Jump to
S1C2
S1C3
Energy calculated at M06-2X/6-31G*
| | hartrees |
| Energy at 0K | -209.099525 |
| Energy at 298.15K | -209.105517 |
| HF Energy | -209.099525 |
| Nuclear repulsion energy | 119.382412 |
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 M06-2X/6-31G*
| 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' |
3641 |
3448 |
34.80 |
|
|
|
| 2 |
A' |
3169 |
3001 |
15.05 |
|
|
|
| 3 |
A' |
3077 |
2914 |
45.48 |
|
|
|
| 4 |
A' |
3005 |
2846 |
81.29 |
|
|
|
| 5 |
A' |
1876 |
1777 |
501.29 |
|
|
|
| 6 |
A' |
1562 |
1479 |
24.65 |
|
|
|
| 7 |
A' |
1517 |
1436 |
21.94 |
|
|
|
| 8 |
A' |
1495 |
1415 |
10.25 |
|
|
|
| 9 |
A' |
1420 |
1344 |
16.28 |
|
|
|
| 10 |
A' |
1320 |
1250 |
105.19 |
|
|
|
| 11 |
A' |
1195 |
1132 |
30.14 |
|
|
|
| 12 |
A' |
1032 |
977 |
45.84 |
|
|
|
| 13 |
A' |
624 |
591 |
16.58 |
|
|
|
| 14 |
A' |
357 |
338 |
8.54 |
|
|
|
| 15 |
A" |
3143 |
2976 |
26.63 |
|
|
|
| 16 |
A" |
1513 |
1433 |
6.00 |
|
|
|
| 17 |
A" |
1160 |
1099 |
0.68 |
|
|
|
| 18 |
A" |
1061 |
1005 |
0.00 |
|
|
|
| 19 |
A" |
604 |
572 |
146.00 |
|
|
|
| 20 |
A" |
192 |
182 |
1.99 |
|
|
|
| 21 |
A" |
73 |
69 |
1.58 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16516.7 cm
-1
Scaled (by 0.947) Zero Point Vibrational Energy (zpe) 15641.4 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 M06-2X/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.284 |
-0.757 |
0.000 |
| O2 |
1.400 |
-1.228 |
0.000 |
| N3 |
0.000 |
0.571 |
0.000 |
| C4 |
-1.333 |
1.129 |
0.000 |
| H5 |
-0.633 |
-1.379 |
0.000 |
| H6 |
0.802 |
1.189 |
0.000 |
| H7 |
-2.052 |
0.306 |
0.000 |
| H8 |
-1.514 |
1.739 |
0.890 |
| H9 |
-1.514 |
1.739 |
-0.890 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.2110 | 1.3585 | 2.4845 | 1.1079 | 2.0135 | 2.5672 | 3.2031 | 3.2031 |
O2 | 1.2110 | | 2.2796 | 3.6087 | 2.0387 | 2.4894 | 3.7778 | 4.2531 | 4.2531 | N3 | 1.3585 | 2.2796 | | 1.4446 | 2.0499 | 1.0120 | 2.0692 | 2.1094 | 2.1094 | C4 | 2.4845 | 3.6087 | 1.4446 | | 2.6034 | 2.1352 | 1.0932 | 1.0945 | 1.0945 | H5 | 1.1079 | 2.0387 | 2.0499 | 2.6034 | | 2.9409 | 2.2029 | 3.3600 | 3.3600 | H6 | 2.0135 | 2.4894 | 1.0120 | 2.1352 | 2.9409 | | 2.9873 | 2.5416 | 2.5416 | H7 | 2.5672 | 3.7778 | 2.0692 | 1.0932 | 2.2029 | 2.9873 | | 1.7708 | 1.7708 | H8 | 3.2031 | 4.2531 | 2.1094 | 1.0945 | 3.3600 | 2.5416 | 1.7708 | | 1.7808 | H9 | 3.2031 | 4.2531 | 2.1094 | 1.0945 | 3.3600 | 2.5416 | 1.7708 | 1.7808 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
124.801 |
|
C1 |
N3 |
H6 |
115.515 |
| O2 |
C1 |
N3 |
124.945 |
|
O2 |
C1 |
H5 |
