Jump to
S1C2
S1C3
Energy calculated at B3LYP/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -225.312023 |
| Energy at 298.15K | -225.318090 |
| HF Energy | -225.312023 |
| Nuclear repulsion energy | 123.280609 |
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 B3LYP/aug-cc-pVDZ
| 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 |
3686 |
3577 |
38.21 |
|
|
|
| 2 |
A |
3567 |
3462 |
3.48 |
|
|
|
| 3 |
A |
1774 |
1721 |
445.24 |
|
|
|
| 4 |
A |
1615 |
1567 |
0.66 |
|
|
|
| 5 |
A |
1167 |
1133 |
4.95 |
|
|
|
| 6 |
A |
952 |
924 |
10.08 |
|
|
|
| 7 |
A |
519 |
504 |
47.33 |
|
|
|
| 8 |
A |
473 |
459 |
2.77 |
|
|
|
| 9 |
A |
359 |
349 |
71.02 |
|
|
|
| 10 |
B |
3686 |
3577 |
33.97 |
|
|
|
| 11 |
B |
3562 |
3456 |
46.06 |
|
|
|
| 12 |
B |
1617 |
1569 |
191.16 |
|
|
|
| 13 |
B |
1405 |
1363 |
207.83 |
|
|
|
| 14 |
B |
1037 |
1006 |
26.49 |
|
|
|
| 15 |
B |
766 |
743 |
40.54 |
|
|
|
| 16 |
B |
573 |
556 |
58.83 |
|
|
|
| 17 |
B |
528 |
512 |
129.55 |
|
|
|
| 18 |
B |
421 |
408 |
199.13 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13852.5 cm
-1
Scaled (by 0.9704) Zero Point Vibrational Energy (zpe) 13442.5 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 B3LYP/aug-cc-pVDZ
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.141 |
| O2 |
0.000 |
0.000 |
1.364 |
| N3 |
-0.116 |
1.160 |
-0.611 |
| N4 |
0.116 |
-1.160 |
-0.611 |
| H5 |
0.000 |
2.006 |
-0.070 |
| H6 |
0.298 |
1.181 |
-1.533 |
| H7 |
0.000 |
-2.006 |
-0.070 |
| H8 |
-0.298 |
-1.181 |
-1.533 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2233 | 1.3871 | 1.3871 | 2.0173 | 2.0703 | 2.0173 | 2.0703 |
O2 | 1.2233 | | 2.2935 | 2.2935 | 2.4663 | 3.1431 | 2.4663 | 3.1431 | N3 | 1.3871 | 2.2935 | | 2.3313 | 1.0110 | 1.0113 | 3.2140 | 2.5224 | N4 | 1.3871 | 2.2935 | 2.3313 | | 3.2140 | 2.5224 | 1.0110 | 1.0113 | H5 | 2.0173 | 2.4663 | 1.0110 | 3.2140 | | 1.7061 | 4.0124 | 3.5194 | H6 | 2.0703 | 3.1431 | 1.0113 | 2.5224 | 1.7061 | | 3.5194 | 2.4358 | H7 | 2.0173 | 2.4663 | 3.2140 | 1.0110 | 4.0124 | 3.5194 | | 1.7061 | H8 | 2.0703 | 3.1431 | 2.5224 | 1.0113 | 3.5194 | 2.4358 | 1.7061 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
113.603 |
|
C1 |
N3 |
H6 |
118.512 |
| C1 |
N4 |
H7 |
113.603 |
|
C1 |
N4 |
H8 |
118.512 |
| O2 |
C1 |
N3 |
122.825 |
|
O2 |
C1 |
N4 |
122.825 |
| N3 |
C1 |
N4 |
114.351 |
|
H5 |
N3 |
H6 |
115.045 |
| H7 |
N4 |
H8 |
115.045 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.711 |
|
|
|
| 2 |
O |
-0.487 |
|
|
|
| 3 |
N |
0.081 |
|
|
|
| 4 |
N |
0.081 |
|
|
|
| 5 |
H |
-0.066 |
|
|
|
| 6 |
H |
-0.128 |
|
|
|
| 7 |
H |
-0.066 |
|
|
|
| 8 |
H |
-0.128 |
|
|
|
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 |
-3.848 |
3.848 |
| CHELPG |
0.000 |
0.000 |
0.000 |
0.000 |
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.128 |
2.250 |
0.000 |
| y |
2.250 |
-17.661 |
0.000 |
| z |
0.000 |
0.000 |
-25.811 |
|
| Traceless |
| | x | y | z |
| x |
-4.392 |
2.250 |
0.000 |
| y |
2.250 |
8.308 |
0.000 |
| z |
0.000 |
0.000 |
-3.917 |
|
| Polar |
| 3z2-r2 | -7.834 |
| x2-y2 | -8.467 |
| xy | 2.250 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.018 |
-0.119 |
0.000 |
| y |
-0.119 |
6.112 |
0.000 |
| z |
0.000 |
0.000 |
6.184 |
<r2> (average value of r
2) Å
2
| <r2> |
