| O3 |
0.000 |
1.094 |
-0.587 |
| O4 |
0.000 |
-1.094 |
-0.587 |
Atom - Atom Distances (Å)
| |
N1 |
O2 |
O3 |
O4 |
| N1 | | 1.3430 | 1.2016 | 1.2016 |
O2 | 1.3430 | | 2.1401 | 2.1401 | O3 | 1.2016 | 2.1401 | | 2.1890 | O4 | 1.2016 | 2.1401 | 2.1890 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O2 |
N1 |
O3 |
114.382 |
|
O2 |
N1 |
O4 |
114.382 |
| O3 |
N1 |
O4 |
131.237 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
0.093 |
|
|
|
| 2 |
O |
0.004 |
|
|
|
| 3 |
O |
-0.048 |
|
|
|
| 4 |
O |
-0.048 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
0.199 |
0.199 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.201 |
0.000 |
0.000 |
| y |
0.000 |
-23.046 |
0.000 |
| z |
0.000 |
0.000 |
-22.615 |
|
| Traceless |
| | x | y | z |
| x |
2.630 |
0.000 |
0.000 |
| y |
0.000 |
-1.638 |
0.000 |
| z |
0.000 |
0.000 |
-0.992 |
|
| Polar |
| 3z2-r2 | -1.984 |
| x2-y2 | 2.845 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.782 |
0.000 |
0.000 |
| y |
0.000 |
4.743 |
0.000 |
| z |
0.000 |
0.000 |
5.296 |
<r2> (average value of r
2) Å
2
| <r2> |
50.075 |
| (<r2>)1/2 |
7.076 |