Jump to
S1C2
Energy calculated at B97D3/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -93.938558 |
| Energy at 298.15K | -93.939837 |
| HF Energy | -93.938558 |
| Nuclear repulsion energy | 28.154707 |
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 B97D3/6-311+G(3df,2p)
| 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' |
3238 |
3196 |
3.86 |
|
|
|
| 2 |
A' |
2905 |
2867 |
52.40 |
|
|
|
| 3 |
A' |
1804 |
1780 |
24.96 |
|
|
|
| 4 |
A' |
982 |
969 |
150.34 |
|
|
|
| 5 |
A' |
864 |
852 |
89.36 |
|
|
|
| 6 |
A" |
877 |
866 |
3.75 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5334.4 cm
-1
Scaled (by 0.987) Zero Point Vibrational Energy (zpe) 5265.1 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 B97D3/6-311+G(3df,2p)
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 |
-0.687 |
1.400 |
0.000 |
| H4 |
-0.760 |
-1.135 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2257 | 1.1026 | 1.9770 |
N2 | 1.2257 | | 2.1407 | 1.0299 | H3 | 1.1026 | 2.1407 | | 2.5364 | H4 | 1.9770 | 1.0299 | 2.5364 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
122.106 |
|
H3 |
C1 |
N2 |
133.470 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.221 |
|
|
|
| 2 |
N |
-0.555 |
|
|
|
| 3 |
H |
0.162 |
|
|
|
| 4 |
H |
0.172 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.102 |
0.297 |
0.000 |
2.123 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.419 |
0.574 |
0.000 |
| y |
0.574 |
-11.357 |
0.000 |
| z |
0.000 |
0.000 |
-12.861 |
|
| Traceless |
| | x | y | z |
| x |
-0.310 |
0.574 |
0.000 |
| y |
0.574 |
1.283 |
0.000 |
| z |
0.000 |
0.000 |
-0.973 |
|
| Polar |
| 3z2-r2 | -1.947 |
| x2-y2 | -1.062 |
| xy | 0.574 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.040 |
0.152 |
0.000 |
| y |
0.152 |
4.677 |
0.000 |
| z |
0.000 |
0.000 |
2.388 |
<r2> (average value of r
2) Å
2
| <r2> |
16.946 |
| (<r2>)1/2 |
4.117 |
Jump to
S1C1
Energy calculated at B97D3/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -93.945828 |
| Energy at 298.15K | -93.947160 |
| HF Energy | -93.945828 |
| Nuclear repulsion energy | 28.079964 |
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 B97D3/6-311+G(3df,2p)
| 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' |
3358 |
3315 |
4.00 |
|
|
|
| 2 |
A' |
2953 |
2915 |
27.55 |
|
|
|
| 3 |
A' |
1746 |
1724 |
24.44 |
|
|
|
| 4 |
A' |
1171 |
1156 |
12.23 |
|
|
|
| 5 |
A' |
896 |
885 |
207.43 |
|
|
|
| 6 |
A" |
952 |
940 |
102.02 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5538.5 cm
-1
Scaled (by 0.987) Zero Point Vibrational Energy (zpe) 5466.5 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 B97D3/6-311+G(3df,2p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.001 |
0.651 |
0.000 |
| N2 |
-0.001 |
-0.585 |
0.000 |
| H3 |
0.908 |
1.272 |
0.000 |
| H4 |
-0.899 |
-1.078 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2362 | 1.1007 | 1.9481 |
N2 | 1.2362 | | 2.0678 | 1.0242 | H3 | 1.1007 | 2.0678 | | 2.9642 | H4 | 1.9481 | 1.0242 | 2.9642 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
118.786 |
|
H3 |
C1 |
N2 |
124.343 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.201 |
|
|
|
| 2 |
N |
-0.540 |
|
|
|
| 3 |
H |
0.155 |
|
|
|
| 4 |
H |
0.184 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.393 |
0.103 |
0.000 |
0.406 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.582 |
3.200 |
0.000 |
| y |
3.200 |
-11.780 |
0.000 |
| z |
0.000 |
0.000 |
-12.917 |
|
| Traceless |
| | x | y | z |
| x |
0.766 |
3.200 |
0.000 |
| y |
3.200 |
0.470 |
0.000 |
| z |
0.000 |
0.000 |
-1.236 |
|
| Polar |
| 3z2-r2 | -2.472 |
| x2-y2 | 0.198 |
| xy | 3.200 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.125 |
0.144 |
0.000 |
| y |
0.144 |
4.527 |
0.000 |
| z |
0.000 |
0.000 |
2.459 |
<r2> (average value of r
2) Å
2
| <r2> |
16.906 |
| (<r2>)1/2 |
4.112 |