Jump to
S1C2
Energy calculated at ROHF/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -93.412655 |
| Energy at 298.15K | -93.414029 |
| HF Energy | -93.412655 |
| Nuclear repulsion energy | 28.210625 |
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/aug-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' |
3581 |
3581 |
5.13 |
|
|
|
| 2 |
A' |
3199 |
3199 |
22.85 |
|
|
|
| 3 |
A' |
1690 |
1690 |
5.16 |
|
|
|
| 4 |
A' |
1238 |
1238 |
119.21 |
|
|
|
| 5 |
A' |
995 |
995 |
31.59 |
|
|
|
| 6 |
A" |
1035 |
1035 |
3.36 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5868.7 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 5868.7 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/aug-cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.114 |
0.636 |
0.000 |
| N2 |
0.114 |
-0.597 |
0.000 |
| H3 |
-0.674 |
1.391 |
0.000 |
| H4 |
-0.807 |
-1.023 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2331 | 1.0912 | 1.8974 |
N2 | 1.2331 | | 2.1385 | 1.0144 | H3 | 1.0912 | 2.1385 | | 2.4179 | H4 | 1.8974 | 1.0144 | 2.4179 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
114.840 |
|
H3 |
C1 |
N2 |
133.786 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at ROHF/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.322 |
|
|
|
| 2 |
N |
-0.278 |
|
|
|
| 3 |
H |
-0.081 |
|
|
|
| 4 |
H |
0.037 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.176 |
1.010 |
0.000 |
2.398 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.086 |
0.932 |
0.000 |
| y |
0.932 |
-11.571 |
0.000 |
| z |
0.000 |
0.000 |
-13.038 |
|
| Traceless |
| | x | y | z |
| x |
0.218 |
0.932 |
0.000 |
| y |
0.932 |
0.991 |
0.000 |
| z |
0.000 |
0.000 |
-1.209 |
|
| Polar |
| 3z2-r2 | -2.418 |
| x2-y2 | -0.515 |
| xy | 0.932 |
| 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> |
16.817 |
| (<r2>)1/2 |
4.101 |
Jump to
S1C1
Energy calculated at ROHF/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -93.418273 |
| Energy at 298.15K | -93.419661 |
| HF Energy | -93.418273 |
| Nuclear repulsion energy | 28.240985 |
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/aug-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' |
3669 |
3669 |
12.92 |
|
|
|
| 2 |
A' |
3239 |
3239 |
14.22 |
|
|
|
| 3 |
A' |
1723 |
1723 |
19.69 |
|
|
|
| 4 |
A' |
1293 |
1293 |
18.11 |
|
|
|
| 5 |
A' |
1012 |
1012 |
163.83 |
|
|
|
| 6 |
A" |
1074 |
1074 |
95.73 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6005.0 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 6005.0 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/aug-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 |
-0.592 |
0.000 |
| H3 |
0.867 |
1.306 |
0.000 |
| H4 |
-0.916 |
-1.010 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2332 | 1.0892 | 1.8904 |
N2 | 1.2332 | | 2.0848 | 1.0103 | H3 | 1.0892 | 2.0848 | | 2.9227 | H4 | 1.8904 | 1.0103 | 2.9227 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
114.466 |
|
H3 |
C1 |
N2 |
127.593 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at ROHF/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.252 |
|
|
|
| 2 |
N |
-0.242 |
|
|
|
| 3 |
H |
-0.094 |
|
|
|
| 4 |
H |
0.084 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.687 |
0.862 |
0.000 |
1.103 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.417 |
3.175 |
0.000 |
| y |
3.175 |
-11.719 |
0.000 |
| z |
0.000 |
0.000 |
-13.064 |
|
| Traceless |
| | x | y | z |
| x |
0.974 |
3.175 |
0.000 |
| y |
3.175 |
0.521 |
0.000 |
| z |
0.000 |
0.000 |
-1.496 |
|
| Polar |
| 3z2-r2 | -2.992 |
| x2-y2 | 0.302 |
| xy | 3.175 |
| 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> |
16.773 |
| (<r2>)1/2 |
4.095 |