Jump to
S1C2
Energy calculated at B3LYP/6-31G**
| | hartrees |
| Energy at 0K | -93.962062 |
| Energy at 298.15K | -93.963352 |
| HF Energy | -93.962062 |
| Nuclear repulsion energy | 28.145754 |
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/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' |
3299 |
3170 |
5.54 |
|
|
|
| 2 |
A' |
2972 |
2855 |
57.09 |
|
|
|
| 3 |
A' |
1873 |
1800 |
26.21 |
|
|
|
| 4 |
A' |
1016 |
976 |
128.70 |
|
|
|
| 5 |
A' |
872 |
838 |
125.56 |
|
|
|
| 6 |
A" |
899 |
863 |
6.32 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5465.5 cm
-1
Scaled (by 0.9608) Zero Point Vibrational Energy (zpe) 5251.2 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 B3LYP/6-31G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.111 |
0.639 |
0.000 |
| N2 |
0.111 |
-0.588 |
0.000 |
| H3 |
-0.678 |
1.408 |
0.000 |
| H4 |
-0.768 |
-1.124 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2265 | 1.1020 | 1.9700 |
N2 | 1.2265 | | 2.1461 | 1.0297 | H3 | 1.1020 | 2.1461 | | 2.5339 | H4 | 1.9700 | 1.0297 | 2.5339 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
121.400 |
|
H3 |
C1 |
N2 |
134.275 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.050 |
|
|
|
| 2 |
N |
-0.421 |
|
|
|
| 3 |
H |
0.117 |
|
|
|
| 4 |
H |
0.254 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.145 |
0.365 |
0.000 |
2.176 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.895 |
0.712 |
0.000 |
| y |
0.712 |
-10.946 |
0.000 |
| z |
0.000 |
0.000 |
-12.350 |
|
| Traceless |
| | x | y | z |
| x |
-0.247 |
0.712 |
0.000 |
| y |
0.712 |
1.177 |
0.000 |
| z |
0.000 |
0.000 |
-0.930 |
|
| Polar |
| 3z2-r2 | -1.859 |
| x2-y2 | -0.949 |
| xy | 0.712 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.958 |
0.053 |
0.000 |
| y |
0.053 |
3.846 |
0.000 |
| z |
0.000 |
0.000 |
1.200 |
<r2> (average value of r
2) Å
2
| <r2> |
16.649 |
| (<r2>)1/2 |
4.080 |
Jump to
S1C1
Energy calculated at B3LYP/6-31G**
| | hartrees |
| Energy at 0K | -93.970040 |
| Energy at 298.15K | -93.971383 |
| HF Energy | -93.970040 |
| Nuclear repulsion energy | 28.065787 |
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/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' |
3428 |
3294 |
1.76 |
|
|
|
| 2 |
A' |
3021 |
2903 |
33.58 |
|
|
|
| 3 |
A' |
1814 |
1743 |
25.28 |
|
|
|
| 4 |
A' |
1214 |
1166 |
10.19 |
|
|
|
| 5 |
A' |
918 |
882 |
214.04 |
|
|
|
| 6 |
A" |
977 |
939 |
108.90 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5686.1 cm
-1
Scaled (by 0.9608) Zero Point Vibrational Energy (zpe) 5463.2 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 B3LYP/6-31G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.000 |
0.651 |
0.000 |
| N2 |
-0.000 |
-0.587 |
0.000 |
| H3 |
0.910 |
1.269 |
0.000 |
| H4 |
-0.904 |
-1.068 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2376 | 1.1004 | 1.9421 |
N2 | 1.2376 | | 2.0669 | 1.0242 | H3 | 1.1004 | 2.0669 | | 2.9586 | H4 | 1.9421 | 1.0242 | 2.9586 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
118.028 |
|
H3 |
C1 |
N2 |
124.161 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.016 |
|
|
|
| 2 |
N |
-0.414 |
|
|
|
| 3 |
H |
0.128 |
|
|
|
| 4 |
H |
0.270 |
|
|
|
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 |
-11.048 |
2.982 |
0.000 |
| y |
2.982 |
-11.339 |
0.000 |
| z |
0.000 |
0.000 |
-12.387 |
|
| Traceless |
| | x | y | z |
| x |
0.815 |
2.982 |
0.000 |
| y |
2.982 |
0.379 |
0.000 |
| z |
0.000 |
0.000 |
-1.193 |
|
| Polar |
| 3z2-r2 | -2.387 |
| x2-y2 | 0.291 |
| xy | 2.982 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.203 |
0.561 |
0.000 |
| y |
0.561 |
3.631 |
0.000 |
| z |
0.000 |
0.000 |
1.249 |
<r2> (average value of r
2) Å
2
| <r2> |
16.589 |
| (<r2>)1/2 |
4.073 |