Jump to
S1C2
S1C3
Energy calculated at B3PW91/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -209.138295 |
| Energy at 298.15K | -209.144370 |
| HF Energy | -209.138295 |
| Nuclear repulsion energy | 119.504180 |
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 B3PW91/6-31G(2df,p)
| 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' |
3637 |
3497 |
26.04 |
|
|
|
| 2 |
A' |
3131 |
3011 |
13.32 |
|
|
|
| 3 |
A' |
3029 |
2912 |
52.75 |
|
|
|
| 4 |
A' |
2923 |
2810 |
88.95 |
|
|
|
| 5 |
A' |
1839 |
1768 |
434.32 |
|
|
|
| 6 |
A' |
1530 |
1471 |
18.91 |
|
|
|
| 7 |
A' |
1484 |
1427 |
9.74 |
|
|
|
| 8 |
A' |
1461 |
1405 |
8.60 |
|
|
|
| 9 |
A' |
1398 |
1344 |
11.44 |
|
|
|
| 10 |
A' |
1308 |
1258 |
93.73 |
|
|
|
| 11 |
A' |
1175 |
1129 |
23.52 |
|
|
|
| 12 |
A' |
1016 |
977 |
43.30 |
|
|
|
| 13 |
A' |
615 |
592 |
14.43 |
|
|
|
| 14 |
A' |
341 |
328 |
8.10 |
|
|
|
| 15 |
A" |
3089 |
2970 |
27.56 |
|
|
|
| 16 |
A" |
1476 |
1419 |
5.33 |
|
|
|
| 17 |
A" |
1151 |
1106 |
0.21 |
|
|
|
| 18 |
A" |
1048 |
1008 |
0.23 |
|
|
|
| 19 |
A" |
621 |
597 |
107.18 |
|
|
|
| 20 |
A" |
208 |
200 |
0.80 |
|
|
|
| 21 |
A" |
111 |
106 |
0.43 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16295.4 cm
-1
Scaled (by 0.9614) Zero Point Vibrational Energy (zpe) 15666.4 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 B3PW91/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.284 |
-0.757 |
0.000 |
| O2 |
1.397 |
-1.230 |
0.000 |
| N3 |
0.000 |
0.570 |
0.000 |
| C4 |
-1.327 |
1.129 |
0.000 |
| H5 |
-0.641 |
-1.372 |
0.000 |
| H6 |
0.798 |
1.188 |
0.000 |
| H7 |
-2.053 |
0.312 |
0.000 |
| H8 |
-1.511 |
1.743 |
0.889 |
| H9 |
-1.511 |
1.743 |
-0.889 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.2095 | 1.3569 | 2.4806 | 1.1114 | 2.0116 | 2.5700 | 3.2039 | 3.2039 |
O2 | 1.2095 | | 2.2786 | 3.6039 | 2.0433 | 2.4915 | 3.7792 | 4.2533 | 4.2533 | N3 | 1.3569 | 2.2786 | | 1.4401 | 2.0455 | 1.0091 | 2.0695 | 2.1098 | 2.1098 | C4 | 2.4806 | 3.6039 | 1.4401 | | 2.5942 | 2.1253 | 1.0937 | 1.0963 | 1.0963 | H5 | 1.1114 | 2.0433 | 2.0455 | 2.5942 | | 2.9372 | 2.1978 | 3.3551 | 3.3551 | H6 | 2.0116 | 2.4915 | 1.0091 | 2.1253 | 2.9372 | | 2.9825 | 2.5355 | 2.5355 | H7 | 2.5700 | 3.7792 | 2.0695 | 1.0937 | 2.1978 | 2.9825 | | 1.7705 | 1.7705 | H8 | 3.2039 | 4.2533 | 2.1098 | 1.0963 | 3.3551 | 2.5355 | 1.7705 | | 1.7788 | H9 | 3.2039 | 4.2533 | 2.1098 | 1.0963 | 3.3551 | 2.5355 | 1.7705 | 1.7788 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
124.945 |
|
C1 |
N3 |
H6 |
115.698 |
| O2 |
C1 |
N3 |
125.117 |
|
O2 |
C1 |
H5 |
