Jump to
S1C2
Energy calculated at B3PW91/3-21G
| | hartrees |
| Energy at 0K | -93.394860 |
| Energy at 298.15K | -93.396161 |
| HF Energy | -93.394860 |
| Nuclear repulsion energy | 28.060765 |
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 B3PW91/3-21G
| 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' |
3185 |
3061 |
5.97 |
|
|
|
| 2 |
A' |
2966 |
2851 |
57.39 |
|
|
|
| 3 |
A' |
1865 |
1792 |
14.74 |
|
|
|
| 4 |
A' |
971 |
933 |
96.08 |
|
|
|
| 5 |
A' |
899 |
864 |
211.47 |
|
|
|
| 6 |
A" |
948 |
911 |
9.24 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5416.6 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 5206.4 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 B3PW91/3-21G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.106 |
0.643 |
0.000 |
| N2 |
0.106 |
-0.583 |
0.000 |
| H3 |
-0.659 |
1.433 |
0.000 |
| H4 |
-0.717 |
-1.214 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2264 | 1.0998 | 2.0318 |
N2 | 1.2264 | | 2.1566 | 1.0373 | H3 | 1.0998 | 2.1566 | | 2.6480 | H4 | 2.0318 | 1.0373 | 2.6480 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
127.477 |
|
H3 |
C1 |
N2 |
135.903 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.044 |
|
|
|
| 2 |
N |
-0.554 |
|
|
|
| 3 |
H |
0.207 |
|
|
|
| 4 |
H |
0.303 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.412 |
0.064 |
0.000 |
2.413 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.126 |
0.675 |
0.000 |
| y |
0.675 |
-10.658 |
0.000 |
| z |
0.000 |
0.000 |
-12.365 |
|
| Traceless |
| | x | y | z |
| x |
-0.615 |
0.675 |
0.000 |
| y |
0.675 |
1.587 |
0.000 |
| z |
0.000 |
0.000 |
-0.972 |
|
| Polar |
| 3z2-r2 | -1.944 |
| x2-y2 | -1.468 |
| xy | 0.675 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.538 |
0.087 |
0.000 |
| y |
0.087 |
3.713 |
0.000 |
| z |
0.000 |
0.000 |
0.946 |
<r2> (average value of r
2) Å
2
| <r2> |
16.804 |
| (<r2>)1/2 |
4.099 |
Jump to
S1C1
Energy calculated at B3PW91/3-21G
| | hartrees |
| Energy at 0K | -93.401935 |
| Energy at 298.15K | -93.403289 |
| HF Energy | -93.401935 |
| Nuclear repulsion energy | 27.948552 |
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 B3PW91/3-21G
| 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' |
3344 |
3214 |
1.08 |
|
|
|
| 2 |
A' |
3029 |
2912 |
31.61 |
|
|
|
| 3 |
A' |
1780 |
1711 |
12.16 |
|
|
|
| 4 |
A' |
1204 |
1158 |
18.91 |
|
|
|
| 5 |
A' |
939 |
903 |
241.46 |
|
|
|
| 6 |
A" |
1009 |
969 |
134.67 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5652.5 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 5433.2 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 B3PW91/3-21G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.002 |
0.656 |
0.000 |
| N2 |
-0.002 |
-0.585 |
0.000 |
| H3 |
0.900 |
1.282 |
0.000 |
| H4 |
-0.881 |
-1.123 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2416 | 1.0978 | 1.9851 |
N2 | 1.2416 | | 2.0740 | 1.0308 | H3 | 1.0978 | 2.0740 | | 2.9933 | H4 | 1.9851 | 1.0308 | 2.9933 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
121.476 |
|
H3 |
C1 |
N2 |
124.769 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.001 |
|
|
|
| 2 |
N |
-0.541 |
|
|
|
| 3 |
H |
0.224 |
|
|
|
| 4 |
H |
0.318 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.556 |
-0.040 |
0.000 |
0.558 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.078 |
3.346 |
0.000 |
| y |
3.346 |
-11.225 |
0.000 |
| z |
0.000 |
0.000 |
-12.413 |
|
| Traceless |
| | x | y | z |
| x |
0.741 |
3.346 |
0.000 |
| y |
3.346 |
0.521 |
0.000 |
| z |
0.000 |
0.000 |
-1.262 |
|
| Polar |
| 3z2-r2 | -2.524 |
| x2-y2 | 0.146 |
| xy | 3.346 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.909 |
0.538 |
0.000 |
| y |
0.538 |
3.424 |
0.000 |
| z |
0.000 |
0.000 |
0.985 |
<r2> (average value of r
2) Å
2
| <r2> |
16.703 |
| (<r2>)1/2 |
4.087 |