Jump to
S1C2
S1C3
Energy calculated at B3LYP/6-311G*
| | hartrees |
| Energy at 0K | -225.326805 |
| Energy at 298.15K | -225.333010 |
| HF Energy | -225.326805 |
| Nuclear repulsion energy | 123.573702 |
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/6-311G*
| 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 |
3683 |
3559 |
16.97 |
|
|
|
| 2 |
A |
3576 |
3455 |
1.21 |
|
|
|
| 3 |
A |
1822 |
1761 |
400.32 |
|
|
|
| 4 |
A |
1674 |
1618 |
0.68 |
|
|
|
| 5 |
A |
1198 |
1158 |
4.63 |
|
|
|
| 6 |
A |
949 |
917 |
7.51 |
|
|
|
| 7 |
A |
606 |
585 |
93.79 |
|
|
|
| 8 |
A |
476 |
460 |
3.60 |
|
|
|
| 9 |
A |
388 |
375 |
74.57 |
|
|
|
| 10 |
B |
3683 |
3559 |
19.87 |
|
|
|
| 11 |
B |
3571 |
3451 |
27.05 |
|
|
|
| 12 |
B |
1675 |
1618 |
191.25 |
|
|
|
| 13 |
B |
1418 |
1370 |
213.48 |
|
|
|
| 14 |
B |
1061 |
1026 |
29.94 |
|
|
|
| 15 |
B |
793 |
766 |
100.99 |
|
|
|
| 16 |
B |
585 |
565 |
142.51 |
|
|
|
| 17 |
B |
554 |
535 |
174.87 |
|
|
|
| 18 |
B |
451 |
436 |
104.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14080.5 cm
-1
Scaled (by 0.9663) Zero Point Vibrational Energy (zpe) 13606.0 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/6-311G*
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.147 |
| O2 |
0.000 |
0.000 |
1.360 |
| N3 |
-0.118 |
1.156 |
-0.615 |
| N4 |
0.118 |
-1.156 |
-0.615 |
| H5 |
0.000 |
1.997 |
-0.070 |
| H6 |
0.348 |
1.178 |
-1.509 |
| H7 |
0.000 |
-1.997 |
-0.070 |
| H8 |
-0.348 |
-1.178 |
-1.509 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2138 | 1.3892 | 1.3892 | 2.0084 | 2.0616 | 2.0084 | 2.0616 |
O2 | 1.2138 | | 2.2915 | 2.2915 | 2.4564 | 3.1215 | 2.4564 | 3.1215 | N3 | 1.3892 | 2.2915 | | 2.3243 | 1.0084 | 1.0092 | 3.2016 | 2.5099 | N4 | 1.3892 | 2.2915 | 2.3243 | | 3.2016 | 2.5099 | 1.0084 | 1.0092 | H5 | 2.0084 | 2.4564 | 1.0084 | 3.2016 | | 1.6920 | 3.9933 | 3.5026 | H6 | 2.0616 | 3.1215 | 1.0092 | 2.5099 | 1.6920 | | 3.5026 | 2.4558 | H7 | 2.0084 | 2.4564 | 3.2016 | 1.0084 | 3.9933 | 3.5026 | | 1.6920 | H8 | 2.0616 | 3.1215 | 2.5099 | 1.0092 | 3.5026 | 2.4558 | 1.6920 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
112.829 |
|
C1 |
N3 |
H6 |
117.662 |
| C1 |
N4 |
H7 |
112.829 |
|
C1 |
N4 |
H8 |
117.662 |
| O2 |
C1 |
N3 |
123.224 |
|
O2 |
C1 |
N4 |
123.224 |
| N3 |
C1 |
N4 |
113.551 |
|
H5 |
N3 |
H6 |
113.991 |
| H7 |
N4 |
H8 |
113.991 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.550 |
|
|
|
| 2 |
O |
-0.379 |
|
|
|
| 3 |
N |
-0.764 |
|
|
|
| 4 |
N |
-0.764 |
|
|
|
| 5 |
H |
0.347 |
|
|
|
| 6 |
H |
0.331 |
|
|
|
| 7 |
H |
0.347 |
|
|
|
| 8 |
H |
0.331 |
|
|
|
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 |
-3.590 |
3.590 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
0.009 |
-0.006 |
-3.601 |
3.601 |
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.383 |
2.690 |
0.000 |
| y |
2.690 |
-17.135 |
0.000 |
| z |
0.000 |
0.000 |
-25.013 |
|
| Traceless |
| | x | y | z |
| x |
-4.309 |
2.690 |
0.000 |
| y |
2.690 |
8.063 |
0.000 |
| z |
0.000 |
0.000 |
-3.754 |
|
| Polar |
| 3z2-r2 | -7.508 |
| x2-y2 | -8.248 |
| xy | 2.690 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.441 |
-0.069 |
0.000 |
| y |
-0.069 |
4.836 |
0.000 |
| z |
0.000 |
0.000 |
4.944 |
<r2> (average value of r
