Jump to
S1C2
S1C3
Energy calculated at B3LYP/6-31+G**
| | hartrees |
| Energy at 0K | -225.291760 |
| Energy at 298.15K | -225.297863 |
| HF Energy | -225.291760 |
| Nuclear repulsion energy | 123.287814 |
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/6-31+G**
| 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 |
3708 |
3575 |
43.35 |
|
|
|
| 2 |
A |
3587 |
3459 |
4.04 |
|
|
|
| 3 |
A |
1792 |
1728 |
489.96 |
|
|
|
| 4 |
A |
1635 |
1576 |
0.26 |
|
|
|
| 5 |
A |
1173 |
1131 |
2.96 |
|
|
|
| 6 |
A |
956 |
922 |
10.32 |
|
|
|
| 7 |
A |
544 |
524 |
66.84 |
|
|
|
| 8 |
A |
475 |
458 |
2.33 |
|
|
|
| 9 |
A |
363 |
350 |
71.70 |
|
|
|
| 10 |
B |
3707 |
3575 |
38.39 |
|
|
|
| 11 |
B |
3582 |
3453 |
51.67 |
|
|
|
| 12 |
B |
1636 |
1578 |
215.46 |
|
|
|
| 13 |
B |
1413 |
1363 |
238.35 |
|
|
|
| 14 |
B |
1040 |
1003 |
24.84 |
|
|
|
| 15 |
B |
769 |
742 |
56.27 |
|
|
|
| 16 |
B |
575 |
555 |
70.80 |
|
|
|
| 17 |
B |
538 |
519 |
177.81 |
|
|
|
| 18 |
B |
445 |
429 |
192.59 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13969.5 cm
-1
Scaled (by 0.9642) Zero Point Vibrational Energy (zpe) 13469.4 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/6-31+G**
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.140 |
| O2 |
0.000 |
0.000 |
1.364 |
| N3 |
-0.112 |
1.160 |
-0.611 |
| N4 |
0.112 |
-1.160 |
-0.611 |
| H5 |
0.000 |
2.005 |
-0.069 |
| H6 |
0.301 |
1.185 |
-1.533 |
| H7 |
0.000 |
-2.005 |
-0.069 |
| H8 |
-0.301 |
-1.185 |
-1.533 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2246 | 1.3863 | 1.3863 | 2.0159 | 2.0719 | 2.0159 | 2.0719 |
O2 | 1.2246 | | 2.2935 | 2.2935 | 2.4646 | 3.1447 | 2.4646 | 3.1447 | N3 | 1.3863 | 2.2935 | | 2.3308 | 1.0103 | 1.0105 | 3.2132 | 2.5268 | N4 | 1.3863 | 2.2935 | 2.3308 | | 3.2132 | 2.5268 | 1.0103 | 1.0105 | H5 | 2.0159 | 2.4646 | 1.0103 | 3.2132 | | 1.7052 | 4.0103 | 3.5229 | H6 | 2.0719 | 3.1447 | 1.0105 | 2.5268 | 1.7052 | | 3.5229 | 2.4450 | H7 | 2.0159 | 2.4646 | 3.2132 | 1.0103 | 4.0103 | 3.5229 | | 1.7052 | H8 | 2.0719 | 3.1447 | 2.5268 | 1.0105 | 3.5229 | 2.4450 | 1.7052 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
113.605 |
|
C1 |
N3 |
H6 |
118.802 |
| C1 |
N4 |
H7 |
113.605 |
|
C1 |
N4 |
H8 |
118.802 |
| O2 |
C1 |
N3 |
122.789 |
|
O2 |
C1 |
N4 |
122.789 |
| N3 |
C1 |
N4 |
114.423 |
|
H5 |
N3 |
H6 |
115.095 |
| H7 |
N4 |
H8 |
115.095 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.521 |
|
|
|
| 2 |
O |
-0.551 |
|
|
|
| 3 |
N |
-0.590 |
|
|
|
| 4 |
N |
-0.590 |
|
|
|
| 5 |
H |
0.316 |
|
|
|
| 6 |
H |
0.289 |
|
|
|
| 7 |
H |
0.316 |
|
|
|
| 8 |
H |
0.289 |
|
|
|
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 |
-3.975 |
3.975 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
0.011 |
-0.006 |
-3.961 |
3.961 |
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.363 |
2.461 |
0.000 |
| y |
2.461 |
-17.458 |
0.000 |
| z |
0.000 |
0.000 |
-25.777 |
|
| Traceless |
| | x | y | z |
| x |
-4.745 |
2.461 |
0.000 |
| y |
2.461 |
8.612 |
0.000 |
| z |
0.000 |
0.000 |
-3.866 |
|
| Polar |
| 3z2-r2 | -7.732 |
| x2-y2 | -8.905 |
| xy | 2.461 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.598 |
-0.122 |
0.000 |
| y |
-0.122 |
5.425 |
0.000 |
| z |
0.000 |
0.000 |
5.796 |
<r2> (average value of r
