Jump to
S1C2
Energy calculated at wB97X-D/6-31+G**
| | hartrees |
| Energy at 0K | -209.082409 |
| Energy at 298.15K | -209.088397 |
| HF Energy | -209.082409 |
| Nuclear repulsion energy | 117.484905 |
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/6-31+G**
| 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' |
3913 |
3726 |
105.44 |
|
|
|
| 2 |
A' |
3179 |
3028 |
12.34 |
|
|
|
| 3 |
A' |
3146 |
2996 |
11.83 |
|
|
|
| 4 |
A' |
3063 |
2917 |
19.01 |
|
|
|
| 5 |
A' |
1778 |
1694 |
1.22 |
|
|
|
| 6 |
A' |
1486 |
1415 |
13.56 |
|
|
|
| 7 |
A' |
1457 |
1387 |
5.42 |
|
|
|
| 8 |
A' |
1410 |
1343 |
29.76 |
|
|
|
| 9 |
A' |
1303 |
1241 |
54.98 |
|
|
|
| 10 |
A' |
1161 |
1106 |
3.95 |
|
|
|
| 11 |
A' |
1053 |
1003 |
163.59 |
|
|
|
| 12 |
A' |
929 |
885 |
5.82 |
|
|
|
| 13 |
A' |
577 |
549 |
14.44 |
|
|
|
| 14 |
A' |
330 |
314 |
2.88 |
|
|
|
| 15 |
A" |
3130 |
2981 |
13.03 |
|
|
|
| 16 |
A" |
1491 |
1419 |
12.28 |
|
|
|
| 17 |
A" |
1088 |
1036 |
1.50 |
|
|
|
| 18 |
A" |
920 |
876 |
11.85 |
|
|
|
| 19 |
A" |
402 |
383 |
158.19 |
|
|
|
| 20 |
A" |
293 |
279 |
1.07 |
|
|
|
| 21 |
A" |
166 |
158 |
0.27 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16136.5 cm
-1
Scaled (by 0.9523) Zero Point Vibrational Energy (zpe) 15366.8 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/6-31+G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-1.299 |
1.306 |
0.000 |
| C2 |
0.000 |
0.565 |
0.000 |
| N3 |
0.016 |
-0.706 |
0.000 |
| O4 |
1.306 |
-1.218 |
0.000 |
| H5 |
1.177 |
-2.171 |
0.000 |
| H6 |
-2.137 |
0.605 |
0.000 |
| H7 |
-1.370 |
1.950 |
0.883 |
| H8 |
-1.370 |
1.950 |
-0.883 |
| H9 |
0.938 |
1.128 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4952 | 2.4030 | 3.6272 | 4.2686 | 1.0919 | 1.0950 | 1.0950 | 2.2445 |
C2 | 1.4952 | | 1.2712 | 2.2107 | 2.9790 | 2.1371 | 2.1386 | 2.1386 | 1.0940 | N3 | 2.4030 | 1.2712 | | 1.3885 | 1.8701 | 2.5202 | 3.1227 | 3.1227 | 2.0526 | O4 | 3.6272 | 2.2107 | 1.3885 | | 0.9614 | 3.8959 | 4.2401 | 4.2401 | 2.3747 | H5 | 4.2686 | 2.9790 | 1.8701 | 0.9614 | | 4.3235 | 4.9245 | 4.9245 | 3.3075 | H6 | 1.0919 | 2.1371 | 2.5202 | 3.8959 | 4.3235 | | 1.7815 | 1.7815 | 3.1192 | H7 | 1.0950 | 2.1386 | 3.1227 | 4.2401 | 4.9245 | 1.7815 | | 1.7655 | 2.6048 | H8 | 1.0950 | 2.1386 | 3.1227 | 4.2401 | 4.9245 | 1.7815 | 1.7655 | | 2.6048 | H9 | 2.2445 | 1.0940 | 2.0526 | 2.3747 | 3.3075 | 3.1192 | 2.6048 | 2.6048 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
