Jump to
S1C2
Energy calculated at B2PLYP=FULLultrafine/6-31G*
| | hartrees |
| Energy at 0K | -168.423232 |
| Energy at 298.15K | |
| HF Energy | -168.251572 |
| Nuclear repulsion energy | 59.975887 |
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 B2PLYP=FULLultrafine/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 |
Σ |
3564 |
3381 |
242.08 |
30.86 |
0.24 |
0.39 |
| 2 |
Σ |
2320 |
2201 |
309.81 |
11.81 |
0.15 |
0.26 |
| 3 |
Σ |
1298 |
1231 |
78.52 |
24.10 |
0.28 |
0.44 |
| 4 |
Π |
559 |
531 |
0.76 |
0.50 |
0.75 |
0.86 |
| 4 |
Π |
559 |
531 |
0.76 |
0.50 |
0.75 |
0.86 |
| 5 |
Π |
179i |
170i |
88.10 |
2.24 |
0.75 |
0.86 |
| 5 |
Π |
179i |
170i |
88.10 |
2.24 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 3970.5 cm
-1
Scaled (by 0.9487) Zero Point Vibrational Energy (zpe) 3766.8 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 B2PLYP=FULLultrafine/6-31G*
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.000 |
1.192 |
| N2 |
0.000 |
0.000 |
-0.020 |
| C3 |
0.000 |
0.000 |
-1.191 |
| H4 |
0.000 |
0.000 |
-2.252 |
Atom - Atom Distances (Å)
| |
O1 |
N2 |
C3 |
H4 |
| O1 | | 1.2114 | 2.3827 | 3.4443 |
N2 | 1.2114 | | 1.1713 | 2.2329 | C3 | 2.3827 | 1.1713 | | 1.0616 | H4 | 3.4443 | 2.2329 | 1.0616 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
N2 |
C3 |
180.000 |
|
N2 |
C3 |
H4 |
180.000 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.442 |
|
|
|
| 2 |
N |
0.178 |
|
|
|
| 3 |
C |
-0.015 |
|
|
|
| 4 |
H |
0.279 |
|
|
|
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 |
-3.115 |
3.115 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.516 |
0.000 |
0.000 |
| y |
0.000 |
-16.516 |
0.000 |
| z |
0.000 |
0.000 |
-13.544 |
|
| Traceless |
| | x | y | z |
| x |
-1.486 |
0.000 |
0.000 |
| y |
0.000 |
-1.486 |
0.000 |
| z |
0.000 |
0.000 |
2.972 |
|
| Polar |
| 3z2-r2 | 5.944 |
| 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 |
1.335 |
0.000 |
0.000 |
| y |
0.000 |
1.335 |
0.000 |
| z |
0.000 |
0.000 |
5.548 |
<r2> (average value of r
2) Å
2
| <r2> |
34.642 |
| (<r2>)1/2 |
5.886 |
Jump to
S1C1
Energy calculated at B2PLYP=FULLultrafine/6-31G*
| | hartrees |
| Energy at 0K | -168.423363 |
| Energy at 298.15K | |
| HF Energy | -168.249979 |
| Nuclear repulsion energy | 59.958142 |
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 B2PLYP=FULLultrafine/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' |
3527 |
3346 |
190.36 |
44.37 |
0.24 |
0.39 |
| 2 |
A' |
2295 |
2178 |
325.57 |
8.83 |
0.15 |
0.25 |
| 3 |
A' |
1303 |
1236 |
62.51 |
27.00 |
0.28 |
0.44 |
| 4 |
A' |
555 |
526 |
3.75 |
0.50 |
0.75 |
0.86 |
| 5 |
A' |
268 |
254 |
143.66 |
3.69 |
0.25 |
0.40 |
| 6 |
A" |
558 |
529 |
1.07 |
0.61 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4252.7 cm
-1
Scaled (by 0.9487) Zero Point Vibrational Energy (zpe) 4034.5 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 B2PLYP=FULLultrafine/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
-0.830 |
0.851 |
0.000 |
| N2 |
0.000 |
-0.028 |
0.000 |
| C3 |
0.880 |
-0.809 |
0.000 |
| H4 |
1.360 |
-1.759 |
0.000 |
Atom - Atom Distances (Å)
| |
O1 |
N2 |
C3 |
H4 |
| O1 | | 1.2090 | 2.3838 | 3.4072 |
N2 | 1.2090 | | 1.1771 | 2.2014 | C3 | 2.3838 | 1.1771 | | 1.0639 | H4 | 3.4072 | 2.2014 | 1.0639 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
N2 |
C3 |
174.968 |
|
N2 |
C3 |
H4 |
158.401 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.426 |
|
|
|
| 2 |
N |
0.233 |
|
|
|
| 3 |
C |
-0.068 |
|
|
|
| 4 |
H |
0.261 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.676 |
-2.372 |
0.000 |
2.905 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.189 |
-1.203 |
-0.002 |
| y |
-1.203 |
-14.219 |
0.002 |
| z |
-0.002 |
0.002 |
-16.539 |
|
| Traceless |
| | x | y | z |
| x |
-0.809 |
-1.203 |
-0.002 |
| y |
-1.203 |
2.145 |
0.002 |
| z |
-0.002 |
0.002 |
-1.335 |
|
| Polar |
| 3z2-r2 | -2.671 |
| x2-y2 | -1.970 |
| xy | -1.203 |
| xz | -0.002 |
| yz | 0.002 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.586 |
-2.111 |
0.000 |
| y |
-2.111 |
3.422 |
-0.000 |
| z |
0.000 |
-0.000 |
1.331 |
<r2> (average value of r
2) Å
2
| <r2> |
34.610 |
| (<r2>)1/2 |
5.883 |