Jump to
S1C2
S1C3
Energy calculated at HF/6-31G*
| | hartrees |
| Energy at 0K | -223.984692 |
| Energy at 298.15K | -223.991116 |
| HF Energy | -223.984692 |
| Nuclear repulsion energy | 125.065896 |
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 HF/6-31G*
| 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 |
3926 |
3528 |
54.02 |
|
|
|
| 2 |
A |
3815 |
3428 |
5.46 |
|
|
|
| 3 |
A |
2000 |
1797 |
538.30 |
|
|
|
| 4 |
A |
1806 |
1622 |
0.02 |
|
|
|
| 5 |
A |
1304 |
1171 |
5.57 |
|
|
|
| 6 |
A |
1035 |
930 |
8.42 |
|
|
|
| 7 |
A |
649 |
583 |
90.91 |
|
|
|
| 8 |
A |
514 |
462 |
3.61 |
|
|
|
| 9 |
A |
417 |
375 |
99.25 |
|
|
|
| 10 |
B |
3926 |
3528 |
33.57 |
|
|
|
| 11 |
B |
3811 |
3424 |
69.33 |
|
|
|
| 12 |
B |
1812 |
1628 |
226.69 |
|
|
|
| 13 |
B |
1550 |
1393 |
244.17 |
|
|
|
| 14 |
B |
1166 |
1048 |
24.18 |
|
|
|
| 15 |
B |
882 |
793 |
180.94 |
|
|
|
| 16 |
B |
630 |
566 |
122.39 |
|
|
|
| 17 |
B |
599 |
538 |
239.29 |
|
|
|
| 18 |
B |
483 |
434 |
96.61 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15162.9 cm
-1
Scaled (by 0.8985) Zero Point Vibrational Energy (zpe) 13623.9 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 HF/6-31G*
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.144 |
| O2 |
0.000 |
0.000 |
1.341 |
| N3 |
0.000 |
1.152 |
-0.604 |
| N4 |
0.000 |
-1.152 |
-0.604 |
| H5 |
0.200 |
1.969 |
-0.071 |
| H6 |
0.440 |
1.124 |
-1.497 |
| H7 |
-0.200 |
-1.969 |
-0.071 |
| H8 |
-0.440 |
-1.124 |
-1.497 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.1973 | 1.3733 | 1.3733 | 1.9913 | 2.0377 | 1.9913 | 2.0377 |
O2 | 1.1973 | | 2.2609 | 2.2609 | 2.4321 | 3.0850 | 2.4321 | 3.0850 | N3 | 1.3733 | 2.2609 | | 2.3031 | 0.9964 | 0.9962 | 3.1724 | 2.4841 | N4 | 1.3733 | 2.2609 | 2.3031 | | 3.1724 | 2.4841 | 0.9964 | 0.9962 | H5 | 1.9913 | 2.4321 | 0.9964 | 3.1724 | | 1.6750 | 3.9591 | 3.4661 | H6 | 2.0377 | 3.0850 | 0.9962 | 2.4841 | 1.6750 | | 3.4661 | 2.4146 | H7 | 1.9913 | 2.4321 | 3.1724 | 0.9964 | 3.9591 | 3.4661 | | 1.6750 | H8 | 2.0377 | 3.0850 | 2.4841 | 0.9962 | 3.4661 | 2.4146 | 1.6750 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
113.388 |
|
C1 |
N3 |
H6 |
117.744 |
| C1 |
N4 |
H7 |
113.388 |
|
C1 |
N4 |
H8 |
117.744 |
| O2 |
C1 |
N3 |
123.017 |
|
O2 |
C1 |
N4 |
123.017 |
| N3 |
C1 |
N4 |
113.967 |
|
H5 |
N3 |
H6 |
114.410 |
| H7 |
N4 |
H8 |
114.410 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.882 |
|
|
|
| 2 |
O |
-0.607 |
|
|
|
| 3 |
N |
-0.903 |
|
|
|
| 4 |
N |
-0.903 |
|
|
|
| 5 |
H |
0.391 |
|
|
|
| 6 |
H |
0.375 |
|
|
|
| 7 |
H |
0.391 |
|
|
|
| 8 |
H |
0.375 |
|
|
|
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 |
-3.846 |
3.846 |
| CHELPG |
0.000 |
0.000 |
-3.881 |
3.881 |
| AIM |
0.000 |
0.000 |
0.764 |
0.764 |
| ESP |
0.008 |
-0.005 |
-3.860 |
3.860 |
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.519 |
3.604 |
0.000 |
| y |
3.604 |
-17.664 |
0.000 |
| z |
0.000 |
0.000 |
-25.190 |
|
| Traceless |
| | x | y | z |
| x |
-3.092 |
3.604 |
0.000 |
| y |
3.604 |
7.191 |
0.000 |
| z |
0.000 |
0.000 |
-4.099 |
|
| Polar |
| 3z2-r2 | -8.198 |
| x2-y2 | -6.855 |
| xy | 3.604 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.948 |
0.141 |
0.000 |
| y |
0.141 |
3.936 |
0.000 |
| z |
0.000 |
0.000 |
