Jump to
S1C2
Energy calculated at B3LYP/aug-cc-pVQZ
| | hartrees |
| Energy at 0K | -94.008857 |
| Energy at 298.15K | -94.010148 |
| HF Energy | -94.008857 |
| Nuclear repulsion energy | 28.339565 |
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/aug-cc-pVQZ
| 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' |
3299 |
3197 |
1.57 |
|
|
|
| 2 |
A' |
2964 |
2871 |
47.02 |
|
|
|
| 3 |
A' |
1856 |
1799 |
32.80 |
|
|
|
| 4 |
A' |
1002 |
971 |
148.06 |
|
|
|
| 5 |
A' |
866 |
839 |
106.63 |
|
|
|
| 6 |
A" |
902 |
874 |
4.11 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5444.6 cm
-1
Scaled (by 0.9689) Zero Point Vibrational Energy (zpe) 5275.3 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/aug-cc-pVQZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.110 |
0.635 |
0.000 |
| N2 |
0.110 |
-0.581 |
0.000 |
| H3 |
-0.679 |
1.397 |
0.000 |
| H4 |
-0.751 |
-1.137 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2166 | 1.0964 | 1.9701 |
N2 | 1.2166 | | 2.1297 | 1.0247 | H3 | 1.0964 | 2.1297 | | 2.5347 | H4 | 1.9701 | 1.0247 | 2.5347 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
122.818 |
|
H3 |
C1 |
N2 |
134.013 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/aug-cc-pVQZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.165 |
|
|
|
| 2 |
N |
-0.503 |
|
|
|
| 3 |
H |
0.368 |
|
|
|
| 4 |
H |
0.300 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.110 |
0.316 |
0.000 |
2.134 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.525 |
0.572 |
0.000 |
| y |
0.572 |
-11.329 |
0.000 |
| z |
0.000 |
0.000 |
-12.918 |
|
| Traceless |
| | x | y | z |
| x |
-0.402 |
0.572 |
0.000 |
| y |
0.572 |
1.392 |
0.000 |
| z |
0.000 |
0.000 |
-0.991 |
|
| Polar |
| 3z2-r2 | -1.982 |
| x2-y2 | -1.196 |
| xy | 0.572 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.183 |
0.140 |
0.000 |
| y |
0.140 |
4.694 |
0.000 |
| z |
0.000 |
0.000 |
2.493 |
<r2> (average value of r
2) Å
2
| <r2> |
16.868 |
| (<r2>)1/2 |
4.107 |
Jump to
S1C1
Energy calculated at B3LYP/aug-cc-pVQZ
| | hartrees |
| Energy at 0K | -94.016108 |
| Energy at 298.15K | -94.017447 |
| HF Energy | -94.016108 |
| Nuclear repulsion energy | 28.268525 |
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/aug-cc-pVQZ
| 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' |
3425 |
3319 |
8.54 |
|
|
|
| 2 |
A' |
3013 |
2919 |
22.74 |
|
|
|
| 3 |
A' |
1801 |
1745 |
32.53 |
|
|
|
| 4 |
A' |
1182 |
1145 |
12.68 |
|
|
|
| 5 |
A' |
909 |
880 |
219.80 |
|
|
|
| 6 |
A" |
967 |
937 |
105.15 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5648.5 cm
-1
Scaled (by 0.9689) Zero Point Vibrational Energy (zpe) 5472.8 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/aug-cc-pVQZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.000 |
0.645 |
0.000 |
| N2 |
-0.000 |
-0.581 |
0.000 |
| H3 |
0.892 |
1.279 |
0.000 |
| H4 |
-0.887 |
-1.084 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2264 | 1.0943 | 1.9429 |
N2 | 1.2264 | | 2.0630 | 1.0189 | H3 | 1.0943 | 2.0630 | | 2.9572 | H4 | 1.9429 | 1.0189 | 2.9572 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
119.554 |
|
H3 |
C1 |
N2 |
125.386 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/aug-cc-pVQZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.239 |
|
|
|
| 2 |
N |
-0.448 |
|
|
|
| 3 |
H |
0.373 |
|
|
|
| 4 |
H |
0.313 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.402 |
0.142 |
0.000 |
0.427 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.689 |
3.236 |
0.000 |
| y |
3.236 |
-11.727 |
0.000 |
| z |
0.000 |
0.000 |
-12.984 |
|
| Traceless |
| | x | y | z |
| x |
0.667 |
3.236 |
0.000 |
| y |
3.236 |
0.610 |
0.000 |
| z |
0.000 |
0.000 |
-1.277 |
|
| Polar |
| 3z2-r2 | -2.554 |
| x2-y2 | 0.038 |
| xy | 3.236 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.230 |
0.159 |
0.000 |
| y |
0.159 |
4.521 |
0.000 |
| z |
0.000 |
0.000 |
2.555 |
<r2> (average value of r
2) Å
2
| <r2> |
16.832 |
| (<r2>)1/2 |
4.103 |