2) Å
2
| <r2> |
69.479 |
| (<r2>)1/2 |
8.335 |
Jump to
S1C1
S1C3
Energy calculated at B3LYP/6-31+G**
| | hartrees |
| Energy at 0K | -225.290530 |
| Energy at 298.15K | |
| HF Energy | -225.290530 |
| Nuclear repulsion energy | 123.347099 |
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/6-31+G**
| 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' |
3739 |
3605 |
47.58 |
|
|
|
| 2 |
A' |
3611 |
3482 |
8.61 |
|
|
|
| 3 |
A' |
1781 |
1718 |
523.99 |
|
|
|
| 4 |
A' |
1638 |
1580 |
8.32 |
|
|
|
| 5 |
A' |
1161 |
1120 |
2.32 |
|
|
|
| 6 |
A' |
964 |
929 |
11.16 |
|
|
|
| 7 |
A' |
762 |
735 |
15.18 |
|
|
|
| 8 |
A' |
547 |
527 |
26.62 |
|
|
|
| 9 |
A' |
478 |
461 |
8.24 |
|
|
|
| 10 |
A' |
328 |
317 |
434.68 |
|
|
|
| 11 |
A" |
3737 |
3603 |
45.73 |
|
|
|
| 12 |
A" |
3602 |
3473 |
55.05 |
|
|
|
| 13 |
A" |
1628 |
1570 |
245.27 |
|
|
|
| 14 |
A" |
1418 |
1367 |
242.30 |
|
|
|
| 15 |
A" |
1007 |
971 |
20.34 |
|
|
|
| 16 |
A" |
568 |
547 |
17.83 |
|
|
|
| 17 |
A" |
390 |
376 |
36.20 |
|
|
|
| 18 |
A" |
40i |
39i |
37.49 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13659.0 cm
-1
Scaled (by 0.9642) Zero Point Vibrational Energy (zpe) 13170.0 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/6-31+G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.005 |
0.137 |
0.000 |
| O2 |
0.030 |
1.363 |
0.000 |
| N3 |
0.030 |
-0.602 |
1.167 |
| N4 |
0.030 |
-0.602 |
-1.167 |
| H5 |
-0.127 |
-0.074 |
2.011 |
| H6 |
-0.217 |
-1.579 |
1.184 |
| H7 |
-0.127 |
-0.074 |
-2.011 |
| H8 |
-0.217 |
-1.579 |
-1.184 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2262 | 1.3811 | 1.3811 | 2.0268 | 2.0970 | 2.0268 | 2.0970 |
O2 | 1.2262 | | 2.2850 | 2.2850 | 2.4770 | 3.1812 | 2.4770 | 3.1812 | N3 | 1.3811 | 2.2850 | | 2.3334 | 1.0084 | 1.0083 | 3.2255 | 2.5581 | N4 | 1.3811 | 2.2850 | 2.3334 | | 3.2255 | 2.5581 | 1.0084 | 1.0083 | H5 | 2.0268 | 2.4770 | 1.0084 | 3.2255 | | 1.7198 | 4.0229 | 3.5336 | H6 | 2.0970 | 3.1812 | 1.0083 | 2.5581 | 1.7198 | | 3.5336 | 2.3687 | H7 | 2.0268 | 2.4770 | 3.2255 | 1.0084 | 4.0229 | 3.5336 | | 1.7198 | H8 | 2.0970 | 3.1812 | 2.5581 | 1.0083 | 3.5336 | 2.3687 | 1.7198 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
115.148 |
|
C1 |
N3 |
H6 |
121.936 |
| C1 |
N4 |
H7 |
115.148 |
|
C1 |
N4 |
H8 |
121.936 |
| O2 |
C1 |
N3 |
122.305 |
|
O2 |
C1 |
N4 |
122.305 |
| N3 |
C1 |
N4 |
115.287 |
|
H5 |
N3 |
H6 |
117.033 |
| H7 |
N4 |
H8 |
117.033 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.554 |
|
|
|
| 2 |
O |
-0.569 |
|
|
|
| 3 |
N |
-0.591 |
|
|
|
| 4 |
N |
-0.591 |
|
|
|
| 5 |
H |
0.319 |
|
|
|
| 6 |
H |
0.280 |
|
|
|
| 7 |
H |
0.319 |
|
|
|
| 8 |
H |
0.280 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.353 |
-4.326 |
0.000 |
4.533 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.451 |
1.456 |
0.000 |
| y |
1.456 |
-25.142 |
0.000 |
| z |
0.000 |
0.000 |
-17.410 |
|
| Traceless |
| | x | y | z |
| x |
-5.176 |
1.456 |
0.000 |
| y |
1.456 |
-3.212 |
0.000 |
| z |
0.000 |
0.000 |
8.387 |
|
| Polar |
| 3z2-r2 | 16.775 |
| x2-y2 | -1.309 |
| xy | 1.456 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.572 |
0.031 |
0.000 |
| y |
0.031 |
5.716 |
0.000 |
| z |
0.000 |
0.000 |
5.437 |
<r2> (average value of r
