Jump to
S1C2
S1C3
Energy calculated at HF/Def2TZVPP
| | hartrees |
| Energy at 0K | -224.092711 |
| Energy at 298.15K | -224.099063 |
| HF Energy | -224.092711 |
| Nuclear repulsion energy | 125.490961 |
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/Def2TZVPP
| 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 |
3559 |
62.72 |
|
|
|
| 2 |
A |
3813 |
3456 |
6.70 |
|
|
|
| 3 |
A |
1947 |
1765 |
583.52 |
|
|
|
| 4 |
A |
1774 |
1608 |
0.26 |
|
|
|
| 5 |
A |
1284 |
1164 |
6.54 |
|
|
|
| 6 |
A |
1025 |
929 |
11.11 |
|
|
|
| 7 |
A |
578 |
524 |
53.79 |
|
|
|
| 8 |
A |
516 |
467 |
2.33 |
|
|
|
| 9 |
A |
396 |
359 |
88.03 |
|
|
|
| 10 |
B |
3926 |
3558 |
31.19 |
|
|
|
| 11 |
B |
3808 |
3451 |
73.78 |
|
|
|
| 12 |
B |
1779 |
1613 |
208.99 |
|
|
|
| 13 |
B |
1526 |
1383 |
245.56 |
|
|
|
| 14 |
B |
1142 |
1035 |
26.73 |
|
|
|
| 15 |
B |
875 |
793 |
84.20 |
|
|
|
| 16 |
B |
630 |
571 |
48.71 |
|
|
|
| 17 |
B |
572 |
519 |
181.17 |
|
|
|
| 18 |
B |
470 |
426 |
207.02 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14993.0 cm
-1
Scaled (by 0.9064) Zero Point Vibrational Energy (zpe) 13589.7 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 HF/Def2TZVPP
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.143 |
| O2 |
0.000 |
0.000 |
1.334 |
| N3 |
0.000 |
1.151 |
-0.600 |
| N4 |
0.000 |
-1.151 |
-0.600 |
| H5 |
0.199 |
1.967 |
-0.071 |
| H6 |
0.426 |
1.121 |
-1.495 |
| H7 |
-0.199 |
-1.967 |
-0.071 |
| H8 |
-0.426 |
-1.121 |
-1.495 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.1917 | 1.3698 | 1.3698 | 1.9885 | 2.0297 | 1.9885 | 2.0297 |
O2 | 1.1917 | | 2.2509 | 2.2509 | 2.4256 | 3.0730 | 2.4256 | 3.0730 | N3 | 1.3698 | 2.2509 | | 2.3022 | 0.9925 | 0.9919 | 3.1689 | 2.4786 | N4 | 1.3698 | 2.2509 | 2.3022 | | 3.1689 | 2.4786 | 0.9925 | 0.9919 | H5 | 1.9885 | 2.4256 | 0.9925 | 3.1689 | | 1.6721 | 3.9541 | 3.4572 | H6 | 2.0297 | 3.0730 | 0.9919 | 2.4786 | 1.6721 | | 3.4572 | 2.3976 | H7 | 1.9885 | 2.4256 | 3.1689 | 0.9925 | 3.9541 | 3.4572 | | 1.6721 | H8 | 2.0297 | 3.0730 | 2.4786 | 0.9919 | 3.4572 | 2.3976 | 1.6721 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
113.697 |
|
C1 |
N3 |
H6 |
117.610 |
| C1 |
N4 |
H7 |
113.697 |
|
C1 |
N4 |
H8 |
117.610 |
| O2 |
C1 |
N3 |
122.826 |
|
O2 |
C1 |
N4 |
122.826 |
| N3 |
C1 |
N4 |
114.348 |
|
H5 |
N3 |
H6 |
114.838 |
| H7 |
N4 |
H8 |
114.838 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/Def2TZVPP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.576 |
|
|
|
| 2 |
O |
-0.507 |
|
|
|
| 3 |
N |
-0.413 |
|
|
|
| 4 |
N |
-0.413 |
|
|
|
| 5 |
H |
0.206 |
|
|
|
| 6 |
H |
0.173 |
|
|
|
| 7 |
H |
0.206 |
|
|
|
| 8 |
H |
0.173 |
|
|
|
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 |
-4.050 |
4.050 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.006 |
3.084 |
0.000 |
| y |
3.084 |
-17.624 |
0.000 |
| z |
0.000 |
0.000 |
-25.308 |
|
| Traceless |
| | x | y | z |
| x |
-3.540 |
3.084 |
0.000 |
| y |
3.084 |
7.533 |
0.000 |
| z |
0.000 |
0.000 |
-3.993 |
|
| Polar |
| 3z2-r2 | -7.986 |
| x2-y2 | -7.382 |
| xy | 3.084 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.049 |
0.099 |
0.000 |
| y |
0.099 |
4.626 |
0.000 |
| z |
0.000 |
0.000 |
4.905 |
<r2> (average value of r
2) Å
2
| <r2> |
67.311 |
| (<r2>)1/2 |
8.204 |
Jump to
S1C1