123.027 |
| N3 |
C1 |
H5 |
112.028 |
|
N3 |
C4 |
H7 |
108.453 |
| N3 |
C4 |
H8 |
111.611 |
|
N3 |
C4 |
H9 |
111.611 |
| C4 |
N3 |
H6 |
119.684 |
|
H7 |
C4 |
H8 |
108.082 |
| H7 |
C4 |
H9 |
108.082 |
|
H8 |
C4 |
H9 |
108.877 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.388 |
|
|
|
| 2 |
O |
-0.483 |
|
|
|
| 3 |
N |
-0.596 |
|
|
|
| 4 |
C |
-0.334 |
|
|
|
| 5 |
H |
0.116 |
|
|
|
| 6 |
H |
0.359 |
|
|
|
| 7 |
H |
0.184 |
|
|
|
| 8 |
H |
0.182 |
|
|
|
| 9 |
H |
0.182 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.962 |
2.723 |
0.000 |
4.023 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.044 |
3.963 |
0.000 |
| y |
3.963 |
-24.066 |
0.000 |
| z |
0.000 |
0.000 |
-24.617 |
|
| Traceless |
| | x | y | z |
| x |
-1.703 |
3.963 |
0.000 |
| y |
3.963 |
1.265 |
0.000 |
| z |
0.000 |
0.000 |
0.438 |
|
| Polar |
| 3z2-r2 | 0.875 |
| x2-y2 | -1.979 |
| xy | 3.963 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.367 |
-1.026 |
0.000 |
| y |
-1.026 |
5.437 |
0.000 |
| z |
0.000 |
0.000 |
2.957 |
<r2> (average value of r
2) Å
2
| <r2> |
88.696 |
| (<r2>)1/2 |
9.418 |
Jump to
S1C1
S1C3
Energy calculated at M06-2X/6-31G*
| | hartrees |
| Energy at 0K | -209.099525 |
| Energy at 298.15K | -209.105517 |
| HF Energy | -209.099525 |
| Nuclear repulsion energy | 119.382412 |
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 M06-2X/6-31G*
Geometric Data calculated at M06-2X/6-31G*
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
Energy calculated at M06-2X/6-31G*
| | hartrees |
| Energy at 0K | -209.101467 |
| Energy at 298.15K | -209.107528 |
| HF Energy | -209.101467 |
| Nuclear repulsion energy | 121.666805 |
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 M06-2X/6-31G*
| 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 |
3677 |
3482 |
35.12 |
|
|
|
| 2 |
A |
3207 |
3037 |
0.33 |
|
|
|
| 3 |
A |
3154 |
2987 |
28.10 |
|
|
|
| 4 |
A |
3091 |
2927 |
37.49 |
|
|
|
| 5 |
A |
3039 |
2877 |
107.66 |
|
|
|
| 6 |
A |
1860 |
1762 |
347.90 |
|
|
|
| 7 |
A |
1588 |
1504 |
116.54 |
|
|
|
| 8 |
A |
1535 |
1454 |
7.90 |
|
|
|
| 9 |
A |
1526 |
1445 |
49.12 |
|
|
|
| 10 |
A |
1470 |
1392 |
18.50 |
|
|
|
| 11 |
A |
1443 |
1367 |
3.02 |
|
|
|
| 12 |
A |
1250 |
1184 |
80.24 |
|
|
|
| 13 |
A |
1179 |
1116 |
20.35 |
|
|
|
| 14 |
A |
1168 |
1106 |
0.85 |
|
|
|
| 15 |
A |
1041 |
986 |
1.21 |
|
|
|
| 16 |
A |
997 |
944 |
22.11 |
|
|
|
| 17 |
A |
784 |
742 |
1.12 |
|
|
|
| 18 |
A |
550 |
521 |
57.67 |
|
|
|
| 19 |
A |
319 |
303 |
13.70 |
|
|
|
| 20 |
A |
271 |
257 |
85.81 |
|
|
|
| 21 |
A |
60 |
