Jump to
S1C2
Energy calculated at PBEPBE/Def2TZVPP
| | hartrees |
| Energy at 0K | -93.884124 |
| Energy at 298.15K | -93.885390 |
| HF Energy | -93.884124 |
| Nuclear repulsion energy | 28.104039 |
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 PBEPBE/Def2TZVPP
| 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' |
3185 |
3147 |
11.01 |
|
|
|
| 2 |
A' |
2883 |
2848 |
56.65 |
|
|
|
| 3 |
A' |
1814 |
1792 |
21.28 |
|
|
|
| 4 |
A' |
956 |
944 |
149.27 |
|
|
|
| 5 |
A' |
846 |
836 |
93.85 |
|
|
|
| 6 |
A" |
873 |
862 |
4.07 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5278.4 cm
-1
Scaled (by 0.9879) Zero Point Vibrational Energy (zpe) 5214.5 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 PBEPBE/Def2TZVPP
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.111 |
0.640 |
0.000 |
| N2 |
0.111 |
-0.587 |
0.000 |
| H3 |
-0.687 |
1.407 |
0.000 |
| H4 |
-0.762 |
-1.142 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2267 | 1.1069 | 1.9843 |
N2 | 1.2267 | | 2.1477 | 1.0345 | H3 | 1.1069 | 2.1477 | | 2.5503 | H4 | 1.9843 | 1.0345 | 2.5503 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
122.457 |
|
H3 |
C1 |
N2 |
133.878 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/Def2TZVPP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.113 |
|
|
|
| 2 |
N |
-0.174 |
|
|
|
| 3 |
H |
0.111 |
|
|
|
| 4 |
H |
0.176 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.100 |
0.201 |
0.000 |
2.109 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.456 |
0.521 |
0.000 |
| y |
0.521 |
-11.314 |
0.000 |
| z |
0.000 |
0.000 |
-12.816 |
|
| Traceless |
| | x | y | z |
| x |
-0.392 |
0.521 |
0.000 |
| y |
0.521 |
1.322 |
0.000 |
| z |
0.000 |
0.000 |
-0.931 |
|
| Polar |
| 3z2-r2 | -1.861 |
| x2-y2 | -1.143 |
| xy | 0.521 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.772 |
0.124 |
0.000 |
| y |
0.124 |
4.581 |
0.000 |
| z |
0.000 |
0.000 |
1.976 |
<r2> (average value of r
2) Å
2
| <r2> |
16.984 |
| (<r2>)1/2 |
4.121 |
Jump to
S1C1
Energy calculated at PBEPBE/Def2TZVPP
| | hartrees |
| Energy at 0K | -93.891441 |
| Energy at 298.15K | -93.892767 |
| HF Energy | -93.891441 |
| Nuclear repulsion energy | 28.032538 |
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 PBEPBE/Def2TZVPP
| 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' |
3331 |
3291 |
2.47 |
|
|
|
| 2 |
A' |
2938 |
2902 |
28.82 |
|
|
|
| 3 |
A' |
1757 |
1736 |
21.39 |
|
|
|
| 4 |
A' |
1157 |
1143 |
12.31 |
|
|
|
| 5 |
A' |
887 |
876 |
202.98 |
|
|
|
| 6 |
A" |
949 |
937 |
102.13 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5509.2 cm
-1
Scaled (by 0.9879) Zero Point Vibrational Energy (zpe) 5442.6 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 PBEPBE/Def2TZVPP
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 |
0.910 |
1.275 |
0.000 |
| H4 |
-0.900 |
-1.084 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2367 | 1.1042 | 1.9542 |
N2 | 1.2367 | | 2.0717 | 1.0279 | H3 | 1.1042 | 2.0717 | | 2.9735 | H4 | 1.9542 | 1.0279 | 2.9735 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
119.007 |
|
H3 |
C1 |
N2 |
124.414 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/Def2TZVPP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.136 |
|
|
|
| 2 |
N |
-0.183 |
|
|
|
| 3 |
H |
0.118 |
|
|
|
| 4 |
H |
0.202 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.392 |
-0.003 |
0.000 |
0.392 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.560 |
3.153 |
0.000 |
| y |
3.153 |
-11.733 |
0.000 |
| z |
0.000 |
0.000 |
-12.877 |
|
| Traceless |
| | x | y | z |
| x |
0.744 |
3.153 |
0.000 |
| y |
3.153 |
0.486 |
0.000 |
| z |
0.000 |
0.000 |
-1.230 |
|
| Polar |
| 3z2-r2 | -2.461 |
| x2-y2 | 0.172 |
| xy | 3.153 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.873 |
0.405 |
0.000 |
| y |
0.405 |
4.266 |
0.000 |
| z |
0.000 |
0.000 |
2.063 |
<r2> (average value of r
2) Å
2
| <r2> |
16.917 |
| (<r2>)1/2 |
4.113 |