Jump to
S1C2
S1C3
Energy calculated at M06-2X/6-311G**
| hartrees |
Energy at 0K | -169.841327 |
Energy at 298.15K | -169.845349 |
HF Energy | -169.841327 |
Nuclear repulsion energy | 71.046131 |
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 M06-2X/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' |
3940 |
3940 |
93.90 |
|
|
|
2 |
A' |
3576 |
3576 |
12.61 |
|
|
|
3 |
A' |
3074 |
3074 |
52.94 |
|
|
|
4 |
A' |
1810 |
1810 |
213.37 |
|
|
|
5 |
A' |
1451 |
1451 |
15.67 |
|
|
|
6 |
A' |
1351 |
1351 |
185.47 |
|
|
|
7 |
A' |
1213 |
1213 |
40.09 |
|
|
|
8 |
A' |
1079 |
1079 |
208.22 |
|
|
|
9 |
A' |
630 |
630 |
1.05 |
|
|
|
10 |
A" |
1072 |
1072 |
4.71 |
|
|
|
11 |
A" |
845 |
845 |
62.84 |
|
|
|
12 |
A" |
401 |
401 |
76.66 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 10221.0 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 10221.0 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 M06-2X/6-311G**
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.372 |
0.000 |
O2 |
-0.998 |
-0.536 |
0.000 |
N3 |
1.194 |
-0.010 |
0.000 |
H4 |
-0.342 |
1.414 |
0.000 |
H5 |
-1.845 |
-0.085 |
0.000 |
H6 |
1.812 |
0.797 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
O2 |
N3 |
H4 |
H5 |
H6 |
C1 | | 1.3499 | 1.2540 | 1.0963 | 1.9004 | 1.8611 |
O2 | 1.3499 | | 2.2550 | 2.0578 | 0.9591 | 3.1105 | N3 | 1.2540 | 2.2550 | | 2.0945 | 3.0398 | 1.0159 | H4 | 1.0963 | 2.0578 | 2.0945 | | 2.1224 | 2.2406 | H5 | 1.9004 | 0.9591 | 3.0398 | 2.1224 | | 3.7614 | H6 | 1.8611 | 3.1105 | 1.0159 | 2.2406 | 3.7614 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
O2 |
H5 |
109.613 |
|
C1 |
N3 |
H6 |
109.701 |
O2 |
C1 |
N3 |
119.944 |
|
O2 |
C1 |
H4 |
114.140 |
N3 |
C1 |
H4 |
125.915 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.166 |
|
|
|
2 |
O |
-0.322 |
|
|
|
3 |
N |
-0.385 |
|
|
|
4 |
H |
0.091 |
|
|
|
5 |
H |
0.262 |
|
|
|
6 |
H |
0.188 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-2.058 |
3.313 |
0.000 |
3.900 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-13.910 |
1.194 |
0.000 |
y |
1.194 |
-17.784 |
0.000 |
z |
0.000 |
0.000 |
-18.690 |
|
Traceless |
| x | y | z |
x |
4.326 |
1.194 |
0.000 |
y |
1.194 |
-1.483 |
0.000 |
z |
0.000 |
0.000 |
-2.843 |
|
Polar |
3z2-r2 | -5.686 |
x2-y2 | 3.873 |
xy | 1.194 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
4.811 |
0.004 |
0.000 |
y |
0.004 |
2.888 |
0.000 |
z |
0.000 |
0.000 |
1.788 |
<r2> (average value of r
2) Å
2
<r2> |
41.025 |
(<r2>)1/2 |
6.405 |
Jump to
S1C1
S1C3
Energy calculated at M06-2X/6-311G**
| hartrees |
Energy at 0K | -169.851857 |
Energy at 298.15K | -169.856036 |
HF Energy | -169.851857 |
Nuclear repulsion energy | 71.405858 |
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 M06-2X/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' |
3822 |
3822 |
64.73 |
|
|
|
2 |
A' |
3559 |
3559 |
13.67 |
|
|
|
3 |
A' |
3162 |
3162 |
28.12 |
|
|
|
4 |
A' |
1779 |
1779 |
286.31 |
|
|
|
5 |
A' |
1425 |
1425 |
25.21 |
|
|
|
6 |
A' |
1391 |
1391 |
1.84 |
|
|
|
7 |
A' |
1218 |
1218 |
122.85 |
|
|
|
8 |
A' |
1093 |
1093 |
176.54 |
|
|
|
9 |
A' |
606 |
606 |
51.55 |
|
|
|
10 |
A" |
1085 |
1085 |
0.05 |
|
|
|
11 |
A" |
845 |
845 |
31.97 |
|
|
|
12 |
A" |
623 |
623 |
196.13 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 10304.1 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 10304.1 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 M06-2X/6-311G**
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.416 |
0.000 |
O2 |
-1.107 |
-0.340 |
0.000 |
N3 |
1.152 |
-0.089 |
0.000 |
H4 |
-0.264 |
1.475 |
0.000 |
H5 |
-0.810 |
-1.260 |
0.000 |
H6 |
1.865 |
0.634 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
O2 |
N3 |
H4 |
H5 |
H6 |