69.475 |
| (<r2>)1/2 |
8.335 |
Jump to
S1C1
S1C3
Energy calculated at B3LYP/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -225.310916 |
| Energy at 298.15K | |
| HF Energy | -225.310916 |
| Nuclear repulsion energy | 123.362673 |
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 B3LYP/aug-cc-pVDZ
| 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' |
3724 |
3613 |
43.95 |
|
|
|
| 2 |
A' |
3595 |
3489 |
5.87 |
|
|
|
| 3 |
A' |
1762 |
1710 |
478.67 |
|
|
|
| 4 |
A' |
1620 |
1572 |
5.77 |
|
|
|
| 5 |
A' |
1152 |
1118 |
3.39 |
|
|
|
| 6 |
A' |
961 |
933 |
10.95 |
|
|
|
| 7 |
A' |
762 |
740 |
10.41 |
|
|
|
| 8 |
A' |
547 |
530 |
19.40 |
|
|
|
| 9 |
A' |
475 |
460 |
5.74 |
|
|
|
| 10 |
A' |
272 |
264 |
377.22 |
|
|
|
| 11 |
A" |
3722 |
3611 |
40.93 |
|
|
|
| 12 |
A" |
3586 |
3480 |
54.99 |
|
|
|
| 13 |
A" |
1613 |
1565 |
231.28 |
|
|
|
| 14 |
A" |
1410 |
1368 |
210.25 |
|
|
|
| 15 |
A" |
999 |
970 |
20.30 |
|
|
|
| 16 |
A" |
565 |
548 |
18.06 |
|
|
|
| 17 |
A" |
385 |
374 |
21.82 |
|
|
|
| 18 |
A" |
136i |
132i |
35.78 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13505.7 cm
-1
Scaled (by 0.9704) Zero Point Vibrational Energy (zpe) 13106.0 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 B3LYP/aug-cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.005 |
0.138 |
0.000 |
| O2 |
0.028 |
1.363 |
0.000 |
| N3 |
0.028 |
-0.601 |
1.166 |
| N4 |
0.028 |
-0.601 |
-1.166 |
| H5 |
-0.120 |
-0.078 |
2.016 |
| H6 |
-0.201 |
-1.583 |
1.181 |
| H7 |
-0.120 |
-0.078 |
-2.016 |
| H8 |
-0.201 |
-1.583 |
-1.181 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2254 | 1.3808 | 1.3808 | 2.0311 | 2.0977 | 2.0311 | 2.0977 |
O2 | 1.2254 | | 2.2845 | 2.2845 | 2.4824 | 3.1828 | 2.4824 | 3.1828 | N3 | 1.3808 | 2.2845 | | 2.3319 | 1.0087 | 1.0087 | 3.2277 | 2.5541 | N4 | 1.3808 | 2.2845 | 2.3319 | | 3.2277 | 2.5541 | 1.0087 | 1.0087 | H5 | 2.0311 | 2.4824 | 1.0087 | 3.2277 | | 1.7234 | 4.0314 | 3.5339 | H6 | 2.0977 | 3.1828 | 1.0087 | 2.5541 | 1.7234 | | 3.5339 | 2.3611 | H7 | 2.0311 | 2.4824 | 3.2277 | 1.0087 | 4.0314 | 3.5339 | | 1.7234 | H8 | 2.0977 | 3.1828 | 2.5541 | 1.0087 | 3.5339 | 2.3611 | 1.7234 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
115.548 |
|
C1 |
N3 |
H6 |
122.006 |
| C1 |
N4 |
H7 |
115.548 |
|
C1 |
N4 |
H8 |
122.006 |
| O2 |
C1 |
N3 |
122.350 |
|
O2 |
C1 |
N4 |
122.350 |
| N3 |
C1 |
N4 |
115.215 |
|
H5 |
N3 |
H6 |
117.363 |
| H7 |
N4 |
H8 |
117.363 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.808 |
|
|
|
| 2 |
O |
-0.507 |
|
|
|
| 3 |
N |
0.076 |
|
|
|
| 4 |
N |
0.076 |
|
|
|
| 5 |
H |
-0.085 |
|
|
|
| 6 |
H |
-0.141 |
|
|
|
| 7 |
H |
-0.085 |
|
|
|
| 8 |
H |
-0.141 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.162 |
-4.207 |
0.000 |
4.365 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.263 |
1.235 |
0.000 |
| y |
1.235 |
-25.184 |
0.000 |
| z |
0.000 |
0.000 |
-17.509 |
|
| Traceless |
| | x | y | z |
| x |
-4.917 |
1.235 |
0.000 |
| y |
1.235 |
-3.298 |
0.000 |
| z |
0.000 |
0.000 |
8.214 |
|
| Polar |
| 3z2-r2 | 16.429 |
| x2-y2 | -1.079 |
| xy | 1.235 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.006 |
0.048 |
0.000 |
| y |
0.048 |
6.188 |
0.000 |
| z |
0.000 |
0.000 |
6.145 |
<r2> (average value of r
2) Å
2
| <r2> |
