Jump to
S1C2
S1C3
Energy calculated at B3LYP/6-31G
| | hartrees |
| Energy at 0K | -225.194324 |
| Energy at 298.15K | -225.200228 |
| HF Energy | -225.194324 |
| Nuclear repulsion energy | 122.632642 |
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/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 |
3771 |
3628 |
30.06 |
|
|
|
| 2 |
A |
3635 |
3497 |
4.55 |
|
|
|
| 3 |
A |
1747 |
1681 |
370.14 |
|
|
|
| 4 |
A |
1679 |
1615 |
13.18 |
|
|
|
| 5 |
A |
1160 |
1116 |
2.20 |
|
|
|
| 6 |
A |
976 |
939 |
4.78 |
|
|
|
| 7 |
A |
500 |
481 |
0.00 |
|
|
|
| 8 |
A |
484 |
466 |
3.55 |
|
|
|
| 9 |
A |
185 |
178 |
0.00 |
|
|
|
| 10 |
B |
3768 |
3625 |
37.99 |
|
|
|
| 11 |
B |
3626 |
3488 |
48.96 |
|
|
|
| 12 |
B |
1667 |
1604 |
229.10 |
|
|
|
| 13 |
B |
1469 |
1413 |
278.13 |
|
|
|
| 14 |
B |
1025 |
986 |
12.20 |
|
|
|
| 15 |
B |
772 |
743 |
145.41 |
|
|
|
| 16 |
B |
577 |
555 |
124.97 |
|
|
|
| 17 |
B |
560 |
539 |
14.28 |
|
|
|
| 18 |
B |
490 |
472 |
580.57 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14045.7 cm
-1
Scaled (by 0.962) Zero Point Vibrational Energy (zpe) 13512.0 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/6-31G
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.133 |
| O2 |
0.000 |
0.000 |
1.384 |
| N3 |
0.000 |
1.166 |
-0.604 |
| N4 |
0.000 |
-1.166 |
-0.604 |
| H5 |
-0.000 |
2.031 |
-0.092 |
| H6 |
-0.000 |
1.197 |
-1.610 |
| H7 |
0.000 |
-2.031 |
-0.092 |
| H8 |
0.000 |
-1.197 |
-1.610 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2508 | 1.3796 | 1.3796 | 2.0438 | 2.1144 | 2.0438 | 2.1144 |
O2 | 1.2508 | | 2.3048 | 2.3048 | 2.5108 | 3.2241 | 2.5108 | 3.2241 | N3 | 1.3796 | 2.3048 | | 2.3321 | 1.0057 | 1.0061 | 3.2382 | 2.5682 | N4 | 1.3796 | 2.3048 | 2.3321 | | 3.2382 | 2.5682 | 1.0057 | 1.0061 | H5 | 2.0438 | 2.5108 | 1.0057 | 3.2382 | | 1.7322 | 4.0627 | 3.5675 | H6 | 2.1144 | 3.2241 | 1.0061 | 2.5682 | 1.7322 | | 3.5675 | 2.3941 | H7 | 2.0438 | 2.5108 | 3.2382 | 1.0057 | 4.0627 | 3.5675 | | 1.7322 | H8 | 2.1144 | 3.2241 | 2.5682 | 1.0061 | 3.5675 | 2.3941 | 1.7322 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
117.062 |
|
C1 |
N3 |
H6 |
124.071 |
| C1 |
N4 |
H7 |
117.062 |
|
C1 |
N4 |
H8 |
124.071 |
| O2 |
C1 |
N3 |
122.304 |
|
O2 |
C1 |
N4 |
122.304 |
| N3 |
C1 |
N4 |
115.391 |
|
H5 |
N3 |
H6 |
118.868 |
| H7 |
N4 |
H8 |
118.868 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.663 |
|
|
|
| 2 |
O |
-0.480 |
|
|
|
| 3 |
N |
-0.739 |
|
|
|
| 4 |
N |
-0.739 |
|
|
|
| 5 |
H |
0.337 |
|
|
|
| 6 |
H |
0.311 |
|
|
|
| 7 |
H |
0.337 |
|
|
|
| 8 |
H |
0.311 |
|
|
|
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 |
-4.630 |
4.630 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.687 |
-0.002 |
0.000 |
| y |
-0.002 |
-16.113 |
0.000 |
| z |
0.000 |
0.000 |
-24.223 |
|
| Traceless |
| | x | y | z |
| x |
-5.519 |
-0.002 |
0.000 |
| y |
-0.002 |
8.842 |
0.000 |
| z |
0.000 |
0.000 |
-3.323 |
|
| Polar |
| 3z2-r2 | -6.646 |
| x2-y2 | -9.573 |
| xy | -0.002 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.446 |
-0.000 |
0.000 |
| y |
-0.000 |
4.495 |
0.000 |
| z |
0.000 |
0.000 |
4.829 |
<r2> (average value of r
2) Å
2
| <r2> |
69.637 |
| (<r2>)1/2 |
8.345 |
Jump to
