Jump to
S1C2
Energy calculated at wB97X-D/6-31G*
| | hartrees |
| Energy at 0K | -151.155622 |
| Energy at 298.15K | -151.163670 |
| HF Energy | -151.155622 |
| Nuclear repulsion energy | |
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/6-31G*
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
3519 |
3338 |
1.78 |
|
|
|
| 2 |
A1 |
3096 |
2936 |
43.94 |
|
|
|
| 3 |
A1 |
1714 |
1626 |
47.82 |
|
|
|
| 4 |
A1 |
1517 |
1439 |
0.64 |
|
|
|
| 5 |
A1 |
1133 |
1074 |
39.89 |
|
|
|
| 6 |
A1 |
897 |
851 |
1.10 |
|
|
|
| 7 |
A1 |
467 |
443 |
6.36 |
|
|
|
| 8 |
A2 |
3613 |
3427 |
0.00 |
|
|
|
| 9 |
A2 |
1428 |
1354 |
0.00 |
|
|
|
| 10 |
A2 |
1098 |
1042 |
0.00 |
|
|
|
| 11 |
A2 |
271 |
257 |
0.00 |
|
|
|
| 12 |
B1 |
3611 |
3425 |
0.30 |
|
|
|
| 13 |
B1 |
3146 |
2984 |
31.32 |
|
|
|
| 14 |
B1 |
1396 |
1324 |
0.35 |
|
|
|
| 15 |
B1 |
864 |
819 |
0.52 |
|
|
|
| 16 |
B1 |
411 |
390 |
112.18 |
|
|
|
| 17 |
B2 |
3521 |
3339 |
0.34 |
|
|
|
| 18 |
B2 |
1705 |
1617 |
3.29 |
|
|
|
| 19 |
B2 |
1426 |
1353 |
22.45 |
|
|
|
| 20 |
B2 |
1120 |
1063 |
75.52 |
|
|
|
| 21 |
B2 |
817 |
775 |
455.34 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 18383.9 cm
-1
Scaled (by 0.9485) Zero Point Vibrational Energy (zpe) 17437.2 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/6-31G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.537 |
| N2 |
0.000 |
1.283 |
-0.179 |
| N3 |
0.000 |
-1.283 |
-0.179 |
| H4 |
0.882 |
0.000 |
1.182 |
| H5 |
-0.882 |
0.000 |
1.182 |
| H6 |
0.820 |
1.362 |
-0.771 |
| H7 |
-0.820 |
1.362 |
-0.771 |
| H8 |
-0.820 |
-1.362 |
-0.771 |
| H9 |
0.820 |
-1.362 |
-0.771 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
N3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4697 | 1.4697 | 1.0926 | 1.0926 | 2.0588 | 2.0588 | 2.0588 | 2.0588 |
N2 | 1.4697 | | 2.5666 | 2.0680 | 2.0680 | 1.0141 | 1.0141 | 2.8321 | 2.8321 | N3 | 1.4697 | 2.5666 | | 2.0680 | 2.0680 | 2.8321 | 2.8321 | 1.0141 | 1.0141 | H4 | 1.0926 | 2.0680 | 2.0680 | | 1.7650 | 2.3815 | 2.9265 | 2.9265 | 2.3815 | H5 | 1.0926 | 2.0680 | 2.0680 | 1.7650 | | 2.9265 | 2.3815 | 2.3815 | 2.9265 | H6 | 2.0588 | 1.0141 | 2.8321 | 2.3815 | 2.9265 | | 1.6392 | 3.1795 | 2.7244 | H7 | 2.0588 | 1.0141 | 2.8321 | 2.9265 | 2.3815 | 1.6392 | | 2.7244 | 3.1795 | H8 | 2.0588 | 2.8321 | 1.0141 | 2.9265 | 2.3815 | 3.1795 | 2.7244 | | 1.6392 | H9 | 2.0588 | 2.8321 | 1.0141 | 2.3815 | 2.9265 | 2.7244 | 3.1795 | 1.6392 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H6 |
