Jump to
S1C2
Energy calculated at HF/daug-cc-pVTZ
| | hartrees |
| Energy at 0K | -93.434516 |
| Energy at 298.15K | -93.435887 |
| HF Energy | -93.434516 |
| Nuclear repulsion energy | 28.425680 |
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/daug-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' |
3580 |
3239 |
6.73 |
|
|
|
| 2 |
A' |
3185 |
2881 |
25.02 |
|
|
|
| 3 |
A' |
1724 |
1560 |
9.75 |
|
|
|
| 4 |
A' |
1231 |
1114 |
119.45 |
|
|
|
| 5 |
A' |
982 |
889 |
45.17 |
|
|
|
| 6 |
A" |
1052 |
952 |
3.66 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5877.1 cm
-1
Scaled (by 0.9046) Zero Point Vibrational Energy (zpe) 5316.4 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/daug-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 |
-1.034 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2223 | 1.0830 | 1.8959 |
N2 | 1.2223 | | 2.1223 | 1.0090 | H3 | 1.0830 | 2.1223 | | 2.4201 | H4 | 1.8959 | 1.0090 | 2.4201 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
116.039 |
|
H3 |
C1 |
N2 |
133.948 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/daug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.895 |
|
|
|
| 2 |
N |
-0.720 |
|
|
|
| 3 |
H |
1.060 |
|
|
|
| 4 |
H |
0.555 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.162 |
0.964 |
0.000 |
2.367 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.076 |
0.920 |
0.000 |
| y |
0.920 |
-11.436 |
0.000 |
| z |
0.000 |
0.000 |
-12.942 |
|
| Traceless |
| | x | y | z |
| x |
0.113 |
0.920 |
0.000 |
| y |
0.920 |
1.073 |
0.000 |
| z |
0.000 |
0.000 |
-1.186 |
|
| Polar |
| 3z2-r2 | -2.372 |
| x2-y2 | -0.640 |
| xy | 0.920 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.734 |
0.019 |
0.000 |
| y |
0.019 |
4.094 |
0.000 |
| z |
0.000 |
0.000 |
2.334 |
<r2> (average value of r
2) Å
2
| <r2> |
16.647 |
| (<r2>)1/2 |
4.080 |
Jump to
S1C1
Energy calculated at HF/daug-cc-pVTZ
| | hartrees |
| Energy at 0K | -93.440068 |
| Energy at 298.15K | -93.441454 |
| HF Energy | -93.440068 |
| Nuclear repulsion energy | 28.444585 |
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/daug-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 |
3320 |
15.79 |
|
|
|
| 2 |
A' |
3224 |
2916 |
15.53 |
|
|
|
| 3 |
A' |
1751 |
1584 |
27.49 |
|
|
|
| 4 |
A' |
1294 |
1171 |
16.32 |
|
|
|
| 5 |
A' |
1011 |
914 |
176.85 |
|
|
|
| 6 |
A" |
1082 |
979 |
95.89 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6015.5 cm
-1
Scaled (by 0.9046) Zero Point Vibrational Energy (zpe) 5441.6 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 HF/daug-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 |
1.299 |
0.000 |
| H4 |
-0.904 |
-1.017 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2234 | 1.0810 | 1.8871 |
N2 | 1.2234 | | 2.0703 | 1.0048 | H3 | 1.0810 | 2.0703 | | 2.9108 | H4 | 1.8871 | 1.0048 | 2.9108 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
115.409 |
|
H3 |
C1 |
N2 |
127.790 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/daug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.892 |
|
|
|
| 2 |
N |
-0.839 |
|
|
|
| 3 |
H |
1.049 |
|
|
|
| 4 |
H |
0.681 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.669 |
0.822 |
0.000 |
1.060 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.408 |
3.157 |
0.000 |
| y |
3.157 |
-11.598 |
0.000 |
| z |
0.000 |
0.000 |
-12.979 |
|
| Traceless |
| | x | y | z |
| x |
0.880 |
3.157 |
0.000 |
| y |
3.157 |
0.596 |
0.000 |
| z |
0.000 |
0.000 |
-1.476 |
|
| Polar |
| 3z2-r2 | -2.953 |
| x2-y2 | 0.190 |
| xy | 3.157 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.838 |
0.244 |
0.000 |
| y |
0.244 |
4.054 |
0.000 |
| z |
0.000 |
0.000 |
2.351 |
<r2> (average value of r
2) Å
2
| <r2> |
16.611 |
| (<r2>)1/2 |
4.076 |