Jump to
S1C2
S1C3
Energy calculated at B3LYP/3-21G*
| | hartrees |
| Energy at 0K | -208.044198 |
| Energy at 298.15K | -208.050360 |
| HF Energy | -208.044198 |
| Nuclear repulsion energy | 118.089107 |
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/3-21G*
| 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' |
3535 |
3401 |
16.06 |
|
|
|
| 2 |
A' |
3121 |
3002 |
16.28 |
|
|
|
| 3 |
A' |
3037 |
2921 |
46.57 |
|
|
|
| 4 |
A' |
2932 |
2821 |
97.94 |
|
|
|
| 5 |
A' |
1761 |
1694 |
308.63 |
|
|
|
| 6 |
A' |
1589 |
1529 |
14.40 |
|
|
|
| 7 |
A' |
1503 |
1446 |
5.25 |
|
|
|
| 8 |
A' |
1483 |
1426 |
2.09 |
|
|
|
| 9 |
A' |
1443 |
1389 |
14.87 |
|
|
|
| 10 |
A' |
1302 |
1253 |
82.78 |
|
|
|
| 11 |
A' |
1147 |
1103 |
54.77 |
|
|
|
| 12 |
A' |
1008 |
969 |
46.48 |
|
|
|
| 13 |
A' |
607 |
584 |
15.40 |
|
|
|
| 14 |
A' |
348 |
335 |
6.81 |
|
|
|
| 15 |
A" |
3083 |
2966 |
36.95 |
|
|
|
| 16 |
A" |
1553 |
1494 |
8.01 |
|
|
|
| 17 |
A" |
1161 |
1117 |
0.74 |
|
|
|
| 18 |
A" |
1080 |
1039 |
0.13 |
|
|
|
| 19 |
A" |
692 |
666 |
171.76 |
|
|
|
| 20 |
A" |
218 |
210 |
1.46 |
|
|
|
| 21 |
A" |
130 |
125 |
0.11 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16366.3 cm
-1
Scaled (by 0.962) Zero Point Vibrational Energy (zpe) 15744.3 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/3-21G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.295 |
-0.753 |
0.000 |
| O2 |
1.430 |
-1.239 |
0.000 |
| N3 |
0.000 |
0.584 |
0.000 |
| C4 |
-1.363 |
1.121 |
0.000 |
| H5 |
-0.632 |
-1.355 |
0.000 |
| H6 |
0.786 |
1.230 |
0.000 |
| H7 |
-2.062 |
0.279 |
0.000 |
| H8 |
-1.558 |
1.729 |
0.891 |
| H9 |
-1.558 |
1.729 |
-0.891 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.2346 | 1.3691 | 2.5016 | 1.1055 | 2.0423 | 2.5725 | 3.2226 | 3.2226 |
O2 | 1.2346 | | 2.3169 | 3.6561 | 2.0651 | 2.5511 | 3.8071 | 4.3045 | 4.3045 | N3 | 1.3691 | 2.3169 | | 1.4649 | 2.0399 | 1.0170 | 2.0846 | 2.1288 | 2.1288 | C4 | 2.5016 | 3.6561 | 1.4649 | | 2.5813 | 2.1521 | 1.0943 | 1.0963 | 1.0963 | H5 | 1.1055 | 2.0651 | 2.0399 | 2.5813 | | 2.9483 | 2.1709 | 3.3409 | 3.3409 | H6 | 2.0423 | 2.5511 | 1.0170 | 2.1521 | 2.9483 | | 3.0027 | 2.5570 | 2.5570 | H7 | 2.5725 | 3.8071 | 2.0846 | 1.0943 | 2.1709 | 3.0027 | | 1.7752 | 1.7752 | H8 | 3.2226 | 4.3045 | 2.1288 | 1.0963 | 3.3409 | 2.5570 | 1.7752 | | 1.7819 | H9 | 3.2226 | 4.3045 | 2.1288 | 1.0963 | 3.3409 | 2.5570 | 1.7752 | 1.7819 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
123.904 |
|
C1 |
N3 |
H6 |
116.954 |
| O2 |
C1 |
N3 |
125.627 |
|
O2 |
C1 |
H5 |
123.788 |
