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S1C2
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Vibrational Frequencies calculated at B3LYP/LANL2DZ
Geometric Data calculated at B3LYP/LANL2DZ
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
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S1C1
S1C3
Vibrational Frequencies calculated at B3LYP/LANL2DZ
Geometric Data calculated at B3LYP/LANL2DZ
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
Energy calculated at B3LYP/LANL2DZ
| | hartrees |
| Energy at 0K | -210.362715 |
| Energy at 298.15K | -210.371712 |
| HF Energy | -210.362715 |
| Nuclear repulsion energy | 132.937876 |
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 |
3671 |
3529 |
4.48 |
|
|
|
| 2 |
A |
3565 |
3427 |
35.19 |
|
|
|
| 3 |
A |
3547 |
3409 |
2.01 |
|
|
|
| 4 |
A |
3132 |
3010 |
58.54 |
|
|
|
| 5 |
A |
3112 |
2991 |
38.47 |
|
|
|
| 6 |
A |
3013 |
2896 |
121.69 |
|
|
|
| 7 |
A |
2998 |
2882 |
57.62 |
|
|
|
| 8 |
A |
1685 |
1620 |
43.61 |
|
|
|
| 9 |
A |
1527 |
1468 |
2.20 |
|
|
|
| 10 |
A |
1513 |
1454 |
7.08 |
|
|
|
| 11 |
A |
1428 |
1372 |
46.41 |
|
|
|
| 12 |
A |
1411 |
1356 |
4.51 |
|
|
|
| 13 |
A |
1358 |
1306 |
17.55 |
|
|
|
| 14 |
A |
1317 |
1266 |
4.89 |
|
|
|
| 15 |
A |
1240 |
1191 |
32.67 |
|
|
|
| 16 |
A |
1178 |
1132 |
15.13 |
|
|
|
| 17 |
A |
1112 |
1069 |
20.54 |
|
|
|
| 18 |
A |
1044 |
1003 |
73.24 |
|
|
|
| 19 |
A |
991 |
952 |
2.49 |
|
|
|
| 20 |
A |
886 |
852 |
15.66 |
|
|
|
| 21 |
A |
880 |
845 |
27.54 |
|
|
|
| 22 |
A |
699 |
671 |
268.00 |
|
|
|
| 23 |
A |
612 |
588 |
151.00 |
|
|
|
| 24 |
A |
533 |
512 |
21.37 |
|
|
|
| 25 |
A |
314 |
302 |
0.57 |
|
|
|
| 26 |
A |
257 |
247 |
10.67 |
|
|
|
| 27 |
A |
158 |
152 |
7.40 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 21589.1 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 20751.5 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/LANL2DZ
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-1.372 |
-0.547 |
0.128 |
| C2 |
-0.642 |
0.681 |
-0.263 |
| C3 |
0.806 |
0.584 |
0.258 |
| O4 |
1.401 |
-0.674 |
-0.162 |
| H5 |
-1.655 |
-0.585 |
1.104 |
| H6 |
-2.117 |
-0.830 |
-0.501 |
| H7 |
-1.111 |
1.613 |
0.096 |
| H8 |
-0.620 |
0.717 |
-1.359 |
| H9 |
1.424 |
1.388 |
-0.156 |
| H10 |
0.816 |
0.667 |
1.359 |
| H11 |
0.675 |
-1.342 |
-0.109 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
C3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
H11 |
