Jump to
S1C2
Energy calculated at HSEh1PBE/cc-pVTZ
| | hartrees |
| Energy at 0K | -93.889842 |
| Energy at 298.15K | -93.891141 |
| HF Energy | -93.889842 |
| Nuclear repulsion energy | 28.336638 |
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 HSEh1PBE/cc-pVTZ
| 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' |
3347 |
3216 |
2.63 |
|
|
|
| 2 |
A' |
2992 |
2876 |
48.40 |
|
|
|
| 3 |
A' |
1874 |
1801 |
28.59 |
|
|
|
| 4 |
A' |
1018 |
978 |
149.18 |
|
|
|
| 5 |
A' |
868 |
834 |
103.46 |
|
|
|
| 6 |
A" |
920 |
884 |
4.13 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5508.8 cm
-1
Scaled (by 0.9611) Zero Point Vibrational Energy (zpe) 5294.5 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 HSEh1PBE/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.111 |
0.633 |
0.000 |
| N2 |
0.111 |
-0.584 |
0.000 |
| H3 |
-0.673 |
1.402 |
0.000 |
| H4 |
-0.766 |
-1.112 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2174 | 1.0978 | 1.9537 |
N2 | 1.2174 | | 2.1349 | 1.0239 | H3 | 1.0978 | 2.1349 | | 2.5157 | H4 | 1.9537 | 1.0239 | 2.5157 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
121.060 |
|
H3 |
C1 |
N2 |
134.415 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.096 |
|
|
|
| 2 |
N |
-0.171 |
|
|
|
| 3 |
H |
0.105 |
|
|
|
| 4 |
H |
0.162 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.122 |
0.371 |
0.000 |
2.154 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.154 |
0.609 |
0.000 |
| y |
0.609 |
-11.094 |
0.000 |
| z |
0.000 |
0.000 |
-12.659 |
|
| Traceless |
| | x | y | z |
| x |
-0.278 |
0.609 |
0.000 |
| y |
0.609 |
1.313 |
0.000 |
| z |
0.000 |
0.000 |
-1.035 |
|
| Polar |
| 3z2-r2 | -2.070 |
| x2-y2 | -1.060 |
| xy | 0.609 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.502 |
0.075 |
0.000 |
| y |
0.075 |
4.128 |
0.000 |
| z |
0.000 |
0.000 |
1.812 |
<r2> (average value of r
2) Å
2
| <r2> |
16.672 |
| (<r2>)1/2 |
4.083 |
Jump to
S1C1
Energy calculated at HSEh1PBE/cc-pVTZ
| | hartrees |
| Energy at 0K | -93.896736 |
| Energy at 298.15K | -93.898081 |
| HF Energy | -93.896736 |
| Nuclear repulsion energy | 28.266443 |
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 HSEh1PBE/cc-pVTZ
| 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' |
3463 |
3328 |
7.69 |
|
|
|
| 2 |
A' |
3034 |
2916 |
26.52 |
|
|
|
| 3 |
A' |
1825 |
1754 |
30.04 |
|
|
|
| 4 |
A' |
1191 |
1145 |
11.59 |
|
|
|
| 5 |
A' |
909 |
874 |
223.75 |
|
|
|
| 6 |
A" |
981 |
943 |
110.33 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5701.7 cm
-1
Scaled (by 0.9611) Zero Point Vibrational Energy (zpe) 5479.9 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 HSEh1PBE/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.644 |
0.000 |
| N2 |
0.000 |
-0.583 |
0.000 |
| H3 |
0.896 |
1.277 |
0.000 |
| H4 |
-0.897 |
-1.065 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2269 | 1.0963 | 1.9304 |
N2 | 1.2269 | | 2.0638 | 1.0188 | H3 | 1.0963 | 2.0638 | | 2.9492 | H4 | 1.9304 | 1.0188 | 2.9492 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
118.250 |
|
H3 |
C1 |
N2 |
125.235 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.130 |
|
|
|
| 2 |
N |
-0.179 |
|
|
|
| 3 |
H |
0.129 |
|
|
|
| 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 |
| |
-0.446 |
0.171 |
0.000 |
0.478 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.314 |
3.118 |
0.000 |
| y |
3.118 |
-11.434 |
0.000 |
| z |
0.000 |
0.000 |
-12.694 |
|
| Traceless |
| | x | y | z |
| x |
0.750 |
3.118 |
0.000 |
| y |
3.118 |
0.570 |
0.000 |
| z |
0.000 |
0.000 |
-1.320 |
|
| Polar |
| 3z2-r2 | -2.641 |
| x2-y2 | 0.120 |
| xy | 3.118 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.644 |
0.376 |
0.000 |
| y |
0.376 |
3.946 |
0.000 |
| z |
0.000 |
0.000 |
1.857 |
<r2> (average value of r
2) Å
2
| <r2> |
16.617 |
| (<r2>)1/2 |
4.076 |