Jump to
S1C2
S1C3
Energy calculated at wB97X-D/3-21G*
| | hartrees |
| Energy at 0K | -278.532794 |
| Energy at 298.15K | -278.534508 |
| HF Energy | -278.532794 |
| Nuclear repulsion energy | 112.962024 |
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/3-21G*
| 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 |
1148 |
1088 |
71.99 |
|
|
|
| 2 |
A1 |
770 |
730 |
31.70 |
|
|
|
| 3 |
A1 |
537 |
509 |
0.48 |
|
|
|
| 4 |
B1 |
668 |
633 |
13.42 |
|
|
|
| 5 |
B2 |
1420 |
1346 |
168.01 |
|
|
|
| 6 |
B2 |
217 |
206 |
7.57 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2379.5 cm
-1
Scaled (by 0.9478) Zero Point Vibrational Energy (zpe) 2255.3 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/3-21G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
0.000 |
0.000 |
-0.105 |
| O2 |
0.000 |
0.000 |
1.315 |
| O3 |
0.000 |
1.122 |
-0.611 |
| O4 |
0.000 |
-1.122 |
-0.611 |
Atom - Atom Distances (Å)
| |
N1 |
O2 |
O3 |
O4 |
| N1 | | 1.4193 | 1.2314 | 1.2314 |
O2 | 1.4193 | | 2.2291 | 2.2291 | O3 | 1.2314 | 2.2291 | | 2.2445 | O4 | 1.2314 | 2.2291 | 2.2445 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O2 |
N1 |
O3 |
114.303 |
|
O2 |
N1 |
O4 |
114.303 |
| O3 |
N1 |
O4 |
131.394 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C3
Energy calculated at wB97X-D/3-21G*
| | hartrees |
| Energy at 0K | -278.532082 |
| Energy at 298.15K | |
| HF Energy | -278.532082 |
| Nuclear repulsion energy | 114.478914 |
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/3-21G*
| 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 |
1466 |
1389 |
180.12 |
|
|
|
| 2 |
A1 |
953 |
903 |
1.46 |
|
|
|
| 3 |
A1 |
498 |
472 |
9.41 |
|
|
|
| 4 |
B1 |
655 |
621 |
15.09 |
|
|
|
| 5 |
B2 |
585 |
554 |
2.37 |
|
|
|
| 6 |
B2 |
133i |
126i |
132.86 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2011.9 cm
-1
Scaled (by 0.9478) Zero Point Vibrational Energy (zpe) 1906.8 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/3-21G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
0.000 |
0.000 |
0.086 |
| O2 |
0.000 |
0.000 |
1.327 |
| O3 |
0.000 |
1.054 |
-0.701 |
| O4 |
0.000 |
-1.054 |
-0.701 |
Atom - Atom Distances (Å)
| |
N1 |
O2 |
O3 |
O4 |
| N1 | | 1.2410 | 1.3157 | 1.3157 |
O2 | 1.2410 | | 2.2857 | 2.2857 | O3 | 1.3157 | 2.2857 | | 2.1088 | O4 | 1.3157 | 2.2857 | 2.1088 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O2 |
N1 |
O3 |
126.736 |
|
O2 |
N1 |
O4 |
126.736 |
| O3 |
N1 |
O4 |
106.528 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
0.534 |
|
|
|
| 2 |
O |
-0.256 |
|
|
|
| 3 |
O |
-0.139 |
|
|
|
| 4 |
O |
-0.139 |
|
|
|
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 |
0.095 |
0.095 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.753 |
0.000 |
0.000 |
| y |
0.000 |
-21.619 |
0.000 |
| z |
0.000 |
0.000 |
-23.097 |
|
| Traceless |
| | x | y | z |
| x |
2.605 |
0.000 |
0.000 |
| y |
0.000 |
-0.193 |
0.000 |
| z |
0.000 |
0.000 |
-2.411 |
|
| Polar |
| 3z2-r2 | -4.823 |
| x2-y2 | 1.865 |
| 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 |
0.625 |
0.000 |
0.000 |
| y |
0.000 |
4.285 |
0.000 |
| z |
0.000 |
0.000 |
3.329 |
<r2> (average value of r
2) Å
2
| <r2> |
53.326 |
| (<r2>)1/2 |
7.302 |
Jump to
S1C1
S1C2
Energy calculated at wB97X-D/3-21G*
| | hartrees |
| Energy at 0K | -278.532794 |
| Energy at 298.15K | -278.534508 |
| HF Energy | -278.532794 |
| Nuclear repulsion energy | 112.959818 |
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/3-21G*
| 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 |
1148 |
1088 |
71.99 |
|
|
|
| 2 |
A1 |
770 |
730 |
31.74 |
|
|
|
| 3 |
A1 |
537 |
509 |
0.48 |
|
|
|
| 4 |
B1 |
668 |
633 |
13.42 |
|
|
|
| 5 |
B2 |
1420 |
1346 |
168.09 |
|
|
|
| 6 |
B2 |
218 |
206 |
7.56 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2379.8 cm
-1
Scaled (by 0.9478) Zero Point Vibrational Energy (zpe) 2255.6 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/3-21G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
0.000 |
0.000 |
-0.104 |
| O2 |
0.000 |
0.000 |
1.314 |
| O3 |
0.000 |
1.127 |
-0.611 |
| O4 |
0.000 |
-1.127 |
-0.611 |
Atom - Atom Distances (Å)
| |
N1 |
O2 |
O3 |
O4 |
| N1 | | 1.4184 | 1.2359 | 1.2359 |
O2 | 1.4184 | | 2.2309 | 2.2309 | O3 | 1.2359 | 2.2309 | | 2.2545 | O4 | 1.2359 | 2.2309 | 2.2545 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O2 |
N1 |
O3 |
114.206 |
|
O2 |
N1 |
O4 |
114.206 |
| O3 |
N1 |
O4 |
131.588 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
0.539 |
|
|
|
| 2 |
O |
-0.043 |
|
|
|
| 3 |
O |
-0.248 |
|
|
|
| 4 |
O |
-0.248 |
|
|
|
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 |
0.567 |
0.567 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.757 |
0.000 |
0.000 |
| y |
0.000 |
-22.930 |
0.000 |
| z |
0.000 |
0.000 |
-21.757 |
|
| Traceless |
| | x | y | z |
| x |
2.586 |
0.000 |
0.000 |
| y |
0.000 |
-2.172 |
0.000 |
| z |
0.000 |
0.000 |
-0.414 |
|
| Polar |
| 3z2-r2 | -0.828 |
| x2-y2 | 3.172 |
| 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 |
0.621 |
0.000 |
0.000 |
| y |
0.000 |
3.322 |
0.000 |
| z |
0.000 |
0.000 |
3.077 |
<r2> (average value of r
2) Å
2
| <r2> |
54.602 |
| (<r2>)1/2 |
7.389 |