Jump to
S1C2
S1C3
Energy calculated at PBEPBE/6-311G*
| | hartrees |
| Energy at 0K | -225.070330 |
| Energy at 298.15K | -225.076453 |
| HF Energy | -225.070330 |
| Nuclear repulsion energy | 122.832809 |
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 PBEPBE/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 |
3599 |
3562 |
10.82 |
|
|
|
| 2 |
A |
3487 |
3450 |
0.18 |
|
|
|
| 3 |
A |
1776 |
1758 |
346.21 |
|
|
|
| 4 |
A |
1622 |
1605 |
0.57 |
|
|
|
| 5 |
A |
1161 |
1149 |
3.66 |
|
|
|
| 6 |
A |
927 |
917 |
5.78 |
|
|
|
| 7 |
A |
602 |
596 |
93.87 |
|
|
|
| 8 |
A |
459 |
454 |
4.23 |
|
|
|
| 9 |
A |
379 |
375 |
66.82 |
|
|
|
| 10 |
B |
3598 |
3561 |
19.21 |
|
|
|
| 11 |
B |
3481 |
3445 |
16.51 |
|
|
|
| 12 |
B |
1622 |
1605 |
182.98 |
|
|
|
| 13 |
B |
1383 |
1368 |
190.92 |
|
|
|
| 14 |
B |
1026 |
1016 |
27.40 |
|
|
|
| 15 |
B |
762 |
754 |
91.22 |
|
|
|
| 16 |
B |
571 |
565 |
188.48 |
|
|
|
| 17 |
B |
536 |
530 |
121.00 |
|
|
|
| 18 |
B |
444 |
439 |
94.36 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13717.3 cm
-1
Scaled (by 0.9896) Zero Point Vibrational Energy (zpe) 13574.7 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 PBEPBE/6-311G*
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.147 |
| O2 |
0.000 |
0.000 |
1.371 |
| N3 |
0.000 |
1.167 |
-0.620 |
| N4 |
0.000 |
-1.167 |
-0.620 |
| H5 |
0.220 |
1.990 |
-0.067 |
| H6 |
0.483 |
1.137 |
-1.515 |
| H7 |
-0.220 |
-1.990 |
-0.067 |
| H8 |
-0.483 |
-1.137 |
-1.515 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2240 | 1.3962 | 1.3962 | 2.0134 | 2.0707 | 2.0134 | 2.0707 |
O2 | 1.2240 | | 2.3075 | 2.3075 | 2.4646 | 3.1390 | 2.4646 | 3.1390 | N3 | 1.3962 | 2.3075 | | 2.3335 | 1.0159 | 1.0174 | 3.2123 | 2.5186 | N4 | 1.3962 | 2.3075 | 2.3335 | | 3.2123 | 2.5186 | 1.0159 | 1.0174 | H5 | 2.0134 | 2.4646 | 1.0159 | 3.2123 | | 1.7007 | 4.0040 | 3.5174 | H6 | 2.0707 | 3.1390 | 1.0174 | 2.5186 | 1.7007 | | 3.5174 | 2.4719 | H7 | 2.0134 | 2.4646 | 3.2123 | 1.0159 | 4.0040 | 3.5174 | | 1.7007 | H8 | 2.0707 | 3.1390 | 2.5186 | 1.0174 | 3.5174 | 2.4719 | 1.7007 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
112.209 |
|
C1 |
N3 |
H6 |
117.317 |
| C1 |
N4 |
H7 |
112.209 |
|
C1 |
N4 |
H8 |
117.317 |
| O2 |
C1 |
N3 |
123.313 |
|
O2 |
C1 |
N4 |
123.313 |
| N3 |
C1 |
N4 |
113.375 |
|
H5 |
N3 |
H6 |
113.529 |
| H7 |
N4 |
H8 |
113.529 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.502 |
|
|
|
| 2 |
O |
-0.349 |
|
|
|
| 3 |
N |
-0.749 |
|
|
|
| 4 |
N |
-0.749 |
|
|
|
| 5 |
H |
0.344 |
|
|
|
| 6 |
H |
0.329 |
|
|
|
| 7 |
H |
0.344 |
|
|
|
| 8 |
H |
0.329 |
|
|
|
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 |
-3.470 |
3.470 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.781 |
3.581 |
0.000 |
| y |
3.581 |
-17.845 |
0.000 |
| z |
0.000 |
0.000 |
-24.874 |
|
| Traceless |
| | x | y | z |
| x |
-3.421 |
3.581 |
0.000 |
| y |
3.581 |
6.982 |
0.000 |
| z |
0.000 |
0.000 |
-3.561 |
|
| Polar |
| 3z2-r2 | -7.122 |
| x2-y2 | -6.936 |
| xy | 3.581 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.537 |
0.210 |
0.000 |
| y |
0.210 |
5.169 |
0.000 |
| z |
0.000 |
0.000 |
5.174 |
<r2> (average value of r
2) Å
2
| <r2> |
69.322 |
| (<r2>)1/2 |
8.326 |
