Jump to
S1C2
S1C3
Energy calculated at B3LYP/3-21G*
| | hartrees |
| Energy at 0K | -224.013572 |
| Energy at 298.15K | -224.019241 |
| HF Energy | -224.013572 |
| Nuclear repulsion energy | 122.699910 |
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/3-21G*
| 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 |
3687 |
3547 |
24.57 |
|
|
|
| 2 |
A |
3560 |
3425 |
3.62 |
|
|
|
| 3 |
A |
1771 |
1703 |
313.95 |
|
|
|
| 4 |
A |
1687 |
1623 |
0.15 |
|
|
|
| 5 |
A |
1164 |
1120 |
0.88 |
|
|
|
| 6 |
A |
951 |
915 |
6.17 |
|
|
|
| 7 |
A |
488 |
470 |
3.15 |
|
|
|
| 8 |
A |
464 |
447 |
0.00 |
|
|
|
| 9 |
A |
87 |
84 |
0.00 |
|
|
|
| 10 |
B |
3683 |
3543 |
34.44 |
|
|
|
| 11 |
B |
3549 |
3415 |
35.07 |
|
|
|
| 12 |
B |
1660 |
1597 |
167.06 |
|
|
|
| 13 |
B |
1418 |
1364 |
291.71 |
|
|
|
| 14 |
B |
1005 |
967 |
19.80 |
|
|
|
| 15 |
B |
798 |
767 |
114.27 |
|
|
|
| 16 |
B |
578 |
556 |
59.97 |
|
|
|
| 17 |
B |
557 |
536 |
13.34 |
|
|
|
| 18 |
B |
439 |
422 |
612.68 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13773.1 cm
-1
Scaled (by 0.962) Zero Point Vibrational Energy (zpe) 13249.7 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/3-21G*
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.146 |
| O2 |
0.000 |
0.000 |
1.386 |
| N3 |
0.000 |
1.160 |
-0.608 |
| N4 |
0.000 |
-1.160 |
-0.608 |
| H5 |
0.000 |
2.035 |
-0.104 |
| H6 |
0.001 |
1.177 |
-1.619 |
| H7 |
-0.000 |
-2.035 |
-0.104 |
| H8 |
-0.001 |
-1.177 |
-1.619 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2397 | 1.3832 | 1.3832 | 2.0503 | 2.1211 | 2.0503 | 2.1211 |
O2 | 1.2397 | | 2.3065 | 2.3065 | 2.5219 | 3.2266 | 2.5219 | 3.2266 | N3 | 1.3832 | 2.3065 | | 2.3190 | 1.0104 | 1.0106 | 3.2341 | 2.5455 | N4 | 1.3832 | 2.3065 | 2.3190 | | 3.2341 | 2.5455 | 1.0104 | 1.0106 | H5 | 2.0503 | 2.5219 | 1.0104 | 3.2341 | | 1.7410 | 4.0701 | 3.5512 | H6 | 2.1211 | 3.2266 | 1.0106 | 2.5455 | 1.7410 | | 3.5512 | 2.3538 | H7 | 2.0503 | 2.5219 | 3.2341 | 1.0104 | 4.0701 | 3.5512 | | 1.7410 | H8 | 2.1211 | 3.2266 | 2.5455 | 1.0106 | 3.5512 | 2.3538 | 1.7410 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
117.015 |
|
C1 |
N3 |
H6 |
124.027 |
| C1 |
N4 |
H7 |
117.015 |
|
C1 |
N4 |
H8 |
124.027 |
| O2 |
C1 |
N3 |
123.041 |
|
O2 |
C1 |
N4 |
123.041 |
| N3 |
C1 |
N4 |
113.918 |
|
H5 |
N3 |
H6 |
118.959 |
| H7 |
N4 |
H8 |
118.959 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.853 |
|
|
|
| 2 |
O |
-0.536 |
|
|
|
| 3 |
N |
-0.772 |
|
|
|
| 4 |
N |
-0.772 |
|
|
|
| 5 |
H |
0.319 |
|
|
|
| 6 |
H |
0.295 |
|
|
|
| 7 |
H |
0.319 |
|
|
|
| 8 |
H |
0.295 |
|
|
|
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 |
-4.240 |
4.240 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.995 |
0.005 |
0.000 |
| y |
0.005 |
-16.038 |
0.000 |
| z |
0.000 |
0.000 |
-23.322 |
|
| Traceless |
| | x | y | z |
| x |
-5.315 |
0.005 |
0.000 |
| y |
0.005 |
8.120 |
0.000 |
| z |
0.000 |
0.000 |
-2.805 |
|
| Polar |
| 3z2-r2 | -5.610 |
| x2-y2 | -8.956 |
| xy | 0.005 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.070 |
0.000 |
0.000 |
| y |
0.000 |
4.153 |
0.000 |
| z |
0.000 |
0.000 |
4.378 |
<r2> (average value of r
2) Å
2
| <r2> |
69.203 |
| (<r2>)1/2 |
8.319 |
Jump to
