Jump to
S1C2
S1C3
Energy calculated at HF/3-21G*
| | hartrees |
| Energy at 0K | -222.736831 |
| Energy at 298.15K | -222.743087 |
| HF Energy | -222.736831 |
| Nuclear repulsion energy | 124.483403 |
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/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 |
3926 |
3543 |
72.96 |
|
|
|
| 2 |
A |
3803 |
3433 |
9.57 |
|
|
|
| 3 |
A |
1901 |
1716 |
483.92 |
|
|
|
| 4 |
A |
1823 |
1646 |
0.07 |
|
|
|
| 5 |
A |
1263 |
1140 |
3.36 |
|
|
|
| 6 |
A |
1020 |
921 |
10.12 |
|
|
|
| 7 |
A |
568 |
513 |
0.00 |
|
|
|
| 8 |
A |
529 |
478 |
2.71 |
|
|
|
| 9 |
A |
256 |
231 |
0.00 |
|
|
|
| 10 |
B |
3922 |
3540 |
36.71 |
|
|
|
| 11 |
B |
3795 |
3425 |
77.36 |
|
|
|
| 12 |
B |
1794 |
1619 |
194.29 |
|
|
|
| 13 |
B |
1525 |
1376 |
366.44 |
|
|
|
| 14 |
B |
1101 |
994 |
16.86 |
|
|
|
| 15 |
B |
896 |
809 |
302.41 |
|
|
|
| 16 |
B |
618 |
558 |
208.16 |
|
|
|
| 17 |
B |
612 |
553 |
19.73 |
|
|
|
| 18 |
B |
546 |
492 |
508.61 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14949.0 cm
-1
Scaled (by 0.9026) Zero Point Vibrational Energy (zpe) 13492.9 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/3-21G*
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.142 |
| O2 |
0.000 |
0.000 |
1.362 |
| N3 |
0.000 |
1.147 |
-0.597 |
| N4 |
0.000 |
-1.147 |
-0.597 |
| H5 |
0.000 |
2.011 |
-0.103 |
| H6 |
0.001 |
1.163 |
-1.591 |
| H7 |
-0.000 |
-2.011 |
-0.103 |
| H8 |
-0.001 |
-1.163 |
-1.591 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2200 | 1.3648 | 1.3648 | 2.0261 | 2.0872 | 2.0261 | 2.0872 |
O2 | 1.2200 | | 2.2704 | 2.2704 | 2.4884 | 3.1738 | 2.4884 | 3.1738 | N3 | 1.3648 | 2.2704 | | 2.2945 | 0.9952 | 0.9937 | 3.1968 | 2.5151 | N4 | 1.3648 | 2.2704 | 2.2945 | | 3.1968 | 2.5151 | 0.9952 | 0.9937 | H5 | 2.0261 | 2.4884 | 0.9952 | 3.1968 | | 1.7122 | 4.0224 | 3.5058 | H6 | 2.0872 | 3.1738 | 0.9937 | 2.5151 | 1.7122 | | 3.5058 | 2.3266 | H7 | 2.0261 | 2.4884 | 3.1968 | 0.9952 | 4.0224 | 3.5058 | | 1.7122 | H8 | 2.0872 | 3.1738 | 2.5151 | 0.9937 | 3.5058 | 2.3266 | 1.7122 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
117.444 |
|
C1 |
N3 |
H6 |
123.725 |
| C1 |
N4 |
H7 |
117.444 |
|
C1 |
N4 |
H8 |
123.725 |
| O2 |
C1 |
N3 |
122.799 |
|
O2 |
C1 |
N4 |
122.799 |
| N3 |
C1 |
N4 |
114.403 |
|
H5 |
N3 |
H6 |
118.831 |
| H7 |
N4 |
H8 |
118.831 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
1.152 |
|
|
|
| 2 |
O |
-0.673 |
|
|
|
| 3 |
N |
-0.949 |
|
|
|
| 4 |
N |
-0.949 |
|
|
|
| 5 |
H |
0.367 |
|
|
|
| 6 |
H |
0.342 |
|
|
|
| 7 |
H |
0.367 |
|
|
|
| 8 |
H |
0.342 |
|
|
|
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 |
-4.657 |
4.657 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.144 |
0.008 |
0.000 |
| y |
0.008 |
-16.349 |
0.000 |
| z |
0.000 |
0.000 |
-24.306 |
|
| Traceless |
| | x | y | z |
| x |
-4.816 |
0.008 |
0.000 |
| y |
0.008 |
8.376 |
0.000 |
| z |
0.000 |
0.000 |
-3.559 |
|
| Polar |
| 3z2-r2 | -7.119 |
| x2-y2 | -8.795 |
| xy | 0.008 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.994 |
