Jump to
S1C2
S1C3
Energy calculated at B3PW91/6-311G**
| | hartrees |
| Energy at 0K | -209.180095 |
| Energy at 298.15K | -209.186173 |
| HF Energy | -209.180095 |
| Nuclear repulsion energy | 119.423200 |
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 B3PW91/6-311G**
| 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' |
3621 |
3488 |
24.03 |
|
|
|
| 2 |
A' |
3124 |
3008 |
16.60 |
|
|
|
| 3 |
A' |
3027 |
2915 |
54.66 |
|
|
|
| 4 |
A' |
2922 |
2814 |
99.30 |
|
|
|
| 5 |
A' |
1825 |
1758 |
482.47 |
|
|
|
| 6 |
A' |
1532 |
1476 |
21.91 |
|
|
|
| 7 |
A' |
1487 |
1432 |
6.65 |
|
|
|
| 8 |
A' |
1461 |
1407 |
4.37 |
|
|
|
| 9 |
A' |
1392 |
1341 |
10.15 |
|
|
|
| 10 |
A' |
1306 |
1258 |
104.60 |
|
|
|
| 11 |
A' |
1170 |
1126 |
26.16 |
|
|
|
| 12 |
A' |
1014 |
977 |
47.24 |
|
|
|
| 13 |
A' |
615 |
593 |
14.69 |
|
|
|
| 14 |
A' |
340 |
327 |
8.25 |
|
|
|
| 15 |
A" |
3084 |
2971 |
31.40 |
|
|
|
| 16 |
A" |
1480 |
1425 |
7.14 |
|
|
|
| 17 |
A" |
1145 |
1103 |
0.21 |
|
|
|
| 18 |
A" |
1044 |
1005 |
0.69 |
|
|
|
| 19 |
A" |
637 |
613 |
123.16 |
|
|
|
| 20 |
A" |
208 |
200 |
0.67 |
|
|
|
| 21 |
A" |
105 |
101 |
0.68 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16268.5 cm
-1
Scaled (by 0.9631) Zero Point Vibrational Energy (zpe) 15668.2 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 B3PW91/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.285 |
-0.757 |
0.000 |
| O2 |
1.398 |
-1.231 |
0.000 |
| N3 |
0.000 |
0.570 |
0.000 |
| C4 |
-1.330 |
1.131 |
0.000 |
| H5 |
-0.636 |
-1.376 |
0.000 |
| H6 |
0.799 |
1.188 |
0.000 |
| H7 |
-2.055 |
0.314 |
0.000 |
| H8 |
-1.512 |
1.743 |
0.890 |
| H9 |
-1.512 |
1.743 |
-0.890 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.2097 | 1.3576 | 2.4849 | 1.1100 | 2.0121 | 2.5738 | 3.2046 | 3.2046 |
O2 | 1.2097 | | 2.2802 | 3.6088 | 2.0396 | 2.4926 | 3.7832 | 4.2547 | 4.2547 | N3 | 1.3576 | 2.2802 | | 1.4436 | 2.0477 | 1.0099 | 2.0710 | 2.1099 | 2.1099 | C4 | 2.4849 | 3.6088 | 1.4436 | | 2.6015 | 2.1295 | 1.0922 | 1.0947 | 1.0947 | H5 | 1.1100 | 2.0396 | 2.0477 | 2.6015 | | 2.9386 | 2.2069 | 3.3594 | 3.3594 | H6 | 2.0121 | 2.4926 | 1.0099 | 2.1295 | 2.9386 | | 2.9845 | 2.5370 | 2.5370 | H7 | 2.5738 | 3.7832 | 2.0710 | 1.0922 | 2.2069 | 2.9845 | | 1.7684 | 1.7684 | H8 | 3.2046 | 4.2547 | 2.1099 | 1.0947 | 3.3594 | 2.5370 | 1.7684 | | 1.7792 | H9 | 3.2046 | 4.2547 | 2.1099 | 1.0947 | 3.3594 | 2.5370 | 1.7684 | 1.7792 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
124.993 |
|
C1 |
N3 |
H6 |
115.619 |
| O2 |
C1 |
N3 |
125.190 |
|
O2 |
C1 |
H5 |
123.042 |
