Jump to
S1C2
Energy calculated at ROHF/aug-cc-pVQZ
| hartrees |
Energy at 0K | -93.440051 |
Energy at 298.15K | -93.441425 |
HF Energy | -93.440051 |
Nuclear repulsion energy | 28.451944 |
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-pVQZ
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' |
3583 |
3583 |
6.90 |
|
|
|
2 |
A' |
3183 |
3183 |
25.66 |
|
|
|
3 |
A' |
1730 |
1730 |
10.49 |
|
|
|
4 |
A' |
1232 |
1232 |
119.39 |
|
|
|
5 |
A' |
982 |
982 |
46.91 |
|
|
|
6 |
A" |
1053 |
1053 |
3.73 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5881.6 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 5881.6 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-pVQZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.112 |
0.631 |
0.000 |
N2 |
0.112 |
-0.590 |
0.000 |
H3 |
-0.668 |
1.382 |
0.000 |
H4 |
-0.793 |
-1.034 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
N2 |
H3 |
H4 |
C1 | | 1.2209 | 1.0828 | 1.8950 |
N2 | 1.2209 | | 2.1205 | 1.0082 | H3 | 1.0828 | 2.1205 | | 2.4190 | H4 | 1.8950 | 1.0082 | 2.4190 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
N2 |
H4 |
116.123 |
|
H3 |
C1 |
N2 |
133.914 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at ROHF/aug-cc-pVQZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.140 |
|
|
|
2 |
N |
-0.583 |
|
|
|
3 |
H |
0.410 |
|
|
|
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 |
|
-2.160 |
0.959 |
0.000 |
2.363 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-12.068 |
0.918 |
0.000 |
y |
0.918 |
-11.427 |
0.000 |
z |
0.000 |
0.000 |
-12.934 |
|
Traceless |
| x | y | z |
x |
0.112 |
0.918 |
0.000 |
y |
0.918 |
1.075 |
0.000 |
z |
0.000 |
0.000 |
-1.187 |
|
Polar |
3z2-r2 | -2.374 |
x2-y2 | -0.642 |
xy | 0.918 |
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> |
16.626 |
(<r2>)1/2 |
4.078 |
Jump to
S1C1
Energy calculated at ROHF/aug-cc-pVQZ
| hartrees |
Energy at 0K | -93.445595 |
Energy at 298.15K | -93.446983 |
HF Energy | -93.445595 |
Nuclear repulsion energy | 28.466987 |
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-pVQZ
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' |
3672 |
3672 |
15.88 |
|
|
|
2 |
A' |
3223 |
3223 |
15.91 |
|
|
|
3 |
A' |
1755 |
1755 |
28.34 |
|
|
|
4 |
A' |
1295 |
1295 |
16.21 |
|
|
|
5 |
A' |
1012 |
1012 |
178.04 |
|
|
|
6 |
A" |
1083 |
1083 |
95.88 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6019.2 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 6019.2 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-pVQZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.004 |
0.636 |
0.000 |
N2 |
0.004 |
-0.586 |
0.000 |
H3 |
0.858 |
1.299 |
0.000 |
H4 |
-0.903 |
-1.018 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
N2 |
H3 |
H4 |
C1 | | 1.2222 | 1.0807 | 1.8862 |
N2 | 1.2222 | | 2.0690 | 1.0042 | H3 | 1.0807 | 2.0690 | | 2.9095 | H4 | 1.8862 | 1.0042 | 2.9095 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
N2 |
H4 |
115.469 |
|
H3 |
C1 |
N2 |
127.791 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at ROHF/aug-cc-pVQZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.226 |
|
|
|
2 |
N |
-0.524 |
|
|
|
3 |
H |
0.437 |
|
|
|
4 |
H |
0.314 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.669 |
0.818 |
0.000 |
1.057 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-11.401 |
3.153 |
0.000 |
y |
3.153 |
-11.589 |
0.000 |
z |
0.000 |
0.000 |
-12.973 |
|
Traceless |
| x | y | z |
x |
0.879 |
3.153 |
0.000 |
y |
3.153 |
0.598 |
0.000 |
z |
0.000 |
0.000 |
-1.478 |
|
Polar |
3z2-r2 | -2.955 |
x2-y2 | 0.187 |
xy | 3.153 |
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> |
16.593 |
(<r2>)1/2 |
4.073 |