Jump to
S1C2
S1C3
Energy calculated at HF/LANL2DZ
| | hartrees |
| Energy at 0K | -207.898573 |
| Energy at 298.15K | -207.904740 |
| HF Energy | -207.898573 |
| Nuclear repulsion energy | 119.028329 |
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 HF/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' |
3874 |
3486 |
44.86 |
|
|
|
| 2 |
A' |
3314 |
2982 |
53.95 |
|
|
|
| 3 |
A' |
3272 |
2944 |
63.28 |
|
|
|
| 4 |
A' |
3216 |
2894 |
64.02 |
|
|
|
| 5 |
A' |
1854 |
1669 |
646.66 |
|
|
|
| 6 |
A' |
1675 |
1508 |
18.32 |
|
|
|
| 7 |
A' |
1621 |
1459 |
5.60 |
|
|
|
| 8 |
A' |
1613 |
1452 |
4.70 |
|
|
|
| 9 |
A' |
1531 |
1378 |
25.87 |
|
|
|
| 10 |
A' |
1425 |
1282 |
196.90 |
|
|
|
| 11 |
A' |
1263 |
1136 |
49.93 |
|
|
|
| 12 |
A' |
1088 |
979 |
54.63 |
|
|
|
| 13 |
A' |
641 |
577 |
21.75 |
|
|
|
| 14 |
A' |
370 |
333 |
11.93 |
|
|
|
| 15 |
A" |
3293 |
2963 |
56.30 |
|
|
|
| 16 |
A" |
1644 |
1479 |
9.83 |
|
|
|
| 17 |
A" |
1260 |
1134 |
2.91 |
|
|
|
| 18 |
A" |
1161 |
1045 |
0.12 |
|
|
|
| 19 |
A" |
745 |
671 |
255.97 |
|
|
|
| 20 |
A" |
212 |
191 |
0.13 |
|
|
|
| 21 |
A" |
68 |
61 |
0.18 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17570.8 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 15812.0 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 HF/LANL2DZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.283 |
-0.755 |
0.000 |
| O2 |
1.416 |
-1.229 |
0.000 |
| N3 |
0.000 |
0.572 |
0.000 |
| C4 |
-1.349 |
1.128 |
0.000 |
| H5 |
-0.596 |
-1.390 |
0.000 |
| H6 |
0.778 |
1.195 |
0.000 |
| H7 |
-2.072 |
0.323 |
0.000 |
| H8 |
-1.520 |
1.734 |
0.881 |
| H9 |
-1.520 |
1.734 |
-0.881 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.2279 | 1.3568 | 2.4914 | 1.0841 | 2.0119 | 2.5899 | 3.1972 | 3.1972 |
O2 | 1.2279 | | 2.2905 | 3.6324 | 2.0184 | 2.5060 | 3.8173 | 4.2630 | 4.2630 | N3 | 1.3568 | 2.2905 | | 1.4586 | 2.0500 | 0.9967 | 2.0868 | 2.1065 | 2.1065 | C4 | 2.4914 | 3.6324 | 1.4586 | | 2.6273 | 2.1276 | 1.0820 | 1.0827 | 1.0827 | H5 | 1.0841 | 2.0184 | 2.0500 | 2.6273 | | 2.9271 | 2.2607 | 3.3742 | 3.3742 | H6 | 2.0119 | 2.5060 | 0.9967 | 2.1276 | 2.9271 | | 2.9803 | 2.5197 | 2.5197 | H7 | 2.5899 | 3.8173 | 2.0868 | 1.0820 | 2.2607 | 2.9803 | | 1.7520 | 1.7520 | H8 | 3.1972 | 4.2630 | 2.1065 | 1.0827 | 3.3742 | 2.5197 | 1.7520 | | 1.7612 | H9 | 3.1972 | 4.2630 | 2.1065 | 1.0827 | 3.3742 | 2.5197 | 1.7520 | 1.7612 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
124.437 |
|
C1 |
N3 |
H6 |
116.652 |
| O2 |
C1 |
N3 |
124.718 |
|
O2 |
C1 |
H5 |
121.499 |
| N3 |