120.380 |
|
C1 |
C2 |
H9 |
119.385 |
| C2 |
C1 |
H6 |
110.421 |
|
C2 |
C1 |
H7 |
110.353 |
| C2 |
C1 |
H8 |
110.353 |
|
C2 |
N3 |
O4 |
112.364 |
| N3 |
C2 |
H9 |
120.234 |
|
N3 |
O4 |
H5 |
103.982 |
| H6 |
C1 |
H7 |
109.097 |
|
H6 |
C1 |
H8 |
109.097 |
| H7 |
C1 |
H8 |
107.454 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.531 |
|
|
|
| 2 |
C |
-0.006 |
|
|
|
| 3 |
N |
-0.205 |
|
|
|
| 4 |
O |
-0.325 |
|
|
|
| 5 |
H |
0.367 |
|
|
|
| 6 |
H |
0.188 |
|
|
|
| 7 |
H |
0.174 |
|
|
|
| 8 |
H |
0.174 |
|
|
|
| 9 |
H |
0.162 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.432 |
0.713 |
0.000 |
0.834 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.672 |
-2.247 |
0.000 |
| y |
-2.247 |
-18.582 |
0.000 |
| z |
0.000 |
0.000 |
-25.462 |
|
| Traceless |
| | x | y | z |
| x |
-3.650 |
-2.247 |
0.000 |
| y |
-2.247 |
6.985 |
0.000 |
| z |
0.000 |
0.000 |
-3.335 |
|
| Polar |
| 3z2-r2 | -6.670 |
| x2-y2 | -7.090 |
| xy | -2.247 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.730 |
-1.281 |
0.000 |
| y |
-1.281 |
7.216 |
0.000 |
| z |
0.000 |
0.000 |
3.978 |
<r2> (average value of r
2) Å
2
| <r2> |
91.641 |
| (<r2>)1/2 |
9.573 |
Jump to
S1C1
Energy calculated at wB97X-D/6-31+G**
| | hartrees |
| Energy at 0K | -209.082095 |
| Energy at 298.15K | |
| HF Energy | -209.082095 |
| Nuclear repulsion energy | 120.016841 |
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/6-31+G**
| 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' |
3920 |
3733 |
107.77 |
|
|
|
| 2 |
A' |
3208 |
3055 |
8.29 |
|
|
|
| 3 |
A' |
3193 |
3040 |
4.16 |
|
|
|
| 4 |
A' |
3073 |
2927 |
14.00 |
|
|
|
| 5 |
A' |
1782 |
1697 |
11.24 |
|
|
|
| 6 |
A' |
1493 |
1422 |
17.59 |
|
|
|
| 7 |
A' |
1426 |
1358 |
17.76 |
|
|
|
| 8 |
A' |
1387 |
1320 |
38.91 |
|
|
|
| 9 |
A' |
1354 |
1290 |
47.55 |
|
|
|
| 10 |
A' |
1157 |
1102 |
9.62 |
|
|
|
| 11 |
A' |
982 |
935 |
151.59 |
|
|
|
| 12 |
A' |
931 |
886 |
1.03 |
|
|
|
| 13 |
A' |
690 |
657 |
12.17 |
|
|
|
| 14 |
A' |
315 |
300 |
1.63 |
|
|
|
| 15 |
A" |
3139 |
2989 |
11.33 |
|
|
|
| 16 |
A" |
1492 |
1421 |
12.95 |
|
|
|
| 17 |
A" |
1073 |
1022 |
0.52 |
|
|
|
| 18 |
A" |
868 |
826 |
15.54 |
|
|
|
| 19 |
A" |
505 |
481 |
36.83 |
|
|
|
| 20 |
A" |
392 |
374 |
110.02 |
|
|
|
| 21 |
A" |
85i |
81i |
0.05 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16146.3 cm
-1
