Jump to
S1C2
S1C3
Energy calculated at B1B95/6-31+G**
| | hartrees |
| Energy at 0K | -225.203629 |
| Energy at 298.15K | -225.209734 |
| HF Energy | -225.203629 |
| Nuclear repulsion energy | 123.820990 |
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 B1B95/6-31+G**
| 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 |
3746 |
3583 |
49.55 |
|
|
|
| 2 |
A |
3621 |
3464 |
4.40 |
|
|
|
| 3 |
A |
1825 |
1746 |
497.97 |
|
|
|
| 4 |
A |
1631 |
1560 |
0.12 |
|
|
|
| 5 |
A |
1172 |
1121 |
1.81 |
|
|
|
| 6 |
A |
972 |
930 |
10.31 |
|
|
|
| 7 |
A |
541 |
517 |
63.31 |
|
|
|
| 8 |
A |
470 |
450 |
2.65 |
|
|
|
| 9 |
A |
366 |
350 |
74.17 |
|
|
|
| 10 |
B |
3746 |
3583 |
38.34 |
|
|
|
| 11 |
B |
3616 |
3459 |
58.84 |
|
|
|
| 12 |
B |
1636 |
1565 |
249.08 |
|
|
|
| 13 |
B |
1432 |
1370 |
219.87 |
|
|
|
| 14 |
B |
1041 |
996 |
18.64 |
|
|
|
| 15 |
B |
775 |
742 |
54.08 |
|
|
|
| 16 |
B |
575 |
550 |
74.12 |
|
|
|
| 17 |
B |
539 |
516 |
158.90 |
|
|
|
| 18 |
B |
442 |
423 |
209.41 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14073.1 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 13462.3 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 B1B95/6-31+G**
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.139 |
| O2 |
0.000 |
0.000 |
1.359 |
| N3 |
0.000 |
1.159 |
-0.608 |
| N4 |
0.000 |
-1.159 |
-0.608 |
| H5 |
0.191 |
1.987 |
-0.066 |
| H6 |
0.413 |
1.145 |
-1.528 |
| H7 |
-0.191 |
-1.987 |
-0.066 |
| H8 |
-0.413 |
-1.145 |
-1.528 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2201 | 1.3793 | 1.3793 | 2.0064 | 2.0635 | 2.0064 | 2.0635 |
O2 | 1.2201 | | 2.2837 | 2.2837 | 2.4525 | 3.1326 | 2.4525 | 3.1326 | N3 | 1.3793 | 2.2837 | | 2.3184 | 1.0076 | 1.0078 | 3.1980 | 2.5145 | N4 | 1.3793 | 2.2837 | 2.3184 | | 3.1980 | 2.5145 | 1.0076 | 1.0078 | H5 | 2.0064 | 2.4525 | 1.0076 | 3.1980 | | 1.7013 | 3.9917 | 3.5079 | H6 | 2.0635 | 3.1326 | 1.0078 | 2.5145 | 1.7013 | | 3.5079 | 2.4335 | H7 | 2.0064 | 2.4525 | 3.1980 | 1.0076 | 3.9917 | 3.5079 | | 1.7013 | H8 | 2.0635 | 3.1326 | 2.5145 | 1.0078 | 3.5079 | 2.4335 | 1.7013 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
113.485 |
|
C1 |
N3 |
H6 |
118.817 |
| C1 |
N4 |
H7 |
113.485 |
|
C1 |
N4 |
H8 |
118.817 |
| O2 |
C1 |
N3 |
122.815 |
|
O2 |
C1 |
N4 |
122.815 |
| N3 |
C1 |
N4 |
114.371 |
|
H5 |
N3 |
H6 |
115.164 |
| H7 |
N4 |
H8 |
115.164 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.498 |
|
|
|
| 2 |
O |
-0.542 |
|
|
|
| 3 |
N |
-0.597 |
|
|
|
| 4 |
N |
-0.597 |
|
|
|
| 5 |
H |
0.323 |
|
|
|
| 6 |
H |
0.296 |
|
|
|
| 7 |
H |
0.323 |
|
|
|
| 8 |
H |
0.296 |
|
|
|
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 |
-3.958 |
3.958 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.570 |
3.244 |
0.000 |
| y |
3.244 |
-17.738 |
0.000 |
| z |
0.000 |
0.000 |
-25.423 |
|
| Traceless |
| | x | y | z |
| x |
-3.989 |
3.244 |
0.000 |
| y |
3.244 |
7.758 |
0.000 |
| z |
0.000 |
0.000 |
-3.769 |
|
| Polar |
| 3z2-r2 | -7.538 |
| x2-y2 | -7.832 |
| xy | 3.244 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.490 |
0.055 |
0.000 |
| y |
0.055 |
5.306 |
0.000 |
| z |
0.000 |
0.000 |
5.693 |
<r2> (average value of r
2) Å
2
| <r2> |
68.802 |
| (<r2>)1/2 |
8.295 |
Jump to
