Jump to
S1C2
Energy calculated at B97D3/TZVP
| | hartrees |
| Energy at 0K | -93.937075 |
| Energy at 298.15K | -93.938353 |
| HF Energy | -93.937075 |
| Nuclear repulsion energy | 28.136015 |
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 B97D3/TZVP
| 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' |
3216 |
3170 |
8.12 |
|
|
|
| 2 |
A' |
2903 |
2861 |
59.42 |
|
|
|
| 3 |
A' |
1812 |
1786 |
25.06 |
|
|
|
| 4 |
A' |
973 |
959 |
127.53 |
|
|
|
| 5 |
A' |
859 |
847 |
116.31 |
|
|
|
| 6 |
A" |
883 |
870 |
5.42 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5323.2 cm
-1
Scaled (by 0.9856) Zero Point Vibrational Energy (zpe) 5246.5 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 B97D3/TZVP
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.111 |
0.640 |
0.000 |
| N2 |
0.111 |
-0.586 |
0.000 |
| H3 |
-0.684 |
1.405 |
0.000 |
| H4 |
-0.758 |
-1.141 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2259 | 1.1040 | 1.9814 |
N2 | 1.2259 | | 2.1444 | 1.0312 | H3 | 1.1040 | 2.1444 | | 2.5472 | H4 | 1.9814 | 1.0312 | 2.5472 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
122.537 |
|
H3 |
C1 |
N2 |
133.908 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.063 |
|
|
|
| 2 |
N |
-0.239 |
|
|
|
| 3 |
H |
0.107 |
|
|
|
| 4 |
H |
0.195 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.281 |
0.279 |
0.000 |
2.298 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.361 |
0.632 |
0.000 |
| y |
0.632 |
-11.359 |
0.000 |
| z |
0.000 |
0.000 |
-12.695 |
|
| Traceless |
| | x | y | z |
| x |
-0.333 |
0.632 |
0.000 |
| y |
0.632 |
1.169 |
0.000 |
| z |
0.000 |
0.000 |
-0.835 |
|
| Polar |
| 3z2-r2 | -1.671 |
| x2-y2 | -1.001 |
| xy | 0.632 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.435 |
0.124 |
0.000 |
| y |
0.124 |
4.470 |
0.000 |
| z |
0.000 |
0.000 |
1.656 |
<r2> (average value of r
2) Å
2
| <r2> |
16.922 |
| (<r2>)1/2 |
4.114 |
Jump to
S1C1
Energy calculated at B97D3/TZVP
| | hartrees |
| Energy at 0K | -93.945173 |
| Energy at 298.15K | -93.946508 |
| HF Energy | -93.945173 |
| Nuclear repulsion energy | 28.059037 |
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 B97D3/TZVP
| 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 |
3296 |
1.29 |
|
|
|
| 2 |
A' |
2956 |
2914 |
32.83 |
|
|
|
| 3 |
A' |
1752 |
1727 |
22.60 |
|
|
|
| 4 |
A' |
1181 |
1164 |
11.32 |
|
|
|
| 5 |
A' |
897 |
884 |
207.71 |
|
|
|
| 6 |
A" |
962 |
948 |
116.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5546.0 cm
-1
Scaled (by 0.9856) Zero Point Vibrational Energy (zpe) 5466.2 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 B97D3/TZVP
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.001 |
0.652 |
0.000 |
| N2 |
-0.001 |
-0.586 |
0.000 |
| H3 |
0.912 |
1.268 |
0.000 |
| H4 |
-0.900 |
-1.079 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2371 | 1.1018 | 1.9501 |
N2 | 1.2371 | | 2.0665 | 1.0253 | H3 | 1.1018 | 2.0665 | | 2.9653 | H4 | 1.9501 | 1.0253 | 2.9653 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
118.781 |
|
H3 |
C1 |
N2 |
124.040 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.109 |
|
|
|
| 2 |
N |
-0.236 |
|
|
|
| 3 |
H |
0.125 |
|
|
|
| 4 |
H |
0.220 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.470 |
0.072 |
0.000 |
0.476 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.444 |
3.224 |
0.000 |
| y |
3.224 |
-11.770 |
0.000 |
| z |
0.000 |
0.000 |
-12.771 |
|
| Traceless |
| | x | y | z |
| x |
0.826 |
3.224 |
0.000 |
| y |
3.224 |
0.338 |
0.000 |
| z |
0.000 |
0.000 |
-1.164 |
|
| Polar |
| 3z2-r2 | -2.327 |
| x2-y2 | 0.326 |
| xy | 3.224 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.633 |
0.374 |
0.000 |
| y |
0.374 |
4.222 |
0.000 |
| z |
0.000 |
0.000 |
1.795 |
<r2> (average value of r
2) Å
2
| <r2> |
16.854 |
| (<r2>)1/2 |
4.105 |