Jump to
S1C2
S1C3
Energy calculated at wB97X-D/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -209.149096 |
| Energy at 298.15K | -209.155064 |
| HF Energy | -209.149096 |
| Nuclear repulsion energy | 119.598268 |
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 wB97X-D/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 |
3670 |
29.27 |
|
|
|
| 2 |
A' |
3145 |
3145 |
15.24 |
|
|
|
| 3 |
A' |
3043 |
3043 |
51.08 |
|
|
|
| 4 |
A' |
2947 |
2947 |
85.56 |
|
|
|
| 5 |
A' |
1862 |
1862 |
460.13 |
|
|
|
| 6 |
A' |
1539 |
1539 |
27.72 |
|
|
|
| 7 |
A' |
1497 |
1497 |
8.66 |
|
|
|
| 8 |
A' |
1481 |
1481 |
10.04 |
|
|
|
| 9 |
A' |
1409 |
1409 |
12.36 |
|
|
|
| 10 |
A' |
1319 |
1319 |
97.95 |
|
|
|
| 11 |
A' |
1188 |
1188 |
24.12 |
|
|
|
| 12 |
A' |
1028 |
1028 |
44.64 |
|
|
|
| 13 |
A' |
622 |
622 |
14.49 |
|
|
|
| 14 |
A' |
352 |
352 |
8.39 |
|
|
|
| 15 |
A" |
3109 |
3109 |
28.01 |
|
|
|
| 16 |
A" |
1490 |
1490 |
5.66 |
|
|
|
| 17 |
A" |
1155 |
1155 |
0.37 |
|
|
|
| 18 |
A" |
1070 |
1070 |
0.09 |
|
|
|
| 19 |
A" |
621 |
621 |
113.52 |
|
|
|
| 20 |
A" |
202 |
202 |
0.81 |
|
|
|
| 21 |
A" |
43 |
43 |
0.38 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16395.3 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 16395.3 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 wB97X-D/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.284 |
-0.758 |
0.000 |
| O2 |
1.397 |
-1.226 |
0.000 |
| N3 |
0.000 |
0.568 |
0.000 |
| C4 |
-1.328 |
1.128 |
0.000 |
| H5 |
-0.636 |
-1.377 |
0.000 |
| H6 |
0.796 |
1.187 |
0.000 |
| H7 |
-2.056 |
0.313 |
0.000 |
| H8 |
-1.508 |
1.741 |
0.890 |
| H9 |
-1.508 |
1.741 |
-0.890 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.2070 | 1.3562 | 2.4813 | 1.1096 | 2.0107 | 2.5741 | 3.2012 | 3.2012 |
O2 | 1.2070 | | 2.2740 | 3.6011 | 2.0385 | 2.4867 | 3.7807 | 4.2466 | 4.2466 | N3 | 1.3562 | 2.2740 | | 1.4412 | 2.0470 | 1.0078 | 2.0722 | 2.1073 | 2.1073 | C4 | 2.4813 | 3.6011 | 1.4412 | | 2.5993 | 2.1245 | 1.0932 | 1.0950 | 1.0950 | H5 | 1.1096 | 2.0385 | 2.0470 | 2.5993 | | 2.9368 | 2.2078 | 3.3577 | 3.3577 | H6 | 2.0107 | 2.4867 | 1.0078 | 2.1245 | 2.9368 | | 2.9829 | 2.5311 | 2.5311 | H7 | 2.5741 | 3.7807 | 2.0722 | 1.0932 | 2.2078 | 2.9829 | | 1.7692 | 1.7692 | H8 | 3.2012 | 4.2466 | 2.1073 | 1.0950 | 3.3577 | 2.5311 | 1.7692 | | 1.7792 | H9 | 3.2012 | 4.2466 | 2.1073 | 1.0950 | 3.3577 | 2.5311 | 1.7692 | 1.7792 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
124.964 |
|
C1 |
N3 |
H6 |
115.755 |
| O2 |
C1 |
N3 |
124.939 |
|
O2 |
C1 |
H5 |
123.221 |
| N3 |
C1 |
H5 |
