Jump to
S1C2
Energy calculated at HF/STO-3G
| | hartrees |
| Energy at 0K | -92.193441 |
| Energy at 298.15K | -92.194746 |
| HF Energy | -92.193441 |
| Nuclear repulsion energy | 26.694161 |
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 HF/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' |
3709 |
3028 |
5.55 |
|
|
|
| 2 |
A' |
3630 |
2964 |
1.52 |
|
|
|
| 3 |
A' |
1489 |
1216 |
43.03 |
|
|
|
| 4 |
A' |
1275 |
1041 |
8.79 |
|
|
|
| 5 |
A' |
1089 |
889 |
14.19 |
|
|
|
| 6 |
A" |
930 |
759 |
6.51 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6060.6 cm
-1
Scaled (by 0.8165) Zero Point Vibrational Energy (zpe) 4948.5 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 HF/STO-3G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.121 |
0.682 |
0.000 |
| N2 |
0.121 |
-0.645 |
0.000 |
| H3 |
-0.696 |
1.404 |
0.000 |
| H4 |
-0.880 |
-0.985 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.3271 | 1.0903 | 1.9449 |
N2 | 1.3271 | | 2.2058 | 1.0577 | H3 | 1.0903 | 2.2058 | | 2.3961 | H4 | 1.9449 | 1.0577 | 2.3961 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
108.759 |
|
H3 |
C1 |
N2 |
131.450 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.048 |
|
|
|
| 2 |
N |
-0.259 |
|
|
|
| 3 |
H |
0.062 |
|
|
|
| 4 |
H |
0.149 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.696 |
0.971 |
0.000 |
1.954 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-10.551 |
1.085 |
0.000 |
| y |
1.085 |
-11.509 |
0.000 |
| z |
0.000 |
0.000 |
-11.137 |
|
| Traceless |
| | x | y | z |
| x |
0.771 |
1.085 |
0.000 |
| y |
1.085 |
-0.665 |
0.000 |
| z |
0.000 |
0.000 |
-0.107 |
|
| Polar |
| 3z2-r2 | -0.214 |
| x2-y2 | 0.957 |
| xy | 1.085 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.927 |
0.100 |
0.000 |
| y |
0.100 |
1.740 |
0.000 |
| z |
0.000 |
0.000 |
0.515 |
<r2> (average value of r
2) Å
2
| <r2> |
17.007 |
| (<r2>)1/2 |
4.124 |
Jump to
S1C1
Energy calculated at HF/STO-3G
| | hartrees |
| Energy at 0K | -92.198206 |
| Energy at 298.15K | -92.199540 |
| HF Energy | -92.198206 |
| Nuclear repulsion energy | 26.774190 |
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 HF/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' |
3786 |
3091 |
8.10 |
|
|
|
| 2 |
A' |
3653 |
2982 |
2.14 |
|
|
|
| 3 |
A' |
1477 |
1206 |
20.41 |
|
|
|
| 4 |
A' |
1337 |
1092 |
1.74 |
|
|
|
| 5 |
A' |
1099 |
897 |
49.45 |
|
|
|
| 6 |
A" |
1024 |
836 |
25.53 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6187.7 cm
-1
Scaled (by 0.8165) Zero Point Vibrational Energy (zpe) 5052.3 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 HF/STO-3G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.007 |
0.686 |
0.000 |
| N2 |
0.007 |
-0.638 |
0.000 |
| H3 |
0.904 |
1.305 |
0.000 |
| H4 |
-0.998 |
-0.955 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.3239 | 1.0900 | 1.9243 |
N2 | 1.3239 | | 2.1401 | 1.0542 | H3 | 1.0900 | 2.1401 | | 2.9541 | H4 | 1.9243 | 1.0542 | 2.9541 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
107.488 |
|
H3 |
C1 |
N2 |
124.608 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.036 |
|
|
|
| 2 |
N |
-0.258 |
|
|
|
| 3 |
H |
0.069 |
|
|
|
| 4 |
H |
0.153 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.045 |
0.901 |
0.000 |
1.380 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-10.058 |
1.886 |
0.000 |
| y |
1.886 |
-11.590 |
0.000 |
| z |
0.000 |
0.000 |
-11.151 |
|
| Traceless |
| | x | y | z |
| x |
1.312 |
1.886 |
0.000 |
| y |
1.886 |
-0.986 |
0.000 |
| z |
0.000 |
0.000 |
-0.327 |
|
| Polar |
| 3z2-r2 | -0.653 |
| x2-y2 | 1.532 |
| xy | 1.886 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.113 |
0.575 |
0.000 |
| y |
0.575 |
1.732 |
0.000 |
| z |
0.000 |
0.000 |
0.464 |
<r2> (average value of r
2) Å
2
| <r2> |
16.931 |
| (<r2>)1/2 |
4.115 |