Jump to
S1C2
S1C3
Energy calculated at wB97X-D/6-311G*
| | hartrees |
| Energy at 0K | -209.181888 |
| Energy at 298.15K | -209.187791 |
| HF Energy | -209.181888 |
| Nuclear repulsion energy | 119.530202 |
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/6-311G*
| 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' |
3660 |
3660 |
19.22 |
|
|
|
| 2 |
A' |
3146 |
3146 |
22.19 |
|
|
|
| 3 |
A' |
3050 |
3050 |
58.03 |
|
|
|
| 4 |
A' |
2958 |
2958 |
102.03 |
|
|
|
| 5 |
A' |
1851 |
1851 |
517.37 |
|
|
|
| 6 |
A' |
1557 |
1557 |
28.38 |
|
|
|
| 7 |
A' |
1512 |
1512 |
7.65 |
|
|
|
| 8 |
A' |
1493 |
1493 |
4.05 |
|
|
|
| 9 |
A' |
1412 |
1412 |
8.02 |
|
|
|
| 10 |
A' |
1325 |
1325 |
112.04 |
|
|
|
| 11 |
A' |
1189 |
1189 |
28.69 |
|
|
|
| 12 |
A' |
1031 |
1031 |
49.18 |
|
|
|
| 13 |
A' |
623 |
623 |
15.20 |
|
|
|
| 14 |
A' |
353 |
353 |
8.85 |
|
|
|
| 15 |
A" |
3111 |
3111 |
36.67 |
|
|
|
| 16 |
A" |
1511 |
1511 |
8.14 |
|
|
|
| 17 |
A" |
1158 |
1158 |
0.51 |
|
|
|
| 18 |
A" |
1058 |
1058 |
0.28 |
|
|
|
| 19 |
A" |
638 |
638 |
142.77 |
|
|
|
| 20 |
A" |
195 |
195 |
1.29 |
|
|
|
| 21 |
A" |
10 |
10 |
0.70 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16420.1 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 16420.1 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 wB97X-D/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.284 |
-0.759 |
0.000 |
| O2 |
1.395 |
-1.230 |
0.000 |
| N3 |
0.000 |
0.568 |
0.000 |
| C4 |
-1.328 |
1.134 |
0.000 |
| H5 |
-0.631 |
-1.384 |
0.000 |
| H6 |
0.797 |
1.185 |
0.000 |
| H7 |
-2.060 |
0.324 |
0.000 |
| H8 |
-1.503 |
1.745 |
0.890 |
| H9 |
-1.503 |
1.745 |
-0.890 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.2069 | 1.3566 | 2.4865 | 1.1082 | 2.0101 | 2.5827 | 3.2025 | 3.2025 |
O2 | 1.2069 | | 2.2757 | 3.6065 | 2.0321 | 2.4878 | 3.7892 | 4.2479 | 4.2479 | N3 | 1.3566 | 2.2757 | | 1.4439 | 2.0509 | 1.0081 | 2.0747 | 2.1065 | 2.1065 | C4 | 2.4865 | 3.6065 | 1.4439 | | 2.6125 | 2.1260 | 1.0915 | 1.0934 | 1.0934 | H5 | 1.1082 | 2.0321 | 2.0509 | 2.6125 | | 2.9388 | 2.2274 | 3.3679 | 3.3679 | H6 | 2.0101 | 2.4878 | 1.0081 | 2.1260 | 2.9388 | | 2.9842 | 2.5292 | 2.5292 | H7 | 2.5827 | 3.7892 | 2.0747 | 1.0915 | 2.2274 | 2.9842 | | 1.7665 | 1.7665 | H8 | 3.2025 | 4.2479 | 2.1065 | 1.0934 | 3.3679 | 2.5292 | 1.7665 | | 1.7791 | H9 | 3.2025 | 4.2479 | 2.1065 | 1.0934 | 3.3679 | 2.5292 | 1.7665 | 1.7791 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
125.184 |
|
C1 |
N3 |
H6 |
115.647 |
| O2 |
C1 |
N3 |
125.076 |
|
O2 |
C1 |
H5 |
122.686 |