Jump to
S1C1
S1C3
Energy calculated at PBEPBE/6-311G*
| | hartrees |
| Energy at 0K | -225.068215 |
| Energy at 298.15K | -225.073767 |
| HF Energy | -225.068215 |
| Nuclear repulsion energy | 122.880133 |
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 PBEPBE/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' |
3630 |
3593 |
11.10 |
|
|
|
| 2 |
A' |
3512 |
3475 |
4.25 |
|
|
|
| 3 |
A' |
1765 |
1747 |
368.76 |
|
|
|
| 4 |
A' |
1627 |
1610 |
16.42 |
|
|
|
| 5 |
A' |
1154 |
1142 |
3.29 |
|
|
|
| 6 |
A' |
936 |
926 |
7.47 |
|
|
|
| 7 |
A' |
745 |
737 |
22.06 |
|
|
|
| 8 |
A' |
543 |
538 |
50.39 |
|
|
|
| 9 |
A' |
467 |
462 |
28.48 |
|
|
|
| 10 |
A' |
400 |
395 |
358.25 |
|
|
|
| 11 |
A" |
3628 |
3590 |
27.85 |
|
|
|
| 12 |
A" |
3500 |
3464 |
14.08 |
|
|
|
| 13 |
A" |
1611 |
1594 |
195.20 |
|
|
|
| 14 |
A" |
1390 |
1376 |
199.90 |
|
|
|
| 15 |
A" |
989 |
978 |
24.46 |
|
|
|
| 16 |
A" |
554 |
548 |
24.42 |
|
|
|
| 17 |
A" |
402 |
398 |
78.47 |
|
|
|
| 18 |
A" |
111 |
110 |
43.78 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13481.6 cm
-1
Scaled (by 0.9896) Zero Point Vibrational Energy (zpe) 13341.4 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 PBEPBE/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.006 |
0.142 |
0.000 |
| O2 |
0.039 |
1.367 |
0.000 |
| N3 |
0.039 |
-0.608 |
1.170 |
| N4 |
0.039 |
-0.608 |
-1.170 |
| H5 |
-0.161 |
-0.069 |
2.005 |
| H6 |
-0.286 |
-1.570 |
1.185 |
| H7 |
-0.161 |
-0.069 |
-2.005 |
| H8 |
-0.286 |
-1.570 |
-1.185 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2260 | 1.3904 | 1.3904 | 2.0232 | 2.1019 | 2.0232 | 2.1019 |
O2 | 1.2260 | | 2.2962 | 2.2962 | 2.4748 | 3.1837 | 2.4748 | 3.1837 | N3 | 1.3904 | 2.2962 | | 2.3405 | 1.0139 | 1.0151 | 3.2272 | 2.5645 | N4 | 1.3904 | 2.2962 | 2.3405 | | 3.2272 | 2.5645 | 1.0139 | 1.0151 | H5 | 2.0232 | 2.4748 | 1.0139 | 3.2272 | | 1.7148 | 4.0106 | 3.5277 | H6 | 2.1019 | 3.1837 | 1.0151 | 2.5645 | 1.7148 | | 3.5277 | 2.3697 | H7 | 2.0232 | 2.4748 | 3.2272 | 1.0139 | 4.0106 | 3.5277 | | 1.7148 | H8 | 2.1019 | 3.1837 | 2.5645 | 1.0151 | 3.5277 | 2.3697 | 1.7148 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
113.673 |
|
C1 |
N3 |
H6 |
121.018 |
| C1 |
N4 |
H7 |
113.673 |
|
C1 |
N4 |
H8 |
121.018 |
| O2 |
C1 |
N3 |
122.589 |
|
O2 |
C1 |
N4 |
122.589 |
| N3 |
C1 |
N4 |
114.632 |
|
H5 |
N3 |
H6 |
115.377 |
| H7 |
N4 |
H8 |
115.377 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.535 |
|
|
|
| 2 |
O |
-0.361 |
|
|
|
| 3 |
N |
-0.755 |
|
|
|
| 4 |
N |
-0.755 |
|
|
|
| 5 |
H |
0.347 |
|
|
|
| 6 |
H |
0.321 |
|
|
|
| 7 |
H |
0.347 |
|
|
|
| 8 |
H |
0.321 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.746 |
-3.859 |
0.000 |
4.236 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.475 |
1.846 |
0.000 |
| y |
1.846 |
-24.131 |
0.000 |
| z |
0.000 |
0.000 |
-17.163 |
|
| Traceless |
| | x | y | z |
| x |
-4.828 |
1.846 |
0.000 |
| y |
1.846 |
-2.812 |
0.000 |
| z |
0.000 |
0.000 |
7.640 |
|
| Polar |
| 3z2-r2 | 15.280 |
| x2-y2 | -1.344 |
| xy | 1.846 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.439 |
0.158 |
0.000 |
| y |
0.158 |
5.186 |
0.000 |
| z |
0.000 |
0.000 |
5.208 |
<r2> (average value of r
2) Å
2
