Jump to
S1C2
Energy calculated at ROHF/cc-pVDZ
| | hartrees |
| Energy at 0K | -93.405215 |
| Energy at 298.15K | -93.406592 |
| HF Energy | -93.405215 |
| Nuclear repulsion energy | 28.180193 |
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/cc-pVDZ
| 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' |
3560 |
3064 |
5.07 |
|
|
|
| 2 |
A' |
3201 |
2755 |
25.81 |
|
|
|
| 3 |
A' |
1677 |
1443 |
1.25 |
|
|
|
| 4 |
A' |
1250 |
1076 |
121.07 |
|
|
|
| 5 |
A' |
1005 |
865 |
30.31 |
|
|
|
| 6 |
A" |
1046 |
900 |
4.08 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5869.5 cm
-1
Scaled (by 0.8607) Zero Point Vibrational Energy (zpe) 5051.9 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/cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.115 |
0.635 |
0.000 |
| N2 |
0.115 |
-0.599 |
0.000 |
| H3 |
-0.673 |
1.394 |
0.000 |
| H4 |
-0.816 |
-1.013 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2339 | 1.0937 | 1.8923 |
N2 | 1.2339 | | 2.1428 | 1.0182 | H3 | 1.0937 | 2.1428 | | 2.4112 | H4 | 1.8923 | 1.0182 | 2.4112 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
113.997 |
|
H3 |
C1 |
N2 |
133.946 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at ROHF/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.021 |
|
|
|
| 2 |
N |
-0.213 |
|
|
|
| 3 |
H |
0.071 |
|
|
|
| 4 |
H |
0.121 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.150 |
0.925 |
0.000 |
2.340 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.784 |
0.908 |
0.000 |
| y |
0.908 |
-11.425 |
0.000 |
| z |
0.000 |
0.000 |
-12.619 |
|
| Traceless |
| | x | y | z |
| x |
0.238 |
0.908 |
0.000 |
| y |
0.908 |
0.777 |
0.000 |
| z |
0.000 |
0.000 |
-1.014 |
|
| Polar |
| 3z2-r2 | -2.029 |
| x2-y2 | -0.359 |
| xy | 0.908 |
| 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> |
16.647 |
| (<r2>)1/2 |
4.080 |
Jump to
S1C1
Energy calculated at ROHF/cc-pVDZ
| | hartrees |
| Energy at 0K | -93.410473 |
| Energy at 298.15K | -93.411863 |
| HF Energy | -93.410473 |
| Nuclear repulsion energy | 28.210985 |
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/cc-pVDZ
| 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' |
3651 |
3143 |
8.48 |
|
|
|
| 2 |
A' |
3239 |
2788 |
16.24 |
|
|
|
| 3 |
A' |
1713 |
1474 |
13.08 |
|
|
|
| 4 |
A' |
1310 |
1127 |
15.08 |
|
|
|
| 5 |
A' |
1019 |
877 |
162.05 |
|
|
|
| 6 |
A" |
1079 |
929 |
98.67 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6005.6 cm
-1
Scaled (by 0.8607) Zero Point Vibrational Energy (zpe) 5169.1 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 ROHF/cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.004 |
0.641 |
0.000 |
| N2 |
0.004 |
-0.593 |
0.000 |
| H3 |
0.875 |
1.300 |
0.000 |
| H4 |
-0.925 |
-0.999 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2343 | 1.0919 | 1.8855 |
N2 | 1.2343 | | 2.0834 | 1.0140 | H3 | 1.0919 | 2.0834 | | 2.9199 | H4 | 1.8855 | 1.0140 | 2.9199 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
113.628 |
|
H3 |
C1 |
N2 |
127.074 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at ROHF/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.009 |
|
|
|
| 2 |
N |
-0.213 |
|
|
|
| 3 |
H |
0.087 |
|
|
|
| 4 |
H |
0.135 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.738 |
0.783 |
0.000 |
1.076 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.062 |
2.925 |
0.000 |
| y |
2.925 |
-11.494 |
0.000 |
| z |
0.000 |
0.000 |
-12.628 |
|
| Traceless |
| | x | y | z |
| x |
0.999 |
2.925 |
0.000 |
| y |
2.925 |
0.351 |
0.000 |
| z |
0.000 |
0.000 |
-1.350 |
|
| Polar |
| 3z2-r2 | -2.700 |
| x2-y2 | 0.432 |
| xy | 2.925 |
| 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> |
16.564 |
| (<r2>)1/2 |
4.070 |