Jump to
S1C2
Energy calculated at LSDA/6-311G**
| | hartrees |
| Energy at 0K | -93.455615 |
| Energy at 298.15K | -93.456881 |
| HF Energy | -93.455615 |
| Nuclear repulsion energy | 28.220947 |
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/6-311G**
| 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' |
3183 |
3144 |
12.83 |
|
|
|
| 2 |
A' |
2875 |
2840 |
50.88 |
|
|
|
| 3 |
A' |
1874 |
1851 |
20.41 |
|
|
|
| 4 |
A' |
933 |
922 |
162.85 |
|
|
|
| 5 |
A' |
847 |
837 |
101.20 |
|
|
|
| 6 |
A" |
882 |
871 |
6.38 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5297.1 cm
-1
Scaled (by 0.9877) Zero Point Vibrational Energy (zpe) 5231.9 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 LSDA/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.111 |
0.637 |
0.000 |
| N2 |
0.111 |
-0.580 |
0.000 |
| H3 |
-0.692 |
1.404 |
0.000 |
| H4 |
-0.746 |
-1.167 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2166 | 1.1107 | 1.9968 |
N2 | 1.2166 | | 2.1404 | 1.0383 | H3 | 1.1107 | 2.1404 | | 2.5720 | H4 | 1.9968 | 1.0383 | 2.5720 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
124.443 |
|
H3 |
C1 |
N2 |
133.713 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.064 |
|
|
|
| 2 |
N |
-0.294 |
|
|
|
| 3 |
H |
0.144 |
|
|
|
| 4 |
H |
0.214 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.265 |
0.060 |
0.000 |
2.266 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.278 |
0.464 |
0.000 |
| y |
0.464 |
-11.058 |
0.000 |
| z |
0.000 |
0.000 |
-12.662 |
|
| Traceless |
| | x | y | z |
| x |
-0.418 |
0.464 |
0.000 |
| y |
0.464 |
1.412 |
0.000 |
| z |
0.000 |
0.000 |
-0.994 |
|
| Polar |
| 3z2-r2 | -1.988 |
| x2-y2 | -1.220 |
| xy | 0.464 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.260 |
0.106 |
0.000 |
| y |
0.106 |
4.189 |
0.000 |
| z |
0.000 |
0.000 |
1.462 |
<r2> (average value of r
2) Å
2
| <r2> |
16.810 |
| (<r2>)1/2 |
4.100 |
Jump to
S1C1
Energy calculated at LSDA/6-311G**
| | hartrees |
| Energy at 0K | -93.462656 |
| Energy at 298.15K | -93.463980 |
| HF Energy | -93.462656 |
| Nuclear repulsion energy | 28.136241 |
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/6-311G**
| 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' |
3329 |
3288 |
5.97 |
|
|
|
| 2 |
A' |
2925 |
2889 |
22.48 |
|
|
|
| 3 |
A' |
1811 |
1789 |
18.31 |
|
|
|
| 4 |
A' |
1137 |
1123 |
8.21 |
|
|
|
| 5 |
A' |
880 |
869 |
211.93 |
|
|
|
| 6 |
A" |
949 |
937 |
119.49 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5515.1 cm
-1
Scaled (by 0.9877) Zero Point Vibrational Energy (zpe) 5447.2 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/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.002 |
0.648 |
0.000 |
| N2 |
-0.002 |
-0.581 |
0.000 |
| H3 |
0.919 |
1.266 |
0.000 |
| H4 |
-0.899 |
-1.091 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2288 | 1.1089 | 1.9565 |
N2 | 1.2288 | | 2.0636 | 1.0318 | H3 | 1.1089 | 2.0636 | | 2.9763 | H4 | 1.9565 | 1.0318 | 2.9763 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
119.621 |
|
H3 |
C1 |
N2 |
123.873 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.104 |
|
|
|
| 2 |
N |
-0.289 |
|
|
|
| 3 |
H |
0.159 |
|
|
|
| 4 |
H |
0.233 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.418 |
-0.092 |
0.000 |
0.428 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.252 |
3.290 |
0.000 |
| y |
3.290 |
-11.539 |
0.000 |
| z |
0.000 |
0.000 |
-12.707 |
|
| Traceless |
| | x | y | z |
| x |
0.871 |
3.290 |
0.000 |
| y |
3.290 |
0.440 |
0.000 |
| z |
0.000 |
0.000 |
-1.311 |
|
| Polar |
| 3z2-r2 | -2.622 |
| x2-y2 | 0.287 |
| xy | 3.290 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.420 |
0.512 |
0.000 |
| y |
0.512 |
3.795 |
0.000 |
| z |
0.000 |
0.000 |
1.530 |
<r2> (average value of r
2) Å
2
| <r2> |
16.716 |
| (<r2>)1/2 |
4.088 |