S1C1
S1C3
Energy calculated at B3LYP/3-21G*
| | hartrees |
| Energy at 0K | -224.013571 |
| Energy at 298.15K | -224.019245 |
| HF Energy | -224.013571 |
| Nuclear repulsion energy | 122.699437 |
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/3-21G*
| 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' |
3687 |
3547 |
24.53 |
|
|
|
| 2 |
A' |
3560 |
3425 |
3.64 |
|
|
|
| 3 |
A' |
1770 |
1703 |
313.84 |
|
|
|
| 4 |
A' |
1687 |
1623 |
0.12 |
|
|
|
| 5 |
A' |
1164 |
1120 |
0.90 |
|
|
|
| 6 |
A' |
952 |
915 |
6.15 |
|
|
|
| 7 |
A' |
798 |
767 |
114.22 |
|
|
|
| 8 |
A' |
578 |
556 |
59.81 |
|
|
|
| 9 |
A' |
488 |
469 |
3.15 |
|
|
|
| 10 |
A' |
439 |
422 |
612.83 |
|
|
|
| 11 |
A" |
3683 |
3543 |
34.59 |
|
|
|
| 12 |
A" |
3549 |
3414 |
34.97 |
|
|
|
| 13 |
A" |
1660 |
1597 |
167.25 |
|
|
|
| 14 |
A" |
1419 |
1365 |
291.60 |
|
|
|
| 15 |
A" |
1005 |
967 |
19.74 |
|
|
|
| 16 |
A" |
557 |
536 |
13.34 |
|
|
|
| 17 |
A" |
464 |
447 |
0.00 |
|
|
|
| 18 |
A" |
89 |
86 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13774.1 cm
-1
Scaled (by 0.962) Zero Point Vibrational Energy (zpe) 13250.7 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/3-21G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.146 |
0.000 |
| O2 |
0.000 |
1.386 |
0.000 |
| N3 |
0.000 |
-0.608 |
1.160 |
| N4 |
0.000 |
-0.608 |
-1.160 |
| H5 |
0.000 |
-0.104 |
2.035 |
| H6 |
-0.000 |
-1.619 |
1.177 |
| H7 |
0.000 |
-0.104 |
-2.035 |
| H8 |
-0.000 |
-1.619 |
-1.177 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2398 | 1.3831 | 1.3831 | 2.0503 | 2.1210 | 2.0503 | 2.1210 |
O2 | 1.2398 | | 2.3065 | 2.3065 | 2.5219 | 3.2267 | 2.5219 | 3.2267 | N3 | 1.3831 | 2.3065 | | 2.3190 | 1.0104 | 1.0106 | 3.2341 | 2.5457 | N4 | 1.3831 | 2.3065 | 2.3190 | | 3.2341 | 2.5457 | 1.0104 | 1.0106 | H5 | 2.0503 | 2.5219 | 1.0104 | 3.2341 | | 1.7409 | 4.0700 | 3.5513 | H6 | 2.1210 | 3.2267 | 1.0106 | 2.5457 | 1.7409 | | 3.5513 | 2.3540 | H7 | 2.0503 | 2.5219 | 3.2341 | 1.0104 | 4.0700 | 3.5513 | | 1.7409 | H8 | 2.1210 | 3.2267 | 2.5457 | 1.0106 | 3.5513 | 2.3540 | 1.7409 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
117.017 |
|
C1 |
N3 |
H6 |
124.029 |
| C1 |
N4 |
H7 |
117.017 |
|
C1 |
N4 |
H8 |
124.029 |
| O2 |
C1 |
N3 |
123.036 |
|
O2 |
C1 |
N4 |
123.036 |
| N3 |
C1 |
N4 |
113.928 |
|
H5 |
N3 |
H6 |
118.954 |
| H7 |
N4 |
H8 |
118.954 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.853 |
|
|
|
| 2 |
O |
-0.536 |
|
|
|
| 3 |
N |
-0.772 |
|
|
|
| 4 |
N |
-0.772 |
|
|
|
| 5 |
H |
0.319 |
|
|
|
| 6 |
H |
0.295 |
|
|
|
| 7 |
H |
0.319 |
|
|
|
| 8 |
H |
0.295 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.002 |
-4.241 |
0.000 |
4.241 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.995 |
0.003 |
0.000 |
| y |
0.003 |
-23.322 |
0.000 |
| z |
0.000 |
0.000 |
-16.037 |
|
| Traceless |
| | x | y | z |
| x |
-5.315 |
0.003 |
0.000 |
| y |
0.003 |
-2.806 |
0.000 |
| z |
0.000 |
0.000 |
8.121 |
|
| Polar |
| 3z2-r2 | 16.243 |
| x2-y2 | -1.673 |
| xy | 0.003 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.070 |
0.000 |
0.000 |
| y |
0.000 |
4.378 |
0.000 |
| z |
0.000 |
0.000 |
4.153 |
<r2> (average value of r
2) Å
2
| <r2> |
69.202 |
| (<r2>)1/2 |
8.319 |
