Jump to
S1C2
Energy calculated at LSDA/6-31G
| hartrees |
Energy at 0K | -93.391601 |
Energy at 298.15K | -93.392873 |
HF Energy | -93.391601 |
Nuclear repulsion energy | 27.931668 |
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 LSDA/6-31G
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' |
3189 |
3124 |
20.08 |
|
|
|
2 |
A' |
2903 |
2844 |
65.34 |
|
|
|
3 |
A' |
1865 |
1828 |
20.09 |
|
|
|
4 |
A' |
935 |
916 |
81.78 |
|
|
|
5 |
A' |
859 |
842 |
220.39 |
|
|
|
6 |
A" |
907 |
889 |
16.31 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5329.1 cm
-1
Scaled (by 0.9797) Zero Point Vibrational Energy (zpe) 5220.9 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 LSDA/6-31G
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.105 |
0.650 |
0.000 |
N2 |
0.105 |
-0.580 |
0.000 |
H3 |
-0.686 |
1.432 |
0.000 |
H4 |
-0.674 |
-1.269 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
N2 |
H3 |
H4 |
C1 | | 1.2300 | 1.1120 | 2.0706 |
N2 | 1.2300 | | 2.1616 | 1.0396 | H3 | 1.1120 | 2.1616 | | 2.7003 | H4 | 2.0706 | 1.0396 | 2.7003 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
N2 |
H4 |
131.483 |
|
H3 |
C1 |
N2 |
134.666 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.021 |
|
|
|
2 |
N |
-0.437 |
|
|
|
3 |
H |
0.154 |
|
|
|
4 |
H |
0.305 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-2.450 |
-0.108 |
0.000 |
2.453 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-12.462 |
0.613 |
0.000 |
y |
0.613 |
-10.609 |
0.000 |
z |
0.000 |
0.000 |
-12.455 |
|
Traceless |
| x | y | z |
x |
-0.931 |
0.613 |
0.000 |
y |
0.613 |
1.849 |
0.000 |
z |
0.000 |
0.000 |
-0.919 |
|
Polar |
3z2-r2 | -1.837 |
x2-y2 | -1.853 |
xy | 0.613 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
1.815 |
0.080 |
0.000 |
y |
0.080 |
4.227 |
0.000 |
z |
0.000 |
0.000 |
1.096 |
<r2> (average value of r
2) Å
2
<r2> |
17.013 |
(<r2>)1/2 |
4.125 |
Jump to
S1C1
Energy calculated at LSDA/6-31G
| hartrees |
Energy at 0K | -93.398703 |
Energy at 298.15K | -93.400034 |
HF Energy | -93.398703 |
Nuclear repulsion energy | 27.841824 |
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 LSDA/6-31G
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' |
3345 |
3277 |
0.16 |
|
|
|
2 |
A' |
2982 |
2922 |
31.89 |
|
|
|
3 |
A' |
1788 |
1752 |
14.59 |
|
|
|
4 |
A' |
1145 |
1121 |
8.88 |
|
|
|
5 |
A' |
900 |
882 |
235.84 |
|
|
|
6 |
A" |
973 |
953 |
140.33 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5566.7 cm
-1
Scaled (by 0.9797) Zero Point Vibrational Energy (zpe) 5453.7 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 LSDA/6-31G
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.004 |
0.660 |
0.000 |
N2 |
-0.004 |
-0.584 |
0.000 |
H3 |
0.910 |
1.288 |
0.000 |
H4 |
-0.861 |
-1.161 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
N2 |
H3 |
H4 |
C1 | | 1.2443 | 1.1084 | 2.0128 |
N2 | 1.2443 | | 2.0828 | 1.0333 | H3 | 1.1084 | 2.0828 | | 3.0218 | H4 | 2.0128 | 1.0333 | 3.0218 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
N2 |
H4 |
123.928 |
|
H3 |
C1 |
N2 |
124.468 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.058 |
|
|
|
2 |
N |
-0.439 |
|
|
|
3 |
H |
0.171 |
|
|
|
4 |
H |
0.326 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.543 |
-0.167 |
0.000 |
0.568 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-11.310 |
3.536 |
0.000 |
y |
3.536 |
-11.268 |
0.000 |
z |
0.000 |
0.000 |
-12.501 |
|
Traceless |
| x | y | z |
x |
0.575 |
3.536 |
0.000 |
y |
3.536 |
0.637 |
0.000 |
z |
0.000 |
0.000 |
-1.212 |
|
Polar |
3z2-r2 | -2.424 |
x2-y2 | -0.042 |
xy | 3.536 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.110 |
0.590 |
0.000 |
y |
0.590 |
3.730 |
0.000 |
z |
0.000 |
0.000 |
1.117 |
<r2> (average value of r
2) Å
2
<r2> |
16.882 |
(<r2>)1/2 |
4.109 |