Jump to
S1C2
Energy calculated at B3LYP/LANL2DZ
| | hartrees |
| Energy at 0K | -93.939617 |
| Energy at 298.15K | -93.940880 |
| HF Energy | -93.939617 |
| Nuclear repulsion energy | 27.787697 |
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 B3LYP/LANL2DZ
| 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' |
3341 |
3212 |
1.87 |
|
|
|
| 2 |
A' |
3000 |
2884 |
45.10 |
|
|
|
| 3 |
A' |
1818 |
1747 |
25.17 |
|
|
|
| 4 |
A' |
967 |
929 |
68.37 |
|
|
|
| 5 |
A' |
809 |
777 |
245.99 |
|
|
|
| 6 |
A" |
919 |
883 |
7.60 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5426.6 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 5216.0 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 B3LYP/LANL2DZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.104 |
0.655 |
0.000 |
| N2 |
0.104 |
-0.588 |
0.000 |
| H3 |
-0.668 |
1.442 |
0.000 |
| H4 |
-0.685 |
-1.253 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2433 | 1.1028 | 2.0640 |
N2 | 1.2433 | | 2.1726 | 1.0310 | H3 | 1.1028 | 2.1726 | | 2.6949 | H4 | 2.0640 | 1.0310 | 2.6949 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
130.099 |
|
H3 |
C1 |
N2 |
135.562 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.205 |
|
|
|
| 2 |
N |
-0.269 |
|
|
|
| 3 |
H |
0.208 |
|
|
|
| 4 |
H |
0.267 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.677 |
0.110 |
0.000 |
2.679 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.562 |
0.547 |
0.000 |
| y |
0.547 |
-10.657 |
0.000 |
| z |
0.000 |
0.000 |
-12.664 |
|
| Traceless |
| | x | y | z |
| x |
-0.901 |
0.547 |
0.000 |
| y |
0.547 |
1.956 |
0.000 |
| z |
0.000 |
0.000 |
-1.055 |
|
| Polar |
| 3z2-r2 | -2.110 |
| x2-y2 | -1.905 |
| xy | 0.547 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.657 |
0.194 |
0.000 |
| y |
0.194 |
4.135 |
0.000 |
| z |
0.000 |
0.000 |
1.209 |
<r2> (average value of r
2) Å
2
| <r2> |
17.172 |
| (<r2>)1/2 |
4.144 |
Jump to
S1C1
Energy calculated at B3LYP/LANL2DZ
| | hartrees |
| Energy at 0K | -93.948558 |
| Energy at 298.15K | -93.949894 |
| HF Energy | -93.948558 |
| Nuclear repulsion energy | 27.695093 |
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 B3LYP/LANL2DZ
| 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' |
3469 |
3334 |
4.65 |
|
|
|
| 2 |
A' |
3079 |
2960 |
27.64 |
|
|
|
| 3 |
A' |
1743 |
1675 |
22.82 |
|
|
|
| 4 |
A' |
1175 |
1129 |
10.32 |
|
|
|
| 5 |
A' |
903 |
868 |
260.73 |
|
|
|
| 6 |
A" |
992 |
954 |
156.80 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5679.9 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 5459.5 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 B3LYP/LANL2DZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.002 |
0.665 |
0.000 |
| N2 |
-0.002 |
-0.592 |
0.000 |
| H3 |
0.893 |
1.304 |
0.000 |
| H4 |
-0.863 |
-1.152 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2573 | 1.0992 | 2.0108 |
N2 | 1.2573 | | 2.0962 | 1.0266 | H3 | 1.0992 | 2.0962 | | 3.0185 | H4 | 2.0108 | 1.0266 | 3.0185 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
123.073 |
|
H3 |
C1 |
N2 |
125.490 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.212 |
|
|
|
| 2 |
N |
-0.277 |
|
|
|
| 3 |
H |
0.204 |
|
|
|
| 4 |
H |
0.286 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.460 |
0.026 |
0.000 |
0.461 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.476 |
3.738 |
0.000 |
| y |
3.738 |
-11.373 |
0.000 |
| z |
0.000 |
0.000 |
-12.720 |
|
| Traceless |
| | x | y | z |
| x |
0.570 |
3.738 |
0.000 |
| y |
3.738 |
0.726 |
0.000 |
| z |
0.000 |
0.000 |
-1.296 |
|
| Polar |
| 3z2-r2 | -2.592 |
| x2-y2 | -0.104 |
| xy | 3.738 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.075 |
0.288 |
0.000 |
| y |
0.288 |
3.912 |
0.000 |
| z |
0.000 |
0.000 |
1.230 |
<r2> (average value of r
2) Å
2
| <r2> |
17.082 |
| (<r2>)1/2 |
4.133 |