| N3 |
C1 |
H5 |
110.585 |
|
N3 |
C4 |
H7 |
108.215 |
| N3 |
C4 |
H8 |
111.629 |
|
N3 |
C4 |
H9 |
111.629 |
| C4 |
N3 |
H6 |
119.142 |
|
H7 |
C4 |
H8 |
108.265 |
| H7 |
C4 |
H9 |
108.265 |
|
H8 |
C4 |
H9 |
108.725 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.437 |
|
|
|
| 2 |
O |
-0.482 |
|
|
|
| 3 |
N |
-0.667 |
|
|
|
| 4 |
C |
-0.381 |
|
|
|
| 5 |
H |
0.145 |
|
|
|
| 6 |
H |
0.317 |
|
|
|
| 7 |
H |
0.213 |
|
|
|
| 8 |
H |
0.209 |
|
|
|
| 9 |
H |
0.209 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.869 |
2.738 |
0.000 |
3.965 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.818 |
3.744 |
0.000 |
| y |
3.744 |
-24.083 |
0.000 |
| z |
0.000 |
0.000 |
-24.551 |
|
| Traceless |
| | x | y | z |
| x |
-1.501 |
3.744 |
0.000 |
| y |
3.744 |
1.101 |
0.000 |
| z |
0.000 |
0.000 |
0.400 |
|
| Polar |
| 3z2-r2 | 0.799 |
| x2-y2 | -1.734 |
| xy | 3.744 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.026 |
-1.044 |
0.000 |
| y |
-1.044 |
5.098 |
0.000 |
| z |
0.000 |
0.000 |
2.447 |
<r2> (average value of r
2) Å
2
| <r2> |
90.243 |
| (<r2>)1/2 |
9.500 |
Jump to
S1C1
S1C3
Energy calculated at B3LYP/3-21G*
| | hartrees |
| Energy at 0K | -208.044198 |
| Energy at 298.15K | -208.050360 |
| HF Energy | -208.044198 |
| Nuclear repulsion energy | 118.089107 |
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/3-21G*
Geometric Data calculated at B3LYP/3-21G*
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
Energy calculated at B3LYP/3-21G*
| | hartrees |
| Energy at 0K | -208.046793 |
| Energy at 298.15K | -208.053104 |
| HF Energy | -208.046793 |
| Nuclear repulsion energy | 120.585635 |
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/3-21G*
| 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 |
3563 |
3428 |
19.28 |
|
|
|
| 2 |
A |
3152 |
3032 |
0.87 |
|
|
|
| 3 |
A |
3096 |
2978 |
37.11 |
|
|
|
| 4 |
A |
3045 |
2929 |
39.39 |
|
|
|
| 5 |
A |
2960 |
2847 |
122.57 |
|
|
|
| 6 |
A |
1735 |
1669 |
178.96 |
|
|
|
| 7 |
A |
1585 |
1525 |
32.04 |
|
|
|
| 8 |
A |
1574 |
1515 |
10.24 |
|
|
|
| 9 |
A |
1520 |
1462 |
83.79 |
|
|
|
| 10 |
A |
1465 |
1409 |
33.38 |
|
|
|
| 11 |
A |
1431 |
1377 |
5.66 |
|
|
|
| 12 |
A |
1204 |
1158 |
71.88 |
|
|
|
| 13 |
A |
1177 |
1132 |
58.12 |
|
|
|
| 14 |
A |
1165 |
1121 |
1.10 |
|
|
|
| 15 |
A |
1059 |
1019 |
1.61 |
|
|
|
| 16 |
A |
946 |
910 |
12.08 |
|
|
|
| 17 |
A |
786 |
756 |
0.01 |
|
|
|
| 18 |
A |
575 |
553 |
102.76 |
|
|
|
| 19 |
A |
342 |
329 |
63.14 |
|
|
|
| 20 |
A |
311 |
299 |
15.72 |
|
|
|
| 21 |
A |
153 |
147 |
