Jump to
S1C2
S1C3
Energy calculated at B3LYP/LANL2DZ
| | hartrees |
| Energy at 0K | -225.241066 |
| Energy at 298.15K | -225.246939 |
| HF Energy | -225.241066 |
| Nuclear repulsion energy | 121.934819 |
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 B3LYP/LANL2DZ
| 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 |
3783 |
3636 |
39.94 |
|
|
|
| 2 |
A |
3634 |
3493 |
6.64 |
|
|
|
| 3 |
A |
1712 |
1645 |
407.10 |
|
|
|
| 4 |
A |
1651 |
1587 |
46.49 |
|
|
|
| 5 |
A |
1138 |
1094 |
2.07 |
|
|
|
| 6 |
A |
959 |
922 |
4.89 |
|
|
|
| 7 |
A |
480 |
462 |
0.00 |
|
|
|
| 8 |
A |
472 |
454 |
4.37 |
|
|
|
| 9 |
A |
219 |
211 |
0.00 |
|
|
|
| 10 |
B |
3780 |
3633 |
36.26 |
|
|
|
| 11 |
B |
3626 |
3485 |
66.83 |
|
|
|
| 12 |
B |
1644 |
1580 |
227.79 |
|
|
|
| 13 |
B |
1450 |
1394 |
302.77 |
|
|
|
| 14 |
B |
1006 |
967 |
11.03 |
|
|
|
| 15 |
B |
754 |
725 |
78.13 |
|
|
|
| 16 |
B |
564 |
542 |
128.52 |
|
|
|
| 17 |
B |
541 |
520 |
13.68 |
|
|
|
| 18 |
B |
484 |
465 |
599.19 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13948.9 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 13407.6 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 B3LYP/LANL2DZ
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.134 |
| O2 |
0.000 |
0.000 |
1.391 |
| N3 |
0.000 |
1.174 |
-0.608 |
| N4 |
0.000 |
-1.174 |
-0.608 |
| H5 |
-0.000 |
2.041 |
-0.092 |
| H6 |
0.000 |
1.201 |
-1.617 |
| H7 |
0.000 |
-2.041 |
-0.092 |
| H8 |
-0.000 |
-1.201 |
-1.617 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2579 | 1.3888 | 1.3888 | 2.0533 | 2.1232 | 2.0533 | 2.1232 |
O2 | 1.2579 | | 2.3189 | 2.3189 | 2.5228 | 3.2396 | 2.5228 | 3.2396 | N3 | 1.3888 | 2.3189 | | 2.3480 | 1.0093 | 1.0094 | 3.2562 | 2.5804 | N4 | 1.3888 | 2.3189 | 2.3480 | | 3.2562 | 2.5804 | 1.0093 | 1.0094 | H5 | 2.0533 | 2.5228 | 1.0093 | 3.2562 | | 1.7417 | 4.0818 | 3.5830 | H6 | 2.1232 | 3.2396 | 1.0094 | 2.5804 | 1.7417 | | 3.5830 | 2.4019 | H7 | 2.0533 | 2.5228 | 3.2562 | 1.0093 | 4.0818 | 3.5830 | | 1.7417 | H8 | 2.1232 | 3.2396 | 2.5804 | 1.0094 | 3.5830 | 2.4019 | 1.7417 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
116.909 |
|
C1 |
N3 |
H6 |
123.821 |
| C1 |
N4 |
H7 |
116.909 |
|
C1 |
N4 |
H8 |
123.821 |
| O2 |
C1 |
N3 |
122.291 |
|
O2 |
C1 |
N4 |
122.291 |
| N3 |
C1 |
N4 |
115.418 |
|
H5 |
N3 |
H6 |
119.270 |
| H7 |
N4 |
H8 |
119.270 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.303 |
|
|
|
| 2 |
O |
-0.333 |
|
|
|
| 3 |
N |
-0.629 |
|
|
|
| 4 |
N |
-0.629 |
|
|
|
| 5 |
H |
0.341 |
|
|
|
| 6 |
H |
0.303 |
|
|
|
| 7 |
H |
0.341 |
|
|
|
| 8 |
H |
0.303 |
|
|
|
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 |
-4.868 |
4.868 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.269 |
0.000 |
0.000 |
| y |
0.000 |
-16.019 |
0.000 |
| z |
0.000 |
0.000 |
-24.714 |
|
| Traceless |
| | x | y | z |
| x |
-5.902 |
0.000 |
0.000 |
| y |
0.000 |
9.472 |
0.000 |
| z |
0.000 |
0.000 |
-3.570 |
|
| Polar |
| 3z2-r2 | -7.141 |
| x2-y2 | -10.250 |
| 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 |
1.982 |
0.000 |
0.000 |
| y |
0.000 |
4.607 |
0.000 |
| z |
0.000 |
0.000 |
5.074 |
<r2> (average value of r
2) Å
2
| <r2> |
70.486 |
| (<r2>)1/2 |
8.396 |
Jump to
S1C1
S1C3
