Jump to
S1C2
Energy calculated at B2PLYP/6-311G**
| | hartrees |
| Energy at 0K | -169.790026 |
| Energy at 298.15K | -169.793473 |
| HF Energy | -169.619195 |
| Nuclear repulsion energy | 71.174075 |
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 B2PLYP/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' |
3758 |
3758 |
40.40 |
|
|
|
| 2 |
A' |
3616 |
3616 |
36.18 |
|
|
|
| 3 |
A' |
2967 |
2967 |
117.32 |
|
|
|
| 4 |
A' |
1814 |
1814 |
367.96 |
|
|
|
| 5 |
A' |
1630 |
1630 |
60.62 |
|
|
|
| 6 |
A' |
1432 |
1432 |
5.98 |
|
|
|
| 7 |
A' |
1276 |
1276 |
103.32 |
|
|
|
| 8 |
A' |
1058 |
1058 |
4.25 |
|
|
|
| 9 |
A' |
567 |
567 |
11.66 |
|
|
|
| 10 |
A" |
1055 |
1055 |
1.07 |
|
|
|
| 11 |
A" |
650 |
650 |
17.19 |
|
|
|
| 12 |
A" |
65 |
65 |
235.09 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 9943.0 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 9943.0 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 B2PLYP/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.419 |
0.000 |
| O2 |
1.198 |
0.240 |
0.000 |
| N3 |
-0.938 |
-0.568 |
0.000 |
| H4 |
-0.460 |
1.425 |
0.000 |
| H5 |
-0.637 |
-1.528 |
0.000 |
| H6 |
-1.921 |
-0.358 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
H4 |
H5 |
H6 |
| C1 | | 1.2116 | 1.3618 | 1.1055 | 2.0492 | 2.0722 |
O2 | 1.2116 | | 2.2839 | 2.0381 | 2.5483 | 3.1756 | N3 | 1.3618 | 2.2839 | | 2.0488 | 1.0069 | 1.0044 | H4 | 1.1055 | 2.0381 | 2.0488 | | 2.9582 | 2.3049 | H5 | 2.0492 | 2.5483 | 1.0069 | 2.9582 | | 1.7368 | H6 | 2.0722 | 3.1756 | 1.0044 | 2.3049 | 1.7368 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
119.037 |
|
C1 |
N3 |
H6 |
121.531 |
| O2 |
C1 |
N3 |
125.020 |
|
O2 |
C1 |
H4 |
123.124 |
| N3 |
C1 |
H4 |
111.855 |
|
H5 |
N3 |
H6 |
119.432 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.263 |
|
|
|
| 2 |
O |
-0.345 |
|
|
|
| 3 |
N |
-0.428 |
|
|
|
| 4 |
H |
0.055 |
|
|
|
| 5 |
H |
0.229 |
|
|
|
| 6 |
H |
0.226 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.739 |
-0.709 |
0.000 |
3.805 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-18.055 |
-0.114 |
0.000 |
| y |
-0.114 |
-14.870 |
0.000 |
| z |
0.000 |
0.000 |
-18.654 |
|
| Traceless |
| | x | y | z |
| x |
-1.293 |
-0.114 |
0.000 |
| y |
-0.114 |
3.485 |
0.000 |
| z |
0.000 |
0.000 |
-2.191 |
|
| Polar |
| 3z2-r2 | -4.383 |
| x2-y2 | -3.185 |
| xy | -0.114 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.311 |
0.270 |
0.000 |
| y |
0.270 |
3.417 |
0.000 |
| z |
0.000 |
0.000 |
1.780 |
<r2> (average value of r
2) Å
2
| <r2> |
40.956 |
| (<r2>)1/2 |
6.400 |
Jump to
S1C1
Energy calculated at B2PLYP/6-311G**
| | hartrees |
| Energy at 0K | -169.789009 |
| Energy at 298.15K | |
| HF Energy | -169.618913 |
| Nuclear repulsion energy | 71.643682 |
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 B2PLYP/6-311G**
Geometric Data calculated at B2PLYP/6-311G**
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.170 |
0.386 |
0.002 |
| O2 |
1.178 |
-0.250 |
0.010 |
| N3 |
-1.085 |
-0.154 |
-0.065 |
| H4 |
0.161 |
1.490 |
-0.002 |
| H5 |
-1.149 |
-1.143 |
0.131 |
| H6 |
-1.862 |
0.413 |
0.235 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
H4 |
H5 |
H6 |
| C1 | | 1.1917 | 1.3680 | 1.1044 | 2.0238 | 2.0450 |
O2 | 1.1917 | | 2.2661 | 2.0153 | 2.4959 | 3.1191 | N3 | 1.3680 | 2.2661 | | 2.0645 | 1.0101 | 1.0077 | H4 | 1.1044 | 2.0153 | 2.0645 | | 2.9447 | 2.3041 | H5 | 2.0238 | 2.4959 | 1.0101 | 2.9447 | | 1.7145 | H6 | 2.0450 | 3.1191 | 1.0077 | 2.3041 | 1.7145 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
115.824 |
|
C1 |
N3 |
H6 |
118.019 |
| O2 |
C1 |
N3 |
124.433 |
|
O2 |
C1 |
H4 |
122.692 |
| N3 |
C1 |
H4 |
112.805 |
|
H5 |
N3 |
H6 |
116.361 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.245 |
|
|
|
| 2 |
O |
-0.328 |
|
|
|
| 3 |
N |
-0.411 |
|
|
|
| 4 |
H |
0.057 |
|
|
|
| 5 |
H |
0.221 |
|
|
|
| 6 |
H |
0.216 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.335 |
0.822 |
0.761 |
3.518 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-18.121 |
1.051 |
-1.401 |
| y |
1.051 |
-15.389 |
-0.123 |
| z |
-1.401 |
-0.123 |
-18.473 |
|
| Traceless |
| | x | y | z |
| x |
-1.190 |
1.051 |
-1.401 |
| y |
1.051 |
2.908 |
-0.123 |
| z |
-1.401 |
-0.123 |
-1.718 |
|
| Polar |
| 3z2-r2 | -3.436 |
| x2-y2 | -2.732 |
| xy | 1.051 |
| xz | -1.401 |
| yz | -0.123 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.311 |
0.270 |
0.000 |
| y |
0.270 |
3.417 |
0.000 |
| z |
0.000 |
0.000 |
1.780 |
<r2> (average value of r
2) Å
2
| <r2> |
40.510 |
| (<r2>)1/2 |
6.365 |