S1C3
Energy calculated at HF/Def2TZVPP
| | hartrees |
| Energy at 0K | -224.091463 |
| Energy at 298.15K | -224.097017 |
| HF Energy | -224.091463 |
| Nuclear repulsion energy | 125.570914 |
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/Def2TZVPP
| 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' |
3960 |
3589 |
72.08 |
|
|
|
| 2 |
A' |
3837 |
3477 |
10.71 |
|
|
|
| 3 |
A' |
1931 |
1751 |
619.73 |
|
|
|
| 4 |
A' |
1780 |
1614 |
6.54 |
|
|
|
| 5 |
A' |
1272 |
1153 |
5.60 |
|
|
|
| 6 |
A' |
1034 |
937 |
14.53 |
|
|
|
| 7 |
A' |
867 |
785 |
39.42 |
|
|
|
| 8 |
A' |
583 |
529 |
19.51 |
|
|
|
| 9 |
A' |
520 |
471 |
8.18 |
|
|
|
| 10 |
A' |
343 |
311 |
447.78 |
|
|
|
| 11 |
A" |
3956 |
3586 |
33.72 |
|
|
|
| 12 |
A" |
3828 |
3470 |
82.49 |
|
|
|
| 13 |
A" |
1770 |
1605 |
235.80 |
|
|
|
| 14 |
A" |
1528 |
1385 |
257.14 |
|
|
|
| 15 |
A" |
1107 |
1003 |
20.57 |
|
|
|
| 16 |
A" |
625 |
566 |
23.50 |
|
|
|
| 17 |
A" |
441 |
400 |
29.26 |
|
|
|
| 18 |
A" |
8 |
8 |
40.64 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14694.7 cm
-1
Scaled (by 0.9064) Zero Point Vibrational Energy (zpe) 13319.3 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 HF/Def2TZVPP
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.033 |
0.134 |
0.000 |
| O2 |
0.036 |
1.326 |
0.000 |
| N3 |
0.036 |
-0.590 |
1.155 |
| N4 |
0.036 |
-0.590 |
-1.155 |
| H5 |
-0.181 |
-0.061 |
1.965 |
| H6 |
-0.308 |
-1.517 |
1.146 |
| H7 |
-0.181 |
-0.061 |
-1.965 |
| H8 |
-0.308 |
-1.517 |
-1.146 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.1928 | 1.3632 | 1.3632 | 1.9866 | 2.0382 | 1.9866 | 2.0382 |
O2 | 1.1928 | | 2.2376 | 2.2376 | 2.4156 | 3.0851 | 2.4156 | 3.0851 | N3 | 1.3632 | 2.2376 | | 2.3109 | 0.9911 | 0.9892 | 3.1727 | 2.5047 | N4 | 1.3632 | 2.2376 | 2.3109 | | 3.1727 | 2.5047 | 0.9911 | 0.9892 | H5 | 1.9866 | 2.4156 | 0.9911 | 3.1727 | | 1.6759 | 3.9309 | 3.4373 | H6 | 2.0382 | 3.0851 | 0.9892 | 2.5047 | 1.6759 | | 3.4373 | 2.2912 | H7 | 1.9866 | 2.4156 | 3.1727 | 0.9911 | 3.9309 | 3.4373 | | 1.6759 | H8 | 2.0382 | 3.0851 | 2.5047 | 0.9892 | 3.4373 | 2.2912 | 1.6759 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
114.157 |
|
C1 |
N3 |
H6 |
119.238 |
| C1 |
N4 |
H7 |
114.157 |
|
C1 |
N4 |
H8 |
119.238 |
| O2 |
C1 |
N3 |
122.050 |
|
O2 |
C1 |
N4 |
122.050 |
| N3 |
C1 |
N4 |
115.898 |
|
H5 |
N3 |
H6 |
115.622 |
| H7 |
N4 |
H8 |
115.622 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/Def2TZVPP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.579 |
|
|
|
| 2 |
O |
-0.518 |
|
|
|
| 3 |
N |
-0.410 |
|
|
|
| 4 |
N |
-0.410 |
|
|
|
| 5 |
H |
0.213 |
|
|
|
| 6 |
H |
0.167 |
|
|
|
| 7 |
H |
0.213 |
|
|
|
| 8 |
H |
0.167 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.294 |
-4.387 |
0.000 |
4.574 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.557 |
1.326 |
0.000 |
| y |
1.326 |
-24.761 |
0.000 |
| z |
0.000 |
0.000 |
-17.030 |
|
| Traceless |
| | x | y | z |
| x |
-4.662 |
1.326 |
0.000 |
| y |
1.326 |
-3.468 |
0.000 |
| z |
0.000 |
0.000 |
8.130 |
|
| Polar |
| 3z2-r2 | 16.259 |
| x2-y2 | -0.796 |
| xy | 1.326 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.011 |
0.054 |
0.000 |
| y |
0.054 |
4.874 |
0.000 |
| z |
0.000 |
0.000 |
4.617 |
<r2> (average value of r
2) Å
2
| <r2> |
67.301 |
