Jump to
S1C2
S1C3
Energy calculated at B3PW91/6-311G**
| | hartrees |
| Energy at 0K | -225.251224 |
| Energy at 298.15K | -225.257391 |
| HF Energy | -225.251224 |
| Nuclear repulsion energy | 123.881773 |
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 |
3712 |
3575 |
32.74 |
|
|
|
| 2 |
A |
3598 |
3465 |
3.01 |
|
|
|
| 3 |
A |
1834 |
1766 |
412.34 |
|
|
|
| 4 |
A |
1630 |
1570 |
0.37 |
|
|
|
| 5 |
A |
1181 |
1137 |
3.12 |
|
|
|
| 6 |
A |
962 |
926 |
8.00 |
|
|
|
| 7 |
A |
570 |
549 |
71.89 |
|
|
|
| 8 |
A |
473 |
456 |
2.70 |
|
|
|
| 9 |
A |
380 |
366 |
72.82 |
|
|
|
| 10 |
B |
3711 |
3574 |
28.52 |
|
|
|
| 11 |
B |
3593 |
3460 |
42.99 |
|
|
|
| 12 |
B |
1634 |
1573 |
214.64 |
|
|
|
| 13 |
B |
1425 |
1372 |
203.31 |
|
|
|
| 14 |
B |
1046 |
1008 |
23.57 |
|
|
|
| 15 |
B |
790 |
761 |
73.06 |
|
|
|
| 16 |
B |
581 |
560 |
80.02 |
|
|
|
| 17 |
B |
542 |
522 |
171.20 |
|
|
|
| 18 |
B |
444 |
427 |
161.12 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14052.4 cm
-1
Scaled (by 0.9631) Zero Point Vibrational Energy (zpe) 13533.8 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 C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.145 |
| O2 |
0.000 |
0.000 |
1.358 |
| N3 |
0.000 |
1.158 |
-0.611 |
| N4 |
0.000 |
-1.158 |
-0.611 |
| H5 |
0.205 |
1.982 |
-0.069 |
| H6 |
0.442 |
1.131 |
-1.517 |
| H7 |
-0.205 |
-1.982 |
-0.069 |
| H8 |
-0.442 |
-1.131 |
-1.517 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2130 | 1.3835 | 1.3835 | 2.0043 | 2.0584 | 2.0043 | 2.0584 |
O2 | 1.2130 | | 2.2848 | 2.2848 | 2.4509 | 3.1210 | 2.4509 | 3.1210 | N3 | 1.3835 | 2.2848 | | 2.3169 | 1.0076 | 1.0081 | 3.1939 | 2.5014 | N4 | 1.3835 | 2.2848 | 2.3169 | | 3.1939 | 2.5014 | 1.0076 | 1.0081 | H5 | 2.0043 | 2.4509 | 1.0076 | 3.1939 | | 1.6967 | 3.9857 | 3.4942 | H6 | 2.0584 | 3.1210 | 1.0081 | 2.5014 | 1.6967 | | 3.4942 | 2.4285 | H7 | 2.0043 | 2.4509 | 3.1939 | 1.0076 | 3.9857 | 3.4942 | | 1.6967 | H8 | 2.0584 | 3.1210 | 2.5014 | 1.0081 | 3.4942 | 2.4285 | 1.6967 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
112.963 |
|
C1 |
N3 |
H6 |
117.934 |
| C1 |
N4 |
H7 |
112.963 |
|
C1 |
N4 |
H8 |
117.934 |
| O2 |
C1 |
N3 |
123.142 |
|
O2 |
C1 |
N4 |
123.142 |
| N3 |
C1 |
N4 |
113.715 |
|
H5 |
N3 |
H6 |
114.650 |
| H7 |
N4 |
H8 |
114.650 |
|
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 |
0.441 |
|
|
|
| 2 |
O |
-0.394 |
|
|
|
| 3 |
N |
-0.481 |
|
|
|
| 4 |
N |
-0.481 |
|
|
|
| 5 |
H |
0.238 |
|
|
|
| 6 |
H |
0.220 |
|
|
|
| 7 |
H |
0.238 |
|
|
|
| 8 |
H |
0.220 |
|
|
|
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 |
-3.676 |
3.676 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.544 |
3.243 |
0.000 |
| y |
3.243 |
-17.531 |
0.000 |
| z |
0.000 |
0.000 |
-24.729 |
|
| Traceless |
| | x | y | z |
| x |
-3.414 |
3.243 |
0.000 |
| y |
3.243 |
7.106 |
0.000 |
| z |
0.000 |
0.000 |
-3.692 |
|
| Polar |
| 3z2-r2 | -7.384 |
| x2-y2 | -7.013 |
| xy | 3.243 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.528 |
0.166 |
0.000 |
| y |
0.166 |
4.835 |
0.000 |
| z |
0.000 |
0.000 |
4.970 |
<r2> (average value of r
2) Å
2
| <r2> |
68.313 |
| (<r2>)1/2 |
8.265 |
Jump to
S1C1