| N1 | | 1.4806 | 2.4572 | 2.7906 | 1.0175 | 1.0155 | 2.1756 | 2.0913 | 3.4115 | 2.7883 | 2.2084 |
C2 | 1.4806 | | 1.5422 | 2.4532 | 2.1210 | 2.1248 | 1.1040 | 1.0968 | 2.1862 | 2.1814 | 2.4184 | C3 | 2.4572 | 1.5422 | | 1.4531 | 2.8528 | 3.3347 | 2.1824 | 2.1608 | 1.0951 | 1.1042 | 1.9647 | O4 | 2.7906 | 2.4532 | 1.4531 | | 3.3091 | 3.5378 | 3.4070 | 2.7301 | 2.0617 | 2.1103 | 0.9881 | H5 | 1.0175 | 2.1210 | 2.8528 | 3.3091 | | 1.6884 | 2.4784 | 2.9724 | 3.8675 | 2.7815 | 2.7338 | H6 | 1.0155 | 2.1248 | 3.3347 | 3.5378 | 1.6884 | | 2.7085 | 2.3175 | 4.1925 | 3.7820 | 2.8655 | H7 | 2.1756 | 1.1040 | 2.1824 | 3.4070 | 2.4784 | 2.7085 | | 1.7782 | 2.5578 | 2.4912 | 3.4590 | H8 | 2.0913 | 1.0968 | 2.1608 | 2.7301 | 2.9724 | 2.3175 | 1.7782 | | 2.4654 | 3.0751 | 2.7350 | H9 | 3.4115 | 2.1862 | 1.0951 | 2.0617 | 3.8675 | 4.1925 | 2.5578 | 2.4654 | | 1.7843 | 2.8309 | H10 | 2.7883 | 2.1814 | 1.1042 | 2.1103 | 2.7815 | 3.7820 | 2.4912 | 3.0751 | 1.7843 | | 2.4920 | H11 | 2.2084 | 2.4184 | 1.9647 | 0.9881 | 2.7338 | 2.8655 | 3.4590 | 2.7350 | 2.8309 | 2.4920 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
C3 |
108.742 |
|
N1 |
C2 |
H7 |
113.854 |
| N1 |
C2 |
H8 |
107.531 |
|
C2 |
N1 |
H5 |
114.949 |
| C2 |
N1 |
H6 |
115.435 |
|
C2 |
C3 |
O4 |
109.934 |
| C2 |
C3 |
H9 |
110.841 |
|
C2 |
C3 |
H10 |
109.930 |
| C3 |
C2 |
H7 |
110.023 |
|
C3 |
C2 |
H8 |
108.757 |
| C3 |
O4 |
H11 |
105.596 |
|
O4 |
C3 |
H9 |
107.169 |
| O4 |
C3 |
H10 |
110.477 |
|
H5 |
N1 |
H6 |
112.300 |
| H7 |
C2 |
H8 |
107.797 |
|
H9 |
C3 |
H10 |
108.445 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.631 |
|
|
|
| 2 |
C |
-0.346 |
|
|
|
| 3 |
C |
-0.215 |
|
|
|
| 4 |
O |
-0.489 |
|
|
|
| 5 |
H |
0.276 |
|
|
|
| 6 |
H |
0.290 |
|
|
|
| 7 |
H |
0.181 |
|
|
|
| 8 |
H |
0.210 |
|
|
|
| 9 |
H |
0.195 |
|
|
|
| 10 |
H |
0.166 |
|
|
|
| 11 |
H |
0.363 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.572 |
1.212 |
0.621 |
3.822 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-27.468 |
3.309 |
0.661 |
| y |
3.309 |
-24.622 |
-0.246 |
| z |
0.661 |
-0.246 |
-23.976 |
|
| Traceless |
| | x | y | z |
| x |
-3.169 |
3.309 |
0.661 |
| y |
3.309 |
1.101 |
-0.246 |
| z |
0.661 |
-0.246 |
2.069 |
|
| Polar |
| 3z2-r2 | 4.137 |
| x2-y2 | -2.847 |
| xy | 3.309 |
| xz | 0.661 |
| yz | -0.246 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.944 |
0.312 |
0.016 |
| y |
0.312 |
4.843 |
0.079 |
| z |
0.016 |
0.079 |
4.264 |
<r2> (average value of r
2) Å
2
| <r2> |
88.288 |
| (<r2>)1/2 |
9.396 |