Jump to
S1C2
S1C3
Energy calculated at M06-2X/6-311G**
| hartrees |
Energy at 0K | -225.242182 |
Energy at 298.15K | -225.248440 |
HF Energy | -225.242182 |
Nuclear repulsion energy | 124.024635 |
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 |
3728 |
3728 |
50.03 |
|
|
|
2 |
A |
3616 |
3616 |
5.17 |
|
|
|
3 |
A |
1870 |
1870 |
459.06 |
|
|
|
4 |
A |
1633 |
1633 |
1.36 |
|
|
|
5 |
A |
1190 |
1190 |
2.86 |
|
|
|
6 |
A |
974 |
974 |
9.59 |
|
|
|
7 |
A |
591 |
591 |
97.26 |
|
|
|
8 |
A |
482 |
482 |
1.54 |
|
|
|
9 |
A |
409 |
409 |
67.38 |
|
|
|
10 |
B |
3729 |
3729 |
30.09 |
|
|
|
11 |
B |
3611 |
3611 |
64.94 |
|
|
|
12 |
B |
1640 |
1640 |
238.50 |
|
|
|
13 |
B |
1431 |
1431 |
205.96 |
|
|
|
14 |
B |
1060 |
1060 |
21.48 |
|
|
|
15 |
B |
803 |
803 |
88.75 |
|
|
|
16 |
B |
593 |
593 |
76.30 |
|
|
|
17 |
B |
547 |
547 |
227.42 |
|
|
|
18 |
B |
469 |
469 |
108.12 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14187.4 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 14187.4 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 C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.000 |
0.148 |
O2 |
0.000 |
0.000 |
1.355 |
N3 |
0.000 |
1.158 |
-0.612 |
N4 |
0.000 |
-1.158 |
-0.612 |
H5 |
0.205 |
1.982 |
-0.069 |
H6 |
0.458 |
1.121 |
-1.510 |
H7 |
-0.205 |
-1.982 |
-0.069 |
H8 |
-0.458 |
-1.121 |
-1.510 |
Atom - Atom Distances (Å)
|
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.2074 | 1.3845 | 1.3845 | 2.0041 | 2.0522 | 2.0041 | 2.0522 |
O2 | 1.2074 | | 2.2823 | 2.2823 | 2.4488 | 3.1098 | 2.4488 | 3.1098 | N3 | 1.3845 | 2.2823 | | 2.3151 | 1.0082 | 1.0081 | 3.1926 | 2.4911 | N4 | 1.3845 | 2.2823 | 2.3151 | | 3.1926 | 2.4911 | 1.0082 | 1.0081 | H5 | 2.0041 | 2.4488 | 1.0082 | 3.1926 | | 1.6973 | 3.9847 | 3.4844 | H6 | 2.0522 | 3.1098 | 1.0081 | 2.4911 | 1.6973 | | 3.4844 | 2.4212 | H7 | 2.0041 | 2.4488 | 3.1926 | 1.0082 | 3.9847 | 3.4844 | | 1.6973 | H8 | 2.0522 | 3.1098 | 2.4911 | 1.0081 | 3.4844 | 2.4212 | 1.6973 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
N3 |
H5 |
112.823 |
|
C1 |
N3 |
H6 |
117.254 |
C1 |
N4 |
H7 |
112.823 |
|
C1 |
N4 |
H8 |
117.254 |
O2 |
C1 |
N3 |
123.272 |
|
O2 |
C1 |
N4 |
123.272 |
N3 |
C1 |
N4 |
113.455 |
|
H5 |
N3 |
H6 |
114.651 |
H7 |
N4 |
H8 |
114.651 |
|
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 |
0.495 |
|
|
|
2 |
O |
-0.410 |
|
|
|
3 |
N |
-0.533 |
|
|
|
4 |
N |
-0.533 |
|
|
|
5 |
H |
0.253 |
|
|
|
6 |
H |
0.237 |
|
|
|
7 |
H |
0.253 |
|
|
|
8 |
H |
0.237 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.000 |
0.000 |
-3.610 |
3.610 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-24.676 |
3.341 |
0.000 |
y |
3.341 |
-17.791 |
0.000 |
z |
0.000 |
0.000 |
-25.004 |
|
Traceless |
| x | y | z |
x |
-3.278 |
3.341 |
0.000 |
y |
3.341 |
7.049 |
0.000 |
z |
0.000 |
0.000 |
-3.771 |
|
Polar |
3z2-r2 | -7.542 |
x2-y2 | -6.885 |
xy | 3.341 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.516 |
0.158 |
0.000 |
y |
0.158 |
4.684 |
0.000 |
z |
0.000 |
0.000 |
4.895 |
<r2> (average value of r
2) Å
2
<r2> |
68.305 |
(<r2>)1/2 |
8.265 |
Jump to
S1C1
S1C3
