Jump to
S1C2
S1C3
Energy calculated at B3LYP/6-31G*
| | hartrees |
| Energy at 0K | -225.260458 |
| Energy at 298.15K | -225.266671 |
| HF Energy | -225.260458 |
| Nuclear repulsion energy | 123.264775 |
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 |
3671 |
3526 |
21.85 |
|
|
|
| 2 |
A |
3562 |
3420 |
1.62 |
|
|
|
| 3 |
A |
1840 |
1767 |
355.59 |
|
|
|
| 4 |
A |
1660 |
1594 |
0.01 |
|
|
|
| 5 |
A |
1198 |
1150 |
3.55 |
|
|
|
| 6 |
A |
955 |
917 |
6.29 |
|
|
|
| 7 |
A |
630 |
605 |
98.05 |
|
|
|
| 8 |
A |
473 |
454 |
2.48 |
|
|
|
| 9 |
A |
395 |
379 |
69.65 |
|
|
|
| 10 |
B |
3671 |
3526 |
26.48 |
|
|
|
| 11 |
B |
3557 |
3416 |
33.41 |
|
|
|
| 12 |
B |
1663 |
1597 |
180.45 |
|
|
|
| 13 |
B |
1427 |
1370 |
201.29 |
|
|
|
| 14 |
B |
1065 |
1023 |
25.25 |
|
|
|
| 15 |
B |
789 |
758 |
132.51 |
|
|
|
| 16 |
B |
588 |
565 |
222.53 |
|
|
|
| 17 |
B |
557 |
535 |
108.14 |
|
|
|
| 18 |
B |
457 |
439 |
64.73 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14078.7 cm
-1
Scaled (by 0.9603) Zero Point Vibrational Energy (zpe) 13519.8 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/6-31G*
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.145 |
| O2 |
0.000 |
0.000 |
1.365 |
| N3 |
-0.131 |
1.157 |
-0.617 |
| N4 |
0.131 |
-1.157 |
-0.617 |
| H5 |
0.000 |
1.996 |
-0.067 |
| H6 |
0.348 |
1.178 |
-1.509 |
| H7 |
0.000 |
-1.996 |
-0.067 |
| H8 |
-0.348 |
-1.178 |
-1.509 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2201 | 1.3914 | 1.3914 | 2.0071 | 2.0603 | 2.0071 | 2.0603 |
O2 | 1.2201 | | 2.2986 | 2.2986 | 2.4563 | 3.1257 | 2.4563 | 3.1257 | N3 | 1.3914 | 2.2986 | | 2.3285 | 1.0119 | 1.0128 | 3.2031 | 2.5088 | N4 | 1.3914 | 2.2986 | 2.3285 | | 3.2031 | 2.5088 | 1.0119 | 1.0128 | H5 | 2.0071 | 2.4563 | 1.0119 | 3.2031 | | 1.6945 | 3.9918 | 3.5035 | H6 | 2.0603 | 3.1257 | 1.0128 | 2.5088 | 1.6945 | | 3.5035 | 2.4562 | H7 | 2.0071 | 2.4563 | 3.2031 | 1.0119 | 3.9918 | 3.5035 | | 1.6945 | H8 | 2.0603 | 3.1257 | 2.5088 | 1.0128 | 3.5035 | 2.4562 | 1.6945 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
112.303 |
|
C1 |
N3 |
H6 |
117.077 |
| C1 |
N4 |
H7 |
112.303 |
|
C1 |
N4 |
H8 |
117.077 |
| O2 |
C1 |
N3 |
123.201 |
|
O2 |
C1 |
N4 |
123.201 |
| N3 |
C1 |
N4 |
113.599 |
|
H5 |
N3 |
H6 |
113.629 |
| H7 |
N4 |
H8 |
113.629 |
|
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 |
0.657 |
|
|
|
| 2 |
O |
-0.500 |
|
|
|
| 3 |
N |
-0.743 |
|
|
|
| 4 |
N |
-0.743 |
|
|
|
| 5 |
H |
0.340 |
|
|
|
| 6 |
H |
0.325 |
|
|
|
| 7 |
H |
0.340 |
|
|
|
| 8 |
H |
0.325 |
|
|
|
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 |
-3.491 |
3.491 |
| CHELPG |
0.000 |
0.000 |
-3.523 |
3.523 |
| AIM |
0.000 |
0.000 |
0.963 |
0.963 |
| ESP |
0.007 |
-0.006 |
-3.507 |
3.507 |
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.982 |
2.795 |
0.000 |
| y |
2.795 |
-16.925 |
0.000 |
| z |
0.000 |
0.000 |
-24.685 |
|
| Traceless |
| | x | y | z |
| x |
-4.177 |
2.795 |
0.000 |
| y |
2.795 |
7.909 |
0.000 |
| z |
0.000 |
0.000 |
-3.732 |
|
| Polar |
| 3z2-r2 | -7.463 |
| x2-y2 | -8.057 |
| xy | 2.795 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.055 |
-0.092 |
0.000 |
| y |
-0.092 |