Jump to
S1C1
S1C2
Energy calculated at B3LYP/3-21G*
| | hartrees |
| Energy at 0K | -224.013571 |
| Energy at 298.15K | -224.019242 |
| HF Energy | -224.013571 |
| Nuclear repulsion energy | 122.698960 |
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/3-21G*
| 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 |
3687 |
3547 |
24.52 |
|
|
|
| 2 |
A1 |
3560 |
3425 |
3.65 |
|
|
|
| 3 |
A1 |
1771 |
1704 |
314.09 |
|
|
|
| 4 |
A1 |
1687 |
1623 |
0.19 |
|
|
|
| 5 |
A1 |
1164 |
1120 |
0.87 |
|
|
|
| 6 |
A1 |
951 |
915 |
6.18 |
|
|
|
| 7 |
A1 |
488 |
470 |
3.14 |
|
|
|
| 8 |
A2 |
464 |
446 |
0.00 |
|
|
|
| 9 |
A2 |
88 |
85 |
0.00 |
|
|
|
| 10 |
B1 |
797 |
767 |
114.16 |
|
|
|
| 11 |
B1 |
578 |
556 |
59.33 |
|
|
|
| 12 |
B1 |
439 |
422 |
613.45 |
|
|
|
| 13 |
B2 |
3683 |
3543 |
34.55 |
|
|
|
| 14 |
B2 |
3549 |
3414 |
34.96 |
|
|
|
| 15 |
B2 |
1660 |
1597 |
166.91 |
|
|
|
| 16 |
B2 |
1418 |
1364 |
291.69 |
|
|
|
| 17 |
B2 |
1005 |
967 |
19.87 |
|
|
|
| 18 |
B2 |
557 |
536 |
13.32 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13773.1 cm
-1
Scaled (by 0.962) Zero Point Vibrational Energy (zpe) 13249.7 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/3-21G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.146 |
| O2 |
0.000 |
0.000 |
1.386 |
| N3 |
0.000 |
1.159 |
-0.608 |
| N4 |
0.000 |
-1.159 |
-0.608 |
| H5 |
0.000 |
2.035 |
-0.104 |
| H6 |
0.000 |
1.177 |
-1.619 |
| H7 |
0.000 |
-2.035 |
-0.104 |
| H8 |
0.000 |
-1.177 |
-1.619 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2396 | 1.3833 | 1.3833 | 2.0505 | 2.1211 | 2.0505 | 2.1211 |
O2 | 1.2396 | | 2.3066 | 2.3066 | 2.5222 | 3.2266 | 2.5222 | 3.2266 | N3 | 1.3833 | 2.3066 | | 2.3190 | 1.0104 | 1.0106 | 3.2341 | 2.5452 | N4 | 1.3833 | 2.3066 | 2.3190 | | 3.2341 | 2.5452 | 1.0104 | 1.0106 | H5 | 2.0505 | 2.5222 | 1.0104 | 3.2341 | | 1.7410 | 4.0703 | 3.5509 | H6 | 2.1211 | 3.2266 | 1.0106 | 2.5452 | 1.7410 | | 3.5509 | 2.3530 | H7 | 2.0505 | 2.5222 | 3.2341 | 1.0104 | 4.0703 | 3.5509 | | 1.7410 | H8 | 2.1211 | 3.2266 | 2.5452 | 1.0106 | 3.5509 | 2.3530 | 1.7410 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
117.025 |
|
C1 |
N3 |
H6 |
124.015 |
| C1 |
N4 |
H7 |
117.025 |
|
C1 |
N4 |
H8 |
124.015 |
| O2 |
C1 |
N3 |
123.049 |
|
O2 |
C1 |
N4 |
123.049 |
| N3 |
C1 |
N4 |
113.903 |
|
H5 |
N3 |
H6 |
118.960 |
| H7 |
N4 |
H8 |
118.960 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.853 |
|
|
|
| 2 |
O |
-0.536 |
|
|
|
| 3 |
N |
-0.772 |
|
|
|
| 4 |
N |
-0.772 |
|
|
|
| 5 |
H |
0.319 |
|
|
|
| 6 |
H |
0.295 |
|
|
|
| 7 |
H |
0.319 |
|
|
|
| 8 |
H |
0.295 |
|
|
|
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 |
-4.239 |
4.239 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.995 |
0.000 |
0.000 |
| y |
0.000 |
-16.039 |
0.000 |
| z |
0.000 |
0.000 |
-23.322 |
|
| Traceless |
| | x | y | z |
| x |
-5.314 |
0.000 |
0.000 |
| y |
0.000 |
8.119 |
0.000 |
| z |
0.000 |
0.000 |
-2.804 |
|
| Polar |
| 3z2-r2 | -5.609 |
| x2-y2 | -8.956 |
| 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 |
1.070 |
0.000 |
0.000 |
| y |
0.000 |
4.153 |
0.000 |
| z |
0.000 |
0.000 |
4.378 |
<r2> (average value of r
2) Å
2
| <r2> |
69.204 |
| (<r2>)1/2 |
8.319 |