S1C1
S1C3
Energy calculated at B1B95/6-31+G**
| | hartrees |
| Energy at 0K | -225.198474 |
| Energy at 298.15K | |
| HF Energy | -225.198474 |
| Nuclear repulsion energy | 124.020352 |
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 B1B95/6-31+G**
| 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' |
3792 |
3628 |
57.50 |
|
|
|
| 2 |
A' |
3659 |
3500 |
10.74 |
|
|
|
| 3 |
A' |
1824 |
1745 |
539.36 |
|
|
|
| 4 |
A' |
1640 |
1569 |
9.35 |
|
|
|
| 5 |
A' |
1164 |
1114 |
1.34 |
|
|
|
| 6 |
A' |
985 |
942 |
10.45 |
|
|
|
| 7 |
A' |
773 |
739 |
15.45 |
|
|
|
| 8 |
A' |
553 |
529 |
26.20 |
|
|
|
| 9 |
A' |
475 |
454 |
6.86 |
|
|
|
| 10 |
A' |
310 |
296 |
443.45 |
|
|
|
| 11 |
A" |
3790 |
3625 |
46.61 |
|
|
|
| 12 |
A" |
3650 |
3492 |
64.63 |
|
|
|
| 13 |
A" |
1636 |
1565 |
296.67 |
|
|
|
| 14 |
A" |
1444 |
1381 |
212.06 |
|
|
|
| 15 |
A" |
1011 |
967 |
13.71 |
|
|
|
| 16 |
A" |
568 |
544 |
18.49 |
|
|
|
| 17 |
A" |
393 |
376 |
31.49 |
|
|
|
| 18 |
A" |
116i |
111i |
37.44 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13775.0 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 13177.2 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 B1B95/6-31+G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.005 |
0.136 |
0.000 |
| O2 |
0.029 |
1.356 |
0.000 |
| N3 |
0.029 |
-0.598 |
1.159 |
| N4 |
0.029 |
-0.598 |
-1.159 |
| H5 |
-0.123 |
-0.071 |
2.001 |
| H6 |
-0.208 |
-1.574 |
1.179 |
| H7 |
-0.123 |
-0.071 |
-2.001 |
| H8 |
-0.208 |
-1.574 |
-1.179 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2203 | 1.3724 | 1.3724 | 2.0161 | 2.0878 | 2.0161 | 2.0878 |
O2 | 1.2203 | | 2.2721 | 2.2721 | 2.4627 | 3.1670 | 2.4627 | 3.1670 | N3 | 1.3724 | 2.2721 | | 2.3188 | 1.0047 | 1.0043 | 3.2080 | 2.5449 | N4 | 1.3724 | 2.2721 | 2.3188 | | 3.2080 | 2.5449 | 1.0047 | 1.0043 | H5 | 2.0161 | 2.4627 | 1.0047 | 3.2080 | | 1.7152 | 4.0028 | 3.5186 | H6 | 2.0878 | 3.1670 | 1.0043 | 2.5449 | 1.7152 | | 3.5186 | 2.3580 | H7 | 2.0161 | 2.4627 | 3.2080 | 1.0047 | 4.0028 | 3.5186 | | 1.7152 | H8 | 2.0878 | 3.1670 | 2.5449 | 1.0043 | 3.5186 | 2.3580 | 1.7152 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
115.150 |
|
C1 |
N3 |
H6 |
122.148 |
| C1 |
N4 |
H7 |
115.150 |
|
C1 |
N4 |
H8 |
122.148 |
| O2 |
C1 |
N3 |
122.300 |
|
O2 |
C1 |
N4 |
122.300 |
| N3 |
C1 |
N4 |
115.307 |
|
H5 |
N3 |
H6 |
117.244 |
| H7 |
N4 |
H8 |
117.244 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.544 |
|
|
|
| 2 |
O |
-0.566 |
|
|
|
| 3 |
N |
-0.606 |
|
|
|
| 4 |
N |
-0.606 |
|
|
|
| 5 |
H |
0.328 |
|
|
|
| 6 |
H |
0.289 |
|
|
|
| 7 |
H |
0.328 |
|
|
|
| 8 |
H |
0.289 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.308 |
-4.337 |
0.000 |
4.530 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.201 |
1.402 |
0.000 |
| y |
1.402 |
-24.742 |
0.000 |
| z |
0.000 |
0.000 |
-17.071 |
|
| Traceless |
| | x | y | z |
| x |
-5.294 |
1.402 |
0.000 |
| y |
1.402 |
-3.106 |
0.000 |
| z |
0.000 |
0.000 |
8.400 |
|
| Polar |
| 3z2-r2 | 16.801 |
| x2-y2 | -1.459 |
| xy | 1.402 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.435 |
0.031 |
0.000 |
| y |
0.031 |
5.560 |
0.000 |
| z |
0.000 |
0.000 |
5.251 |
<r2> (average value of r
2) Å
2
| <r2> |
68.696 |