S1C1
S1C3
Energy calculated at B3LYP/6-31G
| | hartrees |
| Energy at 0K | -225.194324 |
| Energy at 298.15K | -225.200230 |
| HF Energy | -225.194324 |
| Nuclear repulsion energy | 122.632322 |
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/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' |
3771 |
3628 |
30.04 |
|
|
|
| 2 |
A' |
3635 |
3497 |
4.57 |
|
|
|
| 3 |
A' |
1747 |
1680 |
369.28 |
|
|
|
| 4 |
A' |
1679 |
1615 |
13.87 |
|
|
|
| 5 |
A' |
1160 |
1116 |
2.23 |
|
|
|
| 6 |
A' |
976 |
939 |
4.75 |
|
|
|
| 7 |
A' |
772 |
743 |
145.47 |
|
|
|
| 8 |
A' |
577 |
555 |
124.98 |
|
|
|
| 9 |
A' |
491 |
472 |
580.40 |
|
|
|
| 10 |
A' |
484 |
466 |
3.55 |
|
|
|
| 11 |
A" |
3768 |
3625 |
38.08 |
|
|
|
| 12 |
A" |
3625 |
3488 |
48.90 |
|
|
|
| 13 |
A" |
1668 |
1604 |
229.44 |
|
|
|
| 14 |
A" |
1469 |
1413 |
277.84 |
|
|
|
| 15 |
A" |
1025 |
986 |
12.16 |
|
|
|
| 16 |
A" |
560 |
539 |
14.27 |
|
|
|
| 17 |
A" |
500 |
481 |
0.00 |
|
|
|
| 18 |
A" |
186 |
179 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14046.4 cm
-1
Scaled (by 0.962) Zero Point Vibrational Energy (zpe) 13512.7 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 B3LYP/6-31G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.133 |
0.000 |
| O2 |
0.000 |
1.384 |
0.000 |
| N3 |
0.000 |
-0.604 |
1.166 |
| N4 |
0.000 |
-0.604 |
-1.166 |
| H5 |
-0.001 |
-0.092 |
2.031 |
| H6 |
-0.000 |
-1.610 |
1.197 |
| H7 |
-0.001 |
-0.092 |
-2.031 |
| H8 |
-0.000 |
-1.610 |
-1.197 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2510 | 1.3795 | 1.3795 | 2.0437 | 2.1143 | 2.0437 | 2.1143 |
O2 | 1.2510 | | 2.3048 | 2.3048 | 2.5107 | 3.2242 | 2.5107 | 3.2242 | N3 | 1.3795 | 2.3048 | | 2.3319 | 1.0057 | 1.0061 | 3.2381 | 2.5681 | N4 | 1.3795 | 2.3048 | 2.3319 | | 3.2381 | 2.5681 | 1.0057 | 1.0061 | H5 | 2.0437 | 2.5107 | 1.0057 | 3.2381 | | 1.7322 | 4.0625 | 3.5675 | H6 | 2.1143 | 3.2242 | 1.0061 | 2.5681 | 1.7322 | | 3.5675 | 2.3941 | H7 | 2.0437 | 2.5107 | 3.2381 | 1.0057 | 4.0625 | 3.5675 | | 1.7322 | H8 | 2.1143 | 3.2242 | 2.5681 | 1.0061 | 3.5675 | 2.3941 | 1.7322 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
117.060 |
|
C1 |
N3 |
H6 |
124.074 |
| C1 |
N4 |
H7 |
117.060 |
|
C1 |
N4 |
H8 |
124.074 |
| O2 |
C1 |
N3 |
122.303 |
|
O2 |
C1 |
N4 |
122.303 |
| N3 |
C1 |
N4 |
115.394 |
|
H5 |
N3 |
H6 |
118.865 |
| H7 |
N4 |
H8 |
118.865 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.663 |
|
|
|
| 2 |
O |
-0.480 |
|
|
|
| 3 |
N |
-0.739 |
|
|
|
| 4 |
N |
-0.739 |
|
|
|
| 5 |
H |
0.337 |
|
|
|
| 6 |
H |
0.311 |
|
|
|
| 7 |
H |
0.337 |
|
|
|
| 8 |
H |
0.311 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.004 |
-4.632 |
0.000 |
4.632 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.687 |
0.001 |
0.000 |
| y |
0.001 |
-24.224 |
0.000 |
| z |
0.000 |
0.000 |
-16.113 |
|
| Traceless |
| | x | y | z |
| x |
-5.519 |
0.001 |
0.000 |
| y |
0.001 |
-3.324 |
0.000 |
| z |
0.000 |
0.000 |
8.843 |
|
| Polar |
| 3z2-r2 | 17.685 |
| x2-y2 | -1.463 |
| 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 |
1.446 |
-0.000 |
0.000 |
| y |
-0.000 |
4.829 |
0.000 |
| z |
0.000 |
0.000 |
4.495 |
<r2> (average value of r
2) Å
2
| <r2> |
69.636 |
| (<r2>)1/2 |
8.345 |
