Jump to
S1C2
Energy calculated at HF/Def2TZVPP
| | hartrees |
| Energy at 0K | -130.728228 |
| Energy at 298.15K | -130.727615 |
| HF Energy | -130.728228 |
| Nuclear repulsion energy | 47.492193 |
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 HF/Def2TZVPP
| 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' |
3470 |
3145 |
20.04 |
|
|
|
| 2 |
A' |
1656 |
1501 |
145.42 |
|
|
|
| 3 |
A' |
1204 |
1091 |
5.31 |
|
|
|
| 4 |
A' |
623 |
565 |
18.71 |
|
|
|
| 5 |
A' |
389 |
353 |
0.53 |
|
|
|
| 6 |
A" |
418 |
379 |
0.21 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3879.9 cm
-1
Scaled (by 0.9064) Zero Point Vibrational Energy (zpe) 3516.8 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 HF/Def2TZVPP
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.228 |
-1.207 |
0.000 |
| C2 |
0.000 |
0.091 |
0.000 |
| N3 |
-0.337 |
1.233 |
0.000 |
| H4 |
0.995 |
-1.941 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3177 | 2.5046 | 1.0625 |
C2 | 1.3177 | | 1.1909 | 2.2631 | N3 | 2.5046 | 1.1909 | | 3.4430 | H4 | 1.0625 | 2.2631 | 3.4430 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
173.495 |
|
C2 |
C1 |
H4 |
143.687 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/Def2TZVPP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.048 |
|
|
|
| 2 |
C |
-0.030 |
|
|
|
| 3 |
N |
-0.169 |
|
|
|
| 4 |
H |
0.151 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.123 |
-2.818 |
0.000 |
3.033 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.521 |
-1.077 |
0.000 |
| y |
-1.077 |
-17.392 |
0.000 |
| z |
0.000 |
0.000 |
-17.448 |
|
| Traceless |
| | x | y | z |
| x |
0.899 |
-1.077 |
0.000 |
| y |
-1.077 |
-0.408 |
0.000 |
| z |
0.000 |
0.000 |
-0.491 |
|
| Polar |
| 3z2-r2 | -0.982 |
| x2-y2 | 0.871 |
| xy | -1.077 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.677 |
-0.742 |
0.000 |
| y |
-0.742 |
5.880 |
0.000 |
| z |
0.000 |
0.000 |
2.473 |
<r2> (average value of r
2) Å
2
| <r2> |
35.987 |
| (<r2>)1/2 |
5.999 |
Jump to
S1C1
Energy calculated at HF/Def2TZVPP
| | hartrees |
| Energy at 0K | -130.726230 |
| Energy at 298.15K | |
| HF Energy | -130.726230 |
| Nuclear repulsion energy | 47.580595 |
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 HF/Def2TZVPP
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Σ |
3543 |
3211 |
58.76 |
|
|
|
| 2 |
Σ |
1566 |
1419 |
134.42 |
|
|
|
| 3 |
Σ |
1257 |
1139 |
0.00 |
|
|
|
| 4 |
Π |
415 |
376 |
0.11 |
|
|
|
| 4 |
Π |
415 |
376 |
0.11 |
|
|
|
| 5 |
Π |
412i |
374i |
46.04 |
|
|
|
| 5 |
Π |
412i |
374i |
46.04 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3184.8 cm
-1
Scaled (by 0.9064) Zero Point Vibrational Energy (zpe) 2886.7 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 HF/Def2TZVPP
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.207 |
| C2 |
0.000 |
0.000 |
0.087 |
| N3 |
0.000 |
0.000 |
1.283 |
| H4 |
0.000 |
0.000 |
-2.263 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2939 | 2.4897 | 1.0560 |
C2 | 1.2939 | | 1.1958 | 2.3500 | N3 | 2.4897 | 1.1958 | | 3.5457 | H4 | 1.0560 | 2.3500 | 3.5457 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
180.000 |
|
C2 |
C1 |
H4 |
180.000 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/Def2TZVPP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.138 |
|
|
|
| 2 |
C |
0.076 |
|
|
|
| 3 |
N |
-0.196 |
|
|
|
| 4 |
H |
0.257 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
-3.204 |
3.204 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.426 |
0.000 |
0.000 |
| y |
0.000 |
-17.426 |
0.000 |
| z |
0.000 |
0.000 |
-15.679 |
|
| Traceless |
| | x | y | z |
| x |
-0.873 |
0.000 |
0.000 |
| y |
0.000 |
-0.873 |
0.000 |
| z |
0.000 |
0.000 |
1.747 |
|
| Polar |
| 3z2-r2 | 3.493 |
| x2-y2 | 0.000 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.465 |
0.000 |
0.000 |
| y |
0.000 |
2.465 |
0.000 |
| z |
0.000 |
0.000 |
6.143 |
<r2> (average value of r
2) Å
2
| <r2> |
35.958 |
| (<r2>)1/2 |
5.997 |