Jump to
S1C2
Energy calculated at mPW1PW91/6-311G**
| | hartrees |
| Energy at 0K | -93.957468 |
| Energy at 298.15K | -93.958768 |
| HF Energy | -93.957468 |
| Nuclear repulsion energy | 28.297434 |
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 mPW1PW91/6-311G**
| 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' |
3350 |
3205 |
3.94 |
|
|
|
| 2 |
A' |
2997 |
2867 |
51.22 |
|
|
|
| 3 |
A' |
1878 |
1796 |
29.71 |
|
|
|
| 4 |
A' |
1022 |
978 |
139.86 |
|
|
|
| 5 |
A' |
870 |
832 |
113.36 |
|
|
|
| 6 |
A" |
923 |
883 |
4.84 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5519.5 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 5280.5 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 mPW1PW91/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.111 |
0.634 |
0.000 |
| N2 |
0.111 |
-0.586 |
0.000 |
| H3 |
-0.672 |
1.405 |
0.000 |
| H4 |
-0.770 |
-1.109 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2195 | 1.0984 | 1.9532 |
N2 | 1.2195 | | 2.1385 | 1.0250 | H3 | 1.0984 | 2.1385 | | 2.5157 | H4 | 1.9532 | 1.0250 | 2.5157 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
120.720 |
|
H3 |
C1 |
N2 |
134.554 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.013 |
|
|
|
| 2 |
N |
-0.321 |
|
|
|
| 3 |
H |
0.131 |
|
|
|
| 4 |
H |
0.203 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.242 |
0.410 |
0.000 |
2.279 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.018 |
0.647 |
0.000 |
| y |
0.647 |
-11.075 |
0.000 |
| z |
0.000 |
0.000 |
-12.533 |
|
| Traceless |
| | x | y | z |
| x |
-0.214 |
0.647 |
0.000 |
| y |
0.647 |
1.201 |
0.000 |
| z |
0.000 |
0.000 |
-0.987 |
|
| Polar |
| 3z2-r2 | -1.973 |
| x2-y2 | -0.944 |
| xy | 0.647 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.140 |
0.081 |
0.000 |
| y |
0.081 |
3.946 |
0.000 |
| z |
0.000 |
0.000 |
1.433 |
<r2> (average value of r
2) Å
2
| <r2> |
16.636 |
| (<r2>)1/2 |
4.079 |
Jump to
S1C1
Energy calculated at mPW1PW91/6-311G**
| | hartrees |
| Energy at 0K | -93.965006 |
| Energy at 298.15K | -93.966353 |
| HF Energy | -93.965006 |
| Nuclear repulsion energy | 28.224139 |
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 mPW1PW91/6-311G**
| 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 |
3321 |
6.42 |
|
|
|
| 2 |
A' |
3042 |
2910 |
26.91 |
|
|
|
| 3 |
A' |
1829 |
1750 |
29.91 |
|
|
|
| 4 |
A' |
1203 |
1151 |
9.71 |
|
|
|
| 5 |
A' |
912 |
873 |
225.25 |
|
|
|
| 6 |
A" |
986 |
944 |
121.20 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5721.9 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 5474.1 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 mPW1PW91/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.646 |
0.000 |
| N2 |
0.000 |
-0.584 |
0.000 |
| H3 |
0.900 |
1.273 |
0.000 |
| H4 |
-0.900 |
-1.062 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2295 | 1.0967 | 1.9307 |
N2 | 1.2295 | | 2.0632 | 1.0197 | H3 | 1.0967 | 2.0632 | | 2.9484 | H4 | 1.9307 | 1.0197 | 2.9484 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
117.977 |
|
H3 |
C1 |
N2 |
124.881 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.051 |
|
|
|
| 2 |
N |
-0.314 |
|
|
|
| 3 |
H |
0.145 |
|
|
|
| 4 |
H |
0.220 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.501 |
0.198 |
0.000 |
0.539 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.138 |
3.162 |
0.000 |
| y |
3.162 |
-11.412 |
0.000 |
| z |
0.000 |
0.000 |
-12.574 |
|
| Traceless |
| | x | y | z |
| x |
0.855 |
3.162 |
0.000 |
| y |
3.162 |
0.444 |
0.000 |
| z |
0.000 |
0.000 |
-1.299 |
|
| Polar |
| 3z2-r2 | -2.598 |
| x2-y2 | 0.274 |
| xy | 3.162 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.328 |
0.414 |
0.000 |
| y |
0.414 |
3.763 |
0.000 |
| z |
0.000 |
0.000 |
1.513 |
<r2> (average value of r
2) Å
2
| <r2> |
16.569 |
| (<r2>)1/2 |
4.070 |