2) Å
2
| <r2> |
69.509 |
| (<r2>)1/2 |
8.337 |
Jump to
S1C1
S1C2
Energy calculated at B3LYP/6-31+G**
| | hartrees |
| Energy at 0K | -225.290264 |
| Energy at 298.15K | |
| HF Energy | -225.290264 |
| Nuclear repulsion energy | 123.427236 |
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/6-31+G**
| 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 |
3766 |
3631 |
57.55 |
|
|
|
| 2 |
A1 |
3630 |
3500 |
7.16 |
|
|
|
| 3 |
A1 |
1778 |
1714 |
560.87 |
|
|
|
| 4 |
A1 |
1630 |
1571 |
0.18 |
|
|
|
| 5 |
A1 |
1142 |
1101 |
0.25 |
|
|
|
| 6 |
A1 |
970 |
935 |
10.37 |
|
|
|
| 7 |
A1 |
478 |
461 |
3.30 |
|
|
|
| 8 |
A2 |
364 |
351 |
0.00 |
|
|
|
| 9 |
A2 |
355i |
342i |
0.00 |
|
|
|
| 10 |
B1 |
762 |
734 |
5.05 |
|
|
|
| 11 |
B1 |
561 |
541 |
9.59 |
|
|
|
| 12 |
B1 |
232i |
224i |
503.66 |
|
|
|
| 13 |
B2 |
3763 |
3629 |
51.75 |
|
|
|
| 14 |
B2 |
3621 |
3491 |
70.61 |
|
|
|
| 15 |
B2 |
1623 |
1565 |
289.87 |
|
|
|
| 16 |
B2 |
1420 |
1369 |
255.14 |
|
|
|
| 17 |
B2 |
987 |
951 |
14.49 |
|
|
|
| 18 |
B2 |
562 |
542 |
12.72 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13234.2 cm
-1
Scaled (by 0.9642) Zero Point Vibrational Energy (zpe) 12760.4 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/6-31+G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.138 |
| O2 |
0.000 |
0.000 |
1.365 |
| N3 |
0.000 |
1.163 |
-0.598 |
| N4 |
0.000 |
-1.163 |
-0.598 |
| H5 |
0.000 |
2.029 |
-0.084 |
| H6 |
0.000 |
1.194 |
-1.604 |
| H7 |
0.000 |
-2.029 |
-0.084 |
| H8 |
0.000 |
-1.194 |
-1.604 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2270 | 1.3767 | 1.3767 | 2.0407 | 2.1122 | 2.0407 | 2.1122 |
O2 | 1.2270 | | 2.2821 | 2.2821 | 2.4930 | 3.2004 | 2.4930 | 3.2004 | N3 | 1.3767 | 2.2821 | | 2.3265 | 1.0067 | 1.0065 | 3.2330 | 2.5628 | N4 | 1.3767 | 2.2821 | 2.3265 | | 3.2330 | 2.5628 | 1.0067 | 1.0065 | H5 | 2.0407 | 2.4930 | 1.0067 | 3.2330 | | 1.7345 | 4.0573 | 3.5631 | H6 | 2.1122 | 3.2004 | 1.0065 | 2.5628 | 1.7345 | | 3.5631 | 2.3877 | H7 | 2.0407 | 2.4930 | 3.2330 | 1.0067 | 4.0573 | 3.5631 | | 1.7345 | H8 | 2.1122 | 3.2004 | 2.5628 | 1.0065 | 3.5631 | 2.3877 | 1.7345 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
116.939 |
|
C1 |
N3 |
H6 |
124.078 |
| C1 |
N4 |
H7 |
116.939 |
|
C1 |
N4 |
H8 |
124.078 |
| O2 |
C1 |
N3 |
122.335 |
|
O2 |
C1 |
N4 |
122.335 |
| N3 |
C1 |
N4 |
115.331 |
|
H5 |
N3 |
H6 |
118.983 |
| H7 |
N4 |
H8 |
118.983 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.612 |
|
|
|
| 2 |
O |
-0.591 |
|
|
|
| 3 |
N |
-0.622 |
|
|
|
| 4 |
N |
-0.622 |
|
|
|
| 5 |
H |
0.323 |
|
|
|
| 6 |
H |
0.288 |
|
|
|
| 7 |
H |
0.323 |
|
|
|
| 8 |
H |
0.288 |
|
|
|
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 |
-4.564 |
4.564 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.753 |
0.000 |
0.000 |
| y |
0.000 |
-16.917 |
0.000 |
| z |
0.000 |
0.000 |
-24.787 |
|
| Traceless |
| | x | y | z |
| x |
-5.901 |
0.000 |
0.000 |
| y |
0.000 |
8.853 |
0.000 |
| z |
0.000 |
0.000 |
-2.952 |
|
| Polar |
| 3z2-r2 | -5.903 |
| x2-y2 | -9.836 |
| 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 |
3.534 |
0.000 |
0.000 |
| y |
0.000 |
5.392 |
0.000 |
| z |
0.000 |
0.000 |
5.624 |
<r2> (average value of r
2) Å
2
| <r2> |
69.471 |
| (<r2>)1/2 |
8.335 |