| <r2> |
69.368 |
| (<r2>)1/2 |
8.329 |
Jump to
S1C1
S1C2
Energy calculated at PBEPBE/6-311G*
| | hartrees |
| Energy at 0K | -225.067480 |
| Energy at 298.15K | |
| HF Energy | -225.067480 |
| Nuclear repulsion energy | 123.027160 |
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 PBEPBE/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 |
3677 |
3638 |
19.17 |
|
|
|
| 2 |
A1 |
3545 |
3509 |
1.09 |
|
|
|
| 3 |
A1 |
1763 |
1744 |
405.03 |
|
|
|
| 4 |
A1 |
1609 |
1593 |
0.12 |
|
|
|
| 5 |
A1 |
1121 |
1110 |
0.14 |
|
|
|
| 6 |
A1 |
947 |
937 |
6.40 |
|
|
|
| 7 |
A1 |
464 |
459 |
3.74 |
|
|
|
| 8 |
A2 |
346 |
343 |
0.00 |
|
|
|
| 9 |
A2 |
416i |
411i |
0.00 |
|
|
|
| 10 |
B1 |
750 |
742 |
4.86 |
|
|
|
| 11 |
B1 |
561 |
556 |
11.16 |
|
|
|
| 12 |
B1 |
291i |
288i |
519.40 |
|
|
|
| 13 |
B2 |
3674 |
3636 |
38.73 |
|
|
|
| 14 |
B2 |
3534 |
3497 |
26.38 |
|
|
|
| 15 |
B2 |
1600 |
1584 |
265.96 |
|
|
|
| 16 |
B2 |
1395 |
1380 |
212.34 |
|
|
|
| 17 |
B2 |
956 |
946 |
14.88 |
|
|
|
| 18 |
B2 |
545 |
539 |
13.23 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 12890.3 cm
-1
Scaled (by 0.9896) Zero Point Vibrational Energy (zpe) 12756.2 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 PBEPBE/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 |
1.370 |
| N3 |
0.000 |
1.165 |
-0.602 |
| N4 |
0.000 |
-1.165 |
-0.602 |
| H5 |
0.000 |
2.034 |
-0.086 |
| H6 |
0.000 |
1.202 |
-1.613 |
| H7 |
0.000 |
-2.034 |
-0.086 |
| H8 |
0.000 |
-1.202 |
-1.613 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2272 | 1.3826 | 1.3826 | 2.0468 | 2.1281 | 2.0468 | 2.1281 |
O2 | 1.2272 | | 2.2905 | 2.2905 | 2.5015 | 3.2164 | 2.5015 | 3.2164 | N3 | 1.3826 | 2.2905 | | 2.3295 | 1.0109 | 1.0119 | 3.2401 | 2.5737 | N4 | 1.3826 | 2.2905 | 2.3295 | | 3.2401 | 2.5737 | 1.0109 | 1.0119 | H5 | 2.0468 | 2.5015 | 1.0109 | 3.2401 | | 1.7393 | 4.0680 | 3.5783 | H6 | 2.1281 | 3.2164 | 1.0119 | 2.5737 | 1.7393 | | 3.5783 | 2.4039 | H7 | 2.0468 | 2.5015 | 3.2401 | 1.0109 | 4.0680 | 3.5783 | | 1.7393 | H8 | 2.1281 | 3.2164 | 2.5737 | 1.0119 | 3.5783 | 2.4039 | 1.7393 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
116.697 |
|
C1 |
N3 |
H6 |
124.710 |
| C1 |
N4 |
H7 |
116.697 |
|
C1 |
N4 |
H8 |
124.710 |
| O2 |
C1 |
N3 |
122.603 |
|
O2 |
C1 |
N4 |
122.603 |
| N3 |
C1 |
N4 |
114.794 |
|
H5 |
N3 |
H6 |
118.593 |
| H7 |
N4 |
H8 |
118.593 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.601 |
|
|
|
| 2 |
O |
-0.375 |
|
|
|
| 3 |
N |
-0.800 |
|
|
|
| 4 |
N |
-0.800 |
|
|
|
| 5 |
H |
0.356 |
|
|
|
| 6 |
H |
0.331 |
|
|
|
| 7 |
H |
0.356 |
|
|
|
| 8 |
H |
0.331 |
|
|
|
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 |
-4.242 |
4.242 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.912 |
0.000 |
0.000 |
| y |
0.000 |
-16.275 |
0.000 |
| z |
0.000 |
0.000 |
-23.494 |
|
| Traceless |
| | x | y | z |
| x |
-6.028 |
0.000 |
0.000 |
| y |
0.000 |
8.428 |
0.000 |
| z |
0.000 |
0.000 |
-2.400 |
|
| Polar |
| 3z2-r2 | -4.800 |
| x2-y2 | -9.638 |
| 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 |
2.325 |
0.000 |
0.000 |
| y |
0.000 |
5.186 |
0.000 |
| z |
0.000 |
0.000 |
5.135 |
<r2> (average value of r
2) Å
2
| <r2> |
69.267 |
| (<r2>)1/2 |
8.323 |