Jump to
S1C2
S1C3
Energy calculated at B97D3/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -209.157344 |
| Energy at 298.15K | -209.163321 |
| HF Energy | -209.157344 |
| Nuclear repulsion energy | 118.912352 |
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 B97D3/6-311+G(3df,2p)
| 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' |
3539 |
3493 |
17.51 |
|
|
|
| 2 |
A' |
3060 |
3020 |
16.08 |
|
|
|
| 3 |
A' |
2966 |
2928 |
62.85 |
|
|
|
| 4 |
A' |
2846 |
2809 |
98.37 |
|
|
|
| 5 |
A' |
1738 |
1715 |
483.46 |
|
|
|
| 6 |
A' |
1500 |
1481 |
14.47 |
|
|
|
| 7 |
A' |
1445 |
1426 |
0.66 |
|
|
|
| 8 |
A' |
1435 |
1416 |
8.35 |
|
|
|
| 9 |
A' |
1363 |
1345 |
9.61 |
|
|
|
| 10 |
A' |
1267 |
1251 |
100.32 |
|
|
|
| 11 |
A' |
1127 |
1113 |
35.08 |
|
|
|
| 12 |
A' |
986 |
973 |
39.28 |
|
|
|
| 13 |
A' |
597 |
589 |
11.81 |
|
|
|
| 14 |
A' |
336 |
332 |
7.16 |
|
|
|
| 15 |
A" |
3016 |
2977 |
29.60 |
|
|
|
| 16 |
A" |
1456 |
1438 |
5.39 |
|
|
|
| 17 |
A" |
1126 |
1112 |
0.37 |
|
|
|
| 18 |
A" |
997 |
984 |
2.75 |
|
|
|
| 19 |
A" |
599 |
591 |
101.28 |
|
|
|
| 20 |
A" |
195 |
192 |
0.49 |
|
|
|
| 21 |
A" |
95 |
94 |
0.46 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15844.3 cm
-1
Scaled (by 0.987) Zero Point Vibrational Energy (zpe) 15638.4 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 B97D3/6-311+G(3df,2p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.286 |
-0.759 |
0.000 |
| O2 |
1.406 |
-1.236 |
0.000 |
| N3 |
0.000 |
0.573 |
0.000 |
| C4 |
-1.338 |
1.135 |
0.000 |
| H5 |
-0.637 |
-1.381 |
0.000 |
| H6 |
0.797 |
1.197 |
0.000 |
| H7 |
-2.063 |
0.316 |
0.000 |
| H8 |
-1.516 |
1.748 |
0.891 |
| H9 |
-1.516 |
1.748 |
-0.891 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.2178 | 1.3621 | 2.4947 | 1.1124 | 2.0215 | 2.5826 | 3.2132 | 3.2132 |
O2 | 1.2178 | | 2.2909 | 3.6265 | 2.0483 | 2.5076 | 3.8001 | 4.2703 | 4.2703 | N3 | 1.3621 | 2.2909 | | 1.4515 | 2.0547 | 1.0121 | 2.0786 | 2.1149 | 2.1149 | C4 | 2.4947 | 3.6265 | 1.4515 | | 2.6114 | 2.1362 | 1.0932 | 1.0961 | 1.0961 | H5 | 1.1124 | 2.0483 | 2.0547 | 2.6114 | | 2.9494 | 2.2161 | 3.3697 | 3.3697 | H6 | 2.0215 | 2.5076 | 1.0121 | 2.1362 | 2.9494 | | 2.9922 | 2.5392 | 2.5392 | H7 | 2.5826 | 3.8001 | 2.0786 | 1.0932 | 2.2161 | 2.9922 | | 1.7730 | 1.7730 | H8 | 3.2132 | 4.2703 | 2.1149 | 1.0961 | 3.3697 | 2.5392 | 1.7730 | | 1.7818 | H9 | 3.2132 | 4.2703 | 2.1149 | 1.0961 | 3.3697 | 2.5392 | 1.7730 | 1.7818 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
124.810 |
|
C1 |
N3 |
H6 |
115.986 |
| O2 |
C1 |
N3 |
125.489 |
|
O2 |
C1 |
H5 |
122.753 |
