Jump to
S1C2
S1C3
Energy calculated at B3LYP/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -209.217588 |
| Energy at 298.15K | -209.223648 |
| HF Energy | -209.217588 |
| Nuclear repulsion energy | 119.266049 |
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/6-31G(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' |
3612 |
3485 |
22.70 |
|
|
|
| 2 |
A' |
3118 |
3009 |
14.58 |
|
|
|
| 3 |
A' |
3022 |
2916 |
53.52 |
|
|
|
| 4 |
A' |
2916 |
2814 |
86.76 |
|
|
|
| 5 |
A' |
1825 |
1761 |
423.38 |
|
|
|
| 6 |
A' |
1533 |
1479 |
14.81 |
|
|
|
| 7 |
A' |
1484 |
1432 |
5.72 |
|
|
|
| 8 |
A' |
1468 |
1417 |
12.10 |
|
|
|
| 9 |
A' |
1405 |
1356 |
11.03 |
|
|
|
| 10 |
A' |
1303 |
1257 |
100.19 |
|
|
|
| 11 |
A' |
1166 |
1125 |
30.72 |
|
|
|
| 12 |
A' |
1011 |
976 |
41.90 |
|
|
|
| 13 |
A' |
612 |
591 |
13.97 |
|
|
|
| 14 |
A' |
343 |
331 |
7.86 |
|
|
|
| 15 |
A" |
3073 |
2966 |
30.26 |
|
|
|
| 16 |
A" |
1482 |
1430 |
4.61 |
|
|
|
| 17 |
A" |
1155 |
1115 |
0.38 |
|
|
|
| 18 |
A" |
1049 |
1012 |
0.13 |
|
|
|
| 19 |
A" |
617 |
595 |
104.53 |
|
|
|
| 20 |
A" |
204 |
197 |
0.75 |
|
|
|
| 21 |
A" |
107 |
103 |
0.41 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16251.8 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 15683.0 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/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.286 |
-0.760 |
0.000 |
| O2 |
1.400 |
-1.233 |
0.000 |
| N3 |
0.000 |
0.570 |
0.000 |
| C4 |
-1.332 |
1.134 |
0.000 |
| H5 |
-0.638 |
-1.376 |
0.000 |
| H6 |
0.798 |
1.189 |
0.000 |
| H7 |
-2.059 |
0.318 |
0.000 |
| H8 |
-1.513 |
1.749 |
0.889 |
| H9 |
-1.513 |
1.749 |
-0.889 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.2107 | 1.3600 | 2.4902 | 1.1104 | 2.0148 | 2.5801 | 3.2122 | 3.2122 |
O2 | 1.2107 | | 2.2824 | 3.6142 | 2.0434 | 2.4951 | 3.7904 | 4.2621 | 4.2621 | N3 | 1.3600 | 2.2824 | | 1.4460 | 2.0476 | 1.0099 | 2.0743 | 2.1141 | 2.1141 | C4 | 2.4902 | 3.6142 | 1.4460 | | 2.6035 | 2.1304 | 1.0934 | 1.0962 | 1.0962 | H5 | 1.1104 | 2.0434 | 2.0476 | 2.6035 | | 2.9393 | 2.2102 | 3.3641 | 3.3641 | H6 | 2.0148 | 2.4951 | 1.0099 | 2.1304 | 2.9393 | | 2.9869 | 2.5389 | 2.5389 | H7 | 2.5801 | 3.7904 | 2.0743 | 1.0934 | 2.2102 | 2.9869 | | 1.7710 | 1.7710 | H8 | 3.2122 | 4.2621 | 2.1141 | 1.0962 | 3.3641 | 2.5389 | 1.7710 | | 1.7784 | H9 | 3.2122 | 4.2621 | 2.1141 | 1.0962 | 3.3641 | 2.5389 | 1.7710 | 1.7784 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
125.076 |
|
C1 |
N3 |
H6 |
115.666 |
| O2 |
C1 |
N3 |
125.113 |
|
O2 |
C1 |
H5 |
123.321 |