Scaled (by 0.9523) Zero Point Vibrational Energy (zpe) 15376.1 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/6-31+G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-1.448 |
0.483 |
0.000 |
| C2 |
0.000 |
0.860 |
0.000 |
| N3 |
1.014 |
0.087 |
0.000 |
| O4 |
0.659 |
-1.261 |
0.000 |
| H5 |
1.511 |
-1.707 |
0.000 |
| H6 |
-1.583 |
-0.598 |
0.000 |
| H7 |
-1.940 |
0.907 |
0.881 |
| H8 |
-1.940 |
0.907 |
-0.881 |
| H9 |
0.269 |
1.914 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4963 | 2.4940 | 2.7353 | 3.6812 | 1.0892 | 1.0949 | 1.0949 | 2.2353 |
C2 | 1.4963 | | 1.2752 | 2.2213 | 2.9784 | 2.1520 | 2.1315 | 2.1315 | 1.0879 | N3 | 2.4940 | 1.2752 | | 1.3945 | 1.8613 | 2.6861 | 3.1902 | 3.1902 | 1.9731 | O4 | 2.7353 | 2.2213 | 1.3945 | | 0.9616 | 2.3380 | 3.4976 | 3.4976 | 3.1993 | H5 | 3.6812 | 2.9784 | 1.8613 | 0.9616 | | 3.2868 | 4.4180 | 4.4180 | 3.8278 | H6 | 1.0892 | 2.1520 | 2.6861 | 2.3380 | 3.2868 | | 1.7802 | 1.7802 | 3.1209 | H7 | 1.0949 | 2.1315 | 3.1902 | 3.4976 | 4.4180 | 1.7802 | | 1.7630 | 2.5830 | H8 | 1.0949 | 2.1315 | 3.1902 | 3.4976 | 4.4180 | 1.7802 | 1.7630 | | 2.5830 | H9 | 2.2353 | 1.0879 | 1.9731 | 3.1993 | 3.8278 | 3.1209 | 2.5830 | 2.5830 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
128.102 |
|
C1 |
C2 |
H9 |
118.913 |
| C2 |
C1 |
H6 |
111.709 |
|
C2 |
C1 |
H7 |
109.715 |
| C2 |
C1 |
H8 |
109.715 |
|
C2 |
N3 |
O4 |
112.541 |
| N3 |
C2 |
H9 |
112.985 |
|
N3 |
O4 |
H5 |
102.816 |
| H6 |
C1 |
H7 |
109.180 |
|
H6 |
C1 |
H8 |
109.180 |
| H7 |
C1 |
H8 |
107.233 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.550 |
|
|
|
| 2 |
C |
0.003 |
|
|
|
| 3 |
N |
-0.219 |
|
|
|
| 4 |
O |
-0.332 |
|
|
|
| 5 |
H |
0.378 |
|
|
|
| 6 |
H |
0.202 |
|
|
|
| 7 |
H |
0.176 |
|
|
|
| 8 |
H |
0.176 |
|
|
|
| 9 |
H |
0.166 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.800 |
0.291 |
0.000 |
0.851 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.151 |
-4.149 |
0.000 |
| y |
-4.149 |
-21.212 |
0.000 |
| z |
0.000 |
0.000 |
-25.494 |
|
| Traceless |
| | x | y | z |
| x |
0.202 |
-4.149 |
0.000 |
| y |
-4.149 |
3.110 |
0.000 |
| z |
0.000 |
0.000 |
-3.312 |
|
| Polar |
| 3z2-r2 | -6.625 |
| x2-y2 | -1.939 |
| xy | -4.149 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.263 |
-1.178 |
0.000 |
| y |
-1.178 |
6.317 |
0.000 |
| z |
0.000 |
0.000 |
3.985 |
<r2> (average value of r
2) Å
2
| <r2> |
78.940 |
| (<r2>)1/2 |
8.885 |