Jump to
S1C2
Energy calculated at TPSSh/6-31+G**
| | hartrees |
| Energy at 0K | -209.158387 |
| Energy at 298.15K | -209.164361 |
| HF Energy | -209.158387 |
| Nuclear repulsion energy | 116.780281 |
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 TPSSh/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' |
3794 |
3651 |
82.95 |
|
|
|
| 2 |
A' |
3149 |
3031 |
16.25 |
|
|
|
| 3 |
A' |
3114 |
2997 |
14.19 |
|
|
|
| 4 |
A' |
3038 |
2924 |
23.45 |
|
|
|
| 5 |
A' |
1718 |
1654 |
0.65 |
|
|
|
| 6 |
A' |
1499 |
1443 |
10.40 |
|
|
|
| 7 |
A' |
1440 |
1386 |
2.84 |
|
|
|
| 8 |
A' |
1403 |
1351 |
19.58 |
|
|
|
| 9 |
A' |
1280 |
1232 |
56.32 |
|
|
|
| 10 |
A' |
1151 |
1108 |
3.45 |
|
|
|
| 11 |
A' |
997 |
960 |
136.73 |
|
|
|
| 12 |
A' |
899 |
865 |
32.42 |
|
|
|
| 13 |
A' |
555 |
535 |
15.49 |
|
|
|
| 14 |
A' |
315 |
303 |
2.88 |
|
|
|
| 15 |
A" |
3093 |
2977 |
17.06 |
|
|
|
| 16 |
A" |
1497 |
1441 |
9.60 |
|
|
|
| 17 |
A" |
1077 |
1036 |
1.85 |
|
|
|
| 18 |
A" |
908 |
874 |
10.84 |
|
|
|
| 19 |
A" |
407 |
391 |
149.52 |
|
|
|
| 20 |
A" |
282 |
271 |
0.87 |
|
|
|
| 21 |
A" |
199 |
192 |
0.21 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15906.4 cm
-1
Scaled (by 0.9625) Zero Point Vibrational Energy (zpe) 15309.9 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 TPSSh/6-31+G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-1.304 |
1.311 |
0.000 |
| C2 |
0.000 |
0.572 |
0.000 |
| N3 |
0.015 |
-0.706 |
0.000 |
| O4 |
1.313 |
-1.229 |
0.000 |
| H5 |
1.175 |
-2.186 |
0.000 |
| H6 |
-2.140 |
0.608 |
0.000 |
| H7 |
-1.379 |
1.956 |
0.883 |
| H8 |
-1.379 |
1.956 |
-0.883 |
| H9 |
0.936 |
1.139 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4987 | 2.4095 | 3.6469 | 4.2865 | 1.0922 | 1.0961 | 1.0961 | 2.2470 |
C2 | 1.4987 | | 1.2778 | 2.2290 | 2.9981 | 2.1406 | 2.1438 | 2.1438 | 1.0947 | N3 | 2.4095 | 1.2778 | | 1.3997 | 1.8808 | 2.5242 | 3.1315 | 3.1315 | 2.0620 | O4 | 3.6469 | 2.2290 | 1.3997 | | 0.9674 | 3.9117 | 4.2627 | 4.2627 | 2.3979 | H5 | 4.2865 | 2.9981 | 1.8808 | 0.9674 | | 4.3357 | 4.9456 | 4.9456 | 3.3340 | H6 | 1.0922 | 2.1406 | 2.5242 | 3.9117 | 4.3357 | | 1.7822 | 1.7822 | 3.1222 | H7 | 1.0961 | 2.1438 | 3.1315 | 4.2627 | 4.9456 | 1.7822 | | 1.7658 | 2.6090 | H8 | 1.0961 | 2.1438 | 3.1315 | 4.2627 | 4.9456 | 1.7822 | 1.7658 | | 2.6090 | H9 | 2.2470 | 1.0947 | 2.0620 | 2.3979 | 3.3340 | 3.1222 | 2.6090 | 2.6090 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
120.203 |
|
C1 |
C2 |
H9 |
119.274 |
| C2 |
C1 |
H6 |
110.437 |
|
C2 |
C1 |
H7 |
110.453 |
| C2 |
C1 |
H8 |
110.453 |
|
C2 |
N3 |
O4 |
112.631 |
| N3 |
C2 |
H9 |
120.522 |
|
N3 |
O4 |
H5 |
103.723 |
| H6 |
C1 |
H7 |
109.058 |
|
H6 |
C1 |
H8 |
109.058 |
| H7 |
C1 |
H8 |
107.309 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at TPSSh/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.520 |
|
|
|
| 2 |
C |
-0.040 |
|
|
|
| 3 |
N |
-0.188 |
|
|
|
| 4 |
O |
-0.297 |
|
|
|
| 5 |
H |
0.359 |
|
|
|
| 6 |
H |
0.184 |
|
|
|
| 7 |
H |
0.171 |
|
|
|
| 8 |
H |
0.171 |
|
|
|
| 9 |
H |
0.159 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.465 |
0.705 |
0.000 |
0.845 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.006 |
-1.431 |
0.000 |
| y |
-1.431 |
7.448 |
0.000 |
| z |
0.000 |
0.000 |
4.009 |
<r2> (average value of r
2) Å
2
| <r2> |
92.469 |
| (<r2>)1/2 |
