Jump to
S1C2
Energy calculated at B1B95/6-311G*
| | hartrees |
| Energy at 0K | -93.933587 |
| Energy at 298.15K | -93.934883 |
| HF Energy | -93.933587 |
| Nuclear repulsion energy | 28.338283 |
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 B1B95/6-311G*
| 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' |
3339 |
3201 |
5.45 |
|
|
|
| 2 |
A' |
2981 |
2857 |
60.29 |
|
|
|
| 3 |
A' |
1892 |
1814 |
29.27 |
|
|
|
| 4 |
A' |
1016 |
974 |
141.18 |
|
|
|
| 5 |
A' |
879 |
843 |
133.12 |
|
|
|
| 6 |
A" |
915 |
877 |
7.77 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5510.5 cm
-1
Scaled (by 0.9586) Zero Point Vibrational Energy (zpe) 5282.4 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 B1B95/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.111 |
0.635 |
0.000 |
| N2 |
0.111 |
-0.582 |
0.000 |
| H3 |
-0.686 |
1.391 |
0.000 |
| H4 |
-0.757 |
-1.126 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2169 | 1.0989 | 1.9629 |
N2 | 1.2169 | | 2.1280 | 1.0243 | H3 | 1.0989 | 2.1280 | | 2.5174 | H4 | 1.9629 | 1.0243 | 2.5174 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
122.047 |
|
H3 |
C1 |
N2 |
133.469 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.086 |
|
|
|
| 2 |
N |
-0.441 |
|
|
|
| 3 |
H |
0.215 |
|
|
|
| 4 |
H |
0.312 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.325 |
0.292 |
0.000 |
2.343 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.051 |
0.632 |
0.000 |
| y |
0.632 |
-11.059 |
0.000 |
| z |
0.000 |
0.000 |
-12.594 |
|
| Traceless |
| | x | y | z |
| x |
-0.224 |
0.632 |
0.000 |
| y |
0.632 |
1.264 |
0.000 |
| z |
0.000 |
0.000 |
-1.040 |
|
| Polar |
| 3z2-r2 | -2.079 |
| x2-y2 | -0.992 |
| xy | 0.632 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.101 |
0.085 |
0.000 |
| y |
0.085 |
3.933 |
0.000 |
| z |
0.000 |
0.000 |
1.385 |
<r2> (average value of r
2) Å
2
| <r2> |
16.629 |
| (<r2>)1/2 |
4.078 |
Jump to
S1C1
Energy calculated at B1B95/6-311G*
| | hartrees |
| Energy at 0K | -93.941992 |
| Energy at 298.15K | -93.943342 |
| HF Energy | -93.941992 |
| Nuclear repulsion energy | 28.254858 |
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 B1B95/6-311G*
| 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' |
3469 |
3325 |
2.44 |
|
|
|
| 2 |
A' |
3038 |
2912 |
32.79 |
|
|
|
| 3 |
A' |
1834 |
1758 |
29.06 |
|
|
|
| 4 |
A' |
1225 |
1174 |
12.37 |
|
|
|
| 5 |
A' |
928 |
889 |
230.07 |
|
|
|
| 6 |
A" |
988 |
947 |
126.89 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5740.2 cm
-1
Scaled (by 0.9586) Zero Point Vibrational Energy (zpe) 5502.5 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 B1B95/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.001 |
0.647 |
0.000 |
| N2 |
-0.001 |
-0.581 |
0.000 |
| H3 |
0.910 |
1.257 |
0.000 |
| H4 |
-0.895 |
-1.069 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2281 | 1.0967 | 1.9350 |
N2 | 1.2281 | | 2.0517 | 1.0187 | H3 | 1.0967 | 2.0517 | | 2.9447 | H4 | 1.9350 | 1.0187 | 2.9447 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
118.621 |
|
H3 |
C1 |
N2 |
123.802 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.120 |
|
|
|
| 2 |
N |
-0.434 |
|
|
|
| 3 |
H |
0.228 |
|
|
|
| 4 |
H |
0.326 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.509 |
0.102 |
0.000 |
0.519 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.125 |
3.237 |
0.000 |
| y |
3.237 |
-11.445 |
0.000 |
| z |
0.000 |
0.000 |
-12.634 |
|
| Traceless |
| | x | y | z |
| x |
0.915 |
3.237 |
0.000 |
| y |
3.237 |
0.434 |
0.000 |
| z |
0.000 |
0.000 |
-1.349 |
|
| Polar |
| 3z2-r2 | -2.698 |
| x2-y2 | 0.320 |
| xy | 3.237 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.290 |
0.421 |
0.000 |
| y |
0.421 |
3.718 |
0.000 |
| z |
0.000 |
0.000 |
1.451 |
<r2> (average value of r
2) Å
2
| <r2> |
16.558 |
| (<r2>)1/2 |
4.069 |