Jump to
S1C2
Energy calculated at HF/3-21G
| hartrees |
Energy at 0K | -166.678766 |
Energy at 298.15K | |
HF Energy | -166.678766 |
Nuclear repulsion energy | 59.005469 |
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 HF/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 |
Σ |
3704 |
3354 |
243.28 |
14.72 |
0.18 |
0.31 |
2 |
Σ |
2406 |
2179 |
94.06 |
63.57 |
0.26 |
0.41 |
3 |
Σ |
805 |
729 |
116.20 |
0.65 |
0.43 |
0.60 |
4 |
Π |
880 |
797 |
104.22 |
2.77 |
0.75 |
0.86 |
4 |
Π |
880 |
797 |
104.22 |
2.77 |
0.75 |
0.86 |
5 |
Π |
532 |
482 |
1.20 |
0.96 |
0.75 |
0.86 |
5 |
Π |
532 |
482 |
1.20 |
0.96 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4869.8 cm
-1
Scaled (by 0.9056) Zero Point Vibrational Energy (zpe) 4410.1 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 HF/3-21G
Point Group is C∞v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
0.000 |
0.000 |
1.229 |
N2 |
0.000 |
0.000 |
-0.060 |
C3 |
0.000 |
0.000 |
-1.195 |
H4 |
0.000 |
0.000 |
-2.243 |
Atom - Atom Distances (Å)
|
O1 |
N2 |
C3 |
H4 |
O1 | | 1.2885 | 2.4235 | 3.4722 |
N2 | 1.2885 | | 1.1350 | 2.1837 | C3 | 2.4235 | 1.1350 | | 1.0488 | H4 | 3.4722 | 2.1837 | 1.0488 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
N2 |
C3 |
180.000 |
|
N2 |
C3 |
H4 |
180.000 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/3-21G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
O |
-0.456 |
|
|
|
2 |
N |
-0.218 |
|
|
|
3 |
C |
0.264 |
|
|
|
4 |
H |
0.410 |
|
|
|
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 |
-4.755 |
4.755 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-16.639 |
0.000 |
0.000 |
y |
0.000 |
-16.639 |
0.000 |
z |
0.000 |
0.000 |
-13.772 |
|
Traceless |
| x | y | z |
x |
-1.434 |
0.000 |
0.000 |
y |
0.000 |
-1.434 |
0.000 |
z |
0.000 |
0.000 |
2.867 |
|
Polar |
3z2-r2 | 5.734 |
x2-y2 | 0.000 |
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 |
0.858 |
0.000 |
0.000 |
y |
0.000 |
0.858 |
0.000 |
z |
0.000 |
0.000 |
4.984 |
<r2> (average value of r
2) Å
2
<r2> |
35.496 |
(<r2>)1/2 |
5.958 |
Jump to
S1C1
Energy calculated at HF/3-21G
| hartrees |
Energy at 0K | -166.678765 |
Energy at 298.15K | -166.679804 |
HF Energy | -166.678765 |
Nuclear repulsion energy | 59.018531 |
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 HF/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 |
A' |
3702 |
3352 |
243.63 |
|
|
|
2 |
A' |
2407 |
2180 |
94.35 |
|
|
|
3 |
A' |
881 |
798 |
104.35 |
|
|
|
4 |
A' |
807 |
731 |
116.63 |
|
|
|
5 |
A' |
532 |
482 |
1.14 |
|
|
|
6 |
A" |
863 |
782 |
92.48 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4596.4 cm
-1
Scaled (by 0.9056) Zero Point Vibrational Energy (zpe) 4162.5 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 HF/3-21G
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
-0.014 |
-1.228 |
0.000 |
N2 |
0.000 |
0.060 |
0.000 |
C3 |
0.014 |
1.194 |
0.000 |
H4 |
0.028 |
2.243 |
0.000 |
Atom - Atom Distances (Å)
|
O1 |
N2 |
C3 |
H4 |
O1 | | 1.2880 | 2.4228 | 3.4718 |
N2 | 1.2880 | | 1.1348 | 2.1838 | C3 | 2.4228 | 1.1348 | | 1.0490 | H4 | 3.4718 | 2.1838 | 1.0490 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
N2 |
C3 |
179.917 |
|
N2 |
C3 |
H4 |
179.926 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/3-21G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
O |
-0.457 |
|
|
|
2 |
N |
-0.217 |
|
|
|
3 |
C |
0.264 |
|
|
|
4 |
H |
0.410 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.058 |
4.753 |
0.000 |
4.754 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-16.638 |
0.041 |
0.000 |
y |
0.041 |
-13.776 |
0.000 |
z |
0.000 |
0.000 |
-16.639 |
|
Traceless |
| x | y | z |
x |
-1.431 |
0.041 |
0.000 |
y |
0.041 |
2.862 |
0.000 |
z |
0.000 |
0.000 |
-1.432 |
|
Polar |
3z2-r2 | -2.863 |
x2-y2 | -2.862 |
xy | 0.041 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
0.859 |
0.049 |
0.000 |
y |
0.049 |
4.983 |
0.000 |
z |
0.000 |
0.000 |
0.858 |
<r2> (average value of r
2) Å
2
<r2> |
35.486 |
(<r2>)1/2 |
5.957 |