0.000 |
0.000 |
| y |
0.000 |
3.465 |
0.000 |
| z |
0.000 |
0.000 |
3.933 |
<r2> (average value of r
2) Å
2
| <r2> |
67.960 |
| (<r2>)1/2 |
8.244 |
Jump to
S1C1
S1C3
Energy calculated at HF/3-21G*
| | hartrees |
| Energy at 0K | -222.736831 |
| Energy at 298.15K | -222.743086 |
| HF Energy | -222.736831 |
| Nuclear repulsion energy | 124.483434 |
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/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' |
3926 |
3543 |
72.95 |
|
|
|
| 2 |
A' |
3803 |
3433 |
9.58 |
|
|
|
| 3 |
A' |
1901 |
1716 |
483.96 |
|
|
|
| 4 |
A' |
1823 |
1646 |
0.07 |
|
|
|
| 5 |
A' |
1263 |
1140 |
3.36 |
|
|
|
| 6 |
A' |
1020 |
921 |
10.13 |
|
|
|
| 7 |
A' |
896 |
809 |
302.32 |
|
|
|
| 8 |
A' |
618 |
558 |
208.26 |
|
|
|
| 9 |
A' |
546 |
492 |
508.63 |
|
|
|
| 10 |
A' |
529 |
478 |
2.71 |
|
|
|
| 11 |
A" |
3922 |
3540 |
36.72 |
|
|
|
| 12 |
A" |
3795 |
3426 |
77.33 |
|
|
|
| 13 |
A" |
1794 |
1619 |
194.26 |
|
|
|
| 14 |
A" |
1525 |
1376 |
366.45 |
|
|
|
| 15 |
A" |
1101 |
994 |
16.86 |
|
|
|
| 16 |
A" |
612 |
553 |
19.71 |
|
|
|
| 17 |
A" |
568 |
513 |
0.00 |
|
|
|
| 18 |
A" |
255 |
230 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14948.8 cm
-1
Scaled (by 0.9026) Zero Point Vibrational Energy (zpe) 13492.7 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/3-21G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.142 |
0.000 |
| O2 |
-0.000 |
1.362 |
0.000 |
| N3 |
0.000 |
-0.597 |
1.147 |
| N4 |
0.000 |
-0.597 |
-1.147 |
| H5 |
0.000 |
-0.103 |
2.011 |
| H6 |
0.000 |
-1.591 |
1.163 |
| H7 |
0.000 |
-0.103 |
-2.011 |
| H8 |
0.000 |
-1.591 |
-1.163 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2200 | 1.3648 | 1.3648 | 2.0261 | 2.0872 | 2.0261 | 2.0872 |
O2 | 1.2200 | | 2.2705 | 2.2705 | 2.4885 | 3.1738 | 2.4885 | 3.1738 | N3 | 1.3648 | 2.2705 | | 2.2944 | 0.9952 | 0.9937 | 3.1968 | 2.5150 | N4 | 1.3648 | 2.2705 | 2.2944 | | 3.1968 | 2.5150 | 0.9952 | 0.9937 | H5 | 2.0261 | 2.4885 | 0.9952 | 3.1968 | | 1.7122 | 4.0224 | 3.5056 | H6 | 2.0872 | 3.1738 | 0.9937 | 2.5150 | 1.7122 | | 3.5056 | 2.3265 | H7 | 2.0261 | 2.4885 | 3.1968 | 0.9952 | 4.0224 | 3.5056 | | 1.7122 | H8 | 2.0872 | 3.1738 | 2.5150 | 0.9937 | 3.5056 | 2.3265 | 1.7122 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
117.445 |
|
C1 |
N3 |
H6 |
123.725 |
| C1 |
N4 |
H7 |
117.445 |
|
C1 |
N4 |
H8 |
123.725 |
| O2 |
C1 |
N3 |
122.801 |
|
O2 |
C1 |
N4 |
122.801 |
| N3 |
C1 |
N4 |
114.398 |
|
H5 |
N3 |
H6 |
118.830 |
| H7 |
N4 |
H8 |
118.830 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
1.152 |
|
|
|
| 2 |
O |
-0.673 |
|
|
|
| 3 |
N |
-0.949 |
|
|
|
| 4 |
N |
-0.949 |
|
|
|
| 5 |
H |
0.367 |
|
|
|
| 6 |
H |
0.342 |
|
|
|
| 7 |
H |
0.367 |
|
|
|
| 8 |
H |
0.342 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.002 |
-4.657 |
0.000 |
4.657 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.144 |
0.001 |
0.000 |
| y |
0.001 |
-24.306 |
0.000 |
| z |
0.000 |
0.000 |
-16.349 |
|
| Traceless |
| | x | y | z |
| x |
