Jump to
S1C2
Energy calculated at HF/cc-pVTZ
| | hartrees |
| Energy at 0K | -93.432491 |
| Energy at 298.15K | -93.433867 |
| HF Energy | -93.432491 |
| Nuclear repulsion energy | 28.420697 |
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/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' |
3577 |
3255 |
4.94 |
|
|
|
| 2 |
A' |
3182 |
2896 |
27.80 |
|
|
|
| 3 |
A' |
1720 |
1565 |
5.73 |
|
|
|
| 4 |
A' |
1236 |
1125 |
123.40 |
|
|
|
| 5 |
A' |
987 |
899 |
44.74 |
|
|
|
| 6 |
A" |
1057 |
962 |
4.42 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5879.5 cm
-1
Scaled (by 0.9101) Zero Point Vibrational Energy (zpe) 5350.9 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/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.113 |
0.631 |
0.000 |
| N2 |
0.113 |
-0.592 |
0.000 |
| H3 |
-0.667 |
1.383 |
0.000 |
| H4 |
-0.797 |
-1.029 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2227 | 1.0833 | 1.8926 |
N2 | 1.2227 | | 2.1233 | 1.0092 | H3 | 1.0833 | 2.1233 | | 2.4155 | H4 | 1.8926 | 1.0092 | 2.4155 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
115.658 |
|
H3 |
C1 |
N2 |
133.989 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.063 |
|
|
|
| 2 |
N |
-0.243 |
|
|
|
| 3 |
H |
0.128 |
|
|
|
| 4 |
H |
0.179 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.160 |
0.936 |
0.000 |
2.355 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.932 |
0.913 |
0.000 |
| y |
0.913 |
-11.370 |
0.000 |
| z |
0.000 |
0.000 |
-12.779 |
|
| Traceless |
| | x | y | z |
| x |
0.143 |
0.913 |
0.000 |
| y |
0.913 |
0.985 |
0.000 |
| z |
0.000 |
0.000 |
-1.128 |
|
| Polar |
| 3z2-r2 | -2.256 |
| x2-y2 | -0.562 |
| xy | 0.913 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.293 |
0.003 |
0.000 |
| y |
0.003 |
3.781 |
0.000 |
| z |
0.000 |
0.000 |
1.776 |
<r2> (average value of r
2) Å
2
| <r2> |
16.568 |
| (<r2>)1/2 |
4.070 |
Jump to
S1C1
Energy calculated at HF/cc-pVTZ
| | hartrees |
| Energy at 0K | -93.437820 |
| Energy at 298.15K | -93.439210 |
| HF Energy | -93.437820 |
| Nuclear repulsion energy | 28.433589 |
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/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' |
3666 |
3336 |
11.97 |
|
|
|
| 2 |
A' |
3218 |
2929 |
18.14 |
|
|
|
| 3 |
A' |
1746 |
1589 |
21.85 |
|
|
|
| 4 |
A' |
1301 |
1184 |
16.05 |
|
|
|
| 5 |
A' |
1014 |
923 |
178.11 |
|
|
|
| 6 |
A" |
1086 |
988 |
100.44 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6015.0 cm
-1
Scaled (by 0.9101) Zero Point Vibrational Energy (zpe) 5474.3 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/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 |
-0.587 |
0.000 |
| H3 |
0.860 |
1.297 |
0.000 |
| H4 |
-0.907 |
-1.012 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2242 | 1.0815 | 1.8843 |
N2 | 1.2242 | | 2.0698 | 1.0051 | H3 | 1.0815 | 2.0698 | | 2.9083 | H4 | 1.8843 | 1.0051 | 2.9083 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
115.048 |
|
H3 |
C1 |
N2 |
127.613 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.089 |
|
|
|
| 2 |
N |
-0.262 |
|
|
|
| 3 |
H |
0.156 |
|
|
|
| 4 |
H |
0.194 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.691 |
0.792 |
0.000 |
1.051 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.243 |
3.053 |
0.000 |
| y |
3.053 |
-11.486 |
0.000 |
| z |
0.000 |
0.000 |
-12.799 |
|
| Traceless |
| | x | y | z |
| x |
0.899 |
3.053 |
0.000 |
| y |
3.053 |
0.535 |
0.000 |
| z |
0.000 |
0.000 |
-1.434 |
|
| Polar |
| 3z2-r2 | -2.868 |
| x2-y2 | 0.243 |
| xy | 3.053 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.423 |
0.402 |
0.000 |
| y |
0.402 |
3.706 |
0.000 |
| z |
0.000 |
0.000 |
1.784 |
<r2> (average value of r
2) Å
2
| <r2> |
16.515 |
| (<r2>)1/2 |
4.064 |