| N3 |
C1 |
H5 |
111.566 |
|
N3 |
C4 |
H7 |
108.747 |
| N3 |
C4 |
H8 |
111.793 |
|
N3 |
C4 |
H9 |
111.793 |
| C4 |
N3 |
H6 |
119.258 |
|
H7 |
C4 |
H8 |
107.970 |
| H7 |
C4 |
H9 |
107.970 |
|
H8 |
C4 |
H9 |
108.428 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.159 |
|
|
|
| 2 |
O |
-0.327 |
|
|
|
| 3 |
N |
-0.238 |
|
|
|
| 4 |
C |
-0.323 |
|
|
|
| 5 |
H |
0.066 |
|
|
|
| 6 |
H |
0.251 |
|
|
|
| 7 |
H |
0.144 |
|
|
|
| 8 |
H |
0.134 |
|
|
|
| 9 |
H |
0.134 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.802 |
2.694 |
0.000 |
3.887 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.032 |
3.841 |
0.000 |
| y |
3.841 |
-24.069 |
0.000 |
| z |
0.000 |
0.000 |
-24.310 |
|
| Traceless |
| | x | y | z |
| x |
-1.843 |
3.841 |
0.000 |
| y |
3.841 |
1.102 |
0.000 |
| z |
0.000 |
0.000 |
0.741 |
|
| Polar |
| 3z2-r2 | 1.481 |
| x2-y2 | -1.963 |
| xy | 3.841 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.664 |
-1.042 |
0.000 |
| y |
-1.042 |
5.786 |
0.000 |
| z |
0.000 |
0.000 |
3.331 |
<r2> (average value of r
2) Å
2
| <r2> |
88.873 |
| (<r2>)1/2 |
9.427 |
Jump to
S1C1
S1C3
Energy calculated at B3LYP/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -209.217588 |
| Energy at 298.15K | -209.223648 |
| HF Energy | -209.217588 |
| Nuclear repulsion energy | 119.266049 |
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/6-31G(2df,p)
Geometric Data calculated at B3LYP/6-31G(2df,p)
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
Energy calculated at B3LYP/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -209.219074 |
| Energy at 298.15K | -209.225130 |
| HF Energy | -209.219074 |
| Nuclear repulsion energy | 121.418157 |
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/6-31G(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 |
3643 |
3516 |
21.62 |
|
|
|
| 2 |
A |
3155 |
3045 |
0.93 |
|
|
|
| 3 |
A |
3083 |
2975 |
29.87 |
|
|
|
| 4 |
A |
3031 |
2925 |
44.85 |
|
|
|
| 5 |
A |
2934 |
2831 |
112.73 |
|
|
|
| 6 |
A |
1812 |
1748 |
293.27 |
|
|
|
| 7 |
A |
1554 |
1500 |
78.48 |
|
|
|
| 8 |
A |
1499 |
1447 |
5.43 |
|
|
|
| 9 |
A |
1491 |
1439 |
41.38 |
|
|
|
| 10 |
A |
1440 |
1390 |
19.79 |
|
|
|
| 11 |
A |
1430 |
1380 |
0.48 |
|
|
|
| 12 |
A |
1223 |
1180 |
81.71 |
|
|
|
| 13 |
A |
1161 |
1121 |
21.57 |
|
|
|
| 14 |
A |
1157 |
1117 |
0.70 |
|
|
|
| 15 |
A |
1029 |
993 |
0.48 |
|
|
|
| 16 |
A |
961 |
928 |
16.00 |
|
|
|
| 17 |
A |
770 |
743 |
0.45 |
|
|
|
| 18 |
A |
539 |
520 |
38.96 |
|
|
|
| 19 |
A |
299 |
288 |
13.10 |
|
|
|
| 20 |
A |
264 |
255 |
62.62 |
|
|