| N3 |
C1 |
H5 |
112.238 |
|
N3 |
C4 |
H7 |
109.035 |
| N3 |
C4 |
H8 |
111.491 |
|
N3 |
C4 |
H9 |
111.491 |
| C4 |
N3 |
H6 |
119.168 |
|
H7 |
C4 |
H8 |
107.901 |
| H7 |
C4 |
H9 |
107.901 |
|
H8 |
C4 |
H9 |
108.891 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.209 |
|
|
|
| 2 |
O |
-0.368 |
|
|
|
| 3 |
N |
-0.527 |
|
|
|
| 4 |
C |
-0.498 |
|
|
|
| 5 |
H |
0.148 |
|
|
|
| 6 |
H |
0.349 |
|
|
|
| 7 |
H |
0.225 |
|
|
|
| 8 |
H |
0.231 |
|
|
|
| 9 |
H |
0.231 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.038 |
2.795 |
0.000 |
4.128 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.242 |
4.104 |
0.000 |
| y |
4.104 |
-24.162 |
0.000 |
| z |
0.000 |
0.000 |
-24.689 |
|
| Traceless |
| | x | y | z |
| x |
-1.817 |
4.104 |
0.000 |
| y |
4.104 |
1.304 |
0.000 |
| z |
0.000 |
0.000 |
0.513 |
|
| Polar |
| 3z2-r2 | 1.026 |
| x2-y2 | -2.081 |
| xy | 4.104 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.538 |
-0.989 |
0.000 |
| y |
-0.989 |
5.575 |
0.000 |
| z |
0.000 |
0.000 |
3.239 |
<r2> (average value of r
2) Å
2
| <r2> |
88.705 |
| (<r2>)1/2 |
9.418 |
Jump to
S1C1
S1C3
Energy calculated at wB97X-D/6-311G*
| | hartrees |
| Energy at 0K | -209.181888 |
| Energy at 298.15K | -209.187791 |
| HF Energy | -209.181888 |
| Nuclear repulsion energy | 119.530202 |
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/6-311G*
Geometric Data calculated at wB97X-D/6-311G*
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
Energy calculated at wB97X-D/6-311G*
| | hartrees |
| Energy at 0K | -209.183675 |
| Energy at 298.15K | -209.189703 |
| HF Energy | -209.183675 |
| Nuclear repulsion energy | 121.715420 |
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/6-311G*
| 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 |
3691 |
3691 |
20.04 |
|
|
|
| 2 |
A |
3183 |
3183 |
2.51 |
|
|
|
| 3 |
A |
3118 |
3118 |
38.14 |
|
|
|
| 4 |
A |
3056 |
3056 |
48.89 |
|
|
|
| 5 |
A |
2971 |
2971 |
134.03 |
|
|
|
| 6 |
A |
1840 |
1840 |
357.03 |
|
|
|
| 7 |
A |
1593 |
1593 |
124.35 |
|
|
|
| 8 |
A |
1527 |
1527 |
10.65 |
|
|
|
| 9 |
A |
1517 |
1517 |
29.81 |
|
|
|
| 10 |
A |
1470 |
1470 |
19.45 |
|
|
|
| 11 |
A |
1439 |
1439 |
4.74 |
|
|
|
| 12 |
A |
1250 |
1250 |
76.13 |
|
|
|
| 13 |
A |
1182 |
1182 |
20.48 |
|
|
|
| 14 |
A |
1168 |
1168 |
1.75 |
|
|
|
| 15 |
A |
1033 |
1033 |
0.46 |
|
|
|
| 16 |
A |
986 |
986 |
22.10 |
|
|
|
| 17 |
A |
785 |
785 |
1.27 |
|
|
|
| 18 |
A |
546 |
546 |
56.69 |
|
|
|
| 19 |
A |
314 |
314 |
13.30 |
|
|
|
| 20 |
A |
277 |
277 |
83.65 |
|
|
|
| 21 |
A |
37 |
37 |