123.328 |
| N3 |
C1 |
H5 |
111.554 |
|
N3 |
C4 |
H7 |
108.750 |
| N3 |
C4 |
H8 |
111.856 |
|
N3 |
C4 |
H9 |
111.856 |
| C4 |
N3 |
H6 |
119.357 |
|
H7 |
C4 |
H8 |
107.893 |
| H7 |
C4 |
H9 |
107.893 |
|
H8 |
C4 |
H9 |
108.442 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.175 |
|
|
|
| 2 |
O |
-0.348 |
|
|
|
| 3 |
N |
-0.291 |
|
|
|
| 4 |
C |
-0.372 |
|
|
|
| 5 |
H |
0.085 |
|
|
|
| 6 |
H |
0.275 |
|
|
|
| 7 |
H |
0.164 |
|
|
|
| 8 |
H |
0.155 |
|
|
|
| 9 |
H |
0.155 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.811 |
2.718 |
0.000 |
3.910 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.809 |
3.852 |
0.000 |
| y |
3.852 |
-23.874 |
0.000 |
| z |
0.000 |
0.000 |
-24.234 |
|
| Traceless |
| | x | y | z |
| x |
-1.755 |
3.852 |
0.000 |
| y |
3.852 |
1.148 |
0.000 |
| z |
0.000 |
0.000 |
0.607 |
|
| Polar |
| 3z2-r2 | 1.214 |
| x2-y2 | -1.936 |
| xy | 3.852 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.662 |
-1.044 |
0.000 |
| y |
-1.044 |
5.777 |
0.000 |
| z |
0.000 |
0.000 |
3.354 |
<r2> (average value of r
2) Å
2
| <r2> |
88.407 |
| (<r2>)1/2 |
9.403 |
Jump to
S1C1
S1C3
Energy calculated at B3PW91/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -209.138295 |
| Energy at 298.15K | -209.144370 |
| HF Energy | -209.138295 |
| Nuclear repulsion energy | 119.504180 |
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 B3PW91/6-31G(2df,p)
Geometric Data calculated at B3PW91/6-31G(2df,p)
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
Energy calculated at B3PW91/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -209.139806 |
| Energy at 298.15K | -209.145895 |
| HF Energy | -209.139806 |
| Nuclear repulsion energy | 121.702322 |
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 B3PW91/6-31G(2df,p)
| 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 |
3670 |
3529 |
25.57 |
|
|
|
| 2 |
A |
3167 |
3044 |
0.57 |
|
|
|
| 3 |
A |
3100 |
2981 |
27.04 |
|
|
|
| 4 |
A |
3038 |
2921 |
44.20 |
|
|
|
| 5 |
A |
2944 |
2831 |
113.15 |
|
|
|
| 6 |
A |
1826 |
1755 |
300.74 |
|
|
|
| 7 |
A |
1557 |
1497 |
87.63 |
|
|
|
| 8 |
A |
1493 |
1436 |
6.26 |
|
|
|
| 9 |
A |
1488 |
1430 |
34.64 |
|
|
|
| 10 |
A |
1432 |
1377 |
19.84 |
|
|
|
| 11 |
A |
1424 |
1369 |
0.37 |
|
|
|
| 12 |
A |
1232 |
1185 |
69.77 |
|
|
|
| 13 |
A |
1157 |
1112 |
21.51 |
|
|
|
| 14 |
A |
1153 |
1109 |
0.51 |
|
|
|
| 15 |
A |
1029 |
989 |
0.28 |
|
|
|
| 16 |
A |
977 |
940 |
18.77 |
|
|
|
| 17 |
A |
771 |
741 |
0.43 |
|
|
|
| 18 |
A |
544 |
523 |
41.15 |
|
|
|
| 19 |
A |
297 |
286 |
13.67 |
|
|
|
| 20 |
A |
271 |
261 |
63.82 |
