Jump to
S1C2
Energy calculated at B3PW91/6-311G*
| | hartrees |
| Energy at 0K | -169.870772 |
| Energy at 298.15K | -169.874477 |
| HF Energy | -169.870772 |
| Nuclear repulsion energy | 71.317736 |
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' |
3748 |
3608 |
28.98 |
|
|
|
| 2 |
A' |
3610 |
3475 |
24.25 |
|
|
|
| 3 |
A' |
2942 |
2833 |
128.29 |
|
|
|
| 4 |
A' |
1841 |
1773 |
402.70 |
|
|
|
| 5 |
A' |
1652 |
1591 |
68.08 |
|
|
|
| 6 |
A' |
1428 |
1375 |
5.45 |
|
|
|
| 7 |
A' |
1283 |
1235 |
100.22 |
|
|
|
| 8 |
A' |
1067 |
1027 |
3.98 |
|
|
|
| 9 |
A' |
567 |
546 |
11.50 |
|
|
|
| 10 |
A" |
1042 |
1003 |
0.68 |
|
|
|
| 11 |
A" |
660 |
636 |
22.63 |
|
|
|
| 12 |
A" |
224 |
215 |
269.07 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 10032.5 cm
-1
Scaled (by 0.9627) Zero Point Vibrational Energy (zpe) 9658.2 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 |
0.000 |
0.417 |
0.000 |
| O2 |
1.195 |
0.243 |
0.000 |
| N3 |
-0.935 |
-0.568 |
0.000 |
| H4 |
-0.460 |
1.425 |
0.000 |
| H5 |
-0.637 |
-1.530 |
0.000 |
| H6 |
-1.919 |
-0.363 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
H4 |
H5 |
H6 |
| C1 | | 1.2077 | 1.3575 | 1.1087 | 2.0480 | 2.0712 |
O2 | 1.2077 | | 2.2788 | 2.0344 | 2.5491 | 3.1722 | N3 | 1.3575 | 2.2788 | | 2.0487 | 1.0073 | 1.0049 | H4 | 1.1087 | 2.0344 | 2.0487 | | 2.9604 | 2.3079 | H5 | 2.0480 | 2.5491 | 1.0073 | 2.9604 | | 1.7331 | H6 | 2.0712 | 3.1722 | 1.0049 | 2.3079 | 1.7331 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
119.271 |
|
C1 |
N3 |
H6 |
121.795 |
| O2 |
C1 |
N3 |
125.241 |
|
O2 |
C1 |
H4 |
122.809 |
| N3 |
C1 |
H4 |
111.950 |
|
H5 |
N3 |
H6 |
118.934 |
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.230 |
|
|
|
| 2 |
O |
-0.361 |
|
|
|
| 3 |
N |
-0.740 |
|
|
|
| 4 |
H |
0.150 |
|
|
|
| 5 |
H |
0.360 |
|
|
|
| 6 |
H |
0.360 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.852 |
-0.783 |
0.000 |
3.931 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.801 |
-0.085 |
0.000 |
| y |
-0.085 |
-14.586 |
0.000 |
| z |
0.000 |
0.000 |
-18.672 |
|
| Traceless |
| | x | y | z |
| x |
-1.172 |
-0.085 |
0.000 |
| y |
-0.085 |
3.650 |
0.000 |
| z |
0.000 |
0.000 |
-2.478 |
|
| Polar |
| 3z2-r2 | -4.956 |
| x2-y2 | -3.215 |
| xy | -0.085 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.213 |
0.265 |
0.000 |
| y |
0.265 |
3.367 |
0.000 |
| z |
0.000 |
0.000 |
1.721 |
<r2> (average value of r
2) Å
2
| <r2> |
40.744 |
| (<r2>)1/2 |
6.383 |
Jump to
S1C1
Energy calculated at B3PW91/6-311G*
| | hartrees |
| Energy at 0K | -169.870771 |
| Energy at 298.15K | -169.874471 |
| HF Energy | -169.870771 |
| Nuclear repulsion energy | 71.317804 |
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 |
3748 |
3608 |
29.01 |
|
|
|
| 2 |
A |
3610 |
3475 |
24.27 |
|
|
|
| 3 |
A |
2943 |
2833 |
128.20 |
|
|
|
| 4 |
A |
1841 |
1772 |
402.78 |
|
|
|
| 5 |
A |
1652 |
1591 |
67.91 |
|
|
|
| 6 |
A |
1428 |
1375 |
5.46 |
|
|
|
| 7 |
A |
1284 |
1236 |
100.10 |
|
|
|
| 8 |
A |
1067 |
1027 |
3.94 |
|
|
|
| 9 |
A |
1042 |
1004 |
0.69 |
|
|
|
| 10 |
A |
661 |
636 |
23.16 |
|
|
|
| 11 |
A |
568 |
546 |
11.51 |
|
|
|
| 12 |
A |
220 |
212 |
268.40 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 10031.2 cm
-1
Scaled (by 0.9627) Zero Point Vibrational Energy (zpe) 9657.0 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 |
0.163 |
0.383 |
0.000 |
| O2 |
1.195 |
-0.245 |
-0.000 |
| N3 |
-1.082 |
-0.156 |
-0.000 |
| H4 |
0.135 |
1.492 |
0.000 |
| H5 |
-1.185 |
-1.158 |
0.000 |
| H6 |
-1.908 |
0.417 |
-0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
H4 |
H5 |
H6 |
| C1 | | 1.2078 | 1.3573 | 1.1086 | 2.0478 | 2.0712 |
O2 | 1.2078 | | 2.2788 | 2.0342 | 2.5488 | 3.1723 | N3 | 1.3573 | 2.2788 | | 2.0488 | 1.0073 | 1.0049 | H4 | 1.1086 | 2.0342 | 2.0488 | | 2.9604 | 2.3083 | H5 | 2.0478 | 2.5488 | 1.0073 | 2.9604 | | 1.7332 | H6 | 2.0712 | 3.1723 | 1.0049 | 2.3083 | 1.7332 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
119.256 |
|
C1 |
N3 |
H6 |
121.805 |
| O2 |
C1 |
N3 |
125.238 |
|
O2 |
C1 |
H4 |
122.788 |
| N3 |
C1 |
H4 |
111.974 |
|
H5 |
N3 |
H6 |
118.939 |
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 |
0.229 |
|
|
|
| 2 |
O |
-0.361 |
|
|
|
| 3 |
N |
-0.740 |
|
|
|
| 4 |
H |
0.151 |
|
|
|
| 5 |
H |
0.360 |
|
|
|
| 6 |
H |
0.360 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.853 |
0.787 |
0.000 |
3.932 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.370 |
1.099 |
0.001 |
| y |
1.099 |
-15.017 |
-0.001 |
| z |
0.001 |
-0.001 |
-18.672 |
|
| Traceless |
| | x | y | z |
| x |
-0.526 |
1.099 |
0.001 |
| y |
1.099 |
3.004 |
-0.001 |
| z |
0.001 |
-0.001 |
-2.478 |
|
| Polar |
| 3z2-r2 | -4.957 |
| x2-y2 | -2.353 |
| xy | 1.099 |
| xz | 0.001 |
| yz | -0.001 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.274 |
-0.121 |
0.000 |
| y |
-0.121 |
3.306 |
0.000 |
| z |
0.000 |
0.000 |
1.720 |
<r2> (average value of r
2) Å
2
| <r2> |
40.743 |
| (<r2>)1/2 |
6.383 |