Jump to
S1C2
Energy calculated at B3LYP/6-311G**
| | hartrees |
| Energy at 0K | -93.988595 |
| Energy at 298.15K | -93.989888 |
| HF Energy | -93.988595 |
| Nuclear repulsion energy | 28.250111 |
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 B3LYP/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' |
3281 |
3172 |
6.03 |
|
|
|
| 2 |
A' |
2948 |
2850 |
55.27 |
|
|
|
| 3 |
A' |
1861 |
1799 |
25.53 |
|
|
|
| 4 |
A' |
1002 |
969 |
149.90 |
|
|
|
| 5 |
A' |
875 |
846 |
109.43 |
|
|
|
| 6 |
A" |
905 |
875 |
5.08 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5435.8 cm
-1
Scaled (by 0.9668) Zero Point Vibrational Energy (zpe) 5255.3 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 B3LYP/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.111 |
0.636 |
0.000 |
| N2 |
0.111 |
-0.585 |
0.000 |
| H3 |
-0.678 |
1.403 |
0.000 |
| H4 |
-0.763 |
-1.127 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2206 | 1.1002 | 1.9676 |
N2 | 1.2206 | | 2.1386 | 1.0286 | H3 | 1.1002 | 2.1386 | | 2.5315 | H4 | 1.9676 | 1.0286 | 2.5315 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
121.812 |
|
H3 |
C1 |
N2 |
134.217 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.021 |
|
|
|
| 2 |
N |
-0.296 |
|
|
|
| 3 |
H |
0.120 |
|
|
|
| 4 |
H |
0.197 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.216 |
0.312 |
0.000 |
2.238 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.143 |
0.596 |
0.000 |
| y |
0.596 |
-11.165 |
0.000 |
| z |
0.000 |
0.000 |
-12.585 |
|
| Traceless |
| | x | y | z |
| x |
-0.268 |
0.596 |
0.000 |
| y |
0.596 |
1.199 |
0.000 |
| z |
0.000 |
0.000 |
-0.931 |
|
| Polar |
| 3z2-r2 | -1.862 |
| x2-y2 | -0.977 |
| xy | 0.596 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.169 |
0.088 |
0.000 |
| y |
0.088 |
4.013 |
0.000 |
| z |
0.000 |
0.000 |
1.435 |
<r2> (average value of r
2) Å
2
| <r2> |
16.733 |
| (<r2>)1/2 |
4.091 |
Jump to
S1C1
Energy calculated at B3LYP/6-311G**
| | hartrees |
| Energy at 0K | -93.996184 |
| Energy at 298.15K | -93.997528 |
| HF Energy | -93.996184 |
| Nuclear repulsion energy | 28.164038 |
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 B3LYP/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' |
3416 |
3302 |
4.18 |
|
|
|
| 2 |
A' |
2997 |
2898 |
29.37 |
|
|
|
| 3 |
A' |
1802 |
1742 |
25.59 |
|
|
|
| 4 |
A' |
1200 |
1160 |
10.11 |
|
|
|
| 5 |
A' |
914 |
884 |
220.25 |
|
|
|
| 6 |
A" |
974 |
942 |
120.06 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5651.5 cm
-1
Scaled (by 0.9668) Zero Point Vibrational Energy (zpe) 5463.9 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 B3LYP/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.000 |
0.648 |
0.000 |
| N2 |
-0.000 |
-0.584 |
0.000 |
| H3 |
0.904 |
1.271 |
0.000 |
| H4 |
-0.899 |
-1.072 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2320 | 1.0983 | 1.9409 |
N2 | 1.2320 | | 2.0634 | 1.0224 | H3 | 1.0983 | 2.0634 | | 2.9564 | H4 | 1.9409 | 1.0224 | 2.9564 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
118.547 |
|
H3 |
C1 |
N2 |
124.519 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.056 |
|
|
|
| 2 |
N |
-0.291 |
|
|
|
| 3 |
H |
0.133 |
|
|
|
| 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 |
| |
-0.470 |
0.115 |
0.000 |
0.484 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.246 |
3.130 |
0.000 |
| y |
3.130 |
-11.518 |
0.000 |
| z |
0.000 |
0.000 |
-12.623 |
|
| Traceless |
| | x | y | z |
| x |
0.825 |
3.130 |
0.000 |
| y |
3.130 |
0.417 |
0.000 |
| z |
0.000 |
0.000 |
-1.242 |
|
| Polar |
| 3z2-r2 | -2.483 |
| x2-y2 | 0.272 |
| xy | 3.130 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.355 |
0.453 |
0.000 |
| y |
0.453 |
3.774 |
0.000 |
| z |
0.000 |
0.000 |
1.517 |
<r2> (average value of r
2) Å
2
| <r2> |
16.664 |
| (<r2>)1/2 |
4.082 |