Jump to
S1C2
Energy calculated at ROHF/6-31G*
| | hartrees |
| Energy at 0K | -93.392963 |
| Energy at 298.15K | -93.394340 |
| HF Energy | -93.392963 |
| Nuclear repulsion energy | 28.231842 |
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 ROHF/6-31G*
| 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' |
3584 |
3191 |
2.51 |
|
|
|
| 2 |
A' |
3250 |
2894 |
33.00 |
|
|
|
| 3 |
A' |
1666 |
1484 |
0.67 |
|
|
|
| 4 |
A' |
1266 |
1127 |
116.68 |
|
|
|
| 5 |
A' |
1013 |
902 |
45.27 |
|
|
|
| 6 |
A" |
1063 |
947 |
8.55 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5920.8 cm
-1
Scaled (by 0.8904) Zero Point Vibrational Energy (zpe) 5271.9 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 ROHF/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.113 |
0.637 |
0.000 |
| N2 |
0.113 |
-0.597 |
0.000 |
| H3 |
-0.669 |
1.387 |
0.000 |
| H4 |
-0.803 |
-1.028 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2338 | 1.0835 | 1.8999 |
N2 | 1.2338 | | 2.1325 | 1.0121 | H3 | 1.0835 | 2.1325 | | 2.4186 | H4 | 1.8999 | 1.0121 | 2.4186 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
115.194 |
|
H3 |
C1 |
N2 |
133.824 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at ROHF/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.040 |
|
|
|
| 2 |
N |
-0.569 |
|
|
|
| 3 |
H |
0.178 |
|
|
|
| 4 |
H |
0.351 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.254 |
1.025 |
0.000 |
2.476 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.773 |
1.114 |
0.000 |
| y |
1.114 |
-11.427 |
0.000 |
| z |
0.000 |
0.000 |
-12.609 |
|
| Traceless |
| | x | y | z |
| x |
0.246 |
1.114 |
0.000 |
| y |
1.114 |
0.763 |
0.000 |
| z |
0.000 |
0.000 |
-1.009 |
|
| Polar |
| 3z2-r2 | -2.018 |
| x2-y2 | -0.345 |
| xy | 1.114 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.000 |
0.000 |
0.000 |
| y |
0.000 |
0.000 |
0.000 |
| z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
| <r2> |
16.621 |
| (<r2>)1/2 |
4.077 |
Jump to
S1C1
Energy calculated at ROHF/6-31G*
| | hartrees |
| Energy at 0K | -93.398748 |
| Energy at 298.15K | -93.400139 |
| HF Energy | -93.398748 |
| Nuclear repulsion energy | 28.279002 |
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 ROHF/6-31G*
| 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' |
3679 |
3275 |
3.76 |
|
|
|
| 2 |
A' |
3294 |
2933 |
20.16 |
|
|
|
| 3 |
A' |
1705 |
1518 |
10.90 |
|
|
|
| 4 |
A' |
1332 |
1186 |
19.27 |
|
|
|
| 5 |
A' |
1033 |
920 |
169.67 |
|
|
|
| 6 |
A" |
1100 |
979 |
98.80 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6070.8 cm
-1
Scaled (by 0.8904) Zero Point Vibrational Energy (zpe) 5405.4 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 ROHF/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.004 |
0.642 |
0.000 |
| N2 |
0.004 |
-0.591 |
0.000 |
| H3 |
0.867 |
1.293 |
0.000 |
| H4 |
-0.913 |
-1.010 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2335 | 1.0811 | 1.8900 |
N2 | 1.2335 | | 2.0724 | 1.0079 | H3 | 1.0811 | 2.0724 | | 2.9110 | H4 | 1.8900 | 1.0079 | 2.9110 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
114.587 |
|
H3 |
C1 |
N2 |
126.988 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at ROHF/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.012 |
|
|
|
| 2 |
N |
-0.568 |
|
|
|
| 3 |
H |
0.195 |
|
|
|
| 4 |
H |
0.361 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.885 |
0.890 |
0.000 |
1.255 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.058 |
3.001 |
0.000 |
| y |
3.001 |
-11.512 |
0.000 |
| z |
0.000 |
0.000 |
-12.620 |
|
| Traceless |
| | x | y | z |
| x |
1.008 |
3.001 |
0.000 |
| y |
3.001 |
0.327 |
0.000 |
| z |
0.000 |
0.000 |
-1.335 |
|
| Polar |
| 3z2-r2 | -2.670 |
| x2-y2 | 0.454 |
| xy | 3.001 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.000 |
0.000 |
0.000 |
| y |
0.000 |
0.000 |
0.000 |
| z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
| <r2> |
16.527 |
| (<r2>)1/2 |
4.065 |