57 |
0.02 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16604.3 cm
-1
Scaled (by 0.947) Zero Point Vibrational Energy (zpe) 15724.3 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 M06-2X/6-31G*
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.862 |
0.436 |
0.003 |
| O2 |
1.356 |
-0.674 |
0.000 |
| N3 |
-0.471 |
0.664 |
-0.021 |
| C4 |
-1.407 |
-0.444 |
0.005 |
| H5 |
1.463 |
1.361 |
0.019 |
| H6 |
-0.806 |
1.612 |
0.060 |
| H7 |
-2.409 |
-0.069 |
-0.208 |
| H8 |
-1.122 |
-1.173 |
-0.756 |
| H9 |
-1.404 |
-0.944 |
0.979 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.2150 | 1.3524 | 2.4335 | 1.1036 | 2.0415 | 3.3163 | 2.6645 | 2.8267 |
O2 | 1.2150 | | 2.2648 | 2.7730 | 2.0379 | 3.1470 | 3.8191 | 2.6383 | 2.9411 | N3 | 1.3524 | 2.2648 | | 1.4505 | 2.0567 | 1.0085 | 2.0804 | 2.0830 | 2.1105 | C4 | 2.4335 | 2.7730 | 1.4505 | | 3.3909 | 2.1421 | 1.0906 | 1.0921 | 1.0947 | H5 | 1.1036 | 2.0379 | 2.0567 | 3.3909 | | 2.2839 | 4.1343 | 3.7020 | 3.8024 | H6 | 2.0415 | 3.1470 | 1.0085 | 2.1421 | 2.2839 | | 2.3378 | 2.9190 | 2.7807 | H7 | 3.3163 | 3.8191 | 2.0804 | 1.0906 | 4.1343 | 2.3378 | | 1.7822 | 1.7843 | H8 | 2.6645 | 2.6383 | 2.0830 | 1.0921 | 3.7020 | 2.9190 | 1.7822 | | 1.7724 | H9 | 2.8267 | 2.9411 | 2.1105 | 1.0947 | 3.8024 | 2.7807 | 1.7843 | 1.7724 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
120.465 |
|
C1 |
N3 |
H6 |
118.985 |
| O2 |
C1 |
N3 |
123.707 |
|
O2 |
C1 |
H5 |
122.947 |
| N3 |
C1 |
H5 |
113.344 |
|
N3 |
C4 |
H7 |
109.088 |
| N3 |
C4 |
H8 |
109.210 |
|
N3 |
C4 |
H9 |
111.275 |
| C4 |
N3 |
H6 |
120.113 |
|
H7 |
C4 |
H8 |
109.473 |
| H7 |
C4 |
H9 |
109.478 |
|
H8 |
C4 |
H9 |
108.294 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.380 |
|
|
|
| 2 |
O |
-0.481 |
|
|
|
| 3 |
N |
-0.607 |
|
|
|
| 4 |
C |
-0.343 |
|
|
|
| 5 |
H |
0.125 |
|
|
|
| 6 |
H |
0.350 |
|
|
|
| 7 |
H |
0.175 |
|
|
|
| 8 |
H |
0.224 |
|
|
|
| 9 |
H |
0.175 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.810 |
2.589 |
0.000 |
3.821 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.230 |
2.550 |
-0.000 |
| y |
2.550 |
-21.761 |
0.000 |
| z |
-0.000 |
0.000 |
-24.642 |
|
| Traceless |
| | x | y | z |
| x |
-2.029 |
2.550 |
-0.000 |
| y |
2.550 |
3.175 |
0.000 |
| z |
-0.000 |
0.000 |
-1.146 |
|
| Polar |
| 3z2-r2 | -2.292 |
| x2-y2 | -3.469 |
| xy | 2.550 |
| xz | -0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.785 |
-0.136 |
0.000 |
| y |
-0.136 |
4.759 |
0.000 |
| z |
0.000 |
0.000 |
2.952 |
<r2> (average value of r
2) Å
2
| <r2> |
77.875 |
| (<r2>)1/2 |
8.825 |