Jump to
S1C2
S1C3
Energy calculated at HSEh1PBE/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -208.995599 |
| Energy at 298.15K | -209.001695 |
| HF Energy | -208.995599 |
| Nuclear repulsion energy | 119.724752 |
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 HSEh1PBE/6-31G(2df,p)
| 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' |
3655 |
3500 |
28.03 |
|
|
|
| 2 |
A' |
3144 |
3011 |
12.85 |
|
|
|
| 3 |
A' |
3041 |
2912 |
51.15 |
|
|
|
| 4 |
A' |
2936 |
2812 |
86.56 |
|
|
|
| 5 |
A' |
1856 |
1777 |
446.95 |
|
|
|
| 6 |
A' |
1536 |
1471 |
21.85 |
|
|
|
| 7 |
A' |
1491 |
1428 |
11.25 |
|
|
|
| 8 |
A' |
1465 |
1403 |
7.86 |
|
|
|
| 9 |
A' |
1402 |
1343 |
11.93 |
|
|
|
| 10 |
A' |
1316 |
1260 |
92.09 |
|
|
|
| 11 |
A' |
1184 |
1134 |
21.90 |
|
|
|
| 12 |
A' |
1022 |
978 |
43.40 |
|
|
|
| 13 |
A' |
621 |
594 |
14.89 |
|
|
|
| 14 |
A' |
345 |
330 |
8.25 |
|
|
|
| 15 |
A" |
3104 |
2972 |
26.34 |
|
|
|
| 16 |
A" |
1478 |
1416 |
5.48 |
|
|
|
| 17 |
A" |
1154 |
1105 |
0.22 |
|
|
|
| 18 |
A" |
1056 |
1012 |
0.15 |
|
|
|
| 19 |
A" |
625 |
598 |
108.19 |
|
|
|
| 20 |
A" |
211 |
202 |
0.80 |
|
|
|
| 21 |
A" |
112 |
107 |
0.44 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16376.1 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 15683.4 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 HSEh1PBE/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.284 |
-0.754 |
0.000 |
| O2 |
1.395 |
-1.226 |
0.000 |
| N3 |
0.000 |
0.570 |
0.000 |
| C4 |
-1.325 |
1.125 |
0.000 |
| H5 |
-0.641 |
-1.370 |
0.000 |
| H6 |
0.797 |
1.187 |
0.000 |
| H7 |
-2.049 |
0.304 |
0.000 |
| H8 |
-1.512 |
1.738 |
0.889 |
| H9 |
-1.512 |
1.738 |
-0.889 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.2072 | 1.3540 | 2.4738 | 1.1113 | 2.0080 | 2.5617 | 3.1977 | 3.1977 |
O2 | 1.2072 | | 2.2743 | 3.5955 | 2.0413 | 2.4866 | 3.7687 | 4.2458 | 4.2458 | N3 | 1.3540 | 2.2743 | | 1.4367 | 2.0426 | 1.0082 | 2.0657 | 2.1072 | 2.1072 | C4 | 2.4738 | 3.5955 | 1.4367 | | 2.5865 | 2.1231 | 1.0935 | 1.0959 | 1.0959 | H5 | 1.1113 | 2.0413 | 2.0426 | 2.5865 | | 2.9336 | 2.1873 | 3.3473 | 3.3473 | H6 | 2.0080 | 2.4866 | 1.0082 | 2.1231 | 2.9336 | | 2.9793 | 2.5346 | 2.5346 | H7 | 2.5617 | 3.7687 | 2.0657 | 1.0935 | 2.1873 | 2.9793 | | 1.7698 | 1.7698 | H8 | 3.1977 | 4.2458 | 2.1072 | 1.0959 | 3.3473 | 2.5346 | 1.7698 | | 1.7780 | H9 | 3.1977 | 4.2458 | 2.1072 | 1.0959 | 3.3473 | 2.5346 | 1.7698 | 1.7780 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
124.834 |
|
C1 |
N3 |
H6 |
115.660 |
| O2 |
C1 |
N3 |
125.140 |
|
O2 |
C1 |
H5 |
123.338 |
| N3 |