4.296 |
<r2> (average value of r
2) Å
2
| <r2> |
67.470 |
| (<r2>)1/2 |
8.214 |
Jump to
S1C1
S1C3
Energy calculated at HF/6-31G*
| | hartrees |
| Energy at 0K | -223.982603 |
| Energy at 298.15K | |
| HF Energy | -223.982603 |
| Nuclear repulsion energy | 125.161502 |
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 HF/6-31G*
| 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' |
3964 |
3561 |
64.64 |
|
|
|
| 2 |
A' |
3845 |
3455 |
15.85 |
|
|
|
| 3 |
A' |
1981 |
1780 |
579.52 |
|
|
|
| 4 |
A' |
1810 |
1627 |
11.24 |
|
|
|
| 5 |
A' |
1289 |
1158 |
5.12 |
|
|
|
| 6 |
A' |
1047 |
940 |
12.37 |
|
|
|
| 7 |
A' |
861 |
773 |
79.60 |
|
|
|
| 8 |
A' |
587 |
527 |
31.25 |
|
|
|
| 9 |
A' |
522 |
469 |
17.18 |
|
|
|
| 10 |
A' |
375 |
337 |
545.17 |
|
|
|
| 11 |
A" |
3961 |
3559 |
38.63 |
|
|
|
| 12 |
A" |
3836 |
3447 |
71.22 |
|
|
|
| 13 |
A" |
1800 |
1617 |
252.96 |
|
|
|
| 14 |
A" |
1554 |
1396 |
258.92 |
|
|
|
| 15 |
A" |
1123 |
1009 |
16.30 |
|
|
|
| 16 |
A" |
622 |
559 |
28.46 |
|
|
|
| 17 |
A" |
454 |
408 |
46.28 |
|
|
|
| 18 |
A" |
103i |
92i |
50.31 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14763.2 cm
-1
Scaled (by 0.8985) Zero Point Vibrational Energy (zpe) 13264.8 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 HF/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.011 |
0.141 |
0.000 |
| O2 |
0.030 |
1.340 |
0.000 |
| N3 |
0.030 |
-0.593 |
1.152 |
| N4 |
0.030 |
-0.593 |
-1.152 |
| H5 |
-0.136 |
-0.078 |
1.987 |
| H6 |
-0.229 |
-1.552 |
1.161 |
| H7 |
-0.136 |
-0.078 |
-1.987 |
| H8 |
-0.229 |
-1.552 |
-1.161 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.1998 | 1.3663 | 1.3663 | 2.0041 | 2.0666 | 2.0041 | 2.0666 |
O2 | 1.1998 | | 2.2509 | 2.2509 | 2.4469 | 3.1276 | 2.4469 | 3.1276 | N3 | 1.3663 | 2.2509 | | 2.3046 | 0.9944 | 0.9936 | 3.1852 | 2.5173 | N4 | 1.3663 | 2.2509 | 2.3046 | | 3.1852 | 2.5173 | 0.9944 | 0.9936 | H5 | 2.0041 | 2.4469 | 0.9944 | 3.1852 | | 1.6921 | 3.9732 | 3.4765 | H6 | 2.0666 | 3.1276 | 0.9936 | 2.5173 | 1.6921 | | 3.4765 | 2.3213 | H7 | 2.0041 | 2.4469 | 3.1852 | 0.9944 | 3.9732 | 3.4765 | | 1.6921 | H8 | 2.0666 | 3.1276 | 2.5173 | 0.9936 | 3.4765 | 2.3213 | 1.6921 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
115.289 |
|
C1 |
N3 |
H6 |
121.461 |
| C1 |
N4 |
H7 |
115.289 |
|
C1 |
N4 |
H8 |
121.461 |
| O2 |
C1 |
N3 |
122.469 |
|
O2 |
C1 |
N4 |
122.469 |
| N3 |
C1 |
N4 |
114.997 |
|
H5 |
N3 |
H6 |
116.676 |
| H7 |
N4 |
H8 |
116.676 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.915 |
|
|
|
| 2 |
O |
-0.622 |
|
|
|
| 3 |
N |
-0.915 |
|
|
|
| 4 |
N |
-0.915 |
|
|
|
| 5 |
H |
0.396 |
|
|
|
| 6 |
H |
0.372 |
|
|
|
| 7 |
H |
0.396 |
|
|
|
| 8 |
H |
0.372 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.635 |
-4.303 |
0.000 |
4.603 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.236 |
1.629 |
0.000 |
| y |
1.629 |
-24.409 |
0.000 |
| z |
0.000 |
0.000 |
-16.901 |
|
| Traceless |
| | x | y | z |
| x |
-4.580 |
1.629 |
0.000 |
| y |
1.629 |
-3.341 |
0.000 |
| z |
0.000 |
0.000 |
7.921 |
|
| Polar |
| 3z2-r2 | 15.842 |
| x2-y2 | -0.826 |
| xy | 1.629 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.835 |
0.112 |
0.000 |
| y |
0.112 |
4.278 |
0.000 |
| z |
0.000 |
0.000 |
3.948 |
<r2> (average value of r