2) Å
2
| <r2> |
68.745 |
| (<r2>)1/2 |
8.291 |
Jump to
S1C1
S1C3
Energy calculated at B3LYP/6-311G*
| | hartrees |
| Energy at 0K | -225.324771 |
| Energy at 298.15K | |
| HF Energy | -225.324771 |
| Nuclear repulsion energy | 123.638120 |
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/6-311G*
| 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' |
3720 |
3594 |
19.08 |
|
|
|
| 2 |
A' |
3604 |
3483 |
5.65 |
|
|
|
| 3 |
A' |
1811 |
1750 |
433.36 |
|
|
|
| 4 |
A' |
1677 |
1621 |
12.58 |
|
|
|
| 5 |
A' |
1187 |
1147 |
3.58 |
|
|
|
| 6 |
A' |
959 |
926 |
9.67 |
|
|
|
| 7 |
A' |
776 |
749 |
28.27 |
|
|
|
| 8 |
A' |
554 |
535 |
36.45 |
|
|
|
| 9 |
A' |
482 |
465 |
14.96 |
|
|
|
| 10 |
A' |
367 |
355 |
427.83 |
|
|
|
| 11 |
A" |
3717 |
3592 |
27.39 |
|
|
|
| 12 |
A" |
3594 |
3473 |
27.77 |
|
|
|
| 13 |
A" |
1661 |
1605 |
207.36 |
|
|
|
| 14 |
A" |
1422 |
1375 |
230.45 |
|
|
|
| 15 |
A" |
1019 |
985 |
25.19 |
|
|
|
| 16 |
A" |
573 |
553 |
22.15 |
|
|
|
| 17 |
A" |
404 |
390 |
57.36 |
|
|
|
| 18 |
A" |
90i |
87i |
48.79 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13717.8 cm
-1
Scaled (by 0.9663) Zero Point Vibrational Energy (zpe) 13255.5 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 B3LYP/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.008 |
0.143 |
0.000 |
| O2 |
0.034 |
1.358 |
0.000 |
| N3 |
0.034 |
-0.603 |
1.165 |
| N4 |
0.034 |
-0.603 |
-1.165 |
| H5 |
-0.146 |
-0.076 |
2.003 |
| H6 |
-0.253 |
-1.567 |
1.178 |
| H7 |
-0.146 |
-0.076 |
-2.003 |
| H8 |
-0.253 |
-1.567 |
-1.178 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2156 | 1.3831 | 1.3831 | 2.0207 | 2.0931 | 2.0207 | 2.0931 |
O2 | 1.2156 | | 2.2808 | 2.2808 | 2.4700 | 3.1670 | 2.4700 | 3.1670 | N3 | 1.3831 | 2.2808 | | 2.3292 | 1.0063 | 1.0067 | 3.2160 | 2.5494 | N4 | 1.3831 | 2.2808 | 2.3292 | | 3.2160 | 2.5494 | 1.0063 | 1.0067 | H5 | 2.0207 | 2.4700 | 1.0063 | 3.2160 | | 1.7080 | 4.0058 | 3.5146 | H6 | 2.0931 | 3.1670 | 1.0067 | 2.5494 | 1.7080 | | 3.5146 | 2.3554 | H7 | 2.0207 | 2.4700 | 3.2160 | 1.0063 | 4.0058 | 3.5146 | | 1.7080 | H8 | 2.0931 | 3.1670 | 2.5494 | 1.0067 | 3.5146 | 2.3554 | 1.7080 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
114.572 |
|
C1 |
N3 |
H6 |
121.486 |
| C1 |
N4 |
H7 |
114.572 |
|
C1 |
N4 |
H8 |
121.486 |
| O2 |
C1 |
N3 |
122.589 |
|
O2 |
C1 |
N4 |
122.589 |
| N3 |
C1 |
N4 |
114.704 |
|
H5 |
N3 |
H6 |
116.092 |
| H7 |
N4 |
H8 |
116.092 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.587 |
|
|
|
| 2 |
O |
-0.391 |
|
|
|
| 3 |
N |
-0.775 |
|
|
|
| 4 |
N |
-0.775 |
|
|
|
| 5 |
H |
0.351 |
|
|
|
| 6 |
H |
0.326 |
|
|
|
| 7 |
H |
0.351 |
|
|
|
| 8 |
H |
0.326 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.605 |
-4.025 |
0.000 |
4.333 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.454 |
1.677 |
0.000 |
| y |
1.677 |
-24.214 |
0.000 |
| z |
0.000 |
0.000 |
-17.066 |
|
| Traceless |
| | x | y | z |
| x |
-4.814 |
1.677 |
0.000 |
| y |
1.677 |
-2.954 |
0.000 |
| z |
0.000 |
0.000 |
7.768 |
|
| Polar |
| 3z2-r2 | 15.537 |
| x2-y2 | -1.240 |
| xy | 1.677 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.356 |
0.126 |
0.000 |
| y |
0.126 |
4.929 |
0.000 |
| z |
0.000 |
0.000 |
4.849 |
<r2> (average value of r
2) Å