C1 |
H5 |
113.783 |
|
N3 |
C4 |
H7 |
109.552 |
| N3 |
C4 |
H8 |
111.106 |
|
N3 |
C4 |
H9 |
111.106 |
| C4 |
N3 |
H6 |
118.911 |
|
H7 |
C4 |
H8 |
108.068 |
| H7 |
C4 |
H9 |
108.068 |
|
H8 |
C4 |
H9 |
108.842 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.252 |
|
|
|
| 2 |
O |
-0.433 |
|
|
|
| 3 |
N |
-0.545 |
|
|
|
| 4 |
C |
-0.398 |
|
|
|
| 5 |
H |
0.153 |
|
|
|
| 6 |
H |
0.378 |
|
|
|
| 7 |
H |
0.187 |
|
|
|
| 8 |
H |
0.203 |
|
|
|
| 9 |
H |
0.203 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-4.116 |
3.026 |
0.000 |
5.109 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-28.226 |
5.498 |
0.000 |
| y |
5.498 |
-25.002 |
0.000 |
| z |
0.000 |
0.000 |
-25.201 |
|
| Traceless |
| | x | y | z |
| x |
-3.125 |
5.498 |
0.000 |
| y |
5.498 |
1.712 |
0.000 |
| z |
0.000 |
0.000 |
1.413 |
|
| Polar |
| 3z2-r2 | 2.826 |
| x2-y2 | -3.225 |
| xy | 5.498 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.945 |
-1.029 |
0.000 |
| y |
-1.029 |
4.812 |
0.000 |
| z |
0.000 |
0.000 |
2.725 |
<r2> (average value of r
2) Å
2
| <r2> |
90.077 |
| (<r2>)1/2 |
9.491 |
Jump to
S1C1
S1C3
Energy calculated at HF/LANL2DZ
| | hartrees |
| Energy at 0K | -207.898573 |
| Energy at 298.15K | -207.904740 |
| HF Energy | -207.898573 |
| Nuclear repulsion energy | 119.028329 |
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 HF/LANL2DZ
Geometric Data calculated at HF/LANL2DZ
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
Energy calculated at HF/LANL2DZ
| | hartrees |
| Energy at 0K | -207.900071 |
| Energy at 298.15K | -207.906278 |
| HF Energy | -207.900071 |
| Nuclear repulsion energy | 121.375311 |
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 HF/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 |
3917 |
3525 |
51.90 |
|
|
|
| 2 |
A |
3330 |
2996 |
36.40 |
|
|
|
| 3 |
A |
3316 |
2984 |
49.34 |
|
|
|
| 4 |
A |
3276 |
2948 |
82.89 |
|
|
|
| 5 |
A |
3230 |
2907 |
53.57 |
|
|
|
| 6 |
A |
1837 |
1654 |
388.10 |
|
|
|
| 7 |
A |
1681 |
1513 |
175.72 |
|
|
|
| 8 |
A |
1654 |
1488 |
77.88 |
|
|
|
| 9 |
A |
1636 |
1472 |
11.39 |
|
|
|
| 10 |
A |
1607 |
1446 |
26.83 |
|
|
|
| 11 |
A |
1523 |
1370 |
35.69 |
|
|
|
| 12 |
A |
1347 |
1212 |
97.29 |
|
|
|
| 13 |
A |
1291 |
1162 |
0.54 |
|
|
|
| 14 |
A |
1269 |
1142 |
0.61 |
|
|
|
| 15 |
A |
1149 |
1034 |
4.70 |
|
|
|
| 16 |
A |
1015 |
913 |
22.61 |
|
|
|
| 17 |
A |
817 |
736 |
9.63 |
|
|
|
| 18 |
A |
575 |
517 |
146.46 |
|
|
|
| 19 |
A |
375 |
338 |
87.78 |
|
|
|
| 20 |
A |
289 |
260 |
15.42 |
|
|
|
| 21 |
A |
47 |
42 |