69.500 |
| (<r2>)1/2 |
8.337 |
Jump to
S1C1
S1C2
Energy calculated at B3LYP/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -225.310764 |
| Energy at 298.15K | |
| HF Energy | -225.310764 |
| Nuclear repulsion energy | 123.442606 |
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 B3LYP/aug-cc-pVDZ
| 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 |
3749 |
3638 |
51.51 |
|
|
|
| 2 |
A1 |
3613 |
3506 |
6.10 |
|
|
|
| 3 |
A1 |
1759 |
1707 |
501.50 |
|
|
|
| 4 |
A1 |
1616 |
1568 |
0.09 |
|
|
|
| 5 |
A1 |
1135 |
1101 |
1.43 |
|
|
|
| 6 |
A1 |
966 |
938 |
10.32 |
|
|
|
| 7 |
A1 |
474 |
460 |
3.39 |
|
|
|
| 8 |
A2 |
383 |
372 |
0.00 |
|
|
|
| 9 |
A2 |
311i |
302i |
0.00 |
|
|
|
| 10 |
B1 |
766 |
743 |
4.19 |
|
|
|
| 11 |
B1 |
567 |
550 |
8.93 |
|
|
|
| 12 |
B1 |
188i |
183i |
420.60 |
|
|
|
| 13 |
B2 |
3746 |
3636 |
45.67 |
|
|
|
| 14 |
B2 |
3604 |
3497 |
66.51 |
|
|
|
| 15 |
B2 |
1614 |
1566 |
263.88 |
|
|
|
| 16 |
B2 |
1413 |
1371 |
219.27 |
|
|
|
| 17 |
B2 |
982 |
953 |
16.39 |
|
|
|
| 18 |
B2 |
560 |
543 |
13.85 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13223.1 cm
-1
Scaled (by 0.9704) Zero Point Vibrational Energy (zpe) 12831.7 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 B3LYP/aug-cc-pVDZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.139 |
| O2 |
0.000 |
0.000 |
1.365 |
| N3 |
0.000 |
1.163 |
-0.598 |
| N4 |
0.000 |
-1.163 |
-0.598 |
| H5 |
0.000 |
2.031 |
-0.087 |
| H6 |
0.000 |
1.188 |
-1.605 |
| H7 |
0.000 |
-2.031 |
-0.087 |
| H8 |
0.000 |
-1.188 |
-1.605 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2260 | 1.3769 | 1.3769 | 2.0432 | 2.1100 | 2.0432 | 2.1100 |
O2 | 1.2260 | | 2.2818 | 2.2818 | 2.4965 | 3.1987 | 2.4965 | 3.1987 | N3 | 1.3769 | 2.2818 | | 2.3258 | 1.0071 | 1.0070 | 3.2342 | 2.5573 | N4 | 1.3769 | 2.2818 | 2.3258 | | 3.2342 | 2.5573 | 1.0071 | 1.0070 | H5 | 2.0432 | 2.4965 | 1.0071 | 3.2342 | | 1.7360 | 4.0613 | 3.5585 | H6 | 2.1100 | 3.1987 | 1.0070 | 2.5573 | 1.7360 | | 3.5585 | 2.3759 | H7 | 2.0432 | 2.4965 | 3.2342 | 1.0071 | 4.0613 | 3.5585 | | 1.7360 | H8 | 2.1100 | 3.1987 | 2.5573 | 1.0070 | 3.5585 | 2.3759 | 1.7360 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
117.134 |
|
C1 |
N3 |
H6 |
123.797 |
| C1 |
N4 |
H7 |
117.134 |
|
C1 |
N4 |
H8 |
123.797 |
| O2 |
C1 |
N3 |
122.371 |
|
O2 |
C1 |
N4 |
122.371 |
| N3 |
C1 |
N4 |
115.257 |
|
H5 |
N3 |
H6 |
119.069 |
| H7 |
N4 |
H8 |
119.069 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.815 |
|
|
|
| 2 |
O |
-0.513 |
|
|
|
| 3 |
N |
0.106 |
|
|
|
| 4 |
N |
0.106 |
|
|
|
| 5 |
H |
-0.102 |
|
|
|
| 6 |
H |
-0.155 |
|
|
|
| 7 |
H |
-0.102 |
|
|
|
| 8 |
H |
-0.155 |
|
|
|
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 |
-4.386 |
4.386 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.511 |
0.000 |
0.000 |
| y |
0.000 |
-17.095 |
0.000 |
| z |
0.000 |
0.000 |
-24.927 |
|
| Traceless |
| | x | y | z |
| x |
-5.500 |
0.000 |
0.000 |
| y |
0.000 |
8.624 |
0.000 |
| z |
0.000 |
0.000 |
-3.124 |
|
| Polar |
| 3z2-r2 | -6.248 |
| x2-y2 | -9.416 |
| 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 |
4.006 |
0.000 |
0.000 |
| y |
0.000 |
6.145 |
0.000 |
| z |
0.000 |
0.000 |
6.189 |
<r2> (average value of r
2) Å
2
| <r2> |
69.468 |
| (<r2>)1/2 |
8.335 |