C1 | | 1.3407 | 1.2581 | 1.0912 | 1.8618 | 1.8780 |
O2 | 1.3407 | | 2.2735 | 2.0010 | 0.9669 | 3.1280 | N3 | 1.2581 | 2.2735 | | 2.1099 | 2.2856 | 1.0154 | H4 | 1.0912 | 2.0010 | 2.1099 | | 2.7889 | 2.2894 | H5 | 1.8618 | 0.9669 | 2.2856 | 2.7889 | | 3.2783 | H6 | 1.8780 | 3.1280 | 1.0154 | 2.2894 | 3.2783 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
O2 |
H5 |
106.445 |
|
C1 |
N3 |
H6 |
110.934 |
O2 |
C1 |
N3 |
122.012 |
|
O2 |
C1 |
H4 |
110.312 |
N3 |
C1 |
H4 |
127.675 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.199 |
|
|
|
2 |
O |
-0.344 |
|
|
|
3 |
N |
-0.440 |
|
|
|
4 |
H |
0.120 |
|
|
|
5 |
H |
0.267 |
|
|
|
6 |
H |
0.198 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.143 |
1.067 |
0.000 |
1.077 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-19.599 |
3.264 |
0.000 |
y |
3.264 |
-13.946 |
0.000 |
z |
0.000 |
0.000 |
-18.694 |
|
Traceless |
| x | y | z |
x |
-3.279 |
3.264 |
0.000 |
y |
3.264 |
5.201 |
0.000 |
z |
0.000 |
0.000 |
-1.922 |
|
Polar |
3z2-r2 | -3.845 |
x2-y2 | -5.653 |
xy | 3.264 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
4.326 |
0.060 |
0.000 |
y |
0.060 |
3.299 |
0.000 |
z |
0.000 |
0.000 |
1.779 |
<r2> (average value of r
2) Å
2
<r2> |
40.368 |
(<r2>)1/2 |
6.354 |
Jump to
S1C1
S1C2
Energy calculated at M06-2X/6-311G**
| hartrees |
Energy at 0K | -169.846142 |
Energy at 298.15K | -169.850246 |
HF Energy | -169.846142 |
Nuclear repulsion energy | 71.041460 |
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 M06-2X/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' |
3855 |
3855 |
43.52 |
|
|
|
2 |
A' |
3482 |
3482 |
4.99 |
|
|
|
3 |
A' |
3207 |
3207 |
11.27 |
|
|
|
4 |
A' |
1787 |
1787 |
290.45 |
|
|
|
5 |
A' |
1423 |
1423 |
1.56 |
|
|
|
6 |
A' |
1365 |
1365 |
28.14 |
|
|
|
7 |
A' |
1147 |
1147 |
275.49 |
|
|
|
8 |
A' |
1103 |
1103 |
30.89 |
|
|
|
9 |
A' |
607 |
607 |
39.55 |
|
|
|
10 |
A" |
1100 |
1100 |
65.71 |
|
|
|
11 |
A" |
867 |
867 |
66.06 |
|
|
|
12 |
A" |
504 |
504 |
84.77 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 10223.4 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 10223.4 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 M06-2X/6-311G**
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.440 |
0.000 |
O2 |
-1.093 |
-0.353 |
0.000 |
N3 |
1.217 |
0.124 |
0.000 |
H4 |
-0.302 |
1.485 |
0.000 |
H5 |
-0.821 |
-1.278 |
0.000 |
H6 |
1.352 |
-0.889 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
O2 |
N3 |
H4 |
H5 |
H6 |
C1 | | 1.3513 | 1.2574 | 1.0874 | 1.9045 | 1.8962 |
O2 | 1.3513 | | 2.3593 | 2.0014 | 0.9640 | 2.5035 | N3 | 1.2574 | 2.3593 | | 2.0396 | 2.4736 | 1.0222 | H4 | 1.0874 | 2.0014 | 2.0396 | | 2.8113 | 2.8936 | H5 | 1.9045 | 0.9640 | 2.4736 | 2.8113 | | 2.2074 | H6 | 1.8962 | 2.5035 | 1.0222 | 2.8936 | 2.2074 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
O2 |
H5 |
109.549 |
|
C1 |
N3 |
H6 |
112.165 |
O2 |
C1 |
N3 |
129.449 |
|
O2 |
C1 |
H4 |
109.837 |
N3 |
C1 |
H4 |
120.714 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.186 |
|
|
|
2 |
O |
-0.341 |
|
|
|
3 |
N |
-0.408 |
|
|
|
4 |
H |
0.147 |
|
|
|
5 |
H |
0.250 |
|
|
|
6 |
H |
0.166 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.936 |
-1.858 |
0.000 |
2.080 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-23.124 |
-1.969 |
0.000 |
y |
-1.969 |
-12.908 |
0.000 |
z |
0.000 |
0.000 |
-18.672 |
|
Traceless |
| x | y | z |
x |
-7.334 |
-1.969 |
0.000 |
y |
-1.969 |
7.990 |
0.000 |
z |
0.000 |
0.000 |
-0.656 |
|
Polar |
3z2-r2 | -1.312 |
x2-y2 | -10.215 |
xy | -1.969 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
4.115 |
-0.181 |
0.000 |
y |
-0.181 |
3.464 |
0.000 |
z |
0.000 |
0.000 |
1.803 |
<r2> (average value of r
2) Å
2
<r2> |
40.815 |
(<r2>)1/2 |
6.389 |