Jump to
S1C2
S1C3
Energy calculated at B3PW91/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -209.153134 |
| Energy at 298.15K | -209.159191 |
| HF Energy | -209.153134 |
| Nuclear repulsion energy | 119.111274 |
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 B3PW91/aug-cc-pVDZ
| 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' |
3612 |
3485 |
26.89 |
|
|
|
| 2 |
A' |
3138 |
3027 |
13.35 |
|
|
|
| 3 |
A' |
3034 |
2926 |
56.16 |
|
|
|
| 4 |
A' |
2949 |
2844 |
79.95 |
|
|
|
| 5 |
A' |
1790 |
1726 |
534.29 |
|
|
|
| 6 |
A' |
1517 |
1463 |
22.12 |
|
|
|
| 7 |
A' |
1470 |
1418 |
4.77 |
|
|
|
| 8 |
A' |
1439 |
1388 |
4.21 |
|
|
|
| 9 |
A' |
1372 |
1324 |
10.68 |
|
|
|
| 10 |
A' |
1304 |
1258 |
104.01 |
|
|
|
| 11 |
A' |
1168 |
1127 |
20.89 |
|
|
|
| 12 |
A' |
1010 |
975 |
40.95 |
|
|
|
| 13 |
A' |
611 |
590 |
13.97 |
|
|
|
| 14 |
A' |
339 |
327 |
8.10 |
|
|
|
| 15 |
A" |
3099 |
2989 |
24.03 |
|
|
|
| 16 |
A" |
1454 |
1403 |
6.57 |
|
|
|
| 17 |
A" |
1136 |
1096 |
0.31 |
|
|
|
| 18 |
A" |
1028 |
992 |
2.58 |
|
|
|
| 19 |
A" |
622 |
600 |
109.66 |
|
|
|
| 20 |
A" |
207 |
200 |
0.25 |
|
|
|
| 21 |
A" |
102 |
98 |
0.42 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16200.4 cm
-1
Scaled (by 0.9646) Zero Point Vibrational Energy (zpe) 15626.9 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 B3PW91/aug-cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.280 |
-0.757 |
0.000 |
| O2 |
1.402 |
-1.234 |
0.000 |
| N3 |
0.000 |
0.570 |
0.000 |
| C4 |
-1.331 |
1.134 |
0.000 |
| H5 |
-0.638 |
-1.386 |
0.000 |
| H6 |
0.802 |
1.188 |
0.000 |
| H7 |
-2.061 |
0.315 |
0.000 |
| H8 |
-1.508 |
1.750 |
0.894 |
| H9 |
-1.508 |
1.750 |
-0.894 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.2185 | 1.3572 | 2.4847 | 1.1132 | 2.0145 | 2.5750 | 3.2069 | 3.2069 |
O2 | 1.2185 | | 2.2848 | 3.6157 | 2.0460 | 2.4953 | 3.7931 | 4.2625 | 4.2625 | N3 | 1.3572 | 2.2848 | | 1.4451 | 2.0581 | 1.0123 | 2.0764 | 2.1129 | 2.1129 | C4 | 2.4847 | 3.6157 | 1.4451 | | 2.6136 | 2.1331 | 1.0972 | 1.0997 | 1.0997 | H5 | 1.1132 | 2.0460 | 2.0581 | 2.6136 | | 2.9499 | 2.2174 | 3.3747 | 3.3747 | H6 | 2.0145 | 2.4953 | 1.0123 | 2.1331 | 2.9499 | | 2.9927 | 2.5398 | 2.5398 | H7 | 2.5750 | 3.7931 | 2.0764 | 1.0972 | 2.2174 | 2.9927 | | 1.7782 | 1.7782 | H8 | 3.2069 | 4.2625 | 2.1129 | 1.0997 | 3.3747 | 2.5398 | 1.7782 | | 1.7875 | H9 | 3.2069 | 4.2625 | 2.1129 | 1.0997 | 3.3747 | 2.5398 | 1.7782 | 1.7875 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
124.881 |
|
C1 |
N3 |
H6 |
115.699 |
| O2 |
C1 |
N3 |
124.925 |
|
O2 |
C1 |
H5 |
122.614 |