4.653 |
0.000 |
| z |
0.000 |
0.000 |
4.797 |
<r2> (average value of r
2) Å
2
| <r2> |
68.750 |
| (<r2>)1/2 |
8.292 |
Jump to
S1C1
S1C3
Energy calculated at B3LYP/6-31G*
| | hartrees |
| Energy at 0K | -225.258278 |
| Energy at 298.15K | -225.264034 |
| HF Energy | -225.258278 |
| Nuclear repulsion energy | 123.311578 |
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' |
3702 |
3555 |
23.00 |
|
|
|
| 2 |
A' |
3588 |
3445 |
8.10 |
|
|
|
| 3 |
A' |
1829 |
1757 |
376.54 |
|
|
|
| 4 |
A' |
1668 |
1601 |
15.74 |
|
|
|
| 5 |
A' |
1191 |
1143 |
3.87 |
|
|
|
| 6 |
A' |
963 |
925 |
8.42 |
|
|
|
| 7 |
A' |
767 |
737 |
46.70 |
|
|
|
| 8 |
A' |
552 |
530 |
56.95 |
|
|
|
| 9 |
A' |
486 |
467 |
69.83 |
|
|
|
| 10 |
A' |
429 |
412 |
328.71 |
|
|
|
| 11 |
A" |
3699 |
3553 |
34.52 |
|
|
|
| 12 |
A" |
3577 |
3435 |
30.28 |
|
|
|
| 13 |
A" |
1652 |
1586 |
193.30 |
|
|
|
| 14 |
A" |
1432 |
1375 |
208.31 |
|
|
|
| 15 |
A" |
1028 |
987 |
22.57 |
|
|
|
| 16 |
A" |
571 |
548 |
28.95 |
|
|
|
| 17 |
A" |
434 |
417 |
87.77 |
|
|
|
| 18 |
A" |
175 |
168 |
38.87 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13870.8 cm
-1
Scaled (by 0.9603) Zero Point Vibrational Energy (zpe) 13320.1 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 |
0.008 |
0.141 |
0.000 |
| O2 |
0.039 |
1.362 |
0.000 |
| N3 |
0.039 |
-0.606 |
1.167 |
| N4 |
0.039 |
-0.606 |
-1.167 |
| H5 |
-0.165 |
-0.070 |
1.998 |
| H6 |
-0.294 |
-1.560 |
1.174 |
| H7 |
-0.165 |
-0.070 |
-1.998 |
| H8 |
-0.294 |
-1.560 |
-1.174 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2219 | 1.3861 | 1.3861 | 2.0167 | 2.0888 | 2.0167 | 2.0888 |
O2 | 1.2219 | | 2.2884 | 2.2884 | 2.4668 | 3.1670 | 2.4668 | 3.1670 | N3 | 1.3861 | 2.2884 | | 2.3345 | 1.0100 | 1.0106 | 3.2171 | 2.5504 | N4 | 1.3861 | 2.2884 | 2.3345 | | 3.2171 | 2.5504 | 1.0100 | 1.0106 | H5 | 2.0167 | 2.4668 | 1.0100 | 3.2171 | | 1.7078 | 3.9964 | 3.5075 | H6 | 2.0888 | 3.1670 | 1.0106 | 2.5504 | 1.7078 | | 3.5075 | 2.3487 | H7 | 2.0167 | 2.4668 | 3.2171 | 1.0100 | 3.9964 | 3.5075 | | 1.7078 | H8 | 2.0888 | 3.1670 | 2.5504 | 1.0106 | 3.5075 | 2.3487 | 1.7078 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
113.717 |
|
C1 |
N3 |
H6 |
120.474 |
| C1 |
N4 |
H7 |
113.717 |
|
C1 |
N4 |
H8 |
120.474 |
| O2 |
C1 |
N3 |
122.549 |
|
O2 |
C1 |
N4 |
122.549 |
| N3 |
C1 |
N4 |
114.737 |
|
H5 |
N3 |
H6 |
115.390 |
| H7 |
N4 |
H8 |
115.390 |
|
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 |
0.679 |
|
|
|
| 2 |
O |
-0.512 |
|
|
|
| 3 |
N |
-0.742 |
|
|
|
| 4 |
N |
-0.742 |
|
|
|
| 5 |
H |
0.342 |
|
|
|
| 6 |
H |
0.316 |
|
|
|
| 7 |
H |
0.342 |
|
|
|
| 8 |
H |
0.316 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.851 |
-3.845 |
0.000 |
4.268 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.917 |
1.881 |
0.000 |
| y |
1.881 |
-24.040 |
0.000 |
| z |
0.000 |
0.000 |
-17.002 |
|
| Traceless |
| | x | y | z |
| x |
-4.396 |
1.881 |
0.000 |
| y |
1.881 |
-3.080 |
0.000 |
| z |
0.000 |
0.000 |
7.476 |
|
| Polar |
| 3z2-r2 | 14.952 |
| x2-y2 | -0.877 |
| xy | 1.881 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.945 |
0.178 |
0.000 |
| y |
0.178 |
4.825 |
0.000 |
| z |
0.000 |
0.000 |