Energy calculated at B3LYP/LANL2DZ
| | hartrees |
| Energy at 0K | -225.241066 |
| Energy at 298.15K | -225.246940 |
| HF Energy | -225.241066 |
| Nuclear repulsion energy | 121.936635 |
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 B3LYP/LANL2DZ
| 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' |
3783 |
3636 |
39.96 |
|
|
|
| 2 |
A' |
3634 |
3493 |
6.65 |
|
|
|
| 3 |
A' |
1712 |
1645 |
406.86 |
|
|
|
| 4 |
A' |
1651 |
1587 |
46.69 |
|
|
|
| 5 |
A' |
1138 |
1094 |
2.08 |
|
|
|
| 6 |
A' |
959 |
922 |
4.88 |
|
|
|
| 7 |
A' |
754 |
725 |
78.20 |
|
|
|
| 8 |
A' |
564 |
542 |
128.26 |
|
|
|
| 9 |
A' |
484 |
465 |
599.36 |
|
|
|
| 10 |
A' |
472 |
454 |
4.37 |
|
|
|
| 11 |
A" |
3780 |
3633 |
36.26 |
|
|
|
| 12 |
A" |
3626 |
3485 |
66.80 |
|
|
|
| 13 |
A" |
1644 |
1580 |
227.95 |
|
|
|
| 14 |
A" |
1450 |
1394 |
302.66 |
|
|
|
| 15 |
A" |
1006 |
967 |
11.02 |
|
|
|
| 16 |
A" |
541 |
520 |
13.68 |
|
|
|
| 17 |
A" |
480 |
462 |
0.00 |
|
|
|
| 18 |
A" |
219 |
211 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13949.2 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 13408.0 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 B3LYP/LANL2DZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.000 |
0.134 |
0.000 |
| O2 |
-0.000 |
1.392 |
0.000 |
| N3 |
-0.000 |
-0.608 |
1.174 |
| N4 |
-0.000 |
-0.608 |
-1.174 |
| H5 |
0.000 |
-0.091 |
2.041 |
| H6 |
0.000 |
-1.617 |
1.201 |
| H7 |
0.000 |
-0.091 |
-2.041 |
| H8 |
0.000 |
-1.617 |
-1.201 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2579 | 1.3887 | 1.3887 | 2.0532 | 2.1232 | 2.0532 | 2.1232 |
O2 | 1.2579 | | 2.3189 | 2.3189 | 2.5227 | 3.2397 | 2.5227 | 3.2397 | N3 | 1.3887 | 2.3189 | | 2.3479 | 1.0093 | 1.0094 | 3.2560 | 2.5803 | N4 | 1.3887 | 2.3189 | 2.3479 | | 3.2560 | 2.5803 | 1.0093 | 1.0094 | H5 | 2.0532 | 2.5227 | 1.0093 | 3.2560 | | 1.7418 | 4.0816 | 3.5829 | H6 | 2.1232 | 3.2397 | 1.0094 | 2.5803 | 1.7418 | | 3.5829 | 2.4019 | H7 | 2.0532 | 2.5227 | 3.2560 | 1.0093 | 4.0816 | 3.5829 | | 1.7418 | H8 | 2.1232 | 3.2397 | 2.5803 | 1.0094 | 3.5829 | 2.4019 | 1.7418 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
116.902 |
|
C1 |
N3 |
H6 |
123.825 |
| C1 |
N4 |
H7 |
116.902 |
|
C1 |
N4 |
H8 |
123.825 |
| O2 |
C1 |
N3 |
122.292 |
|
O2 |
C1 |
N4 |
122.292 |
| N3 |
C1 |
N4 |
115.416 |
|
H5 |
N3 |
H6 |
119.273 |
| H7 |
N4 |
H8 |
119.273 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.303 |
|
|
|
| 2 |
O |
-0.333 |
|
|
|
| 3 |
N |
-0.629 |
|
|
|
| 4 |
N |
-0.629 |
|
|
|
| 5 |
H |
0.341 |
|
|
|
| 6 |
H |
0.303 |
|
|
|
| 7 |
H |
0.341 |
|
|
|
| 8 |
H |
0.303 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.002 |
-4.868 |
0.000 |
4.868 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.268 |
-0.001 |
0.000 |
| y |
-0.001 |
-24.714 |
0.000 |
| z |
0.000 |
0.000 |
-16.020 |
|
| Traceless |
| | x | y | z |
| x |
-5.901 |
-0.001 |
0.000 |
| y |
-0.001 |
-3.570 |
0.000 |
| z |
0.000 |
0.000 |
9.472 |
|
| Polar |
| 3z2-r2 | 18.943 |
| x2-y2 | -1.554 |
| xy | -0.001 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.982 |
0.000 |
0.000 |
| y |
0.000 |
5.074 |
0.000 |
| z |
0.000 |
0.000 |
4.606 |
<r2> (average value of r
2) Å
2
| <r2> |
70.484 |
| (<r2>)1/2 |