S1C3
Energy calculated at B3PW91/6-311G**
| | hartrees |
| Energy at 0K | -225.249565 |
| Energy at 298.15K | -225.255086 |
| HF Energy | -225.249565 |
| Nuclear repulsion energy | 123.917241 |
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' |
3742 |
3604 |
36.66 |
|
|
|
| 2 |
A' |
3622 |
3488 |
8.69 |
|
|
|
| 3 |
A' |
1825 |
1758 |
437.59 |
|
|
|
| 4 |
A' |
1636 |
1576 |
12.50 |
|
|
|
| 5 |
A' |
1172 |
1128 |
2.67 |
|
|
|
| 6 |
A' |
969 |
933 |
9.15 |
|
|
|
| 7 |
A' |
779 |
750 |
25.08 |
|
|
|
| 8 |
A' |
550 |
530 |
32.63 |
|
|
|
| 9 |
A' |
478 |
461 |
11.52 |
|
|
|
| 10 |
A' |
369 |
356 |
392.64 |
|
|
|
| 11 |
A" |
3739 |
3601 |
34.52 |
|
|
|
| 12 |
A" |
3612 |
3479 |
43.97 |
|
|
|
| 13 |
A" |
1626 |
1566 |
241.02 |
|
|
|
| 14 |
A" |
1427 |
1374 |
204.82 |
|
|
|
| 15 |
A" |
1011 |
974 |
19.49 |
|
|
|
| 16 |
A" |
573 |
551 |
21.54 |
|
|
|
| 17 |
A" |
406 |
391 |
49.40 |
|
|
|
| 18 |
A" |
71 |
68 |
42.97 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13802.6 cm
-1
Scaled (by 0.9631) Zero Point Vibrational Energy (zpe) 13293.3 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 B3PW91/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.008 |
0.142 |
0.000 |
| O2 |
0.034 |
1.356 |
0.000 |
| N3 |
0.034 |
-0.602 |
1.161 |
| N4 |
0.034 |
-0.602 |
-1.161 |
| H5 |
-0.146 |
-0.074 |
1.998 |
| H6 |
-0.251 |
-1.566 |
1.169 |
| H7 |
-0.146 |
-0.074 |
-1.998 |
| H8 |
-0.251 |
-1.566 |
-1.169 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2143 | 1.3788 | 1.3788 | 2.0153 | 2.0862 | 2.0153 | 2.0862 |
O2 | 1.2143 | | 2.2759 | 2.2759 | 2.4633 | 3.1604 | 2.4633 | 3.1604 | N3 | 1.3788 | 2.2759 | | 2.3216 | 1.0059 | 1.0058 | 3.2075 | 2.5379 | N4 | 1.3788 | 2.2759 | 2.3216 | | 3.2075 | 2.5379 | 1.0059 | 1.0058 | H5 | 2.0153 | 2.4633 | 1.0059 | 3.2075 | | 1.7104 | 3.9957 | 3.5029 | H6 | 2.0862 | 3.1604 | 1.0058 | 2.5379 | 1.7104 | | 3.5029 | 2.3386 | H7 | 2.0153 | 2.4633 | 3.2075 | 1.0059 | 3.9957 | 3.5029 | | 1.7104 | H8 | 2.0862 | 3.1604 | 2.5379 | 1.0058 | 3.5029 | 2.3386 | 1.7104 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
114.465 |
|
C1 |
N3 |
H6 |
121.267 |
| C1 |
N4 |
H7 |
114.465 |
|
C1 |
N4 |
H8 |
121.267 |
| O2 |
C1 |
N3 |
122.601 |
|
O2 |
C1 |
N4 |
122.601 |
| N3 |
C1 |
N4 |
114.679 |
|
H5 |
N3 |
H6 |
116.471 |
| H7 |
N4 |
H8 |
116.471 |
|
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 |
0.463 |
|
|
|
| 2 |
O |
-0.403 |
|
|
|
| 3 |
N |
-0.484 |
|
|
|
| 4 |
N |
-0.484 |
|
|
|
| 5 |
H |
0.242 |
|
|
|
| 6 |
H |
0.212 |
|
|
|
| 7 |
H |
0.242 |
|
|
|
| 8 |
H |
0.212 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.507 |
-4.031 |
0.000 |
4.304 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.149 |
1.579 |
0.000 |
| y |
1.579 |
-24.075 |
0.000 |
| z |
0.000 |
0.000 |
-16.932 |
|
| Traceless |
| | x | y | z |
| x |
-4.646 |
1.579 |
0.000 |
| y |
1.579 |
-3.034 |
0.000 |
| z |
0.000 |
0.000 |
7.680 |
|
| Polar |
| 3z2-r2 | 15.360 |
| x2-y2 | -1.074 |
| xy | 1.579 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.449 |
0.118 |
0.000 |
| y |
0.118 |
4.956 |
0.000 |
| z |
0.000 |
0.000 |
4.850 |
<r2> (average value of r
2) Å
2
| <r2> |
68.365 |