Energy calculated at M06-2X/6-311G**
| hartrees |
Energy at 0K | -225.240314 |
Energy at 298.15K | -225.245932 |
HF Energy | -225.240314 |
Nuclear repulsion energy | 124.084979 |
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' |
3761 |
3761 |
56.63 |
|
|
|
2 |
A' |
3640 |
3640 |
14.42 |
|
|
|
3 |
A' |
1856 |
1856 |
491.82 |
|
|
|
4 |
A' |
1640 |
1640 |
15.29 |
|
|
|
5 |
A' |
1180 |
1180 |
2.63 |
|
|
|
6 |
A' |
981 |
981 |
11.46 |
|
|
|
7 |
A' |
789 |
789 |
30.65 |
|
|
|
8 |
A' |
556 |
556 |
32.30 |
|
|
|
9 |
A' |
488 |
488 |
13.80 |
|
|
|
10 |
A' |
382 |
382 |
410.52 |
|
|
|
11 |
A" |
3759 |
3759 |
37.46 |
|
|
|
12 |
A" |
3631 |
3631 |
64.87 |
|
|
|
13 |
A" |
1632 |
1632 |
272.34 |
|
|
|
14 |
A" |
1434 |
1434 |
205.54 |
|
|
|
15 |
A" |
1020 |
1020 |
17.09 |
|
|
|
16 |
A" |
585 |
585 |
24.04 |
|
|
|
17 |
A" |
417 |
417 |
50.45 |
|
|
|
18 |
A" |
95 |
95 |
43.79 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13922.2 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 13922.2 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 M06-2X/6-311G**
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.009 |
0.144 |
0.000 |
O2 |
0.034 |
1.353 |
0.000 |
N3 |
0.034 |
-0.601 |
1.159 |
N4 |
0.034 |
-0.601 |
-1.159 |
H5 |
-0.146 |
-0.074 |
1.997 |
H6 |
-0.254 |
-1.565 |
1.161 |
H7 |
-0.146 |
-0.074 |
-1.997 |
H8 |
-0.254 |
-1.565 |
-1.161 |
Atom - Atom Distances (Å)
|
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.2092 | 1.3787 | 1.3787 | 2.0153 | 2.0828 | 2.0153 | 2.0828 |
O2 | 1.2092 | | 2.2725 | 2.2725 | 2.4616 | 3.1537 | 2.4616 | 3.1537 | N3 | 1.3787 | 2.2725 | | 2.3189 | 1.0062 | 1.0055 | 3.2057 | 2.5292 | N4 | 1.3787 | 2.2725 | 2.3189 | | 3.2057 | 2.5292 | 1.0062 | 1.0055 | H5 | 2.0153 | 2.4616 | 1.0062 | 3.2057 | | 1.7125 | 3.9949 | 3.4944 | H6 | 2.0828 | 3.1537 | 1.0055 | 2.5292 | 1.7125 | | 3.4944 | 2.3225 | H7 | 2.0153 | 2.4616 | 3.2057 | 1.0062 | 3.9949 | 3.4944 | | 1.7125 | H8 | 2.0828 | 3.1537 | 2.5292 | 1.0055 | 3.4944 | 2.3225 | 1.7125 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
N3 |
H5 |
114.445 |
|
C1 |
N3 |
H6 |
120.962 |
C1 |
N4 |
H7 |
114.445 |
|
C1 |
N4 |
H8 |
120.962 |
O2 |
C1 |
N3 |
122.702 |
|
O2 |
C1 |
N4 |
122.702 |
N3 |
C1 |
N4 |
114.486 |
|
H5 |
N3 |
H6 |
116.692 |
H7 |
N4 |
H8 |
116.692 |
|
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 |
0.519 |
|
|
|
2 |
O |
-0.421 |
|
|
|
3 |
N |
-0.537 |
|
|
|
4 |
N |
-0.537 |
|
|
|
5 |
H |
0.258 |
|
|
|
6 |
H |
0.230 |
|
|
|
7 |
H |
0.258 |
|
|
|
8 |
H |
0.230 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-1.547 |
-4.021 |
0.000 |
4.308 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-25.343 |
1.628 |
0.000 |
y |
1.628 |
-24.265 |
0.000 |
z |
0.000 |
0.000 |
-17.138 |
|
Traceless |
| x | y | z |
x |
-4.641 |
1.628 |
0.000 |
y |
1.628 |
-3.025 |
0.000 |
z |
0.000 |
0.000 |
7.666 |
|
Polar |
3z2-r2 | 15.331 |
x2-y2 | -1.077 |
xy | 1.628 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.433 |
0.116 |
0.000 |
y |
0.116 |
4.871 |
0.000 |
z |
0.000 |
0.000 |
4.695 |
<r2> (average value of r
2) Å
2
<r2> |
68.335 |
(<r2>)1/2 |