8.395 |
Jump to
S1C1
S1C2
Energy calculated at B3LYP/LANL2DZ
| | hartrees |
| Energy at 0K | -225.241066 |
| Energy at 298.15K | -225.246937 |
| HF Energy | -225.241066 |
| Nuclear repulsion energy | 121.931559 |
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 B3LYP/LANL2DZ
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
3783 |
3637 |
39.91 |
|
|
|
| 2 |
A1 |
3634 |
3493 |
6.62 |
|
|
|
| 3 |
A1 |
1712 |
1645 |
408.24 |
|
|
|
| 4 |
A1 |
1652 |
1587 |
45.49 |
|
|
|
| 5 |
A1 |
1138 |
1094 |
2.05 |
|
|
|
| 6 |
A1 |
959 |
922 |
4.91 |
|
|
|
| 7 |
A1 |
472 |
454 |
4.36 |
|
|
|
| 8 |
A2 |
480 |
461 |
0.00 |
|
|
|
| 9 |
A2 |
219 |
210 |
0.00 |
|
|
|
| 10 |
B1 |
754 |
725 |
77.96 |
|
|
|
| 11 |
B1 |
564 |
542 |
127.26 |
|
|
|
| 12 |
B1 |
483 |
465 |
600.70 |
|
|
|
| 13 |
B2 |
3780 |
3634 |
36.34 |
|
|
|
| 14 |
B2 |
3626 |
3486 |
66.85 |
|
|
|
| 15 |
B2 |
1644 |
1580 |
227.49 |
|
|
|
| 16 |
B2 |
1450 |
1393 |
302.86 |
|
|
|
| 17 |
B2 |
1006 |
967 |
11.08 |
|
|
|
| 18 |
B2 |
541 |
520 |
13.67 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13948.0 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 13406.8 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 B3LYP/LANL2DZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.134 |
| O2 |
0.000 |
0.000 |
1.391 |
| N3 |
0.000 |
1.174 |
-0.608 |
| N4 |
0.000 |
-1.174 |
-0.608 |
| H5 |
0.000 |
2.041 |
-0.092 |
| H6 |
0.000 |
1.201 |
-1.617 |
| H7 |
0.000 |
-2.041 |
-0.092 |
| H8 |
0.000 |
-1.201 |
-1.617 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2578 | 1.3889 | 1.3889 | 2.0536 | 2.1231 | 2.0536 | 2.1231 |
O2 | 1.2578 | | 2.3189 | 2.3189 | 2.5231 | 3.2395 | 2.5231 | 3.2395 | N3 | 1.3889 | 2.3189 | | 2.3482 | 1.0092 | 1.0094 | 3.2565 | 2.5802 | N4 | 1.3889 | 2.3189 | 2.3482 | | 3.2565 | 2.5802 | 1.0092 | 1.0094 | H5 | 2.0536 | 2.5231 | 1.0092 | 3.2565 | | 1.7418 | 4.0823 | 3.5828 | H6 | 2.1231 | 3.2395 | 1.0094 | 2.5802 | 1.7418 | | 3.5828 | 2.4013 | H7 | 2.0536 | 2.5231 | 3.2565 | 1.0092 | 4.0823 | 3.5828 | | 1.7418 | H8 | 2.1231 | 3.2395 | 2.5802 | 1.0094 | 3.5828 | 2.4013 | 1.7418 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
116.926 |
|
C1 |
N3 |
H6 |
123.796 |
| C1 |
N4 |
H7 |
116.926 |
|
C1 |
N4 |
H8 |
123.796 |
| O2 |
C1 |
N3 |
122.290 |
|
O2 |
C1 |
N4 |
122.290 |
| N3 |
C1 |
N4 |
115.421 |
|
H5 |
N3 |
H6 |
119.278 |
| H7 |
N4 |
H8 |
119.278 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.303 |
|
|
|
| 2 |
O |
-0.333 |
|
|
|
| 3 |
N |
-0.629 |
|
|
|
| 4 |
N |
-0.629 |
|
|
|
| 5 |
H |
0.341 |
|
|
|
| 6 |
H |
0.303 |
|
|
|
| 7 |
H |
0.341 |
|
|
|
| 8 |
H |
0.303 |
|
|
|
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 |
-4.867 |
4.867 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.269 |
0.000 |
0.000 |
| y |
0.000 |
-16.019 |
0.000 |
| z |
0.000 |
0.000 |
-24.715 |
|
| Traceless |
| | x | y | z |
| x |
-5.902 |
0.000 |
0.000 |
| y |
0.000 |
9.473 |
0.000 |
| z |
0.000 |
0.000 |
-3.571 |
|
| Polar |
| 3z2-r2 | -7.142 |
| x2-y2 | -10.250 |
| 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 |
1.982 |
0.000 |
0.000 |
| y |
0.000 |
4.607 |
0.000 |
| z |
0.000 |
0.000 |
5.074 |
<r2> (average value of r
2) Å
2
| <r2> |
70.490 |
| (<r2>)1/2 |
8.396 |