4.680 |
<r2> (average value of r
2) Å
2
| <r2> |
68.797 |
| (<r2>)1/2 |
8.294 |
Jump to
S1C1
S1C2
Energy calculated at B3LYP/6-31G*
| | hartrees |
| Energy at 0K | -225.257325 |
| Energy at 298.15K | |
| HF Energy | -225.257325 |
| Nuclear repulsion energy | 123.475357 |
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 |
3750 |
3601 |
36.23 |
|
|
|
| 2 |
A1 |
3625 |
3482 |
5.42 |
|
|
|
| 3 |
A1 |
1824 |
1752 |
416.33 |
|
|
|
| 4 |
A1 |
1649 |
1584 |
1.93 |
|
|
|
| 5 |
A1 |
1154 |
1108 |
0.25 |
|
|
|
| 6 |
A1 |
975 |
936 |
7.15 |
|
|
|
| 7 |
A1 |
478 |
459 |
3.42 |
|
|
|
| 8 |
A2 |
372 |
357 |
0.00 |
|
|
|
| 9 |
A2 |
443i |
425i |
0.00 |
|
|
|
| 10 |
B1 |
767 |
737 |
13.78 |
|
|
|
| 11 |
B1 |
572 |
549 |
10.52 |
|
|
|
| 12 |
B1 |
330i |
317i |
561.58 |
|
|
|
| 13 |
B2 |
3748 |
3599 |
46.13 |
|
|
|
| 14 |
B2 |
3615 |
3472 |
51.49 |
|
|
|
| 15 |
B2 |
1642 |
1577 |
269.97 |
|
|
|
| 16 |
B2 |
1436 |
1379 |
222.13 |
|
|
|
| 17 |
B2 |
991 |
952 |
12.84 |
|
|
|
| 18 |
B2 |
561 |
539 |
14.61 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13193.0 cm
-1
Scaled (by 0.9603) Zero Point Vibrational Energy (zpe) 12669.3 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 |
0.142 |
| O2 |
0.000 |
0.000 |
1.366 |
| N3 |
0.000 |
1.161 |
-0.599 |
| N4 |
0.000 |
-1.161 |
-0.599 |
| H5 |
0.000 |
2.028 |
-0.088 |
| H6 |
0.000 |
1.192 |
-1.606 |
| H7 |
0.000 |
-2.028 |
-0.088 |
| H8 |
0.000 |
-1.192 |
-1.606 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2234 | 1.3776 | 1.3776 | 2.0410 | 2.1161 | 2.0410 | 2.1161 |
O2 | 1.2234 | | 2.2825 | 2.2825 | 2.4952 | 3.2021 | 2.4952 | 3.2021 | N3 | 1.3776 | 2.2825 | | 2.3215 | 1.0068 | 1.0073 | 3.2295 | 2.5587 | N4 | 1.3776 | 2.2825 | 2.3215 | | 3.2295 | 2.5587 | 1.0068 | 1.0073 | H5 | 2.0410 | 2.4952 | 1.0068 | 3.2295 | | 1.7336 | 4.0559 | 3.5596 | H6 | 2.1161 | 3.2021 | 1.0073 | 2.5587 | 1.7336 | | 3.5596 | 2.3831 | H7 | 2.0410 | 2.4952 | 3.2295 | 1.0068 | 4.0559 | 3.5596 | | 1.7336 | H8 | 2.1161 | 3.2021 | 2.5587 | 1.0073 | 3.5596 | 2.3831 | 1.7336 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
116.875 |
|
C1 |
N3 |
H6 |
124.337 |
| C1 |
N4 |
H7 |
116.875 |
|
C1 |
N4 |
H8 |
124.337 |
| O2 |
C1 |
N3 |
122.586 |
|
O2 |
C1 |
N4 |
122.586 |
| N3 |
C1 |
N4 |
114.827 |
|
H5 |
N3 |
H6 |
118.788 |
| H7 |
N4 |
H8 |
118.788 |
|
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 |
0.725 |
|
|
|
| 2 |
O |
-0.528 |
|
|
|
| 3 |
N |
-0.768 |
|
|
|
| 4 |
N |
-0.768 |
|
|
|
| 5 |
H |
0.347 |
|
|
|
| 6 |
H |
0.323 |
|
|
|
| 7 |
H |
0.347 |
|
|
|
| 8 |
H |
0.323 |
|
|
|
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 |
-4.261 |
4.261 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.366 |
0.000 |
0.000 |
| y |
0.000 |
-16.073 |
0.000 |
| z |
0.000 |
0.000 |
-23.369 |
|
| Traceless |
| | x | y | z |
| x |
-5.645 |
0.000 |
0.000 |
| y |
0.000 |
8.295 |
0.000 |
| z |
0.000 |
0.000 |
-2.649 |
|
| Polar |
| 3z2-r2 | -5.299 |
| x2-y2 | -9.293 |
| 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 |
1.805 |
0.000 |
0.000 |
| y |
0.000 |
4.653 |
0.000 |
| z |
0.000 |
0.000 |
4.789 |
<r2> (average value of r
2) Å
2
| <r2> |
68.674 |
| (<r2>)1/2 |
8.287 |