|
| 21 |
A |
82 |
79 |
0.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16279.2 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 15709.4 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/6-31G(2df,p)
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.866 |
0.434 |
0.004 |
| O2 |
1.373 |
-0.672 |
-0.000 |
| N3 |
-0.469 |
0.658 |
-0.020 |
| C4 |
-1.424 |
-0.439 |
0.005 |
| H5 |
1.456 |
1.369 |
0.018 |
| H6 |
-0.799 |
1.605 |
0.056 |
| H7 |
-2.421 |
-0.050 |
-0.215 |
| H8 |
-1.151 |
-1.179 |
-0.750 |
| H9 |
-1.440 |
-0.939 |
0.979 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.2165 | 1.3545 | 2.4514 | 1.1058 | 2.0371 | 3.3297 | 2.6909 | 2.8556 |
O2 | 1.2165 | | 2.2725 | 2.8075 | 2.0430 | 3.1481 | 3.8505 | 2.6817 | 2.9908 | N3 | 1.3545 | 2.2725 | | 1.4546 | 2.0527 | 1.0063 | 2.0850 | 2.0913 | 2.1190 | C4 | 2.4514 | 2.8075 | 1.4546 | | 3.4009 | 2.1385 | 1.0915 | 1.0923 | 1.0954 | H5 | 1.1058 | 2.0430 | 2.0527 | 3.4009 | | 2.2678 | 4.1348 | 3.7256 | 3.8261 | H6 | 2.0371 | 3.1481 | 1.0063 | 2.1385 | 2.2678 | | 2.3334 | 2.9206 | 2.7816 | H7 | 3.3297 | 3.8505 | 2.0850 | 1.0915 | 4.1348 | 2.3334 | | 1.7814 | 1.7823 | H8 | 2.6909 | 2.6817 | 2.0913 | 1.0923 | 3.7256 | 2.9206 | 1.7814 | | 1.7697 | H9 | 2.8556 | 2.9908 | 2.1190 | 1.0954 | 3.8261 | 2.7816 | 1.7823 | 1.7697 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
121.500 |
|
C1 |
N3 |
H6 |
118.539 |
| O2 |
C1 |
N3 |
124.140 |
|
O2 |
C1 |
H5 |
123.155 |
| N3 |
C1 |
H5 |
112.702 |
|
N3 |
C4 |
H7 |
109.124 |
| N3 |
C4 |
H8 |
109.577 |
|
N3 |
C4 |
H9 |
111.626 |
| C4 |
N3 |
H6 |
119.567 |
|
H7 |
C4 |
H8 |
109.322 |
| H7 |
C4 |
H9 |
109.174 |
|
H8 |
C4 |
H9 |
107.985 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.160 |
|
|
|
| 2 |
O |
-0.320 |
|
|
|
| 3 |
N |
-0.262 |
|
|
|
| 4 |
C |
-0.328 |
|
|
|
| 5 |
H |
0.072 |
|
|
|
| 6 |
H |
0.248 |
|
|
|
| 7 |
H |
0.128 |
|
|
|
| 8 |
H |
0.173 |
|
|
|
| 9 |
H |
0.128 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.780 |
2.453 |
0.000 |
3.708 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.251 |
2.302 |
0.000 |
| y |
2.302 |
-21.937 |
0.000 |
| z |
0.000 |
0.000 |
-24.329 |
|
| Traceless |
| | x | y | z |
| x |
-2.118 |
2.302 |
0.000 |
| y |
2.302 |
2.853 |
0.000 |
| z |
0.000 |
0.000 |
-0.735 |
|
| Polar |
| 3z2-r2 | -1.470 |
| x2-y2 | -3.314 |
| xy | 2.302 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.209 |
-0.009 |
0.000 |
| y |
-0.009 |
5.047 |
0.000 |
| z |
0.000 |
0.000 |
3.316 |
<r2> (average value of r
2) Å
2
| <r2> |
78.359 |
| (<r2>)1/2 |
8.852 |