111.839 |
|
N3 |
C4 |
H7 |
108.920 |
| N3 |
C4 |
H8 |
111.653 |
|
N3 |
C4 |
H9 |
111.653 |
| C4 |
N3 |
H6 |
119.281 |
|
H7 |
C4 |
H8 |
107.905 |
| H7 |
C4 |
H9 |
107.905 |
|
H8 |
C4 |
H9 |
108.666 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.177 |
|
|
|
| 2 |
O |
-0.348 |
|
|
|
| 3 |
N |
-0.305 |
|
|
|
| 4 |
C |
-0.355 |
|
|
|
| 5 |
H |
0.086 |
|
|
|
| 6 |
H |
0.281 |
|
|
|
| 7 |
H |
0.159 |
|
|
|
| 8 |
H |
0.153 |
|
|
|
| 9 |
H |
0.153 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.880 |
2.707 |
0.000 |
3.953 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.876 |
3.921 |
0.000 |
| y |
3.921 |
-23.844 |
0.000 |
| z |
0.000 |
0.000 |
-24.236 |
|
| Traceless |
| | x | y | z |
| x |
-1.836 |
3.921 |
0.000 |
| y |
3.921 |
1.212 |
0.000 |
| z |
0.000 |
0.000 |
0.624 |
|
| Polar |
| 3z2-r2 | 1.248 |
| x2-y2 | -2.032 |
| xy | 3.921 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.578 |
-0.993 |
0.000 |
| y |
-0.993 |
5.678 |
0.000 |
| z |
0.000 |
0.000 |
3.348 |
<r2> (average value of r
2) Å
2
| <r2> |
88.307 |
| (<r2>)1/2 |
9.397 |
Jump to
S1C1
S1C3
Energy calculated at wB97X-D/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -209.149096 |
| Energy at 298.15K | -209.155064 |
| HF Energy | -209.149096 |
| Nuclear repulsion energy | 119.598268 |
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 wB97X-D/6-31G(2df,p)
Geometric Data calculated at wB97X-D/6-31G(2df,p)
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
Energy calculated at wB97X-D/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -209.150707 |
| Energy at 298.15K | -209.156774 |
| HF Energy | -209.150707 |
| Nuclear repulsion energy | 121.781784 |
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 wB97X-D/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 |
3702 |
3702 |
29.95 |
|
|
|
| 2 |
A |
3183 |
3183 |
0.94 |
|
|
|
| 3 |
A |
3121 |
3121 |
28.07 |
|
|
|
| 4 |
A |
3054 |
3054 |
44.48 |
|
|
|
| 5 |
A |
2965 |
2965 |
109.80 |
|
|
|
| 6 |
A |
1850 |
1850 |
318.68 |
|
|
|
| 7 |
A |
1573 |
1573 |
103.40 |
|
|
|
| 8 |
A |
1508 |
1508 |
7.65 |
|
|
|
| 9 |
A |
1504 |
1504 |
34.73 |
|
|
|
| 10 |
A |
1454 |
1454 |
17.93 |
|
|
|
| 11 |
A |
1439 |
1439 |
1.48 |
|
|
|
| 12 |
A |
1249 |
1249 |
71.17 |
|
|
|
| 13 |
A |
1172 |
1172 |
15.18 |
|
|
|
| 14 |
A |
1168 |
1168 |
5.26 |
|
|
|
| 15 |
A |
1044 |
1044 |
0.49 |
|
|
|
| 16 |
A |
987 |
987 |
20.22 |
|
|
|
| 17 |
A |
780 |
780 |
1.02 |
|
|
|
| 18 |
A |
538 |
538 |
42.43 |
|
|
|
| 19 |
A |
307 |
307 |
13.44 |
|
|
|
| 20 |
A |
268 |
268 |
68.19 |
|
|
|
| 21 |
A |
71 |
71 |