C1 |
H5 |
111.522 |
|
N3 |
C4 |
H7 |
108.692 |
| N3 |
C4 |
H8 |
111.914 |
|
N3 |
C4 |
H9 |
111.914 |
| C4 |
N3 |
H6 |
119.506 |
|
H7 |
C4 |
H8 |
107.866 |
| H7 |
C4 |
H9 |
107.866 |
|
H8 |
C4 |
H9 |
108.430 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.173 |
|
|
|
| 2 |
O |
-0.345 |
|
|
|
| 3 |
N |
-0.292 |
|
|
|
| 4 |
C |
-0.371 |
|
|
|
| 5 |
H |
0.085 |
|
|
|
| 6 |
H |
0.275 |
|
|
|
| 7 |
H |
0.164 |
|
|
|
| 8 |
H |
0.156 |
|
|
|
| 9 |
H |
0.156 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.807 |
2.705 |
0.000 |
3.899 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.860 |
3.853 |
0.000 |
| y |
3.853 |
-23.915 |
0.000 |
| z |
0.000 |
0.000 |
-24.279 |
|
| Traceless |
| | x | y | z |
| x |
-1.762 |
3.853 |
0.000 |
| y |
3.853 |
1.155 |
0.000 |
| z |
0.000 |
0.000 |
0.608 |
|
| Polar |
| 3z2-r2 | 1.216 |
| x2-y2 | -1.945 |
| xy | 3.853 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.635 |
-1.030 |
0.000 |
| y |
-1.030 |
5.739 |
0.000 |
| z |
0.000 |
0.000 |
3.346 |
<r2> (average value of r
2) Å
2
| <r2> |
88.128 |
| (<r2>)1/2 |
9.388 |
Jump to
S1C1
S1C3
Energy calculated at HSEh1PBE/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -208.995599 |
| Energy at 298.15K | -209.001695 |
| HF Energy | -208.995599 |
| Nuclear repulsion energy | 119.724752 |
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 HSEh1PBE/6-31G(2df,p)
Geometric Data calculated at HSEh1PBE/6-31G(2df,p)
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
Energy calculated at HSEh1PBE/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -208.997260 |
| Energy at 298.15K | -209.003371 |
| HF Energy | -208.997260 |
| Nuclear repulsion energy | 121.958274 |
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 HSEh1PBE/6-31G(2df,p)
| 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 |
3691 |
3534 |
28.00 |
|
|
|
| 2 |
A |
3177 |
3043 |
0.41 |
|
|
|
| 3 |
A |
3114 |
2983 |
25.82 |
|
|
|
| 4 |
A |
3050 |
2921 |
42.91 |
|
|
|
| 5 |
A |
2960 |
2835 |
109.46 |
|
|
|
| 6 |
A |
1841 |
1763 |
307.96 |
|
|
|
| 7 |
A |
1566 |
1500 |
95.00 |
|
|
|
| 8 |
A |
1496 |
1433 |
6.38 |
|
|
|
| 9 |
A |
1492 |
1429 |
32.52 |
|
|
|
| 10 |
A |
1436 |
1375 |
19.02 |
|
|
|
| 11 |
A |
1427 |
1366 |
0.83 |
|
|
|
| 12 |
A |
1241 |
1188 |
67.49 |
|
|
|
| 13 |
A |
1162 |
1112 |
21.16 |
|
|
|
| 14 |
A |
1157 |
1108 |
0.51 |
|
|
|
| 15 |
A |
1036 |
993 |
0.37 |
|
|
|
| 16 |
A |
988 |
946 |
19.99 |
|
|
|
| 17 |
A |
776 |
743 |
0.48 |
|
|
|
| 18 |
A |
545 |
522 |
40.82 |
|
|
|
| 19 |
A |
303 |
290 |
13.97 |
|
|
|
| 20 |
A |
273 |
261 |
65.20 |
|
|
|
| 21 |
A |