| N3 |
C1 |
H5 |
112.461 |
|
N3 |
C4 |
H7 |
108.748 |
| N3 |
C4 |
H8 |
111.538 |
|
N3 |
C4 |
H9 |
111.538 |
| C4 |
N3 |
H6 |
119.420 |
|
H7 |
C4 |
H8 |
108.081 |
| H7 |
C4 |
H9 |
108.081 |
|
H8 |
C4 |
H9 |
108.735 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.743 |
|
|
|
| 2 |
O |
-0.511 |
|
|
|
| 3 |
N |
-0.068 |
|
|
|
| 4 |
C |
0.768 |
|
|
|
| 5 |
H |
-0.260 |
|
|
|
| 6 |
H |
-0.179 |
|
|
|
| 7 |
H |
-0.197 |
|
|
|
| 8 |
H |
-0.148 |
|
|
|
| 9 |
H |
-0.148 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.195 |
2.887 |
0.000 |
4.306 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-27.013 |
4.274 |
0.000 |
| y |
4.274 |
-24.586 |
0.000 |
| z |
0.000 |
0.000 |
-24.913 |
|
| Traceless |
| | x | y | z |
| x |
-2.263 |
4.274 |
0.000 |
| y |
4.274 |
1.377 |
0.000 |
| z |
0.000 |
0.000 |
0.886 |
|
| Polar |
| 3z2-r2 | 1.772 |
| x2-y2 | -2.427 |
| xy | 4.274 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.807 |
-1.224 |
0.000 |
| y |
-1.224 |
6.714 |
0.000 |
| z |
0.000 |
0.000 |
4.339 |
<r2> (average value of r
2) Å
2
| <r2> |
89.361 |
| (<r2>)1/2 |
9.453 |
Jump to
S1C1
S1C3
Energy calculated at B3PW91/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -209.153134 |
| Energy at 298.15K | -209.159191 |
| HF Energy | -209.153134 |
| Nuclear repulsion energy | 119.111274 |
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 B3PW91/aug-cc-pVDZ
Geometric Data calculated at B3PW91/aug-cc-pVDZ
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
Energy calculated at B3PW91/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -209.154827 |
| Energy at 298.15K | -209.160876 |
| HF Energy | -209.154827 |
| Nuclear repulsion energy | 121.246201 |
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 B3PW91/aug-cc-pVDZ
| 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 |
3648 |
3518 |
25.45 |
|
|
|
| 2 |
A |
3168 |
3056 |
0.47 |
|
|
|
| 3 |
A |
3109 |
2999 |
24.15 |
|
|
|
| 4 |
A |
3042 |
2935 |
46.31 |
|
|
|
| 5 |
A |
2967 |
2862 |
103.30 |
|
|
|
| 6 |
A |
1780 |
1717 |
370.75 |
|
|
|
| 7 |
A |
1558 |
1503 |
107.06 |
|
|
|
| 8 |
A |
1470 |
1418 |
7.24 |
|
|
|
| 9 |
A |
1468 |
1416 |
17.96 |
|
|
|
| 10 |
A |
1415 |
1365 |
17.94 |
|
|
|
| 11 |
A |
1404 |
1354 |
4.43 |
|
|
|
| 12 |
A |
1231 |
1187 |
62.17 |
|
|
|
| 13 |
A |
1150 |
1109 |
21.39 |
|
|
|
| 14 |
A |
1139 |
1099 |
0.75 |
|
|
|
| 15 |
A |
1014 |
979 |
0.20 |
|
|
|
| 16 |
A |
972 |
938 |
22.65 |
|
|
|
| 17 |
A |
763 |
736 |
0.80 |
|
|
|
| 18 |
A |
552 |
532 |
43.98 |
|
|
|
| 19 |
A |
292 |
282 |
14.11 |
|
|
|
| 20 |
A |
282 |
272 |
62.68 |
|
|
|