|
|
|
| 21 |
A |
94 |
90 |
0.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16332.5 cm
-1
Scaled (by 0.9614) Zero Point Vibrational Energy (zpe) 15702.1 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 B3PW91/6-31G(2df,p)
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.863 |
0.434 |
0.004 |
| O2 |
1.369 |
-0.671 |
-0.000 |
| N3 |
-0.470 |
0.657 |
-0.020 |
| C4 |
-1.418 |
-0.439 |
0.005 |
| H5 |
1.452 |
1.370 |
0.017 |
| H6 |
-0.802 |
1.603 |
0.056 |
| H7 |
-2.415 |
-0.055 |
-0.217 |
| H8 |
-1.139 |
-1.179 |
-0.749 |
| H9 |
-1.432 |
-0.937 |
0.980 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.2150 | 1.3516 | 2.4419 | 1.1063 | 2.0347 | 3.3212 | 2.6790 | 2.8458 |
O2 | 1.2150 | | 2.2682 | 2.7964 | 2.0423 | 3.1440 | 3.8399 | 2.6666 | 2.9797 | N3 | 1.3516 | 2.2682 | | 1.4490 | 2.0507 | 1.0054 | 2.0801 | 2.0856 | 2.1133 | C4 | 2.4419 | 2.7964 | 1.4490 | | 3.3926 | 2.1334 | 1.0915 | 1.0925 | 1.0954 | H5 | 1.1063 | 2.0423 | 2.0507 | 3.3926 | | 2.2665 | 4.1277 | 3.7149 | 3.8169 | H6 | 2.0347 | 3.1440 | 1.0054 | 2.1334 | 2.2665 | | 2.3287 | 2.9155 | 2.7755 | H7 | 3.3212 | 3.8399 | 2.0801 | 1.0915 | 4.1277 | 2.3287 | | 1.7818 | 1.7830 | H8 | 2.6790 | 2.6666 | 2.0856 | 1.0925 | 3.7149 | 2.9155 | 1.7818 | | 1.7708 | H9 | 2.8458 | 2.9797 | 2.1133 | 1.0954 | 3.8169 | 2.7755 | 1.7830 | 1.7708 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
121.328 |
|
C1 |
N3 |
H6 |
118.636 |
| O2 |
C1 |
N3 |
124.108 |
|
O2 |
C1 |
H5 |
123.170 |
| N3 |
C1 |
H5 |
112.719 |
|
N3 |
C4 |
H7 |
109.113 |
| N3 |
C4 |
H8 |
109.496 |
|
N3 |
C4 |
H9 |
111.562 |
| C4 |
N3 |
H6 |
119.642 |
|
H7 |
C4 |
H8 |
109.337 |
| H7 |
C4 |
H9 |
109.233 |
|
H8 |
C4 |
H9 |
108.070 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.170 |
|
|
|
| 2 |
O |
-0.339 |
|
|
|
| 3 |
N |
-0.314 |
|
|
|
| 4 |
C |
-0.377 |
|
|
|
| 5 |
H |
0.093 |
|
|
|
| 6 |
H |
0.272 |
|
|
|
| 7 |
H |
0.150 |
|
|
|
| 8 |
H |
0.195 |
|
|
|
| 9 |
H |
0.150 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.794 |
2.475 |
-0.000 |
3.733 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.048 |
2.304 |
0.000 |
| y |
2.304 |
-21.692 |
0.000 |
| z |
0.000 |
0.000 |
-24.254 |
|
| Traceless |
| | x | y | z |
| x |
-2.075 |
2.304 |
0.000 |
| y |
2.304 |
2.959 |
0.000 |
| z |
0.000 |
0.000 |
-0.884 |
|
| Polar |
| 3z2-r2 | -1.767 |
| x2-y2 | -3.356 |
| xy | 2.304 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.200 |
-0.000 |
-0.000 |
| y |
-0.000 |
5.032 |
-0.000 |
| z |
-0.000 |
-0.000 |
3.339 |
<r2> (average value of r
2) Å
2
| <r2> |
77.851 |
| (<r2>)1/2 |
8.823 |