| (<r2>)1/2 |
8.268 |
Jump to
S1C1
S1C2
Energy calculated at B3PW91/6-311G**
| | hartrees |
| Energy at 0K | -225.249118 |
| Energy at 298.15K | |
| HF Energy | -225.249118 |
| Nuclear repulsion energy | 124.024140 |
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 |
A1 |
3778 |
3639 |
50.76 |
|
|
|
| 2 |
A1 |
3647 |
3513 |
6.10 |
|
|
|
| 3 |
A1 |
1819 |
1752 |
470.10 |
|
|
|
| 4 |
A1 |
1625 |
1565 |
2.31 |
|
|
|
| 5 |
A1 |
1147 |
1105 |
0.26 |
|
|
|
| 6 |
A1 |
976 |
940 |
8.07 |
|
|
|
| 7 |
A1 |
478 |
460 |
3.19 |
|
|
|
| 8 |
A2 |
370 |
356 |
0.00 |
|
|
|
| 9 |
A2 |
389i |
375i |
0.00 |
|
|
|
| 10 |
B1 |
780 |
751 |
8.15 |
|
|
|
| 11 |
B1 |
566 |
545 |
9.91 |
|
|
|
| 12 |
B1 |
263i |
253i |
478.17 |
|
|
|
| 13 |
B2 |
3776 |
3637 |
42.63 |
|
|
|
| 14 |
B2 |
3638 |
3504 |
61.75 |
|
|
|
| 15 |
B2 |
1621 |
1562 |
302.48 |
|
|
|
| 16 |
B2 |
1431 |
1378 |
208.48 |
|
|
|
| 17 |
B2 |
986 |
950 |
12.35 |
|
|
|
| 18 |
B2 |
566 |
545 |
14.56 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13275.7 cm
-1
Scaled (by 0.9631) Zero Point Vibrational Energy (zpe) 12785.9 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 C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.143 |
| O2 |
0.000 |
0.000 |
1.358 |
| N3 |
0.000 |
1.157 |
-0.597 |
| N4 |
0.000 |
-1.157 |
-0.597 |
| H5 |
0.000 |
2.020 |
-0.085 |
| H6 |
0.000 |
1.185 |
-1.600 |
| H7 |
0.000 |
-2.020 |
-0.085 |
| H8 |
0.000 |
-1.185 |
-1.600 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2159 | 1.3726 | 1.3726 | 2.0325 | 2.1068 | 2.0325 | 2.1068 |
O2 | 1.2159 | | 2.2715 | 2.2715 | 2.4824 | 3.1865 | 2.4824 | 3.1865 | N3 | 1.3726 | 2.2715 | | 2.3131 | 1.0036 | 1.0034 | 3.2173 | 2.5470 | N4 | 1.3726 | 2.2715 | 2.3131 | | 3.2173 | 2.5470 | 1.0036 | 1.0034 | H5 | 2.0325 | 2.4824 | 1.0036 | 3.2173 | | 1.7299 | 4.0395 | 3.5445 | H6 | 2.1068 | 3.1865 | 1.0034 | 2.5470 | 1.7299 | | 3.5445 | 2.3693 | H7 | 2.0325 | 2.4824 | 3.2173 | 1.0036 | 4.0395 | 3.5445 | | 1.7299 | H8 | 2.1068 | 3.1865 | 2.5470 | 1.0034 | 3.5445 | 2.3693 | 1.7299 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
116.748 |
|
C1 |
N3 |
H6 |
124.186 |
| C1 |
N4 |
H7 |
116.748 |
|
C1 |
N4 |
H8 |
124.186 |
| O2 |
C1 |
N3 |
122.583 |
|
O2 |
C1 |
N4 |
122.583 |
| N3 |
C1 |
N4 |
114.834 |
|
H5 |
N3 |
H6 |
119.066 |
| H7 |
N4 |
H8 |
119.066 |
|
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 |
0.502 |
|
|
|
| 2 |
O |
-0.413 |
|
|
|
| 3 |
N |
-0.513 |
|
|
|
| 4 |
N |
-0.513 |
|
|
|
| 5 |
H |
0.249 |
|
|
|
| 6 |
H |
0.220 |
|
|
|
| 7 |
H |
0.249 |
|
|
|
| 8 |
H |
0.220 |
|
|
|
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 |
-4.330 |
4.330 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.487 |
0.000 |
0.000 |
| y |
0.000 |
-16.267 |
0.000 |
| z |
0.000 |
0.000 |
-23.611 |
|
| Traceless |
| | x | y | z |
| x |
-5.547 |
0.000 |
0.000 |
| y |
0.000 |
8.281 |
0.000 |
| z |
0.000 |
0.000 |
-2.734 |
|
| Polar |
| 3z2-r2 | -5.468 |
| x2-y2 | -9.219 |
| 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 |
2.376 |
0.000 |
0.000 |
| y |
0.000 |
4.824 |
0.000 |
| z |
0.000 |
0.000 |
4.902 |
<r2> (average value of r
2) Å
2
| <r2> |
68.301 |
| (<r2>)1/2 |
8.264 |