Jump to
S1C2
Energy calculated at mPW1PW91/6-31G*
| | hartrees |
| Energy at 0K | -93.927757 |
| Energy at 298.15K | -93.929058 |
| HF Energy | -93.927757 |
| Nuclear repulsion energy | 28.191370 |
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 mPW1PW91/6-31G*
| 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 |
3172 |
3.93 |
|
|
|
| 2 |
A' |
3033 |
2876 |
59.29 |
|
|
|
| 3 |
A' |
1888 |
1790 |
29.12 |
|
|
|
| 4 |
A' |
1043 |
989 |
135.17 |
|
|
|
| 5 |
A' |
888 |
842 |
122.12 |
|
|
|
| 6 |
A" |
922 |
875 |
6.66 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5559.2 cm
-1
Scaled (by 0.9483) Zero Point Vibrational Energy (zpe) 5271.7 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 mPW1PW91/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.111 |
0.637 |
0.000 |
| N2 |
0.111 |
-0.589 |
0.000 |
| H3 |
-0.673 |
1.407 |
0.000 |
| H4 |
-0.775 |
-1.108 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2255 | 1.0992 | 1.9572 |
N2 | 1.2255 | | 2.1440 | 1.0271 | H3 | 1.0992 | 2.1440 | | 2.5170 | H4 | 1.9572 | 1.0271 | 2.5170 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
120.397 |
|
H3 |
C1 |
N2 |
134.451 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.010 |
|
|
|
| 2 |
N |
-0.501 |
|
|
|
| 3 |
H |
0.177 |
|
|
|
| 4 |
H |
0.334 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.239 |
0.471 |
0.000 |
2.288 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.830 |
0.776 |
0.000 |
| y |
0.776 |
-10.903 |
0.000 |
| z |
0.000 |
0.000 |
-12.396 |
|
| Traceless |
| | x | y | z |
| x |
-0.180 |
0.776 |
0.000 |
| y |
0.776 |
1.210 |
0.000 |
| z |
0.000 |
0.000 |
-1.030 |
|
| Polar |
| 3z2-r2 | -2.060 |
| x2-y2 | -0.927 |
| xy | 0.776 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.916 |
0.043 |
0.000 |
| y |
0.043 |
3.776 |
0.000 |
| z |
0.000 |
0.000 |
1.183 |
<r2> (average value of r
2) Å
2
| <r2> |
16.594 |
| (<r2>)1/2 |
4.074 |
Jump to
S1C1
Energy calculated at mPW1PW91/6-31G*
| | hartrees |
| Energy at 0K | -93.935955 |
| Energy at 298.15K | -93.937303 |
| HF Energy | -93.935955 |
| Nuclear repulsion energy | 28.129910 |
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 mPW1PW91/6-31G*
| 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' |
3471 |
3292 |
2.98 |
|
|
|
| 2 |
A' |
3082 |
2922 |
33.33 |
|
|
|
| 3 |
A' |
1841 |
1746 |
29.14 |
|
|
|
| 4 |
A' |
1231 |
1167 |
12.10 |
|
|
|
| 5 |
A' |
929 |
881 |
225.44 |
|
|
|
| 6 |
A" |
995 |
943 |
116.70 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5774.4 cm
-1
Scaled (by 0.9483) Zero Point Vibrational Energy (zpe) 5475.9 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 mPW1PW91/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.000 |
0.649 |
0.000 |
| N2 |
-0.000 |
-0.586 |
0.000 |
| H3 |
0.906 |
1.268 |
0.000 |
| H4 |
-0.904 |
-1.061 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2351 | 1.0975 | 1.9349 |
N2 | 1.2351 | | 2.0634 | 1.0216 | H3 | 1.0975 | 2.0634 | | 2.9502 | H4 | 1.9349 | 1.0216 | 2.9502 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
117.747 |
|
H3 |
C1 |
N2 |
124.300 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.048 |
|
|
|
| 2 |
N |
-0.490 |
|
|
|
| 3 |
H |
0.190 |
|
|
|
| 4 |
H |
0.348 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.585 |
0.245 |
0.000 |
0.634 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-10.976 |
3.095 |
0.000 |
| y |
3.095 |
-11.266 |
0.000 |
| z |
0.000 |
0.000 |
-12.428 |
|
| Traceless |
| | x | y | z |
| x |
0.872 |
3.095 |
0.000 |
| y |
3.095 |
0.436 |
0.000 |
| z |
0.000 |
0.000 |
-1.307 |
|
| Polar |
| 3z2-r2 | -2.615 |
| x2-y2 | 0.291 |
| xy | 3.095 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.151 |
0.500 |
0.000 |
| y |
0.500 |
3.608 |
0.000 |
| z |
0.000 |
0.000 |
1.229 |
<r2> (average value of r
2) Å
2
| <r2> |
16.523 |
| (<r2>)1/2 |
4.065 |