Jump to
S1C2
Energy calculated at B1B95/3-21G*
| | hartrees |
| Energy at 0K | -93.385399 |
| Energy at 298.15K | -93.386701 |
| HF Energy | -93.385399 |
| Nuclear repulsion energy | 28.157621 |
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 B1B95/3-21G*
| 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' |
3233 |
3087 |
3.30 |
|
|
|
| 2 |
A' |
2976 |
2842 |
51.89 |
|
|
|
| 3 |
A' |
1889 |
1804 |
16.75 |
|
|
|
| 4 |
A' |
982 |
938 |
83.94 |
|
|
|
| 5 |
A' |
894 |
853 |
223.27 |
|
|
|
| 6 |
A" |
956 |
913 |
11.38 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5464.7 cm
-1
Scaled (by 0.9549) Zero Point Vibrational Energy (zpe) 5218.2 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 B1B95/3-21G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.105 |
0.643 |
0.000 |
| N2 |
0.105 |
-0.579 |
0.000 |
| H3 |
-0.666 |
1.423 |
0.000 |
| H4 |
-0.702 |
-1.224 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2218 | 1.0977 | 2.0331 |
N2 | 1.2218 | | 2.1460 | 1.0326 | H3 | 1.0977 | 2.1460 | | 2.6469 | H4 | 2.0331 | 1.0326 | 2.6469 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
128.601 |
|
H3 |
C1 |
N2 |
135.326 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.049 |
|
|
|
| 2 |
N |
-0.553 |
|
|
|
| 3 |
H |
0.201 |
|
|
|
| 4 |
H |
0.304 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.410 |
-0.007 |
0.000 |
2.410 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.135 |
0.651 |
0.000 |
| y |
0.651 |
-10.606 |
0.000 |
| z |
0.000 |
0.000 |
-12.332 |
|
| Traceless |
| | x | y | z |
| x |
-0.666 |
0.651 |
0.000 |
| y |
0.651 |
1.627 |
0.000 |
| z |
0.000 |
0.000 |
-0.961 |
|
| Polar |
| 3z2-r2 | -1.922 |
| x2-y2 | -1.529 |
| xy | 0.651 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.513 |
0.072 |
0.000 |
| y |
0.072 |
3.675 |
0.000 |
| z |
0.000 |
0.000 |
0.940 |
<r2> (average value of r
2) Å
2
| <r2> |
16.731 |
| (<r2>)1/2 |
4.090 |
Jump to
S1C1
Energy calculated at B1B95/3-21G*
| | hartrees |
| Energy at 0K | -93.392477 |
| Energy at 298.15K | -93.393831 |
| HF Energy | -93.392477 |
| Nuclear repulsion energy | 28.036661 |
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 B1B95/3-21G*
| 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' |
3372 |
3220 |
1.91 |
|
|
|
| 2 |
A' |
3042 |
2905 |
29.70 |
|
|
|
| 3 |
A' |
1800 |
1718 |
13.40 |
|
|
|
| 4 |
A' |
1205 |
1151 |
16.60 |
|
|
|
| 5 |
A' |
939 |
896 |
242.52 |
|
|
|
| 6 |
A" |
1012 |
967 |
134.42 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5684.9 cm
-1
Scaled (by 0.9549) Zero Point Vibrational Energy (zpe) 5428.5 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 B1B95/3-21G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.002 |
0.655 |
0.000 |
| N2 |
-0.002 |
-0.583 |
0.000 |
| H3 |
0.899 |
1.278 |
0.000 |
| H4 |
-0.873 |
-1.128 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2373 | 1.0956 | 1.9838 |
N2 | 1.2373 | | 2.0671 | 1.0274 | H3 | 1.0956 | 2.0671 | | 2.9877 | H4 | 1.9838 | 1.0274 | 2.9877 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
122.051 |
|
H3 |
C1 |
N2 |
124.655 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.005 |
|
|
|
| 2 |
N |
-0.542 |
|
|
|
| 3 |
H |
0.219 |
|
|
|
| 4 |
H |
0.318 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.545 |
-0.072 |
0.000 |
0.550 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.086 |
3.332 |
0.000 |
| y |
3.332 |
-11.193 |
0.000 |
| z |
0.000 |
0.000 |
-12.383 |
|
| Traceless |
| | x | y | z |
| x |
0.702 |
3.332 |
0.000 |
| y |
3.332 |
0.541 |
0.000 |
| z |
0.000 |
0.000 |
-1.244 |
|
| Polar |
| 3z2-r2 | -2.487 |
| x2-y2 | 0.108 |
| xy | 3.332 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.887 |
0.542 |
0.000 |
| y |
0.542 |
3.392 |
0.000 |
| z |
0.000 |
0.000 |
0.974 |
<r2> (average value of r
2) Å
2
| <r2> |
16.639 |
| (<r2>)1/2 |
4.079 |