Jump to
S1C2
Energy calculated at B3PW91/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -93.927394 |
| Energy at 298.15K | -93.928682 |
| HF Energy | -93.927394 |
| Nuclear repulsion energy | 28.221953 |
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 B3PW91/6-31G(2df,p)
| 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' |
3345 |
3216 |
3.41 |
|
|
|
| 2 |
A' |
2990 |
2875 |
48.05 |
|
|
|
| 3 |
A' |
1872 |
1799 |
24.97 |
|
|
|
| 4 |
A' |
1009 |
971 |
129.09 |
|
|
|
| 5 |
A' |
855 |
822 |
124.36 |
|
|
|
| 6 |
A" |
909 |
873 |
4.97 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5489.5 cm
-1
Scaled (by 0.9614) Zero Point Vibrational Energy (zpe) 5277.6 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 B3PW91/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.111 |
0.636 |
0.000 |
| N2 |
0.111 |
-0.587 |
0.000 |
| H3 |
-0.675 |
1.407 |
0.000 |
| H4 |
-0.766 |
-1.119 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2232 | 1.1005 | 1.9622 |
N2 | 1.2232 | | 2.1429 | 1.0259 | H3 | 1.1005 | 2.1429 | | 2.5272 | H4 | 1.9622 | 1.0259 | 2.5272 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
121.238 |
|
H3 |
C1 |
N2 |
134.429 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.138 |
|
|
|
| 2 |
N |
-0.304 |
|
|
|
| 3 |
H |
0.167 |
|
|
|
| 4 |
H |
0.274 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.035 |
0.352 |
0.000 |
2.065 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.776 |
0.641 |
0.000 |
| y |
0.641 |
-10.781 |
0.000 |
| z |
0.000 |
0.000 |
-12.340 |
|
| Traceless |
| | x | y | z |
| x |
-0.216 |
0.641 |
0.000 |
| y |
0.641 |
1.278 |
0.000 |
| z |
0.000 |
0.000 |
-1.062 |
|
| Polar |
| 3z2-r2 | -2.124 |
| x2-y2 | -0.996 |
| xy | 0.641 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.143 |
0.056 |
0.000 |
| y |
0.056 |
3.834 |
0.000 |
| z |
0.000 |
0.000 |
1.520 |
<r2> (average value of r
2) Å
2
| <r2> |
16.539 |
| (<r2>)1/2 |
4.067 |
Jump to
S1C1
Energy calculated at B3PW91/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -93.934867 |
| Energy at 298.15K | -93.936208 |
| HF Energy | -93.934867 |
| Nuclear repulsion energy | 28.148797 |
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 B3PW91/6-31G(2df,p)
| 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' |
3461 |
3327 |
5.61 |
|
|
|
| 2 |
A' |
3034 |
2917 |
29.16 |
|
|
|
| 3 |
A' |
1819 |
1749 |
25.38 |
|
|
|
| 4 |
A' |
1199 |
1153 |
8.26 |
|
|
|
| 5 |
A' |
905 |
870 |
218.43 |
|
|
|
| 6 |
A" |
982 |
944 |
97.76 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5699.3 cm
-1
Scaled (by 0.9614) Zero Point Vibrational Energy (zpe) 5479.3 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 B3PW91/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.000 |
0.648 |
0.000 |
| N2 |
-0.000 |
-0.585 |
0.000 |
| H3 |
0.906 |
1.271 |
0.000 |
| H4 |
-0.900 |
-1.067 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2333 | 1.0996 | 1.9369 |
N2 | 1.2333 | | 2.0655 | 1.0209 | H3 | 1.0996 | 2.0655 | | 2.9544 | H4 | 1.9369 | 1.0209 | 2.9544 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
118.161 |
|
H3 |
C1 |
N2 |
124.495 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.166 |
|
|
|
| 2 |
N |
-0.294 |
|
|
|
| 3 |
H |
0.175 |
|
|
|
| 4 |
H |
0.285 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.481 |
0.146 |
0.000 |
0.502 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-10.972 |
2.964 |
0.000 |
| y |
2.964 |
-11.191 |
0.000 |
| z |
0.000 |
0.000 |
-12.379 |
|
| Traceless |
| | x | y | z |
| x |
0.813 |
2.964 |
0.000 |
| y |
2.964 |
0.484 |
0.000 |
| z |
0.000 |
0.000 |
-1.297 |
|
| Polar |
| 3z2-r2 | -2.595 |
| x2-y2 | 0.219 |
| xy | 2.964 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.329 |
0.513 |
0.000 |
| y |
0.513 |
3.658 |
0.000 |
| z |
0.000 |
0.000 |
1.558 |
<r2> (average value of r
2) Å
2
| <r2> |
16.494 |
| (<r2>)1/2 |
4.061 |