Jump to
S1C2
Energy calculated at LSDA/cc-pVDZ
| | hartrees |
| Energy at 0K | -93.429817 |
| Energy at 298.15K | -93.431074 |
| HF Energy | -93.429817 |
| Nuclear repulsion energy | 28.024825 |
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 LSDA/cc-pVDZ
| 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' |
3163 |
3128 |
13.98 |
|
|
|
| 2 |
A' |
2874 |
2843 |
53.02 |
|
|
|
| 3 |
A' |
1873 |
1852 |
19.50 |
|
|
|
| 4 |
A' |
926 |
916 |
162.24 |
|
|
|
| 5 |
A' |
841 |
832 |
88.78 |
|
|
|
| 6 |
A" |
863 |
854 |
4.31 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5270.1 cm
-1
Scaled (by 0.989) Zero Point Vibrational Energy (zpe) 5212.1 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 LSDA/cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.113 |
0.640 |
0.000 |
| N2 |
0.113 |
-0.586 |
0.000 |
| H3 |
-0.697 |
1.416 |
0.000 |
| H4 |
-0.766 |
-1.152 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2255 | 1.1214 | 1.9954 |
N2 | 1.2255 | | 2.1591 | 1.0451 | H3 | 1.1214 | 2.1591 | | 2.5688 | H4 | 1.9954 | 1.0451 | 2.5688 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
122.804 |
|
H3 |
C1 |
N2 |
133.800 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.120 |
|
|
|
| 2 |
N |
-0.098 |
|
|
|
| 3 |
H |
0.087 |
|
|
|
| 4 |
H |
0.131 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.116 |
0.016 |
0.000 |
2.116 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.088 |
0.422 |
0.000 |
| y |
0.422 |
-10.969 |
0.000 |
| z |
0.000 |
0.000 |
-12.455 |
|
| Traceless |
| | x | y | z |
| x |
-0.376 |
0.422 |
0.000 |
| y |
0.422 |
1.303 |
0.000 |
| z |
0.000 |
0.000 |
-0.927 |
|
| Polar |
| 3z2-r2 | -1.853 |
| x2-y2 | -1.119 |
| xy | 0.422 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.184 |
0.074 |
0.000 |
| y |
0.074 |
4.041 |
0.000 |
| z |
0.000 |
0.000 |
1.351 |
<r2> (average value of r
2) Å
2
| <r2> |
16.819 |
| (<r2>)1/2 |
4.101 |
Jump to
S1C1
Energy calculated at LSDA/cc-pVDZ
| | hartrees |
| Energy at 0K | -93.436685 |
| Energy at 298.15K | -93.438004 |
| HF Energy | -93.436685 |
| Nuclear repulsion energy | 27.942695 |
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 LSDA/cc-pVDZ
| 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' |
3306 |
3269 |
4.94 |
|
|
|
| 2 |
A' |
2922 |
2890 |
26.17 |
|
|
|
| 3 |
A' |
1811 |
1791 |
16.75 |
|
|
|
| 4 |
A' |
1134 |
1121 |
7.31 |
|
|
|
| 5 |
A' |
872 |
862 |
201.55 |
|
|
|
| 6 |
A" |
937 |
927 |
105.52 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5490.4 cm
-1
Scaled (by 0.989) Zero Point Vibrational Energy (zpe) 5430.0 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 LSDA/cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.002 |
0.652 |
0.000 |
| N2 |
-0.002 |
-0.585 |
0.000 |
| H3 |
0.935 |
1.266 |
0.000 |
| H4 |
-0.915 |
-1.081 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2376 | 1.1200 | 1.9588 |
N2 | 1.2376 | | 2.0749 | 1.0387 | H3 | 1.1200 | 2.0749 | | 2.9881 | H4 | 1.9588 | 1.0387 | 2.9881 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
118.487 |
|
H3 |
C1 |
N2 |
123.224 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.155 |
|
|
|
| 2 |
N |
-0.101 |
|
|
|
| 3 |
H |
0.104 |
|
|
|
| 4 |
H |
0.153 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.392 |
-0.174 |
0.000 |
0.429 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.113 |
3.058 |
0.000 |
| y |
3.058 |
-11.419 |
0.000 |
| z |
0.000 |
0.000 |
-12.486 |
|
| Traceless |
| | x | y | z |
| x |
0.840 |
3.058 |
0.000 |
| y |
3.058 |
0.381 |
0.000 |
| z |
0.000 |
0.000 |
-1.221 |
|
| Polar |
| 3z2-r2 | -2.441 |
| x2-y2 | 0.306 |
| xy | 3.058 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.388 |
0.615 |
0.000 |
| y |
0.615 |
3.666 |
0.000 |
| z |
0.000 |
0.000 |
1.391 |
<r2> (average value of r
2) Å
2
| <r2> |
16.723 |
| (<r2>)1/2 |
4.089 |