Jump to
S1C2
Energy calculated at ROHF/6-31G
| | hartrees |
| Energy at 0K | -93.348119 |
| Energy at 298.15K | -93.349483 |
| HF Energy | -93.348119 |
| Nuclear repulsion energy | 27.895833 |
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' |
3564 |
3190 |
0.12 |
|
|
|
| 2 |
A' |
3282 |
2939 |
19.03 |
|
|
|
| 3 |
A' |
1563 |
1399 |
8.02 |
|
|
|
| 4 |
A' |
1201 |
1075 |
107.57 |
|
|
|
| 5 |
A' |
990 |
886 |
75.90 |
|
|
|
| 6 |
A" |
1041 |
932 |
10.69 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5820.4 cm
-1
Scaled (by 0.8953) Zero Point Vibrational Energy (zpe) 5211.0 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 |
0.109 |
0.651 |
0.000 |
| N2 |
0.109 |
-0.601 |
0.000 |
| H3 |
-0.651 |
1.416 |
0.000 |
| H4 |
-0.760 |
-1.121 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2519 | 1.0781 | 1.9731 |
N2 | 1.2519 | | 2.1551 | 1.0119 | H3 | 1.0781 | 2.1551 | | 2.5389 | H4 | 1.9731 | 1.0119 | 2.5389 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
120.921 |
|
H3 |
C1 |
N2 |
135.183 |
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 |
0.077 |
|
|
|
| 2 |
N |
-0.567 |
|
|
|
| 3 |
H |
0.167 |
|
|
|
| 4 |
H |
0.324 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.580 |
0.966 |
0.000 |
2.755 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.180 |
1.378 |
0.000 |
| y |
1.378 |
-11.441 |
0.000 |
| z |
0.000 |
0.000 |
-12.698 |
|
| Traceless |
| | x | y | z |
| x |
-0.110 |
1.378 |
0.000 |
| y |
1.378 |
0.997 |
0.000 |
| z |
0.000 |
0.000 |
-0.887 |
|
| Polar |
| 3z2-r2 | -1.774 |
| x2-y2 | -0.739 |
| xy | 1.378 |
| 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> |
17.047 |
| (<r2>)1/2 |
4.129 |
Jump to
S1C1
Energy calculated at ROHF/6-31G
| | hartrees |
| Energy at 0K | -93.353900 |
| Energy at 298.15K | -93.355286 |
| HF Energy | -93.353900 |
| Nuclear repulsion energy | 27.966942 |
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' |
3680 |
3295 |
3.62 |
|
|
|
| 2 |
A' |
3342 |
2992 |
8.29 |
|
|
|
| 3 |
A' |
1576 |
1411 |
2.87 |
|
|
|
| 4 |
A' |
1295 |
1159 |
23.19 |
|
|
|
| 5 |
A' |
1024 |
917 |
194.90 |
|
|
|
| 6 |
A" |
1090 |
976 |
123.30 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6003.5 cm
-1
Scaled (by 0.8953) Zero Point Vibrational Energy (zpe) 5375.0 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 |
0.002 |
0.656 |
0.000 |
| N2 |
0.002 |
-0.595 |
0.000 |
| H3 |
0.849 |
1.318 |
0.000 |
| H4 |
-0.876 |
-1.089 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2516 | 1.0746 | 1.9531 |
N2 | 1.2516 | | 2.0922 | 1.0067 | H3 | 1.0746 | 2.0922 | | 2.9604 | H4 | 1.9531 | 1.0067 | 2.9604 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
119.335 |
|
H3 |
C1 |
N2 |
128.003 |
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 |
0.050 |
|
|
|
| 2 |
N |
-0.568 |
|
|
|
| 3 |
H |
0.183 |
|
|
|
| 4 |
H |
0.335 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.077 |
0.870 |
0.000 |
1.385 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.348 |
3.392 |
0.000 |
| y |
3.392 |
-11.578 |
0.000 |
| z |
0.000 |
0.000 |
-12.713 |
|
| Traceless |
| | x | y | z |
| x |
0.797 |
3.392 |
0.000 |
| y |
3.392 |
0.452 |
0.000 |
| z |
0.000 |
0.000 |
-1.249 |
|
| Polar |
| 3z2-r2 | -2.499 |
| x2-y2 | 0.230 |
| xy | 3.392 |
| 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> |
16.894 |
| (<r2>)1/2 |
4.110 |