| N3 |
C1 |
H5 |
111.768 |
|
N3 |
C4 |
H7 |
108.718 |
| N3 |
C4 |
H8 |
111.712 |
|
N3 |
C4 |
H9 |
111.712 |
| C4 |
N3 |
H6 |
119.389 |
|
H7 |
C4 |
H8 |
107.924 |
| H7 |
C4 |
H9 |
107.924 |
|
H8 |
C4 |
H9 |
108.709 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.275 |
|
|
|
| 2 |
O |
-0.367 |
|
|
|
| 3 |
N |
-0.399 |
|
|
|
| 4 |
C |
-0.183 |
|
|
|
| 5 |
H |
0.056 |
|
|
|
| 6 |
H |
0.231 |
|
|
|
| 7 |
H |
0.120 |
|
|
|
| 8 |
H |
0.134 |
|
|
|
| 9 |
H |
0.134 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.000 |
2.783 |
0.000 |
4.093 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.178 |
3.964 |
0.000 |
| y |
3.964 |
-24.184 |
0.000 |
| z |
0.000 |
0.000 |
-24.591 |
|
| Traceless |
| | x | y | z |
| x |
-1.791 |
3.964 |
0.000 |
| y |
3.964 |
1.200 |
0.000 |
| z |
0.000 |
0.000 |
0.590 |
|
| Polar |
| 3z2-r2 | 1.180 |
| x2-y2 | -1.994 |
| xy | 3.964 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.735 |
-1.054 |
0.000 |
| y |
-1.054 |
5.761 |
0.000 |
| z |
0.000 |
0.000 |
3.322 |
<r2> (average value of r
2) Å
2
| <r2> |
88.762 |
| (<r2>)1/2 |
9.421 |
Jump to
S1C1
S1C3
Energy calculated at B3PW91/6-311G**
| | hartrees |
| Energy at 0K | -209.180095 |
| Energy at 298.15K | -209.186173 |
| HF Energy | -209.180095 |
| Nuclear repulsion energy | 119.423200 |
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 B3PW91/6-311G**
Geometric Data calculated at B3PW91/6-311G**
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
Energy calculated at B3PW91/6-311G**
| | hartrees |
| Energy at 0K | -209.181953 |
| Energy at 298.15K | -209.188073 |
| HF Energy | -209.181953 |
| Nuclear repulsion energy | 121.619843 |
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 B3PW91/6-311G**
| 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 |
3520 |
25.01 |
|
|
|
| 2 |
A |
3156 |
3040 |
1.05 |
|
|
|
| 3 |
A |
3093 |
2979 |
32.30 |
|
|
|
| 4 |
A |
3034 |
2922 |
45.00 |
|
|
|
| 5 |
A |
2942 |
2833 |
126.53 |
|
|
|
| 6 |
A |
1811 |
1744 |
336.83 |
|
|
|
| 7 |
A |
1561 |
1503 |
104.66 |
|
|
|
| 8 |
A |
1497 |
1442 |
8.75 |
|
|
|
| 9 |
A |
1489 |
1434 |
29.15 |
|
|
|
| 10 |
A |
1434 |
1381 |
22.27 |
|
|
|
| 11 |
A |
1419 |
1366 |
1.88 |
|
|
|
| 12 |
A |
1226 |
1181 |
72.77 |
|
|
|
| 13 |
A |
1158 |
1115 |
21.95 |
|
|
|
| 14 |
A |
1148 |
1106 |
0.58 |
|
|
|
| 15 |
A |
1023 |
986 |
0.14 |
|
|
|
| 16 |
A |
973 |
937 |
20.92 |
|
|
|
| 17 |
A |
773 |
745 |
0.72 |
|
|
|
| 18 |
A |
548 |
528 |
48.20 |
|
|
|
| 19 |
A |
299 |
288 |
14.02 |
|
|
|
| 20 |
A |
284 |
274 |
72.43 |
|
|
|
| 21 |
A |
96 |
92 |