0.04 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16467.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 16467.9 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 wB97X-D/6-31G(2df,p)
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.863 |
0.433 |
0.003 |
| O2 |
1.364 |
-0.671 |
0.000 |
| N3 |
-0.468 |
0.657 |
-0.020 |
| C4 |
-1.416 |
-0.439 |
0.005 |
| H5 |
1.457 |
1.364 |
0.019 |
| H6 |
-0.799 |
1.602 |
0.058 |
| H7 |
-2.413 |
-0.051 |
-0.210 |
| H8 |
-1.142 |
-1.175 |
-0.754 |
| H9 |
-1.424 |
-0.938 |
0.978 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.2121 | 1.3507 | 2.4402 | 1.1043 | 2.0331 | 3.3188 | 2.6795 | 2.8393 |
O2 | 1.2121 | | 2.2635 | 2.7901 | 2.0371 | 3.1385 | 3.8337 | 2.6656 | 2.9671 | N3 | 1.3507 | 2.2635 | | 1.4489 | 2.0510 | 1.0041 | 2.0784 | 2.0853 | 2.1109 | C4 | 2.4402 | 2.7901 | 1.4489 | | 3.3914 | 2.1327 | 1.0909 | 1.0918 | 1.0945 | H5 | 1.1043 | 2.0371 | 2.0510 | 3.3914 | | 2.2684 | 4.1267 | 3.7144 | 3.8104 | H6 | 2.0331 | 3.1385 | 1.0041 | 2.1327 | 2.2684 | | 2.3262 | 2.9135 | 2.7734 | H7 | 3.3188 | 3.8337 | 2.0784 | 1.0909 | 4.1267 | 2.3262 | | 1.7813 | 1.7825 | H8 | 2.6795 | 2.6656 | 2.0853 | 1.0918 | 3.7144 | 2.9135 | 1.7813 | | 1.7706 | H9 | 2.8393 | 2.9671 | 2.1109 | 1.0945 | 3.8104 | 2.7734 | 1.7825 | 1.7706 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
121.254 |
|
C1 |
N3 |
H6 |
118.658 |
| O2 |
C1 |
N3 |
123.978 |
|
O2 |
C1 |
H5 |
123.078 |
| N3 |
C1 |
H5 |
112.942 |
|
N3 |
C4 |
H7 |
109.017 |
| N3 |
C4 |
H8 |
109.518 |
|
N3 |
C4 |
H9 |
111.426 |
| C4 |
N3 |
H6 |
119.676 |
|
H7 |
C4 |
H8 |
109.384 |
| H7 |
C4 |
H9 |
109.302 |
|
H8 |
C4 |
H9 |
108.167 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.170 |
|
|
|
| 2 |
O |
-0.341 |
|
|
|
| 3 |
N |
-0.328 |
|
|
|
| 4 |
C |
-0.361 |
|
|
|
| 5 |
H |
0.097 |
|
|
|
| 6 |
H |
0.277 |
|
|
|
| 7 |
H |
0.148 |
|
|
|
| 8 |
H |
0.191 |
|
|
|
| 9 |
H |
0.147 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.787 |
2.531 |
-0.031 |
3.765 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.038 |
2.420 |
-0.007 |
| y |
2.420 |
-21.666 |
-0.088 |
| z |
-0.007 |
-0.088 |
-24.260 |
|
| Traceless |
| | x | y | z |
| x |
-2.075 |
2.420 |
-0.007 |
| y |
2.420 |
2.984 |
-0.088 |
| z |
-0.007 |
-0.088 |
-0.908 |
|
| Polar |
| 3z2-r2 | -1.817 |
| x2-y2 | -3.372 |
| xy | 2.420 |
| xz | -0.007 |
| yz | -0.088 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.071 |
-0.033 |
0.005 |
| y |
-0.033 |
4.975 |
0.004 |
| z |
0.005 |
0.004 |
3.333 |
<r2> (average value of r
2) Å
2
| <r2> |
77.785 |
| (<r2>)1/2 |
8.820 |