2.57 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17589.8 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 15829.1 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 HF/LANL2DZ
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.865 |
0.441 |
0.000 |
| O2 |
1.386 |
-0.673 |
0.000 |
| N3 |
-0.472 |
0.660 |
-0.000 |
| C4 |
-1.433 |
-0.443 |
0.000 |
| H5 |
1.461 |
1.346 |
0.000 |
| H6 |
-0.803 |
1.596 |
0.003 |
| H7 |
-2.433 |
-0.036 |
-0.046 |
| H8 |
-1.273 |
-1.088 |
-0.853 |
| H9 |
-1.333 |
-1.040 |
0.897 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.2291 | 1.3552 | 2.4622 | 1.0835 | 2.0298 | 3.3324 | 2.7630 | 2.7980 |
O2 | 1.2291 | | 2.2867 | 2.8283 | 2.0198 | 3.1531 | 3.8718 | 2.8230 | 2.8869 | N3 | 1.3552 | 2.2867 | | 1.4631 | 2.0510 | 0.9932 | 2.0809 | 2.1029 | 2.1062 | C4 | 2.4622 | 2.8283 | 1.4631 | | 3.4021 | 2.1346 | 1.0807 | 1.0813 | 1.0817 | H5 | 1.0835 | 2.0198 | 2.0510 | 3.4021 | | 2.2781 | 4.1316 | 3.7579 | 3.7817 | H6 | 2.0298 | 3.1531 | 0.9932 | 2.1346 | 2.2781 | | 2.3066 | 2.8560 | 2.8334 | H7 | 3.3324 | 3.8718 | 2.0809 | 1.0807 | 4.1316 | 2.3066 | | 1.7619 | 1.7624 | H8 | 2.7630 | 2.8230 | 2.1029 | 1.0813 | 3.7579 | 2.8560 | 1.7619 | | 1.7524 | H9 | 2.7980 | 2.8869 | 2.1062 | 1.0817 | 3.7817 | 2.8334 | 1.7624 | 1.7524 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
121.732 |
|
C1 |
N3 |
H6 |
118.803 |
| O2 |
C1 |
N3 |
124.391 |
|
O2 |
C1 |
H5 |
121.577 |
| N3 |
C1 |
H5 |
114.032 |
|
N3 |
C4 |
H7 |
108.845 |
| N3 |
C4 |
H8 |
110.584 |
|
N3 |
C4 |
H9 |
110.826 |
| C4 |
N3 |
H6 |
119.464 |
|
H7 |
C4 |
H8 |
109.163 |
| H7 |
C4 |
H9 |
109.172 |
|
H8 |
C4 |
H9 |
108.222 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.253 |
|
|
|
| 2 |
O |
-0.441 |
|
|
|
| 3 |
N |
-0.560 |
|
|
|
| 4 |
C |
-0.391 |
|
|
|
| 5 |
H |
0.168 |
|
|
|
| 6 |
H |
0.361 |
|
|
|
| 7 |
H |
0.176 |
|
|
|
| 8 |
H |
0.219 |
|
|
|
| 9 |
H |
0.215 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.241 |
3.550 |
0.002 |
4.807 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.104 |
4.144 |
0.004 |
| y |
4.144 |
-22.610 |
0.027 |
| z |
0.004 |
0.027 |
-25.204 |
|
| Traceless |
| | x | y | z |
| x |
-2.197 |
4.144 |
0.004 |
| y |
4.144 |
3.045 |
0.027 |
| z |
0.004 |
0.027 |
-0.847 |
|
| Polar |
| 3z2-r2 | -1.695 |
| x2-y2 | -3.495 |
| xy | 4.144 |
| xz | 0.004 |
| yz | 0.027 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.905 |
-0.447 |
-0.008 |
| y |
-0.447 |
4.492 |
-0.005 |
| z |
-0.008 |
-0.005 |
2.691 |
<r2> (average value of r
2) Å
2
| <r2> |
78.397 |
| (<r2>)1/2 |
8.854 |