110.635 |
|
C1 |
N2 |
H7 |
110.635 |
| C1 |
N3 |
H8 |
110.635 |
|
C1 |
N3 |
H9 |
110.635 |
| N2 |
C1 |
N3 |
121.661 |
|
N2 |
C1 |
H4 |
106.701 |
| N2 |
C1 |
H5 |
106.701 |
|
N3 |
C1 |
H4 |
106.701 |
| N3 |
C1 |
H5 |
106.701 |
|
H4 |
C1 |
H5 |
107.742 |
| H6 |
N2 |
H7 |
107.851 |
|
H8 |
N3 |
H9 |
107.851 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.100 |
|
|
|
| 2 |
N |
-0.731 |
|
|
|
| 3 |
N |
-0.731 |
|
|
|
| 4 |
H |
0.176 |
|
|
|
| 5 |
H |
0.176 |
|
|
|
| 6 |
H |
0.302 |
|
|
|
| 7 |
H |
0.302 |
|
|
|
| 8 |
H |
0.302 |
|
|
|
| 9 |
H |
0.302 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
-2.123 |
2.123 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.511 |
0.000 |
0.000 |
| y |
0.000 |
-26.141 |
0.000 |
| z |
0.000 |
0.000 |
-17.654 |
|
| Traceless |
| | x | y | z |
| x |
5.387 |
0.000 |
0.000 |
| y |
0.000 |
-9.059 |
0.000 |
| z |
0.000 |
0.000 |
3.672 |
|
| Polar |
| 3z2-r2 | 7.344 |
| x2-y2 | 9.630 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.882 |
0.000 |
0.000 |
| y |
0.000 |
3.762 |
0.000 |
| z |
0.000 |
0.000 |
3.608 |
<r2> (average value of r
2) Å
2
| <r2> |
53.519 |
| (<r2>)1/2 |
7.316 |
Jump to
S1C1
Energy calculated at wB97X-D/6-31G*
| | hartrees |
| Energy at 0K | -151.153082 |
| Energy at 298.15K | -151.161145 |
| HF Energy | -151.153082 |
| Nuclear repulsion energy | |
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/6-31G*
| 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 |
3632 |
3445 |
0.21 |
|
|
|
| 2 |
A |
3534 |
3352 |
0.01 |
|
|
|
| 3 |
A |
2975 |
2822 |
113.13 |
|
|
|
| 4 |
A |
1692 |
1605 |
0.92 |
|
|
|
| 5 |
A |
1567 |
1486 |
2.97 |
|
|
|
| 6 |
A |
1392 |
1321 |
2.44 |
|
|
|
| 7 |
A |
1248 |
1184 |
6.70 |
|
|
|
| 8 |
A |
1006 |
954 |
9.34 |
|
|
|
| 9 |
A |
906 |
859 |
187.79 |
|
|
|
| 10 |
A |
496 |
470 |
0.00 |
|
|
|
| 11 |
A |
322 |
305 |
31.23 |
|
|
|
| 12 |
B |
3633 |
3446 |
0.52 |
|
|
|
| 13 |
B |
3535 |
3353 |
1.38 |
|
|
|
| 14 |
B |
2997 |
2843 |
111.20 |
|
|
|
| 15 |
B |
1690 |
1603 |
85.55 |
|
|
|
| 16 |
B |
1491 |
1414 |
34.65 |
|
|
|
| 17 |
B |
1278 |
1212 |
18.58 |
|
|
|
| 18 |
B |
1174 |
1114 |
19.44 |
|
|
|
| 19 |
B |
1011 |
959 |
30.35 |
|
|
|
| 20 |
B |
869 |
824 |
153.70 |
|
|
|
| 21 |
B |
300 |
285 |
89.17 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 18373.4 cm
-1
