Jump to
S1C2
Energy calculated at B3PW91/STO-3G
| | hartrees |
| Energy at 0K | -92.696784 |
| Energy at 298.15K | -92.698029 |
| HF Energy | -92.696784 |
| Nuclear repulsion energy | 27.381999 |
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/STO-3G
| 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' |
3338 |
2954 |
1.33 |
|
|
|
| 2 |
A' |
3250 |
2876 |
3.47 |
|
|
|
| 3 |
A' |
1857 |
1643 |
5.80 |
|
|
|
| 4 |
A' |
1054 |
933 |
120.66 |
|
|
|
| 5 |
A' |
911 |
806 |
82.21 |
|
|
|
| 6 |
A" |
932 |
825 |
2.30 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5670.6 cm
-1
Scaled (by 0.885) Zero Point Vibrational Energy (zpe) 5018.5 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 B3PW91/STO-3G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.117 |
0.654 |
0.000 |
| N2 |
0.117 |
-0.609 |
0.000 |
| H3 |
-0.676 |
1.436 |
0.000 |
| H4 |
-0.845 |
-1.094 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2626 | 1.1140 | 1.9945 |
N2 | 1.2626 | | 2.1933 | 1.0772 | H3 | 1.1140 | 2.1933 | | 2.5351 | H4 | 1.9945 | 1.0772 | 2.5351 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
116.729 |
|
H3 |
C1 |
N2 |
134.612 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.014 |
|
|
|
| 2 |
N |
-0.284 |
|
|
|
| 3 |
H |
0.089 |
|
|
|
| 4 |
H |
0.181 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.938 |
0.537 |
0.000 |
2.011 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-10.548 |
0.768 |
0.000 |
| y |
0.768 |
-10.675 |
0.000 |
| z |
0.000 |
0.000 |
-11.185 |
|
| Traceless |
| | x | y | z |
| x |
0.382 |
0.768 |
0.000 |
| y |
0.768 |
0.192 |
0.000 |
| z |
0.000 |
0.000 |
-0.574 |
|
| Polar |
| 3z2-r2 | -1.148 |
| x2-y2 | 0.126 |
| xy | 0.768 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.898 |
0.167 |
0.000 |
| y |
0.167 |
2.262 |
0.000 |
| z |
0.000 |
0.000 |
0.476 |
<r2> (average value of r
2) Å
2
| <r2> |
16.513 |
| (<r2>)1/2 |
4.064 |
Jump to
S1C1
Energy calculated at B3PW91/STO-3G
| | hartrees |
| Energy at 0K | -92.708760 |
| Energy at 298.15K | -92.710081 |
| HF Energy | -92.708760 |
| Nuclear repulsion energy | 27.261707 |
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/STO-3G
| 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' |
3475 |
3075 |
1.40 |
|
|
|
| 2 |
A' |
3287 |
2909 |
0.38 |
|
|
|
| 3 |
A' |
1792 |
1586 |
6.96 |
|
|
|
| 4 |
A' |
1313 |
1162 |
14.64 |
|
|
|
| 5 |
A' |
972 |
860 |
157.53 |
|
|
|
| 6 |
A" |
1043 |
923 |
63.97 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5941.2 cm
-1
Scaled (by 0.885) Zero Point Vibrational Energy (zpe) 5258.0 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/STO-3G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.002 |
0.671 |
0.000 |
| N2 |
0.002 |
-0.607 |
0.000 |
| H3 |
0.961 |
1.244 |
0.000 |
| H4 |
-0.984 |
-1.025 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2782 | 1.1170 | 1.9622 |
N2 | 1.2782 | | 2.0845 | 1.0710 | H3 | 1.1170 | 2.0845 | | 2.9887 | H4 | 1.9622 | 1.0710 | 2.9887 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
113.000 |
|
H3 |
C1 |
N2 |
120.839 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.003 |
|
|
|
| 2 |
N |
-0.275 |
|
|
|
| 3 |
H |
0.088 |
|
|
|
| 4 |
H |
0.189 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.650 |
0.269 |
0.000 |
0.703 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-9.874 |
2.268 |
0.000 |
| y |
2.268 |
-11.123 |
0.000 |
| z |
0.000 |
0.000 |
-11.217 |
|
| Traceless |
| | x | y | z |
| x |
1.296 |
2.268 |
0.000 |
| y |
2.268 |
-0.577 |
0.000 |
| z |
0.000 |
0.000 |
-0.719 |
|
| Polar |
| 3z2-r2 | -1.438 |
| x2-y2 | 1.248 |
| xy | 2.268 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.209 |
0.510 |
0.000 |
| y |
0.510 |
2.214 |
0.000 |
| z |
0.000 |
0.000 |
0.514 |
<r2> (average value of r
2) Å
2
| <r2> |
16.479 |
| (<r2>)1/2 |
4.059 |