Jump to
S1C2
Energy calculated at wB97X-D/6-31+G**
| | hartrees |
| Energy at 0K | -93.929858 |
| Energy at 298.15K | -93.931148 |
| HF Energy | -93.929858 |
| Nuclear repulsion energy | 28.184374 |
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 wB97X-D/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' |
3427 |
3264 |
3.05 |
|
|
|
| 2 |
A' |
3027 |
2883 |
44.28 |
|
|
|
| 3 |
A' |
1878 |
1789 |
47.67 |
|
|
|
| 4 |
A' |
1029 |
980 |
112.99 |
|
|
|
| 5 |
A' |
849 |
808 |
148.65 |
|
|
|
| 6 |
A" |
914 |
870 |
5.85 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5561.9 cm
-1
Scaled (by 0.9523) Zero Point Vibrational Energy (zpe) 5296.6 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 wB97X-D/6-31+G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.111 |
0.639 |
0.000 |
| N2 |
0.111 |
-0.587 |
0.000 |
| H3 |
-0.685 |
1.397 |
0.000 |
| H4 |
-0.762 |
-1.123 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2261 | 1.0995 | 1.9664 |
N2 | 1.2261 | | 2.1378 | 1.0243 | H3 | 1.0995 | 2.1378 | | 2.5209 | H4 | 1.9664 | 1.0243 | 2.5209 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
121.555 |
|
H3 |
C1 |
N2 |
133.558 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.090 |
|
|
|
| 2 |
N |
-0.358 |
|
|
|
| 3 |
H |
0.156 |
|
|
|
| 4 |
H |
0.292 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.498 |
0.467 |
0.000 |
2.541 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.357 |
0.748 |
0.000 |
| y |
0.748 |
-11.287 |
0.000 |
| z |
0.000 |
0.000 |
-12.882 |
|
| Traceless |
| | x | y | z |
| x |
-0.272 |
0.748 |
0.000 |
| y |
0.748 |
1.332 |
0.000 |
| z |
0.000 |
0.000 |
-1.060 |
|
| Polar |
| 3z2-r2 | -2.120 |
| x2-y2 | -1.070 |
| xy | 0.748 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.369 |
0.064 |
0.000 |
| y |
0.064 |
4.364 |
0.000 |
| z |
0.000 |
0.000 |
1.753 |
<r2> (average value of r
2) Å
2
| <r2> |
16.893 |
| (<r2>)1/2 |
4.110 |
Jump to
S1C1
Energy calculated at wB97X-D/6-31+G**
| | hartrees |
| Energy at 0K | -93.938444 |
| Energy at 298.15K | -93.939784 |
| HF Energy | -93.938444 |
| Nuclear repulsion energy | 28.128692 |
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 wB97X-D/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' |
3529 |
3360 |
14.40 |
|
|
|
| 2 |
A' |
3079 |
2933 |
19.69 |
|
|
|
| 3 |
A' |
1833 |
1745 |
42.64 |
|
|
|
| 4 |
A' |
1197 |
1139 |
11.70 |
|
|
|
| 5 |
A' |
899 |
856 |
240.53 |
|
|
|
| 6 |
A" |
983 |
936 |
135.09 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5759.4 cm
-1
Scaled (by 0.9523) Zero Point Vibrational Energy (zpe) 5484.7 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 wB97X-D/6-31+G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.000 |
0.649 |
0.000 |
| N2 |
-0.000 |
-0.585 |
0.000 |
| H3 |
0.901 |
1.274 |
0.000 |
| H4 |
-0.896 |
-1.073 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2344 | 1.0965 | 1.9412 |
N2 | 1.2344 | | 2.0661 | 1.0198 | H3 | 1.0965 | 2.0661 | | 2.9558 | H4 | 1.9412 | 1.0198 | 2.9558 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
118.586 |
|
H3 |
C1 |
N2 |
124.743 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.087 |
|
|
|
| 2 |
N |
-0.384 |
|
|
|
| 3 |
H |
0.164 |
|
|
|
| 4 |
H |
0.307 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.537 |
0.272 |
0.000 |
0.602 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.455 |
3.528 |
0.000 |
| y |
3.528 |
-11.689 |
0.000 |
| z |
0.000 |
0.000 |
-12.962 |
|
| Traceless |
| | x | y | z |
| x |
0.870 |
3.528 |
0.000 |
| y |
3.528 |
0.520 |
0.000 |
| z |
0.000 |
0.000 |
-1.390 |
|
| Polar |
| 3z2-r2 | -2.779 |
| x2-y2 | 0.233 |
| xy | 3.528 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.560 |
0.120 |
0.000 |
| y |
0.120 |
4.290 |
0.000 |
| z |
0.000 |
0.000 |
1.888 |
<r2> (average value of r
2) Å
2
| <r2> |
16.842 |
| (<r2>)1/2 |
4.104 |