| N3 |
C1 |
H5 |
111.758 |
|
N3 |
C4 |
H7 |
108.723 |
| N3 |
C4 |
H8 |
111.555 |
|
N3 |
C4 |
H9 |
111.555 |
| C4 |
N3 |
H6 |
119.203 |
|
H7 |
C4 |
H8 |
108.089 |
| H7 |
C4 |
H9 |
108.089 |
|
H8 |
C4 |
H9 |
108.711 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.690 |
|
|
|
| 2 |
O |
-0.655 |
|
|
|
| 3 |
N |
-0.651 |
|
|
|
| 4 |
C |
0.025 |
|
|
|
| 5 |
H |
0.088 |
|
|
|
| 6 |
H |
0.168 |
|
|
|
| 7 |
H |
0.110 |
|
|
|
| 8 |
H |
0.112 |
|
|
|
| 9 |
H |
0.112 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.099 |
2.870 |
0.000 |
4.223 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-27.050 |
4.102 |
0.000 |
| y |
4.102 |
-24.667 |
0.000 |
| z |
0.000 |
0.000 |
-24.962 |
|
| Traceless |
| | x | y | z |
| x |
-2.236 |
4.102 |
0.000 |
| y |
4.102 |
1.340 |
0.000 |
| z |
0.000 |
0.000 |
0.897 |
|
| Polar |
| 3z2-r2 | 1.793 |
| x2-y2 | -2.384 |
| xy | 4.102 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.981 |
-1.272 |
0.000 |
| y |
-1.272 |
6.905 |
0.000 |
| z |
0.000 |
0.000 |
4.389 |
<r2> (average value of r
2) Å
2
| <r2> |
89.744 |
| (<r2>)1/2 |
9.473 |
Jump to
S1C1
S1C3
Energy calculated at B97D3/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -209.157344 |
| Energy at 298.15K | -209.163321 |
| HF Energy | -209.157344 |
| Nuclear repulsion energy | 118.912352 |
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 B97D3/6-311+G(3df,2p)
Geometric Data calculated at B97D3/6-311+G(3df,2p)
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
Energy calculated at B97D3/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -209.158875 |
| Energy at 298.15K | -209.164774 |
| HF Energy | -209.158875 |
| Nuclear repulsion energy | 120.971256 |
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 B97D3/6-311+G(3df,2p)
| 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 |
3567 |
3521 |
14.17 |
|
|
|
| 2 |
A |
3093 |
3052 |
1.61 |
|
|
|
| 3 |
A |
3027 |
2988 |
29.46 |
|
|
|
| 4 |
A |
2975 |
2936 |
52.13 |
|
|
|
| 5 |
A |
2862 |
2824 |
127.96 |
|
|
|
| 6 |
A |
1731 |
1709 |
333.08 |
|
|
|
| 7 |
A |
1518 |
1499 |
74.51 |
|
|
|
| 8 |
A |
1471 |
1452 |
6.25 |
|
|
|
| 9 |
A |
1458 |
1439 |
33.24 |
|
|
|
| 10 |
A |
1411 |
1393 |
19.34 |
|
|
|
| 11 |
A |
1388 |
1370 |
4.67 |
|
|
|
| 12 |
A |
1185 |
1170 |
75.37 |
|
|
|
| 13 |
A |
1133 |
1118 |
23.24 |
|
|
|
| 14 |
A |
1128 |
1113 |
0.84 |
|
|
|
| 15 |
A |
982 |
969 |
0.19 |
|
|
|
| 16 |
A |
928 |
916 |
16.78 |
|
|
|
| 17 |
A |
750 |
740 |
0.28 |
|
|
|
| 18 |
A |
539 |
532 |
39.74 |
|
|
|
| 19 |
A |
288 |
284 |
12.66 |
|
|
|
| 20 |
A |
262 |
259 |
58.67 |
|
|
|
| 21 |
A |
