Jump to
S1C2
Energy calculated at B1B95/STO-3G
| | hartrees |
| Energy at 0K | -92.691105 |
| Energy at 298.15K | -92.692349 |
| HF Energy | -92.691105 |
| Nuclear repulsion energy | 27.492992 |
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/STO-3G
| 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' |
3367 |
2973 |
0.47 |
|
|
|
| 2 |
A' |
3262 |
2880 |
2.41 |
|
|
|
| 3 |
A' |
1898 |
1676 |
7.11 |
|
|
|
| 4 |
A' |
1049 |
926 |
106.08 |
|
|
|
| 5 |
A' |
900 |
794 |
107.13 |
|
|
|
| 6 |
A" |
941 |
831 |
3.31 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5708.4 cm
-1
Scaled (by 0.883) Zero Point Vibrational Energy (zpe) 5040.5 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/STO-3G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.116 |
0.652 |
0.000 |
| N2 |
0.116 |
-0.604 |
0.000 |
| H3 |
-0.681 |
1.428 |
0.000 |
| H4 |
-0.829 |
-1.112 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2560 | 1.1125 | 2.0010 |
N2 | 1.2560 | | 2.1827 | 1.0731 | H3 | 1.1125 | 2.1827 | | 2.5437 | H4 | 2.0010 | 1.0731 | 2.5437 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
118.224 |
|
H3 |
C1 |
N2 |
134.219 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.015 |
|
|
|
| 2 |
N |
-0.288 |
|
|
|
| 3 |
H |
0.087 |
|
|
|
| 4 |
H |
0.186 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.961 |
0.446 |
0.000 |
2.011 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-10.574 |
0.760 |
0.000 |
| y |
0.760 |
-10.618 |
0.000 |
| z |
0.000 |
0.000 |
-11.177 |
|
| Traceless |
| | x | y | z |
| x |
0.324 |
0.760 |
0.000 |
| y |
0.760 |
0.258 |
0.000 |
| z |
0.000 |
0.000 |
-0.582 |
|
| Polar |
| 3z2-r2 | -1.163 |
| x2-y2 | 0.044 |
| xy | 0.760 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.879 |
0.159 |
0.000 |
| y |
0.159 |
2.271 |
0.000 |
| z |
0.000 |
0.000 |
0.473 |
<r2> (average value of r
2) Å
2
| <r2> |
16.445 |
| (<r2>)1/2 |
4.055 |
Jump to
S1C1
Energy calculated at B1B95/STO-3G
| | hartrees |
| Energy at 0K | -92.703187 |
| Energy at 298.15K | -92.704509 |
| HF Energy | -92.703187 |
| Nuclear repulsion energy | 27.355904 |
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/STO-3G
| 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' |
3501 |
3091 |
1.02 |
|
|
|
| 2 |
A' |
3298 |
2912 |
0.18 |
|
|
|
| 3 |
A' |
1823 |
1610 |
7.99 |
|
|
|
| 4 |
A' |
1308 |
1155 |
13.75 |
|
|
|
| 5 |
A' |
970 |
856 |
160.25 |
|
|
|
| 6 |
A" |
1050 |
927 |
63.72 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5974.0 cm
-1
Scaled (by 0.883) Zero Point Vibrational Energy (zpe) 5275.1 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 B1B95/STO-3G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.001 |
0.669 |
0.000 |
| N2 |
0.001 |
-0.603 |
0.000 |
| H3 |
0.960 |
1.240 |
0.000 |
| H4 |
-0.977 |
-1.032 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2728 | 1.1154 | 1.9621 |
N2 | 1.2728 | | 2.0775 | 1.0677 | H3 | 1.1154 | 2.0775 | | 2.9849 | H4 | 1.9621 | 1.0677 | 2.9849 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
113.635 |
|
H3 |
C1 |
N2 |
120.757 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.000 |
|
|
|
| 2 |
N |
-0.279 |
|
|
|
| 3 |
H |
0.087 |
|
|
|
| 4 |
H |
0.192 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.647 |
0.230 |
0.000 |
0.687 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-9.881 |
2.287 |
0.000 |
| y |
2.287 |
-11.109 |
0.000 |
| z |
0.000 |
0.000 |
-11.212 |
|
| Traceless |
| | x | y | z |
| x |
1.279 |
2.287 |
0.000 |
| y |
2.287 |
-0.562 |
0.000 |
| z |
0.000 |
0.000 |
-0.717 |
|
| Polar |
| 3z2-r2 | -1.433 |
| x2-y2 | 1.228 |
| xy | 2.287 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.201 |
0.518 |
0.000 |
| y |
0.518 |
2.205 |
0.000 |
| z |
0.000 |
0.000 |
0.507 |
<r2> (average value of r
2) Å
2
| <r2> |
16.418 |
| (<r2>)1/2 |
4.052 |