0.02 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16309.5 cm
-1
Scaled (by 0.9631) Zero Point Vibrational Energy (zpe) 15707.7 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 B3PW91/6-311G**
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.863 |
0.433 |
0.004 |
| O2 |
1.373 |
-0.670 |
-0.000 |
| N3 |
-0.470 |
0.657 |
-0.019 |
| C4 |
-1.421 |
-0.440 |
0.005 |
| H5 |
1.455 |
1.366 |
0.017 |
| H6 |
-0.800 |
1.605 |
0.056 |
| H7 |
-2.416 |
-0.054 |
-0.220 |
| H8 |
-1.144 |
-1.181 |
-0.747 |
| H9 |
-1.437 |
-0.935 |
0.980 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.2152 | 1.3527 | 2.4456 | 1.1051 | 2.0354 | 3.3230 | 2.6828 | 2.8492 |
O2 | 1.2152 | | 2.2712 | 2.8032 | 2.0382 | 3.1463 | 3.8447 | 2.6741 | 2.9878 | N3 | 1.3527 | 2.2712 | | 1.4513 | 2.0527 | 1.0065 | 2.0810 | 2.0877 | 2.1137 | C4 | 2.4456 | 2.8032 | 1.4513 | | 3.3964 | 2.1372 | 1.0904 | 1.0911 | 1.0942 | H5 | 1.1051 | 2.0382 | 2.0527 | 3.3964 | | 2.2684 | 4.1305 | 3.7184 | 3.8198 | H6 | 2.0354 | 3.1463 | 1.0065 | 2.1372 | 2.2684 | | 2.3321 | 2.9189 | 2.7769 | H7 | 3.3230 | 3.8447 | 2.0810 | 1.0904 | 4.1305 | 2.3321 | | 1.7790 | 1.7814 | H8 | 2.6828 | 2.6741 | 2.0877 | 1.0911 | 3.7184 | 2.9189 | 1.7790 | | 1.7689 | H9 | 2.8492 | 2.9878 | 2.1137 | 1.0942 | 3.8198 | 2.7769 | 1.7814 | 1.7689 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
121.377 |
|
C1 |
N3 |
H6 |
118.514 |
| O2 |
C1 |
N3 |
124.278 |
|
O2 |
C1 |
H5 |
122.839 |
| N3 |
C1 |
H5 |
112.880 |
|
N3 |
C4 |
H7 |
109.094 |
| N3 |
C4 |
H8 |
109.585 |
|
N3 |
C4 |
H9 |
111.501 |
| C4 |
N3 |
H6 |
119.725 |
|
H7 |
C4 |
H8 |
109.278 |
| H7 |
C4 |
H9 |
109.264 |
|
H8 |
C4 |
H9 |
108.087 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.268 |
|
|
|
| 2 |
O |
-0.374 |
|
|
|
| 3 |
N |
-0.406 |
|
|
|
| 4 |
C |
-0.202 |
|
|
|
| 5 |
H |
0.072 |
|
|
|
| 6 |
H |
0.228 |
|
|
|
| 7 |
H |
0.130 |
|
|
|
| 8 |
H |
0.153 |
|
|
|
| 9 |
H |
0.130 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.904 |
2.572 |
-0.000 |
3.879 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.374 |
2.583 |
0.000 |
| y |
2.583 |
-21.992 |
-0.000 |
| z |
0.000 |
-0.000 |
-24.614 |
|
| Traceless |
| | x | y | z |
| x |
-2.071 |
2.583 |
0.000 |
| y |
2.583 |
3.002 |
-0.000 |
| z |
0.000 |
-0.000 |
-0.931 |
|
| Polar |
| 3z2-r2 | -1.863 |
| x2-y2 | -3.382 |
| xy | 2.583 |
| xz | 0.000 |
| yz | -0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.137 |
-0.073 |
-0.000 |
| y |
-0.073 |
5.131 |
-0.000 |
| z |
-0.000 |
-0.000 |
3.307 |
<r2> (average value of r
2) Å
2
| <r2> |
78.187 |
| (<r2>)1/2 |
8.842 |