| (<r2>)1/2 |
8.204 |
Jump to
S1C1
S1C2
Energy calculated at HF/Def2TZVPP
| | hartrees |
| Energy at 0K | -224.091193 |
| Energy at 298.15K | |
| HF Energy | -224.091193 |
| Nuclear repulsion energy | 125.669385 |
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/Def2TZVPP
| 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 |
3985 |
3612 |
86.49 |
|
|
|
| 2 |
A1 |
3853 |
3493 |
9.61 |
|
|
|
| 3 |
A1 |
1920 |
1740 |
651.04 |
|
|
|
| 4 |
A1 |
1772 |
1606 |
0.02 |
|
|
|
| 5 |
A1 |
1253 |
1135 |
3.00 |
|
|
|
| 6 |
A1 |
1040 |
943 |
13.88 |
|
|
|
| 7 |
A1 |
520 |
472 |
3.16 |
|
|
|
| 8 |
A2 |
433 |
392 |
0.00 |
|
|
|
| 9 |
A2 |
378i |
343i |
0.00 |
|
|
|
| 10 |
B1 |
866 |
785 |
21.70 |
|
|
|
| 11 |
B1 |
604 |
547 |
8.18 |
|
|
|
| 12 |
B1 |
247i |
224i |
501.51 |
|
|
|
| 13 |
B2 |
3982 |
3609 |
37.37 |
|
|
|
| 14 |
B2 |
3845 |
3485 |
99.48 |
|
|
|
| 15 |
B2 |
1767 |
1602 |
273.32 |
|
|
|
| 16 |
B2 |
1530 |
1387 |
274.78 |
|
|
|
| 17 |
B2 |
1090 |
988 |
16.58 |
|
|
|
| 18 |
B2 |
621 |
563 |
18.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14227.1 cm
-1
Scaled (by 0.9064) Zero Point Vibrational Energy (zpe) 12895.4 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 HF/Def2TZVPP
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.140 |
| O2 |
0.000 |
0.000 |
1.337 |
| N3 |
0.000 |
1.143 |
-0.587 |
| N4 |
0.000 |
-1.143 |
-0.587 |
| H5 |
0.000 |
1.994 |
-0.088 |
| H6 |
0.000 |
1.162 |
-1.573 |
| H7 |
0.000 |
-1.994 |
-0.088 |
| H8 |
0.000 |
-1.162 |
-1.573 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.1967 | 1.3549 | 1.3549 | 2.0073 | 2.0703 | 2.0073 | 2.0703 |
O2 | 1.1967 | | 2.2378 | 2.2378 | 2.4508 | 3.1337 | 2.4508 | 3.1337 | N3 | 1.3549 | 2.2378 | | 2.2867 | 0.9866 | 0.9869 | 3.1771 | 2.5073 | N4 | 1.3549 | 2.2378 | 2.2867 | | 3.1771 | 2.5073 | 0.9866 | 0.9869 | H5 | 2.0073 | 2.4508 | 0.9866 | 3.1771 | | 1.7033 | 3.9886 | 3.4883 | H6 | 2.0703 | 3.1337 | 0.9869 | 2.5073 | 1.7033 | | 3.4883 | 2.3233 | H7 | 2.0073 | 2.4508 | 3.1771 | 0.9866 | 3.9886 | 3.4883 | | 1.7033 | H8 | 2.0703 | 3.1337 | 2.5073 | 0.9869 | 3.4883 | 2.3233 | 1.7033 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
117.151 |
|
C1 |
N3 |
H6 |
123.514 |
| C1 |
N4 |
H7 |
117.151 |
|
C1 |
N4 |
H8 |
123.514 |
| O2 |
C1 |
N3 |
122.451 |
|
O2 |
C1 |
N4 |
122.451 |
| N3 |
C1 |
N4 |
115.098 |
|
H5 |
N3 |
H6 |
119.335 |
| H7 |
N4 |
H8 |
119.335 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/Def2TZVPP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.593 |
|
|
|
| 2 |
O |
-0.526 |
|
|
|
| 3 |
N |
-0.429 |
|
|
|
| 4 |
N |
-0.429 |
|
|
|
| 5 |
H |
0.220 |
|
|
|
| 6 |
H |
0.175 |
|
|
|
| 7 |
H |
0.220 |
|
|
|
| 8 |
H |
0.175 |
|
|
|
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 |
-4.617 |
4.617 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.816 |
0.000 |
0.000 |
| y |
0.000 |
-16.533 |
0.000 |
| z |
0.000 |
0.000 |
-24.463 |
|
| Traceless |
| | x | y | z |
| x |
-5.318 |
0.000 |
0.000 |
| y |
0.000 |
8.606 |
0.000 |
| z |
0.000 |
0.000 |
-3.288 |
|
| Polar |
| 3z2-r2 | -6.577 |
| x2-y2 | -9.283 |
| 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 |
2.984 |
0.000 |
0.000 |
| y |
0.000 |
4.584 |
0.000 |
| z |
0.000 |
0.000 |
4.829 |
<r2> (average value of r
2) Å
2
| <r2> |
67.228 |
| (<r2>)1/2 |
8.199 |