Jump to
S1C2
Energy calculated at B1B95/6-31+G**
| | hartrees |
| Energy at 0K | -93.921332 |
| Energy at 298.15K | -93.922613 |
| HF Energy | -93.921332 |
| Nuclear repulsion energy | 28.235597 |
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 B1B95/6-31+G**
| 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' |
3386 |
3240 |
1.88 |
|
|
|
| 2 |
A' |
3012 |
2882 |
47.16 |
|
|
|
| 3 |
A' |
1891 |
1809 |
43.06 |
|
|
|
| 4 |
A' |
1008 |
964 |
109.02 |
|
|
|
| 5 |
A' |
838 |
801 |
155.22 |
|
|
|
| 6 |
A" |
904 |
865 |
6.43 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5519.7 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 5280.2 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 B1B95/6-31+G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.110 |
0.638 |
0.000 |
| N2 |
0.110 |
-0.585 |
0.000 |
| H3 |
-0.682 |
1.399 |
0.000 |
| H4 |
-0.754 |
-1.134 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2228 | 1.0986 | 1.9714 |
N2 | 1.2228 | | 2.1364 | 1.0242 | H3 | 1.0986 | 2.1364 | | 2.5340 | H4 | 1.9714 | 1.0242 | 2.5340 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
122.398 |
|
H3 |
C1 |
N2 |
133.873 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.090 |
|
|
|
| 2 |
N |
-0.348 |
|
|
|
| 3 |
H |
0.151 |
|
|
|
| 4 |
H |
0.287 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.443 |
0.361 |
0.000 |
2.470 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.415 |
0.699 |
0.000 |
| y |
0.699 |
-11.276 |
0.000 |
| z |
0.000 |
0.000 |
-12.851 |
|
| Traceless |
| | x | y | z |
| x |
-0.352 |
0.699 |
0.000 |
| y |
0.699 |
1.357 |
0.000 |
| z |
0.000 |
0.000 |
-1.005 |
|
| Polar |
| 3z2-r2 | -2.011 |
| x2-y2 | -1.139 |
| xy | 0.699 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.392 |
0.082 |
0.000 |
| y |
0.082 |
4.385 |
0.000 |
| z |
0.000 |
0.000 |
1.729 |
<r2> (average value of r
2) Å
2
| <r2> |
16.880 |
| (<r2>)1/2 |
4.108 |
Jump to
S1C1
Energy calculated at B1B95/6-31+G**
| | hartrees |
| Energy at 0K | -93.930166 |
| Energy at 298.15K | -93.931504 |
| HF Energy | -93.930166 |
| Nuclear repulsion energy | 28.174801 |
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 B1B95/6-31+G**
| 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' |
3508 |
3356 |
13.65 |
|
|
|
| 2 |
A' |
3075 |
2942 |
20.06 |
|
|
|
| 3 |
A' |
1839 |
1759 |
38.53 |
|
|
|
| 4 |
A' |
1193 |
1141 |
11.74 |
|
|
|
| 5 |
A' |
899 |
860 |
231.06 |
|
|
|
| 6 |
A" |
980 |
938 |
129.39 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5746.8 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 5497.4 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 B1B95/6-31+G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.001 |
0.649 |
0.000 |
| N2 |
-0.001 |
-0.584 |
0.000 |
| H3 |
0.901 |
1.271 |
0.000 |
| H4 |
-0.893 |
-1.077 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2324 | 1.0961 | 1.9423 |
N2 | 1.2324 | | 2.0629 | 1.0191 | H3 | 1.0961 | 2.0629 | | 2.9550 | H4 | 1.9423 | 1.0191 | 2.9550 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
118.928 |
|
H3 |
C1 |
N2 |
124.625 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.085 |
|
|
|
| 2 |
N |
-0.375 |
|
|
|
| 3 |
H |
0.158 |
|
|
|
| 4 |
H |
0.301 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.510 |
0.175 |
0.000 |
0.539 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.490 |
3.476 |
0.000 |
| y |
3.476 |
-11.726 |
0.000 |
| z |
0.000 |
0.000 |
-12.934 |
|
| Traceless |
| | x | y | z |
| x |
0.840 |
3.476 |
0.000 |
| y |
3.476 |
0.486 |
0.000 |
| z |
0.000 |
0.000 |
-1.326 |
|
| Polar |
| 3z2-r2 | -2.651 |
| x2-y2 | 0.236 |
| xy | 3.476 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.569 |
0.138 |
0.000 |
| y |
0.138 |
4.268 |
0.000 |
| z |
0.000 |
0.000 |
1.859 |
<r2> (average value of r
2) Å
2
| <r2> |
16.821 |
| (<r2>)1/2 |
4.101 |