Jump to
S1C2
Energy calculated at wB97X-D/cc-pVDZ
| hartrees |
Energy at 0K | -93.929858 |
Energy at 298.15K | -93.931150 |
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/cc-pVDZ
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 |
3265 |
3.05 |
|
|
|
2 |
A' |
3027 |
2884 |
44.28 |
|
|
|
3 |
A' |
1878 |
1789 |
47.67 |
|
|
|
4 |
A' |
1029 |
980 |
112.99 |
|
|
|
5 |
A' |
849 |
809 |
148.65 |
|
|
|
6 |
A" |
914 |
871 |
5.85 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5561.9 cm
-1
Scaled (by 0.9526) Zero Point Vibrational Energy (zpe) 5298.3 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 wB97X-D/cc-pVDZ
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/cc-pVDZ
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/cc-pVDZ
| hartrees |
Energy at 0K | -93.938444 |
Energy at 298.15K | -93.939786 |
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/cc-pVDZ
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 |
3361 |
14.40 |
|
|
|
2 |
A' |
3079 |
2933 |
19.69 |
|
|
|
3 |
A' |
1833 |
1746 |
42.64 |
|
|
|
4 |
A' |
1197 |
1140 |
11.70 |
|
|
|
5 |
A' |
899 |
857 |
240.53 |
|
|
|
6 |
A" |
983 |
936 |
135.09 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5759.4 cm
-1
Scaled (by 0.9526) Zero Point Vibrational Energy (zpe) 5486.4 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 wB97X-D/cc-pVDZ
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/cc-pVDZ
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 |