0.05 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16490.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 16490.8 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/6-311G*
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.863 |
0.432 |
0.003 |
| O2 |
1.370 |
-0.669 |
0.000 |
| N3 |
-0.470 |
0.657 |
-0.020 |
| C4 |
-1.419 |
-0.439 |
0.005 |
| H5 |
1.459 |
1.360 |
0.018 |
| H6 |
-0.800 |
1.603 |
0.059 |
| H7 |
-2.415 |
-0.053 |
-0.209 |
| H8 |
-1.149 |
-1.175 |
-0.753 |
| H9 |
-1.426 |
-0.938 |
0.978 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.2119 | 1.3517 | 2.4421 | 1.1036 | 2.0343 | 3.3199 | 2.6834 | 2.8394 |
O2 | 1.2119 | | 2.2680 | 2.7980 | 2.0310 | 3.1421 | 3.8403 | 2.6771 | 2.9738 | N3 | 1.3517 | 2.2680 | | 1.4504 | 2.0536 | 1.0048 | 2.0791 | 2.0872 | 2.1104 | C4 | 2.4421 | 2.7980 | 1.4504 | | 3.3943 | 2.1351 | 1.0898 | 1.0902 | 1.0931 | H5 | 1.1036 | 2.0310 | 2.0536 | 3.3943 | | 2.2724 | 4.1301 | 3.7183 | 3.8110 | H6 | 2.0343 | 3.1421 | 1.0048 | 2.1351 | 2.2724 | | 2.3288 | 2.9157 | 2.7737 | H7 | 3.3199 | 3.8403 | 2.0791 | 1.0898 | 4.1301 | 2.3288 | | 1.7773 | 1.7806 | H8 | 2.6834 | 2.6771 | 2.0872 | 1.0902 | 3.7183 | 2.9157 | 1.7773 | | 1.7686 | H9 | 2.8394 | 2.9738 | 2.1104 | 1.0931 | 3.8110 | 2.7737 | 1.7806 | 1.7686 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
121.226 |
|
C1 |
N3 |
H6 |
118.629 |
| O2 |
C1 |
N3 |
124.336 |
|
O2 |
C1 |
H5 |
122.523 |
| N3 |
C1 |
H5 |
113.140 |
|
N3 |
C4 |
H7 |
109.039 |
| N3 |
C4 |
H8 |
109.666 |
|
N3 |
C4 |
H9 |
111.365 |
| C4 |
N3 |
H6 |
119.726 |
|
H7 |
C4 |
H8 |
109.230 |
| H7 |
C4 |
H9 |
109.308 |
|
H8 |
C4 |
H9 |
108.202 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.202 |
|
|
|
| 2 |
O |
-0.371 |
|
|
|
| 3 |
N |
-0.536 |
|
|
|
| 4 |
C |
-0.514 |
|
|
|
| 5 |
H |
0.160 |
|
|
|
| 6 |
H |
0.348 |
|
|
|
| 7 |
H |
0.225 |
|
|
|
| 8 |
H |
0.259 |
|
|
|
| 9 |
H |
0.227 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.917 |
2.662 |
0.032 |
3.949 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.413 |
2.638 |
0.002 |
| y |
2.638 |
-21.887 |
0.080 |
| z |
0.002 |
0.080 |
-24.720 |
|
| Traceless |
| | x | y | z |
| x |
-2.110 |
2.638 |
0.002 |
| y |
2.638 |
3.180 |
0.080 |
| z |
0.002 |
0.080 |
-1.070 |
|
| Polar |
| 3z2-r2 | -2.140 |
| x2-y2 | -3.527 |
| xy | 2.638 |
| xz | 0.002 |
| yz | 0.080 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.911 |
-0.124 |
-0.007 |
| y |
-0.124 |
4.966 |
-0.002 |
| z |
-0.007 |
-0.002 |
3.229 |
<r2> (average value of r
2) Å
2
| <r2> |
78.157 |
| (<r2>)1/2 |
8.841 |