Jump to
S1C2
Energy calculated at HF/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -93.434359 |
| Energy at 298.15K | -93.435734 |
| HF Energy | -93.434359 |
| Nuclear repulsion energy | 28.425935 |
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 HF/aug-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' |
3581 |
3260 |
6.73 |
|
|
|
| 2 |
A' |
3186 |
2901 |
24.92 |
|
|
|
| 3 |
A' |
1724 |
1570 |
9.78 |
|
|
|
| 4 |
A' |
1232 |
1121 |
119.40 |
|
|
|
| 5 |
A' |
983 |
895 |
45.33 |
|
|
|
| 6 |
A" |
1052 |
958 |
3.62 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5878.7 cm
-1
Scaled (by 0.9104) Zero Point Vibrational Energy (zpe) 5351.9 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 HF/aug-cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.112 |
0.631 |
0.000 |
| N2 |
0.112 |
-0.591 |
0.000 |
| H3 |
-0.667 |
1.383 |
0.000 |
| H4 |
-0.794 |
-1.033 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2223 | 1.0830 | 1.8956 |
N2 | 1.2223 | | 2.1222 | 1.0089 | H3 | 1.0830 | 2.1222 | | 2.4195 | H4 | 1.8956 | 1.0089 | 2.4195 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
116.006 |
|
H3 |
C1 |
N2 |
133.942 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.353 |
|
|
|
| 2 |
N |
-0.360 |
|
|
|
| 3 |
H |
0.492 |
|
|
|
| 4 |
H |
0.221 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.163 |
0.965 |
0.000 |
2.368 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.071 |
0.917 |
0.000 |
| y |
0.917 |
-11.440 |
0.000 |
| z |
0.000 |
0.000 |
-12.950 |
|
| Traceless |
| | x | y | z |
| x |
0.124 |
0.917 |
0.000 |
| y |
0.917 |
1.071 |
0.000 |
| z |
0.000 |
0.000 |
-1.195 |
|
| Polar |
| 3z2-r2 | -2.389 |
| x2-y2 | -0.632 |
| xy | 0.917 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.720 |
0.021 |
0.000 |
| y |
0.021 |
4.087 |
0.000 |
| z |
0.000 |
0.000 |
2.325 |
<r2> (average value of r
2) Å
2
| <r2> |
16.648 |
| (<r2>)1/2 |
4.080 |
Jump to
S1C1
Energy calculated at HF/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -93.439909 |
| Energy at 298.15K | -93.441297 |
| HF Energy | -93.439909 |
| Nuclear repulsion energy | 28.443057 |
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 HF/aug-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' |
3670 |
3341 |
15.75 |
|
|
|
| 2 |
A' |
3225 |
2936 |
15.43 |
|
|
|
| 3 |
A' |
1750 |
1594 |
27.46 |
|
|
|
| 4 |
A' |
1294 |
1178 |
16.41 |
|
|
|
| 5 |
A' |
1011 |
920 |
176.84 |
|
|
|
| 6 |
A" |
1082 |
985 |
95.89 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6015.7 cm
-1
Scaled (by 0.9104) Zero Point Vibrational Energy (zpe) 5476.7 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 HF/aug-cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.004 |
0.637 |
0.000 |
| N2 |
0.004 |
-0.586 |
0.000 |
| H3 |
0.858 |
1.300 |
0.000 |
| H4 |
-0.904 |
-1.017 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2235 | 1.0809 | 1.8870 |
N2 | 1.2235 | | 2.0704 | 1.0048 | H3 | 1.0809 | 2.0704 | | 2.9106 | H4 | 1.8870 | 1.0048 | 2.9106 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
115.386 |
|
H3 |
C1 |
N2 |
127.797 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.403 |
|
|
|
| 2 |
N |
-0.362 |
|
|
|
| 3 |
H |
0.509 |
|
|
|
| 4 |
H |
0.256 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.669 |
0.823 |
0.000 |
1.061 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.403 |
3.159 |
0.000 |
| y |
3.159 |
-11.603 |
0.000 |
| z |
0.000 |
0.000 |
-12.986 |
|
| Traceless |
| | x | y | z |
| x |
0.891 |
3.159 |
0.000 |
| y |
3.159 |
0.592 |
0.000 |
| z |
0.000 |
0.000 |
-1.483 |
|
| Polar |
| 3z2-r2 | -2.967 |
| x2-y2 | 0.200 |
| xy | 3.159 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.823 |
0.246 |
0.000 |
| y |
0.246 |
4.048 |
0.000 |
| z |
0.000 |
0.000 |
2.339 |
<r2> (average value of r
2) Å
2
| <r2> |
16.613 |
| (<r2>)1/2 |
4.076 |