Scaled (by 0.9485) Zero Point Vibrational Energy (zpe) 17427.2 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/6-31G*
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.545 |
| N2 |
0.000 |
1.170 |
-0.314 |
| N3 |
0.000 |
-1.170 |
-0.314 |
| H4 |
0.883 |
-0.084 |
1.203 |
| H5 |
-0.883 |
0.084 |
1.203 |
| H6 |
-0.021 |
2.025 |
0.234 |
| H7 |
0.845 |
1.171 |
-0.877 |
| H8 |
0.021 |
-2.025 |
0.234 |
| H9 |
-0.845 |
-1.171 |
-0.877 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
N3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4520 | 1.4520 | 1.1039 | 1.1039 | 2.0487 | 2.0269 | 2.0487 | 2.0269 |
N2 | 1.4520 | | 2.3409 | 2.1570 | 2.0640 | 1.0149 | 1.0158 | 3.2419 | 2.5520 | N3 | 1.4520 | 2.3409 | | 2.0640 | 2.1570 | 3.2419 | 2.5520 | 1.0149 | 1.0158 | H4 | 1.1039 | 2.1570 | 2.0640 | | 1.7739 | 2.4903 | 2.4290 | 2.3344 | 2.9143 | H5 | 1.1039 | 2.0640 | 2.1570 | 1.7739 | | 2.3344 | 2.9143 | 2.4903 | 2.4290 | H6 | 2.0487 | 1.0149 | 3.2419 | 2.4903 | 2.3344 | | 1.6471 | 4.0497 | 3.4821 | H7 | 2.0269 | 1.0158 | 2.5520 | 2.4290 | 2.9143 | 1.6471 | | 3.4821 | 2.8881 | H8 | 2.0487 | 3.2419 | 1.0149 | 2.3344 | 2.4903 | 4.0497 | 3.4821 | | 1.6471 | H9 | 2.0269 | 2.5520 | 1.0158 | 2.9143 | 2.4290 | 3.4821 | 2.8881 | 1.6471 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H6 |
111.056 |
|
C1 |
N2 |
H7 |
109.158 |
| C1 |
N3 |
H8 |
111.056 |
|
C1 |
N3 |
H9 |
109.158 |
| N2 |
C1 |
N3 |
107.435 |
|
N2 |
C1 |
H4 |
114.431 |
| N2 |
C1 |
H5 |
106.920 |
|
N3 |
C1 |
H4 |
106.920 |
| N3 |
C1 |
H5 |
114.431 |
|
H4 |
C1 |
H5 |
106.922 |
| H6 |
N2 |
H7 |
108.403 |
|
H8 |
N3 |
H9 |
108.403 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.039 |
|
|
|
| 2 |
N |
-0.749 |
|
|
|
| 3 |
N |
-0.749 |
|
|
|
| 4 |
H |
0.136 |
|
|
|
| 5 |
H |
0.136 |
|
|
|
| 6 |
H |
0.312 |
|
|
|
| 7 |
H |
0.321 |
|
|
|
| 8 |
H |
0.312 |
|
|
|
| 9 |
H |
0.321 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
1.530 |
1.530 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.551 |
3.303 |
0.000 |
| y |
3.303 |
-16.229 |
0.000 |
| z |
0.000 |
0.000 |
-20.181 |
|
| Traceless |
| | x | y | z |
| x |
-1.345 |
3.303 |
0.000 |
| y |
3.303 |
3.637 |
0.000 |
| z |
0.000 |
0.000 |
-2.291 |
|
| Polar |
| 3z2-r2 | -4.583 |
| x2-y2 | -3.321 |
| xy | 3.303 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.289 |
0.005 |
0.000 |
| y |
0.005 |
4.412 |
0.000 |
| z |
0.000 |
0.000 |
3.724 |
<r2> (average value of r
2) Å
2
| <r2> |
52.466 |
| (<r2>)1/2 |
7.243 |