0.32 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16421.5 cm
-1
Scaled (by 0.962) Zero Point Vibrational Energy (zpe) 15797.5 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/3-21G*
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.866 |
0.446 |
0.001 |
| O2 |
1.382 |
-0.679 |
0.001 |
| N3 |
-0.480 |
0.674 |
-0.013 |
| C4 |
-1.420 |
-0.455 |
0.003 |
| H5 |
1.441 |
1.388 |
0.011 |
| H6 |
-0.831 |
1.624 |
0.047 |
| H7 |
-2.422 |
-0.092 |
-0.233 |
| H8 |
-1.117 |
-1.193 |
-0.745 |
| H9 |
-1.439 |
-0.955 |
0.979 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.2382 | 1.3647 | 2.4567 | 1.1038 | 2.0659 | 3.3399 | 2.6788 | 2.8689 |
O2 | 1.2382 | | 2.3017 | 2.8109 | 2.0681 | 3.1944 | 3.8565 | 2.6582 | 2.9985 | N3 | 1.3647 | 2.3017 | | 1.4692 | 2.0494 | 1.0145 | 2.0996 | 2.1046 | 2.1346 | C4 | 2.4567 | 2.8109 | 1.4692 | | 3.4032 | 2.1612 | 1.0919 | 1.0935 | 1.0966 | H5 | 1.1038 | 2.0681 | 2.0494 | 3.4032 | | 2.2845 | 4.1443 | 3.7120 | 3.8368 | H6 | 2.0659 | 3.1944 | 1.0145 | 2.1612 | 2.2845 | | 2.3569 | 2.9405 | 2.8086 | H7 | 3.3399 | 3.8565 | 2.0996 | 1.0919 | 4.1443 | 2.3569 | | 1.7828 | 1.7832 | H8 | 2.6788 | 2.6582 | 2.1046 | 1.0935 | 3.7120 | 2.9405 | 1.7828 | | 1.7694 | H9 | 2.8689 | 2.9985 | 2.1346 | 1.0966 | 3.8368 | 2.8086 | 1.7832 | 1.7694 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
120.158 |
|
C1 |
N3 |
H6 |
119.803 |
| O2 |
C1 |
N3 |
124.260 |
|
O2 |
C1 |
H5 |
123.928 |
| N3 |
C1 |
H5 |
111.812 |
|
N3 |
C4 |
H7 |
109.247 |
| N3 |
C4 |
H8 |
109.544 |
|
N3 |
C4 |
H9 |
111.776 |
| C4 |
N3 |
H6 |
119.828 |
|
H7 |
C4 |
H8 |
109.324 |
| H7 |
C4 |
H9 |
109.133 |
|
H8 |
C4 |
H9 |
107.778 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.430 |
|
|
|
| 2 |
O |
-0.483 |
|
|
|
| 3 |
N |
-0.666 |
|
|
|
| 4 |
C |
-0.395 |
|
|
|
| 5 |
H |
0.159 |
|
|
|
| 6 |
H |
0.311 |
|
|
|
| 7 |
H |
0.201 |
|
|
|
| 8 |
H |
0.241 |
|
|
|
| 9 |
H |
0.201 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.740 |
2.467 |
-0.003 |
3.687 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.099 |
2.461 |
0.002 |
| y |
2.461 |
-21.857 |
-0.004 |
| z |
0.002 |
-0.004 |
-24.560 |
|
| Traceless |
| | x | y | z |
| x |
-1.891 |
2.461 |
0.002 |
| y |
2.461 |
2.973 |
-0.004 |
| z |
0.002 |
-0.004 |
-1.082 |
|
| Polar |
| 3z2-r2 | -2.165 |
| x2-y2 | -3.242 |
| xy | 2.461 |
| xz | 0.002 |
| yz | -0.004 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.455 |
-0.095 |
-0.000 |
| y |
-0.095 |
4.459 |
-0.000 |
| z |
-0.000 |
-0.000 |
2.442 |
<r2> (average value of r
2) Å
2
| <r2> |
78.504 |
| (<r2>)1/2 |
8.860 |