2) Å
2
| <r2> |
67.443 |
| (<r2>)1/2 |
8.212 |
Jump to
S1C1
S1C2
Energy calculated at HF/6-31G*
| | hartrees |
| Energy at 0K | -223.982192 |
| Energy at 298.15K | |
| HF Energy | -223.982192 |
| Nuclear repulsion energy | 125.271955 |
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 HF/6-31G*
| 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 |
3991 |
3586 |
83.01 |
|
|
|
| 2 |
A1 |
3865 |
3472 |
10.86 |
|
|
|
| 3 |
A1 |
1969 |
1769 |
616.63 |
|
|
|
| 4 |
A1 |
1798 |
1616 |
1.58 |
|
|
|
| 5 |
A1 |
1265 |
1136 |
1.64 |
|
|
|
| 6 |
A1 |
1055 |
948 |
10.72 |
|
|
|
| 7 |
A1 |
521 |
468 |
2.90 |
|
|
|
| 8 |
A2 |
439 |
394 |
0.00 |
|
|
|
| 9 |
A2 |
433i |
390i |
0.00 |
|
|
|
| 10 |
B1 |
861 |
774 |
47.58 |
|
|
|
| 11 |
B1 |
611 |
549 |
10.00 |
|
|
|
| 12 |
B1 |
274i |
247i |
684.87 |
|
|
|
| 13 |
B2 |
3989 |
3584 |
44.02 |
|
|
|
| 14 |
B2 |
3856 |
3465 |
96.21 |
|
|
|
| 15 |
B2 |
1793 |
1611 |
305.39 |
|
|
|
| 16 |
B2 |
1557 |
1399 |
277.01 |
|
|
|
| 17 |
B2 |
1100 |
988 |
10.77 |
|
|
|
| 18 |
B2 |
616 |
554 |
20.17 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14288.1 cm
-1
Scaled (by 0.8985) Zero Point Vibrational Energy (zpe) 12837.9 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 HF/6-31G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.141 |
| O2 |
0.000 |
0.000 |
1.343 |
| N3 |
0.000 |
1.148 |
-0.589 |
| N4 |
0.000 |
-1.148 |
-0.589 |
| H5 |
0.000 |
2.005 |
-0.089 |
| H6 |
0.000 |
1.171 |
-1.581 |
| H7 |
0.000 |
-2.005 |
-0.089 |
| H8 |
0.000 |
-1.171 |
-1.581 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2017 | 1.3603 | 1.3603 | 2.0187 | 2.0826 | 2.0187 | 2.0826 |
O2 | 1.2017 | | 2.2472 | 2.2472 | 2.4643 | 3.1496 | 2.4643 | 3.1496 | N3 | 1.3603 | 2.2472 | | 2.2952 | 0.9929 | 0.9919 | 3.1925 | 2.5221 | N4 | 1.3603 | 2.2472 | 2.2952 | | 3.1925 | 2.5221 | 0.9929 | 0.9919 | H5 | 2.0187 | 2.4643 | 0.9929 | 3.1925 | | 1.7090 | 4.0109 | 3.5096 | H6 | 2.0826 | 3.1496 | 0.9919 | 2.5221 | 1.7090 | | 3.5096 | 2.3427 | H7 | 2.0187 | 2.4643 | 3.1925 | 0.9929 | 4.0109 | 3.5096 | | 1.7090 | H8 | 2.0826 | 3.1496 | 2.5221 | 0.9919 | 3.5096 | 2.3427 | 1.7090 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
117.293 |
|
C1 |
N3 |
H6 |
123.843 |
| C1 |
N4 |
H7 |
117.293 |
|
C1 |
N4 |
H8 |
123.843 |
| O2 |
C1 |
N3 |
122.472 |
|
O2 |
C1 |
N4 |
122.472 |
| N3 |
C1 |
N4 |
115.056 |
|
H5 |
N3 |
H6 |
118.864 |
| H7 |
N4 |
H8 |
118.864 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.948 |
|
|
|
| 2 |
O |
-0.634 |
|
|
|
| 3 |
N |
-0.940 |
|
|
|
| 4 |
N |
-0.940 |
|
|
|
| 5 |
H |
0.402 |
|
|
|
| 6 |
H |
0.380 |
|
|
|
| 7 |
H |
0.402 |
|
|
|
| 8 |
H |
0.380 |
|
|
|
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 |
-4.602 |
4.602 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.556 |
0.000 |
0.000 |
| y |
0.000 |
-16.232 |
0.000 |
| z |
0.000 |
0.000 |
-23.962 |
|
| Traceless |
| | x | y | z |
| x |
-5.460 |
0.000 |
0.000 |
| y |
0.000 |
8.527 |
0.000 |
| z |
0.000 |
0.000 |
-3.068 |
|
| Polar |
| 3z2-r2 | -6.135 |
| x2-y2 | -9.325 |
| 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 |
1.764 |
0.000 |
0.000 |
| y |
0.000 |
3.930 |
0.000 |
| z |
0.000 |
0.000 |
4.232 |
<r2> (average value of r
2) Å
2
| <r2> |
67.334 |
| (<r2>)1/2 |
8.206 |