9.616 |
Jump to
S1C1
Energy calculated at TPSSh/6-31+G**
| | hartrees |
| Energy at 0K | -209.158080 |
| Energy at 298.15K | |
| HF Energy | -209.158080 |
| Nuclear repulsion energy | 119.314280 |
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 TPSSh/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' |
3800 |
3657 |
84.00 |
|
|
|
| 2 |
A' |
3182 |
3062 |
13.75 |
|
|
|
| 3 |
A' |
3168 |
3049 |
1.67 |
|
|
|
| 4 |
A' |
3043 |
2929 |
16.72 |
|
|
|
| 5 |
A' |
1725 |
1660 |
10.77 |
|
|
|
| 6 |
A' |
1495 |
1439 |
13.83 |
|
|
|
| 7 |
A' |
1414 |
1361 |
11.54 |
|
|
|
| 8 |
A' |
1366 |
1314 |
19.21 |
|
|
|
| 9 |
A' |
1337 |
1287 |
61.94 |
|
|
|
| 10 |
A' |
1144 |
1102 |
9.32 |
|
|
|
| 11 |
A' |
924 |
889 |
80.71 |
|
|
|
| 12 |
A' |
904 |
870 |
71.97 |
|
|
|
| 13 |
A' |
669 |
644 |
12.53 |
|
|
|
| 14 |
A' |
305 |
293 |
1.46 |
|
|
|
| 15 |
A" |
3097 |
2981 |
14.27 |
|
|
|
| 16 |
A" |
1504 |
1447 |
10.14 |
|
|
|
| 17 |
A" |
1061 |
1021 |
1.28 |
|
|
|
| 18 |
A" |
861 |
829 |
16.97 |
|
|
|
| 19 |
A" |
498 |
479 |
46.52 |
|
|
|
| 20 |
A" |
393 |
379 |
90.48 |
|
|
|
| 21 |
A" |
40i |
39i |
0.07 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15924.0 cm
-1
Scaled (by 0.9625) Zero Point Vibrational Energy (zpe) 15326.8 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 TPSSh/6-31+G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-1.450 |
0.488 |
0.000 |
| C2 |
0.000 |
0.866 |
0.000 |
| N3 |
1.023 |
0.092 |
0.000 |
| O4 |
0.653 |
-1.275 |
0.000 |
| H5 |
1.516 |
-1.716 |
0.000 |
| H6 |
-1.579 |
-0.594 |
0.000 |
| H7 |
-1.946 |
0.910 |
0.882 |
| H8 |
-1.946 |
0.910 |
-0.882 |
| H9 |
0.273 |
1.920 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4990 | 2.5049 | 2.7442 | 3.6951 | 1.0897 | 1.0963 | 1.0963 | 2.2412 |
C2 | 1.4990 | | 1.2830 | 2.2381 | 2.9939 | 2.1505 | 2.1373 | 2.1373 | 1.0888 | N3 | 2.5049 | 1.2830 | | 1.4156 | 1.8736 | 2.6904 | 3.2038 | 3.2038 | 1.9759 | O4 | 2.7442 | 2.2381 | 1.4156 | | 0.9688 | 2.3329 | 3.5083 | 3.5083 | 3.2170 | H5 | 3.6951 | 2.9939 | 1.8736 | 0.9688 | | 3.2910 | 4.4339 | 4.4339 | 3.8422 | H6 | 1.0897 | 2.1505 | 2.6904 | 2.3329 | 3.2910 | | 1.7823 | 1.7823 | 3.1227 | H7 | 1.0963 | 2.1373 | 3.2038 | 3.5083 | 4.4339 | 1.7823 | | 1.7635 | 2.5933 | H8 | 1.0963 | 2.1373 | 3.2038 | 3.5083 | 4.4339 | 1.7823 | 1.7635 | | 2.5933 | H9 | 2.2412 | 1.0888 | 1.9759 | 3.2170 | 3.8422 | 3.1227 | 2.5933 | 2.5933 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
128.260 |
|
C1 |
C2 |
H9 |
119.162 |
| C2 |
C1 |
H6 |
111.365 |
|
C2 |
C1 |
H7 |
109.909 |
| C2 |
C1 |
H8 |
109.909 |
|
C2 |
N3 |
O4 |
111.975 |
| N3 |
C2 |
H9 |
112.578 |
|
N3 |
O4 |
H5 |
101.953 |
| H6 |
C1 |
H7 |
109.235 |
|
H6 |
C1 |
H8 |
109.235 |
| H7 |
C1 |
H8 |
107.086 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at TPSSh/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.540 |
|
|
|
| 2 |
C |
-0.025 |
|
|
|
| 3 |
N |
-0.204 |
|
|
|
| 4 |
O |
-0.308 |
|
|
|
| 5 |
H |
0.370 |
|
|
|
| 6 |
H |
0.198 |
|
|
|
| 7 |
H |
0.173 |
|
|
|
| 8 |
H |
0.173 |
|
|
|
| 9 |
H |
0.163 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.788 |
0.300 |
0.000 |
0.843 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.465 |
-1.206 |
0.000 |
| y |
-1.206 |
6.532 |
0.000 |
| z |
0.000 |
0.000 |
4.014 |
<r2> (average value of r
2) Å
2
| <r2> |
79.589 |
| (<r2>)1/2 |
8.921 |