97 |
93 |
0.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16412.8 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 15718.5 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 HSEh1PBE/6-31G(2df,p)
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.861 |
0.434 |
0.004 |
| O2 |
1.361 |
-0.671 |
-0.000 |
| N3 |
-0.469 |
0.657 |
-0.020 |
| C4 |
-1.411 |
-0.439 |
0.005 |
| H5 |
1.452 |
1.368 |
0.018 |
| H6 |
-0.801 |
1.602 |
0.056 |
| H7 |
-2.409 |
-0.058 |
-0.217 |
| H8 |
-1.128 |
-1.177 |
-0.749 |
| H9 |
-1.422 |
-0.937 |
0.980 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.2126 | 1.3484 | 2.4331 | 1.1057 | 2.0321 | 3.3134 | 2.6679 | 2.8356 |
O2 | 1.2126 | | 2.2614 | 2.7815 | 2.0403 | 3.1377 | 3.8254 | 2.6484 | 2.9629 | N3 | 1.3484 | 2.2614 | | 1.4456 | 2.0486 | 1.0044 | 2.0768 | 2.0814 | 2.1095 | C4 | 2.4331 | 2.7815 | 1.4456 | | 3.3853 | 2.1310 | 1.0911 | 1.0922 | 1.0950 | H5 | 1.1057 | 2.0403 | 2.0486 | 3.3853 | | 2.2659 | 4.1224 | 3.7044 | 3.8076 | H6 | 2.0321 | 3.1377 | 1.0044 | 2.1310 | 2.2659 | | 2.3271 | 2.9122 | 2.7723 | H7 | 3.3134 | 3.8254 | 2.0768 | 1.0911 | 4.1224 | 2.3271 | | 1.7819 | 1.7830 | H8 | 2.6679 | 2.6484 | 2.0814 | 1.0922 | 3.7044 | 2.9122 | 1.7819 | | 1.7704 | H9 | 2.8356 | 2.9629 | 2.1095 | 1.0950 | 3.8076 | 2.7723 | 1.7830 | 1.7704 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
121.069 |
|
C1 |
N3 |
H6 |
118.739 |
| O2 |
C1 |
N3 |
123.930 |
|
O2 |
C1 |
H5 |
123.250 |
| N3 |
C1 |
H5 |
112.816 |
|
N3 |
C4 |
H7 |
109.111 |
| N3 |
C4 |
H8 |
109.410 |
|
N3 |
C4 |
H9 |
111.525 |
| C4 |
N3 |
H6 |
119.789 |
|
H7 |
C4 |
H8 |
109.395 |
| H7 |
C4 |
H9 |
109.293 |
|
H8 |
C4 |
H9 |
108.078 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.169 |
|
|
|
| 2 |
O |
-0.338 |
|
|
|
| 3 |
N |
-0.316 |
|
|
|
| 4 |
C |
-0.376 |
|
|
|
| 5 |
H |
0.094 |
|
|
|
| 6 |
H |
0.272 |
|
|
|
| 7 |
H |
0.151 |
|
|
|
| 8 |
H |
0.194 |
|
|
|
| 9 |
H |
0.151 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.769 |
2.490 |
-0.001 |
3.724 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.081 |
2.297 |
0.001 |
| y |
2.297 |
-21.727 |
-0.002 |
| z |
0.001 |
-0.002 |
-24.299 |
|
| Traceless |
| | x | y | z |
| x |
-2.068 |
2.297 |
0.001 |
| y |
2.297 |
2.963 |
-0.002 |
| z |
0.001 |
-0.002 |
-0.894 |
|
| Polar |
| 3z2-r2 | -1.789 |
| x2-y2 | -3.354 |
| xy | 2.297 |
| xz | 0.001 |
| yz | -0.002 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.154 |
-0.002 |
-0.000 |
| y |
-0.002 |
5.008 |
-0.000 |
| z |
-0.000 |
-0.000 |
3.332 |
<r2> (average value of r
2) Å
2
| <r2> |
77.529 |
| (<r2>)1/2 |
8.805 |