8.266 |
Jump to
S1C1
S1C2
Energy calculated at M06-2X/6-311G**
| hartrees |
Energy at 0K | -225.239806 |
Energy at 298.15K | |
HF Energy | -225.239806 |
Nuclear repulsion energy | 124.199320 |
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 |
A1 |
3808 |
3808 |
77.42 |
|
|
|
2 |
A1 |
3677 |
3677 |
9.63 |
|
|
|
3 |
A1 |
1847 |
1847 |
531.08 |
|
|
|
4 |
A1 |
1629 |
1629 |
5.13 |
|
|
|
5 |
A1 |
1156 |
1156 |
0.18 |
|
|
|
6 |
A1 |
988 |
988 |
10.27 |
|
|
|
7 |
A1 |
489 |
489 |
2.72 |
|
|
|
8 |
A2 |
373 |
373 |
0.00 |
|
|
|
9 |
A2 |
409i |
409i |
0.00 |
|
|
|
10 |
B1 |
789 |
789 |
10.99 |
|
|
|
11 |
B1 |
566 |
566 |
13.01 |
|
|
|
12 |
B1 |
279i |
279i |
498.10 |
|
|
|
13 |
B2 |
3806 |
3806 |
39.50 |
|
|
|
14 |
B2 |
3668 |
3668 |
92.70 |
|
|
|
15 |
B2 |
1628 |
1628 |
338.48 |
|
|
|
16 |
B2 |
1438 |
1438 |
209.55 |
|
|
|
17 |
B2 |
995 |
995 |
9.83 |
|
|
|
18 |
B2 |
577 |
577 |
15.30 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13372.6 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 13372.6 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 C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.000 |
0.145 |
O2 |
0.000 |
0.000 |
1.356 |
N3 |
0.000 |
1.155 |
-0.596 |
N4 |
0.000 |
-1.155 |
-0.596 |
H5 |
0.000 |
2.019 |
-0.086 |
H6 |
0.000 |
1.176 |
-1.599 |
H7 |
0.000 |
-2.019 |
-0.086 |
H8 |
0.000 |
-1.176 |
-1.599 |
Atom - Atom Distances (Å)
|
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.2111 | 1.3722 | 1.3722 | 2.0326 | 2.1034 | 2.0326 | 2.1034 |
O2 | 1.2111 | | 2.2682 | 2.2682 | 2.4814 | 3.1804 | 2.4814 | 3.1804 | N3 | 1.3722 | 2.2682 | | 2.3096 | 1.0040 | 1.0030 | 3.2150 | 2.5374 | N4 | 1.3722 | 2.2682 | 2.3096 | | 3.2150 | 2.5374 | 1.0040 | 1.0030 | H5 | 2.0326 | 2.4814 | 1.0040 | 3.2150 | | 1.7322 | 4.0389 | 3.5356 | H6 | 2.1034 | 3.1804 | 1.0030 | 2.5374 | 1.7322 | | 3.5356 | 2.3521 | H7 | 2.0326 | 2.4814 | 3.2150 | 1.0040 | 4.0389 | 3.5356 | | 1.7322 | H8 | 2.1034 | 3.1804 | 2.5374 | 1.0030 | 3.5356 | 2.3521 | 1.7322 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
N3 |
H5 |
116.763 |
|
C1 |
N3 |
H6 |
123.906 |
C1 |
N4 |
H7 |
116.763 |
|
C1 |
N4 |
H8 |
123.906 |
O2 |
C1 |
N3 |
122.691 |
|
O2 |
C1 |
N4 |
122.691 |
N3 |
C1 |
N4 |
114.617 |
|
H5 |
N3 |
H6 |
119.331 |
H7 |
N4 |
H8 |
119.331 |
|
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 |
0.558 |
|
|
|
2 |
O |
-0.430 |
|
|
|
3 |
N |
-0.569 |
|
|
|
4 |
N |
-0.569 |
|
|
|
5 |
H |
0.266 |
|
|
|
6 |
H |
0.239 |
|
|
|
7 |
H |
0.266 |
|
|
|
8 |
H |
0.239 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.000 |
0.000 |
-4.340 |
4.340 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-25.696 |
0.000 |
0.000 |
y |
0.000 |
-16.446 |
0.000 |
z |
0.000 |
0.000 |
-23.785 |
|
Traceless |
| x | y | z |
x |
-5.580 |
0.000 |
0.000 |
y |
0.000 |
8.294 |
0.000 |
z |
0.000 |
0.000 |
-2.714 |
|
Polar |
3z2-r2 | -5.429 |
x2-y2 | -9.250 |
xy | 0.000 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.366 |
0.000 |
0.000 |
y |
0.000 |
4.672 |
0.000 |
z |
0.000 |
0.000 |
4.815 |
<r2> (average value of r
2) Å
2
<r2> |
68.258 |
(<r2>)1/2 |
8.262 |