Jump to
S1C2
Energy calculated at wB97X-D/TZVP
| | hartrees |
| Energy at 0K | -93.956814 |
| Energy at 298.15K | -93.958107 |
| HF Energy | -93.956814 |
| Nuclear repulsion energy | 28.343867 |
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/TZVP
| 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' |
3387 |
3235 |
1.69 |
|
|
|
| 2 |
A' |
3008 |
2872 |
41.67 |
|
|
|
| 3 |
A' |
1886 |
1801 |
41.23 |
|
|
|
| 4 |
A' |
1015 |
969 |
114.37 |
|
|
|
| 5 |
A' |
849 |
810 |
149.57 |
|
|
|
| 6 |
A" |
928 |
886 |
6.41 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5535.8 cm
-1
Scaled (by 0.955) Zero Point Vibrational Energy (zpe) 5286.7 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/TZVP
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.111 |
0.635 |
0.000 |
| N2 |
0.111 |
-0.583 |
0.000 |
| H3 |
-0.683 |
1.393 |
0.000 |
| H4 |
-0.759 |
-1.120 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2174 | 1.0980 | 1.9586 |
N2 | 1.2174 | | 2.1293 | 1.0226 | H3 | 1.0980 | 2.1293 | | 2.5143 | H4 | 1.9586 | 1.0226 | 2.5143 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
121.702 |
|
H3 |
C1 |
N2 |
133.683 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.059 |
|
|
|
| 2 |
N |
-0.275 |
|
|
|
| 3 |
H |
0.122 |
|
|
|
| 4 |
H |
0.212 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.408 |
0.366 |
0.000 |
2.436 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.291 |
0.681 |
0.000 |
| y |
0.681 |
-11.214 |
0.000 |
| z |
0.000 |
0.000 |
-12.693 |
|
| Traceless |
| | x | y | z |
| x |
-0.338 |
0.681 |
0.000 |
| y |
0.681 |
1.278 |
0.000 |
| z |
0.000 |
0.000 |
-0.940 |
|
| Polar |
| 3z2-r2 | -1.881 |
| x2-y2 | -1.077 |
| xy | 0.681 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.319 |
0.093 |
0.000 |
| y |
0.093 |
4.288 |
0.000 |
| z |
0.000 |
0.000 |
1.640 |
<r2> (average value of r
2) Å
2
| <r2> |
16.741 |
| (<r2>)1/2 |
4.092 |
Jump to
S1C1
Energy calculated at wB97X-D/TZVP
| | hartrees |
| Energy at 0K | -93.964850 |
| Energy at 298.15K | -93.966192 |
| HF Energy | -93.964850 |
| Nuclear repulsion energy | 28.274933 |
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/TZVP
| 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' |
3491 |
3334 |
9.39 |
|
|
|
| 2 |
A' |
3052 |
2915 |
21.27 |
|
|
|
| 3 |
A' |
1835 |
1752 |
37.47 |
|
|
|
| 4 |
A' |
1193 |
1139 |
10.22 |
|
|
|
| 5 |
A' |
898 |
858 |
236.49 |
|
|
|
| 6 |
A" |
989 |
944 |
127.49 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5729.0 cm
-1
Scaled (by 0.955) Zero Point Vibrational Energy (zpe) 5471.2 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 wB97X-D/TZVP
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 |
0.899 |
1.270 |
0.000 |
| H4 |
-0.894 |
-1.069 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2263 | 1.0953 | 1.9332 |
N2 | 1.2263 | | 2.0585 | 1.0180 | H3 | 1.0953 | 2.0585 | | 2.9476 | H4 | 1.9332 | 1.0180 | 2.9476 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
118.642 |
|
H3 |
C1 |
N2 |
124.819 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.100 |
|
|
|
| 2 |
N |
-0.271 |
|
|
|
| 3 |
H |
0.137 |
|
|
|
| 4 |
H |
0.233 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.508 |
0.196 |
0.000 |
0.545 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.385 |
3.375 |
0.000 |
| y |
3.375 |
-11.609 |
0.000 |
| z |
0.000 |
0.000 |
-12.767 |
|
| Traceless |
| | x | y | z |
| x |
0.803 |
3.375 |
0.000 |
| y |
3.375 |
0.467 |
0.000 |
| z |
0.000 |
0.000 |
-1.270 |
|
| Polar |
| 3z2-r2 | -2.541 |
| x2-y2 | 0.224 |
| xy | 3.375 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.524 |
0.301 |
0.000 |
| y |
0.301 |
4.135 |
0.000 |
| z |
0.000 |
0.000 |
1.771 |
<r2> (average value of r
2) Å
2
| <r2> |
16.687 |
| (<r2>)1/2 |
4.085 |