Jump to
S1C2
Energy calculated at HF/CEP-121G*
| | hartrees |
| Energy at 0K | -16.250989 |
| Energy at 298.15K | -16.252363 |
| HF Energy | -16.250989 |
| Nuclear repulsion energy | 15.654385 |
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/CEP-121G*
| 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' |
3567 |
3222 |
0.80 |
|
|
|
| 2 |
A' |
3211 |
2900 |
35.38 |
|
|
|
| 3 |
A' |
1607 |
1452 |
1.39 |
|
|
|
| 4 |
A' |
1258 |
1137 |
105.89 |
|
|
|
| 5 |
A' |
1004 |
907 |
41.63 |
|
|
|
| 6 |
A" |
1048 |
947 |
6.07 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5847.0 cm
-1
Scaled (by 0.9034) Zero Point Vibrational Energy (zpe) 5282.1 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 HF/CEP-121G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.114 |
0.640 |
0.000 |
| N2 |
0.114 |
-0.601 |
0.000 |
| H3 |
-0.675 |
1.388 |
0.000 |
| H4 |
-0.811 |
-1.017 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2406 | 1.0878 | 1.8980 |
N2 | 1.2406 | | 2.1403 | 1.0150 | H3 | 1.0878 | 2.1403 | | 2.4097 | H4 | 1.8980 | 1.0150 | 2.4097 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
114.214 |
|
H3 |
C1 |
N2 |
133.504 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/CEP-121G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.099 |
|
|
|
| 2 |
N |
-0.381 |
|
|
|
| 3 |
H |
0.166 |
|
|
|
| 4 |
H |
0.313 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.371 |
1.034 |
0.000 |
2.587 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.894 |
1.058 |
0.000 |
| y |
1.058 |
-11.603 |
0.000 |
| z |
0.000 |
0.000 |
-12.831 |
|
| Traceless |
| | x | y | z |
| x |
0.323 |
1.058 |
0.000 |
| y |
1.058 |
0.760 |
0.000 |
| z |
0.000 |
0.000 |
-1.083 |
|
| Polar |
| 3z2-r2 | -2.165 |
| x2-y2 | -0.291 |
| xy | 1.058 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.074 |
-0.002 |
0.000 |
| y |
-0.002 |
3.775 |
0.000 |
| z |
0.000 |
0.000 |
1.491 |
<r2> (average value of r
2) Å
2
| <r2> |
15.200 |
| (<r2>)1/2 |
3.899 |
Jump to
S1C1
Energy calculated at HF/CEP-121G*
| | hartrees |
| Energy at 0K | -16.257425 |
| Energy at 298.15K | -16.258815 |
| HF Energy | -16.257425 |
| Nuclear repulsion energy | 15.679423 |
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/CEP-121G*
| 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' |
3669 |
3314 |
2.75 |
|
|
|
| 2 |
A' |
3262 |
2947 |
20.44 |
|
|
|
| 3 |
A' |
1648 |
1489 |
15.02 |
|
|
|
| 4 |
A' |
1329 |
1201 |
22.45 |
|
|
|
| 5 |
A' |
1025 |
926 |
164.76 |
|
|
|
| 6 |
A" |
1092 |
986 |
104.27 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6012.3 cm
-1
Scaled (by 0.9034) Zero Point Vibrational Energy (zpe) 5431.5 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/CEP-121G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.004 |
0.645 |
0.000 |
| N2 |
0.004 |
-0.595 |
0.000 |
| H3 |
0.870 |
1.298 |
0.000 |
| H4 |
-0.921 |
-1.001 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2400 | 1.0847 | 1.8883 |
N2 | 1.2400 | | 2.0815 | 1.0103 | H3 | 1.0847 | 2.0815 | | 2.9145 | H4 | 1.8883 | 1.0103 | 2.9145 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
113.713 |
|
H3 |
C1 |
N2 |
126.994 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/CEP-121G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.131 |
|
|
|
| 2 |
N |
-0.379 |
|
|
|
| 3 |
H |
0.180 |
|
|
|
| 4 |
H |
0.330 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.838 |
0.885 |
0.000 |
1.219 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.159 |
3.180 |
0.000 |
| y |
3.180 |
-11.681 |
0.000 |
| z |
0.000 |
0.000 |
-12.867 |
|
| Traceless |
| | x | y | z |
| x |
1.114 |
3.180 |
0.000 |
| y |
3.180 |
0.332 |
0.000 |
| z |
0.000 |
0.000 |
-1.447 |
|
| Polar |
| 3z2-r2 | -2.893 |
| x2-y2 | 0.521 |
| xy | 3.180 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.236 |
0.460 |
0.000 |
| y |
0.460 |
3.708 |
0.000 |
| z |
0.000 |
0.000 |
1.509 |
<r2> (average value of r
2) Å
2
| <r2> |
15.160 |
| (<r2>)1/2 |
3.894 |