| (<r2>)1/2 |
8.288 |
Jump to
S1C1
S1C2
Energy calculated at B1B95/6-31+G**
| | hartrees |
| Energy at 0K | -225.198253 |
| Energy at 298.15K | |
| HF Energy | -225.198253 |
| Nuclear repulsion energy | 124.084737 |
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 B1B95/6-31+G**
| 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 |
3816 |
3650 |
68.76 |
|
|
|
| 2 |
A1 |
3676 |
3517 |
8.49 |
|
|
|
| 3 |
A1 |
1821 |
1742 |
573.45 |
|
|
|
| 4 |
A1 |
1633 |
1563 |
2.03 |
|
|
|
| 5 |
A1 |
1149 |
1099 |
0.01 |
|
|
|
| 6 |
A1 |
989 |
946 |
9.31 |
|
|
|
| 7 |
A1 |
476 |
455 |
3.24 |
|
|
|
| 8 |
A2 |
372 |
356 |
0.00 |
|
|
|
| 9 |
A2 |
349i |
334i |
0.00 |
|
|
|
| 10 |
B1 |
773 |
739 |
5.92 |
|
|
|
| 11 |
B1 |
567 |
543 |
9.61 |
|
|
|
| 12 |
B1 |
217i |
207i |
511.21 |
|
|
|
| 13 |
B2 |
3814 |
3648 |
50.63 |
|
|
|
| 14 |
B2 |
3668 |
3509 |
82.24 |
|
|
|
| 15 |
B2 |
1634 |
1563 |
344.02 |
|
|
|
| 16 |
B2 |
1445 |
1382 |
216.04 |
|
|
|
| 17 |
B2 |
993 |
950 |
9.40 |
|
|
|
| 18 |
B2 |
563 |
538 |
13.63 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13411.1 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 12829.0 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 B1B95/6-31+G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.137 |
| O2 |
0.000 |
0.000 |
1.358 |
| N3 |
0.000 |
1.156 |
-0.595 |
| N4 |
0.000 |
-1.156 |
-0.595 |
| H5 |
0.000 |
2.018 |
-0.081 |
| H6 |
0.000 |
1.188 |
-1.597 |
| H7 |
0.000 |
-2.018 |
-0.081 |
| H8 |
0.000 |
-1.188 |
-1.597 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2210 | 1.3685 | 1.3685 | 2.0293 | 2.1020 | 2.0293 | 2.1020 |
O2 | 1.2210 | | 2.2695 | 2.2695 | 2.4779 | 3.1850 | 2.4779 | 3.1850 | N3 | 1.3685 | 2.2695 | | 2.3126 | 1.0033 | 1.0028 | 3.2154 | 2.5495 | N4 | 1.3685 | 2.2695 | 2.3126 | | 3.2154 | 2.5495 | 1.0033 | 1.0028 | H5 | 2.0293 | 2.4779 | 1.0033 | 3.2154 | | 1.7289 | 4.0353 | 3.5463 | H6 | 2.1020 | 3.1850 | 1.0028 | 2.5495 | 1.7289 | | 3.5463 | 2.3758 | H7 | 2.0293 | 2.4779 | 3.2154 | 1.0033 | 4.0353 | 3.5463 | | 1.7289 | H8 | 2.1020 | 3.1850 | 2.5495 | 1.0028 | 3.5463 | 2.3758 | 1.7289 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
116.820 |
|
C1 |
N3 |
H6 |
124.137 |
| C1 |
N4 |
H7 |
116.820 |
|
C1 |
N4 |
H8 |
124.137 |
| O2 |
C1 |
N3 |
122.332 |
|
O2 |
C1 |
N4 |
122.332 |
| N3 |
C1 |
N4 |
115.337 |
|
H5 |
N3 |
H6 |
119.044 |
| H7 |
N4 |
H8 |
119.044 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.602 |
|
|
|
| 2 |
O |
-0.587 |
|
|
|
| 3 |
N |
-0.640 |
|
|
|
| 4 |
N |
-0.640 |
|
|
|
| 5 |
H |
0.333 |
|
|
|
| 6 |
H |
0.299 |
|
|
|
| 7 |
H |
0.333 |
|
|
|
| 8 |
H |
0.299 |
|
|
|
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 |
-4.558 |
4.558 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.483 |
0.000 |
0.000 |
| y |
0.000 |
-16.609 |
0.000 |
| z |
0.000 |
0.000 |
-24.409 |
|
| Traceless |
| | x | y | z |
| x |
-5.974 |
0.000 |
0.000 |
| y |
0.000 |
8.837 |
0.000 |
| z |
0.000 |
0.000 |
-2.863 |
|
| Polar |
| 3z2-r2 | -5.726 |
| x2-y2 | -9.874 |
| 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 |
3.396 |
0.000 |
0.000 |
| y |
0.000 |
5.212 |
0.000 |
| z |
0.000 |
0.000 |
5.473 |
<r2> (average value of r
2) Å
2
| <r2> |
68.671 |
| (<r2>)1/2 |
8.287 |