25 |
25 |
0.12 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15860.3 cm
-1
Scaled (by 0.987) Zero Point Vibrational Energy (zpe) 15654.1 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 B97D3/6-311+G(3df,2p)
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.870 |
0.428 |
-0.000 |
| O2 |
1.417 |
-0.660 |
0.000 |
| N3 |
-0.476 |
0.640 |
-0.000 |
| C4 |
-1.459 |
-0.433 |
-0.000 |
| H5 |
1.433 |
1.386 |
-0.000 |
| H6 |
-0.796 |
1.597 |
-0.000 |
| H7 |
-2.093 |
-0.385 |
-0.892 |
| H8 |
-0.917 |
-1.380 |
0.000 |
| H9 |
-2.093 |
-0.385 |
0.891 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.2186 | 1.3625 | 2.4828 | 1.1108 | 2.0351 | 3.1993 | 2.5418 | 3.1994 |
O2 | 1.2186 | | 2.2968 | 2.8849 | 2.0459 | 3.1615 | 3.6321 | 2.4424 | 3.6324 | N3 | 1.3625 | 2.2968 | | 1.4548 | 2.0502 | 1.0095 | 2.1118 | 2.0668 | 2.1118 | C4 | 2.4828 | 2.8849 | 1.4548 | | 3.4166 | 2.1357 | 1.0953 | 1.0904 | 1.0953 | H5 | 1.1108 | 2.0459 | 2.0502 | 3.4166 | | 2.2398 | 4.0456 | 3.6290 | 4.0457 | H6 | 2.0351 | 3.1615 | 1.0095 | 2.1357 | 2.2398 | | 2.5311 | 2.9791 | 2.5309 | H7 | 3.1993 | 3.6321 | 2.1118 | 1.0953 | 4.0456 | 2.5311 | | 1.7798 | 1.7832 | H8 | 2.5418 | 2.4424 | 2.0668 | 1.0904 | 3.6290 | 2.9791 | 1.7798 | | 1.7798 | H9 | 3.1994 | 3.6324 | 2.1118 | 1.0953 | 4.0457 | 2.5309 | 1.7832 | 1.7798 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
122.419 |
|
C1 |
N3 |
H6 |
118.017 |
| O2 |
C1 |
N3 |
125.279 |
|
O2 |
C1 |
H5 |
122.898 |
| N3 |
C1 |
H5 |
111.812 |
|
N3 |
C4 |
H7 |
109.302 |
| N3 |
C4 |
H8 |
109.361 |
|
N3 |
C4 |
H9 |
111.834 |
| C4 |
N3 |
H6 |
119.025 |
|
H7 |
C4 |
H8 |
109.131 |
| H7 |
C4 |
H9 |
109.026 |
|
H8 |
C4 |
H9 |
108.144 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.670 |
|
|
|
| 2 |
O |
-0.635 |
|
|
|
| 3 |
N |
-0.648 |
|
|
|
| 4 |
C |
0.002 |
|
|
|
| 5 |
H |
0.086 |
|
|
|
| 6 |
H |
0.156 |
|
|
|
| 7 |
H |
0.111 |
|
|
|
| 8 |
H |
0.147 |
|
|
|
| 9 |
H |
0.111 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.032 |
2.492 |
0.000 |
3.924 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.003 |
2.631 |
-0.000 |
| y |
2.631 |
-22.743 |
-0.000 |
| z |
-0.000 |
-0.000 |
-25.033 |
|
| Traceless |
| | x | y | z |
| x |
-2.115 |
2.631 |
-0.000 |
| y |
2.631 |
2.775 |
-0.000 |
| z |
-0.000 |
-0.000 |
-0.660 |
|
| Polar |
| 3z2-r2 | -1.320 |
| x2-y2 | -3.260 |
| xy | 2.631 |
| xz | -0.000 |
| yz | -0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.475 |
-0.076 |
0.000 |
| y |
-0.076 |
6.240 |
0.000 |
| z |
0.000 |
0.000 |
4.445 |
<r2> (average value of r
2) Å
2
| <r2> |
79.455 |
| (<r2>)1/2 |
8.914 |