| 21 |
A |
64 |
62 |
0.08 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16244.1 cm
-1
Scaled (by 0.9646) Zero Point Vibrational Energy (zpe) 15669.1 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 B3PW91/aug-cc-pVDZ
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.865 |
0.437 |
0.003 |
| O2 |
1.378 |
-0.672 |
0.000 |
| N3 |
-0.472 |
0.655 |
-0.019 |
| C4 |
-1.426 |
-0.440 |
0.005 |
| H5 |
1.460 |
1.373 |
0.017 |
| H6 |
-0.799 |
1.607 |
0.056 |
| H7 |
-2.425 |
-0.046 |
-0.213 |
| H8 |
-1.153 |
-1.181 |
-0.756 |
| H9 |
-1.437 |
-0.941 |
0.983 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.2220 | 1.3546 | 2.4526 | 1.1096 | 2.0347 | 3.3320 | 2.6954 | 2.8555 |
O2 | 1.2220 | | 2.2772 | 2.8138 | 2.0466 | 3.1523 | 3.8602 | 2.6905 | 2.9938 | N3 | 1.3546 | 2.2772 | | 1.4525 | 2.0616 | 1.0089 | 2.0842 | 2.0925 | 2.1172 | C4 | 2.4526 | 2.8138 | 1.4525 | | 3.4083 | 2.1409 | 1.0956 | 1.0966 | 1.0994 | H5 | 1.1096 | 2.0466 | 2.0616 | 3.4083 | | 2.2720 | 4.1428 | 3.7349 | 3.8313 | H6 | 2.0347 | 3.1523 | 1.0089 | 2.1409 | 2.2720 | | 2.3341 | 2.9250 | 2.7846 | H7 | 3.3320 | 3.8602 | 2.0842 | 1.0956 | 4.1428 | 2.3341 | | 1.7888 | 1.7909 | H8 | 2.6954 | 2.6905 | 2.0925 | 1.0966 | 3.7349 | 2.9250 | 1.7888 | | 1.7789 | H9 | 2.8555 | 2.9938 | 2.1172 | 1.0994 | 3.8313 | 2.7846 | 1.7909 | 1.7789 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
121.746 |
|
C1 |
N3 |
H6 |
118.091 |
| O2 |
C1 |
N3 |
124.125 |
|
O2 |
C1 |
H5 |
122.677 |
| N3 |
C1 |
H5 |
113.196 |
|
N3 |
C4 |
H7 |
108.953 |
| N3 |
C4 |
H8 |
109.556 |
|
N3 |
C4 |
H9 |
111.373 |
| C4 |
N3 |
H6 |
119.787 |
|
H7 |
C4 |
H8 |
109.372 |
| H7 |
C4 |
H9 |
109.358 |
|
H8 |
C4 |
H9 |
108.204 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.705 |
|
|
|
| 2 |
O |
-0.495 |
|
|
|
| 3 |
N |
-0.097 |
|
|
|
| 4 |
C |
0.760 |
|
|
|
| 5 |
H |
-0.239 |
|
|
|
| 6 |
H |
-0.134 |
|
|
|
| 7 |
H |
-0.148 |
|
|
|
| 8 |
H |
-0.204 |
|
|
|
| 9 |
H |
-0.148 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.020 |
2.615 |
0.000 |
3.995 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.926 |
2.783 |
-0.000 |
| y |
2.783 |
-22.542 |
0.000 |
| z |
-0.000 |
0.000 |
-24.982 |
|
| Traceless |
| | x | y | z |
| x |
-2.164 |
2.783 |
-0.000 |
| y |
2.783 |
2.912 |
0.000 |
| z |
-0.000 |
0.000 |
-0.748 |
|
| Polar |
| 3z2-r2 | -1.497 |
| x2-y2 | -3.384 |
| xy | 2.783 |
| xz | -0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.244 |
-0.095 |
0.000 |
| y |
-0.095 |
6.079 |
0.000 |
| z |
0.000 |
0.000 |
4.385 |
<r2> (average value of r
2) Å
2
| <r2> |
78.894 |
| (<r2>)1/2 |
8.882 |