Jump to
S1C1
S1C2
Energy calculated at B3LYP/6-31G
| | hartrees |
| Energy at 0K | -225.194324 |
| Energy at 298.15K | -225.200227 |
| HF Energy | -225.194324 |
| Nuclear repulsion energy | 122.628488 |
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/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 |
A1 |
3771 |
3628 |
30.02 |
|
|
|
| 2 |
A1 |
3635 |
3497 |
4.54 |
|
|
|
| 3 |
A1 |
1747 |
1681 |
370.43 |
|
|
|
| 4 |
A1 |
1679 |
1615 |
12.92 |
|
|
|
| 5 |
A1 |
1160 |
1116 |
2.19 |
|
|
|
| 6 |
A1 |
976 |
939 |
4.79 |
|
|
|
| 7 |
A1 |
484 |
466 |
3.55 |
|
|
|
| 8 |
A2 |
499 |
480 |
0.00 |
|
|
|
| 9 |
A2 |
185 |
178 |
0.00 |
|
|
|
| 10 |
B1 |
772 |
743 |
145.14 |
|
|
|
| 11 |
B1 |
577 |
555 |
124.28 |
|
|
|
| 12 |
B1 |
490 |
472 |
581.60 |
|
|
|
| 13 |
B2 |
3768 |
3625 |
38.13 |
|
|
|
| 14 |
B2 |
3626 |
3488 |
48.95 |
|
|
|
| 15 |
B2 |
1667 |
1604 |
228.83 |
|
|
|
| 16 |
B2 |
1468 |
1412 |
278.24 |
|
|
|
| 17 |
B2 |
1025 |
986 |
12.24 |
|
|
|
| 18 |
B2 |
560 |
539 |
14.27 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14045.1 cm
-1
Scaled (by 0.962) Zero Point Vibrational Energy (zpe) 13511.3 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/6-31G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.133 |
| O2 |
0.000 |
0.000 |
1.384 |
| N3 |
0.000 |
1.166 |
-0.604 |
| N4 |
0.000 |
-1.166 |
-0.604 |
| H5 |
0.000 |
2.032 |
-0.092 |
| H6 |
0.000 |
1.197 |
-1.610 |
| H7 |
0.000 |
-2.032 |
-0.092 |
| H8 |
0.000 |
-1.197 |
-1.610 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2508 | 1.3797 | 1.3797 | 2.0440 | 2.1142 | 2.0440 | 2.1142 |
O2 | 1.2508 | | 2.3048 | 2.3048 | 2.5110 | 3.2240 | 2.5110 | 3.2240 | N3 | 1.3797 | 2.3048 | | 2.3324 | 1.0057 | 1.0061 | 3.2386 | 2.5682 | N4 | 1.3797 | 2.3048 | 2.3324 | | 3.2386 | 2.5682 | 1.0057 | 1.0061 | H5 | 2.0440 | 2.5110 | 1.0057 | 3.2386 | | 1.7322 | 4.0633 | 3.5675 | H6 | 2.1142 | 3.2240 | 1.0061 | 2.5682 | 1.7322 | | 3.5675 | 2.3938 | H7 | 2.0440 | 2.5110 | 3.2386 | 1.0057 | 4.0633 | 3.5675 | | 1.7322 | H8 | 2.1142 | 3.2240 | 2.5682 | 1.0061 | 3.5675 | 2.3938 | 1.7322 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
117.081 |
|
C1 |
N3 |
H6 |
124.049 |
| C1 |
N4 |
H7 |
117.081 |
|
C1 |
N4 |
H8 |
124.049 |
| O2 |
C1 |
N3 |
122.299 |
|
O2 |
C1 |
N4 |
122.299 |
| N3 |
C1 |
N4 |
115.403 |
|
H5 |
N3 |
H6 |
118.871 |
| H7 |
N4 |
H8 |
118.871 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.663 |
|
|
|
| 2 |
O |
-0.480 |
|
|
|
| 3 |
N |
-0.739 |
|
|
|
| 4 |
N |
-0.739 |
|
|
|
| 5 |
H |
0.337 |
|
|
|
| 6 |
H |
0.311 |
|
|
|
| 7 |
H |
0.337 |
|
|
|
| 8 |
H |
0.311 |
|
|
|
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 |
-4.630 |
4.630 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.687 |
0.000 |
0.000 |
| y |
0.000 |
-16.112 |
0.000 |
| z |
0.000 |
0.000 |
-24.224 |
|
| Traceless |
| | x | y | z |
| x |
-5.519 |
0.000 |
0.000 |
| y |
0.000 |
8.843 |
0.000 |
| z |
0.000 |
0.000 |
-3.324 |
|
| Polar |
| 3z2-r2 | -6.649 |
| x2-y2 | -9.575 |
| 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 |
1.445 |
0.000 |
0.000 |
| y |
0.000 |
4.496 |
0.000 |
| z |
0.000 |
0.000 |
4.829 |
<r2> (average value of r
2) Å
2
| <r2> |
69.642 |
| (<r2>)1/2 |
8.345 |