Jump to
S1C2
Energy calculated at LSDA/6-31G*
| | hartrees |
| Energy at 0K | -93.422927 |
| Energy at 298.15K | -93.424191 |
| HF Energy | -93.422927 |
| Nuclear repulsion energy | 28.082142 |
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/6-31G*
| 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' |
3180 |
3121 |
13.56 |
|
|
|
| 2 |
A' |
2900 |
2846 |
58.44 |
|
|
|
| 3 |
A' |
1884 |
1849 |
21.04 |
|
|
|
| 4 |
A' |
952 |
934 |
138.05 |
|
|
|
| 5 |
A' |
859 |
842 |
126.22 |
|
|
|
| 6 |
A" |
874 |
858 |
8.18 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5324.3 cm
-1
Scaled (by 0.9813) Zero Point Vibrational Energy (zpe) 5224.7 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 LSDA/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.111 |
0.641 |
0.000 |
| N2 |
0.111 |
-0.584 |
0.000 |
| H3 |
-0.696 |
1.407 |
0.000 |
| H4 |
-0.750 |
-1.167 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2243 | 1.1130 | 2.0023 |
N2 | 1.2243 | | 2.1480 | 1.0404 | H3 | 1.1130 | 2.1480 | | 2.5740 | H4 | 2.0023 | 1.0404 | 2.5740 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
124.085 |
|
H3 |
C1 |
N2 |
133.494 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.050 |
|
|
|
| 2 |
N |
-0.446 |
|
|
|
| 3 |
H |
0.170 |
|
|
|
| 4 |
H |
0.327 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.223 |
0.097 |
0.000 |
2.225 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.005 |
0.599 |
0.000 |
| y |
0.599 |
-10.819 |
0.000 |
| z |
0.000 |
0.000 |
-12.434 |
|
| Traceless |
| | x | y | z |
| x |
-0.379 |
0.599 |
0.000 |
| y |
0.599 |
1.401 |
0.000 |
| z |
0.000 |
0.000 |
-1.022 |
|
| Polar |
| 3z2-r2 | -2.045 |
| x2-y2 | -1.186 |
| xy | 0.599 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.004 |
0.071 |
0.000 |
| y |
0.071 |
3.991 |
0.000 |
| z |
0.000 |
0.000 |
1.204 |
<r2> (average value of r
2) Å
2
| <r2> |
16.737 |
| (<r2>)1/2 |
4.091 |
Jump to
S1C1
Energy calculated at LSDA/6-31G*
| | hartrees |
| Energy at 0K | -93.430722 |
| Energy at 298.15K | -93.432048 |
| HF Energy | -93.430722 |
| Nuclear repulsion energy | 28.005087 |
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/6-31G*
| 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' |
3323 |
3261 |
1.90 |
|
|
|
| 2 |
A' |
2955 |
2900 |
30.35 |
|
|
|
| 3 |
A' |
1819 |
1785 |
17.93 |
|
|
|
| 4 |
A' |
1166 |
1144 |
9.46 |
|
|
|
| 5 |
A' |
896 |
879 |
209.01 |
|
|
|
| 6 |
A" |
954 |
937 |
110.78 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5557.0 cm
-1
Scaled (by 0.9813) Zero Point Vibrational Energy (zpe) 5453.0 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/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.002 |
0.652 |
0.000 |
| N2 |
-0.002 |
-0.584 |
0.000 |
| H3 |
0.928 |
1.260 |
0.000 |
| H4 |
-0.905 |
-1.087 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2366 | 1.1109 | 1.9600 |
N2 | 1.2366 | | 2.0654 | 1.0341 | H3 | 1.1109 | 2.0654 | | 2.9783 | H4 | 1.9600 | 1.0341 | 2.9783 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
119.086 |
|
H3 |
C1 |
N2 |
123.158 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.086 |
|
|
|
| 2 |
N |
-0.442 |
|
|
|
| 3 |
H |
0.183 |
|
|
|
| 4 |
H |
0.344 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.505 |
-0.056 |
0.000 |
0.508 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.022 |
3.165 |
0.000 |
| y |
3.165 |
-11.362 |
0.000 |
| z |
0.000 |
0.000 |
-12.475 |
|
| Traceless |
| | x | y | z |
| x |
0.897 |
3.165 |
0.000 |
| y |
3.165 |
0.386 |
0.000 |
| z |
0.000 |
0.000 |
-1.283 |
|
| Polar |
| 3z2-r2 | -2.567 |
| x2-y2 | 0.340 |
| xy | 3.165 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.240 |
0.617 |
0.000 |
| y |
0.617 |
3.635 |
0.000 |
| z |
0.000 |
0.000 |
1.236 |
<r2> (average value of r
2) Å
2
| <r2> |
16.650 |
| (<r2>)1/2 |
4.080 |