2
| <r2> |
68.769 |
| (<r2>)1/2 |
8.293 |
Jump to
S1C1
S1C2
Energy calculated at B3LYP/6-311G*
| | hartrees |
| Energy at 0K | -225.324285 |
| Energy at 298.15K | |
| HF Energy | -225.324285 |
| Nuclear repulsion energy | 123.759504 |
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/6-311G*
| 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 |
3756 |
3630 |
28.70 |
|
|
|
| 2 |
A1 |
3630 |
3508 |
3.38 |
|
|
|
| 3 |
A1 |
1804 |
1743 |
467.35 |
|
|
|
| 4 |
A1 |
1662 |
1606 |
0.04 |
|
|
|
| 5 |
A1 |
1160 |
1121 |
0.58 |
|
|
|
| 6 |
A1 |
968 |
935 |
8.68 |
|
|
|
| 7 |
A1 |
480 |
464 |
3.34 |
|
|
|
| 8 |
A2 |
369 |
357 |
0.00 |
|
|
|
| 9 |
A2 |
408i |
395i |
0.00 |
|
|
|
| 10 |
B1 |
780 |
754 |
11.04 |
|
|
|
| 11 |
B1 |
571 |
552 |
10.47 |
|
|
|
| 12 |
B1 |
266i |
257i |
549.01 |
|
|
|
| 13 |
B2 |
3754 |
3627 |
34.78 |
|
|
|
| 14 |
B2 |
3620 |
3498 |
42.44 |
|
|
|
| 15 |
B2 |
1652 |
1596 |
262.84 |
|
|
|
| 16 |
B2 |
1427 |
1379 |
247.66 |
|
|
|
| 17 |
B2 |
994 |
960 |
16.81 |
|
|
|
| 18 |
B2 |
566 |
547 |
14.28 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13259.2 cm
-1
Scaled (by 0.9663) Zero Point Vibrational Energy (zpe) 12812.3 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/6-311G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.143 |
| O2 |
0.000 |
0.000 |
1.361 |
| N3 |
0.000 |
1.160 |
-0.598 |
| N4 |
0.000 |
-1.160 |
-0.598 |
| H5 |
0.000 |
2.025 |
-0.088 |
| H6 |
0.000 |
1.192 |
-1.601 |
| H7 |
0.000 |
-2.025 |
-0.088 |
| H8 |
0.000 |
-1.192 |
-1.601 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2173 | 1.3765 | 1.3765 | 2.0384 | 2.1130 | 2.0384 | 2.1130 |
O2 | 1.2173 | | 2.2761 | 2.2761 | 2.4901 | 3.1929 | 2.4901 | 3.1929 | N3 | 1.3765 | 2.2761 | | 2.3200 | 1.0040 | 1.0043 | 3.2256 | 2.5571 | N4 | 1.3765 | 2.2761 | 2.3200 | | 3.2256 | 2.5571 | 1.0040 | 1.0043 | H5 | 2.0384 | 2.4901 | 1.0040 | 3.2256 | | 1.7275 | 4.0503 | 3.5551 | H6 | 2.1130 | 3.1929 | 1.0043 | 2.5571 | 1.7275 | | 3.5551 | 2.3837 | H7 | 2.0384 | 2.4901 | 3.2256 | 1.0040 | 4.0503 | 3.5551 | | 1.7275 | H8 | 2.1130 | 3.1929 | 2.5571 | 1.0043 | 3.5551 | 2.3837 | 1.7275 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
116.936 |
|
C1 |
N3 |
H6 |
124.390 |
| C1 |
N4 |
H7 |
116.936 |
|
C1 |
N4 |
H8 |
124.390 |
| O2 |
C1 |
N3 |
122.572 |
|
O2 |
C1 |
N4 |
122.572 |
| N3 |
C1 |
N4 |
114.856 |
|
H5 |
N3 |
H6 |
118.674 |
| H7 |
N4 |
H8 |
118.674 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.639 |
|
|
|
| 2 |
O |
-0.403 |
|
|
|
| 3 |
N |
-0.813 |
|
|
|
| 4 |
N |
-0.813 |
|
|
|
| 5 |
H |
0.359 |
|
|
|
| 6 |
H |
0.336 |
|
|
|
| 7 |
H |
0.359 |
|
|
|
| 8 |
H |
0.336 |
|
|
|
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 |
-4.347 |
4.347 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.808 |
0.000 |
0.000 |
| y |
0.000 |
-16.337 |
0.000 |
| z |
0.000 |
0.000 |
-23.710 |
|
| Traceless |
| | x | y | z |
| x |
-5.785 |
0.000 |
0.000 |
| y |
0.000 |
8.422 |
0.000 |
| z |
0.000 |
0.000 |
-2.638 |
|
| Polar |
| 3z2-r2 | -5.275 |
| x2-y2 | -9.471 |
| 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 |
2.273 |
0.000 |
0.000 |
| y |
0.000 |
4.827 |
0.000 |
| z |
0.000 |
0.000 |
4.874 |
<r2> (average value of r
2) Å
2
| <r2> |
68.673 |
| (<r2>)1/2 |
8.287 |