-4.816 |
0.001 |
0.000 |
| y |
0.001 |
-3.559 |
0.000 |
| z |
0.000 |
0.000 |
8.375 |
|
| Polar |
| 3z2-r2 | 16.751 |
| x2-y2 | -0.838 |
| xy | 0.001 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.994 |
-0.000 |
0.000 |
| y |
-0.000 |
3.933 |
0.000 |
| z |
0.000 |
0.000 |
3.464 |
<r2> (average value of r
2) Å
2
| <r2> |
67.960 |
| (<r2>)1/2 |
8.244 |
Jump to
S1C1
S1C2
Energy calculated at HF/3-21G*
| | hartrees |
| Energy at 0K | -222.736831 |
| Energy at 298.15K | -222.743086 |
| HF Energy | -222.736831 |
| Nuclear repulsion energy | 124.481337 |
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/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 |
3926 |
3543 |
72.93 |
|
|
|
| 2 |
A1 |
3803 |
3433 |
9.59 |
|
|
|
| 3 |
A1 |
1901 |
1716 |
483.94 |
|
|
|
| 4 |
A1 |
1823 |
1646 |
0.10 |
|
|
|
| 5 |
A1 |
1263 |
1140 |
3.34 |
|
|
|
| 6 |
A1 |
1020 |
921 |
10.15 |
|
|
|
| 7 |
A1 |
529 |
478 |
2.71 |
|
|
|
| 8 |
A2 |
568 |
512 |
0.00 |
|
|
|
| 9 |
A2 |
256 |
231 |
0.00 |
|
|
|
| 10 |
B1 |
896 |
809 |
302.19 |
|
|
|
| 11 |
B1 |
618 |
558 |
206.36 |
|
|
|
| 12 |
B1 |
545 |
492 |
510.72 |
|
|
|
| 13 |
B2 |
3922 |
3540 |
36.81 |
|
|
|
| 14 |
B2 |
3795 |
3425 |
77.26 |
|
|
|
| 15 |
B2 |
1794 |
1619 |
194.12 |
|
|
|
| 16 |
B2 |
1524 |
1376 |
366.42 |
|
|
|
| 17 |
B2 |
1101 |
994 |
16.93 |
|
|
|
| 18 |
B2 |
612 |
553 |
19.72 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14948.3 cm
-1
Scaled (by 0.9026) Zero Point Vibrational Energy (zpe) 13492.4 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/3-21G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.142 |
| O2 |
0.000 |
0.000 |
1.362 |
| N3 |
0.000 |
1.147 |
-0.597 |
| N4 |
0.000 |
-1.147 |
-0.597 |
| H5 |
0.000 |
2.011 |
-0.103 |
| H6 |
0.000 |
1.163 |
-1.591 |
| H7 |
0.000 |
-2.011 |
-0.103 |
| H8 |
0.000 |
-1.163 |
-1.591 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2199 | 1.3649 | 1.3649 | 2.0262 | 2.0871 | 2.0262 | 2.0871 |
O2 | 1.2199 | | 2.2705 | 2.2705 | 2.4884 | 3.1737 | 2.4884 | 3.1737 | N3 | 1.3649 | 2.2705 | | 2.2946 | 0.9952 | 0.9937 | 3.1970 | 2.5151 | N4 | 1.3649 | 2.2705 | 2.2946 | | 3.1970 | 2.5151 | 0.9952 | 0.9937 | H5 | 2.0262 | 2.4884 | 0.9952 | 3.1970 | | 1.7123 | 4.0225 | 3.5057 | H6 | 2.0871 | 3.1737 | 0.9937 | 2.5151 | 1.7123 | | 3.5057 | 2.3263 | H7 | 2.0262 | 2.4884 | 3.1970 | 0.9952 | 4.0225 | 3.5057 | | 1.7123 | H8 | 2.0871 | 3.1737 | 2.5151 | 0.9937 | 3.5057 | 2.3263 | 1.7123 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
117.444 |
|
C1 |
N3 |
H6 |
123.714 |
| C1 |
N4 |
H7 |
117.444 |
|
C1 |
N4 |
H8 |
123.714 |
| O2 |
C1 |
N3 |
122.799 |
|
O2 |
C1 |
N4 |
122.799 |
| N3 |
C1 |
N4 |
114.401 |
|
H5 |
N3 |
H6 |
118.842 |
| H7 |
N4 |
H8 |
118.842 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
1.152 |
|
|
|
| 2 |
O |
-0.673 |
|
|
|
| 3 |
N |
-0.949 |
|
|
|
| 4 |
N |
-0.949 |
|
|
|
| 5 |
H |
0.367 |
|
|
|
| 6 |
H |
0.342 |
|
|
|
| 7 |
H |
0.367 |
|
|
|
| 8 |
H |
0.342 |
|
|
|
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 |
-4.656 |
4.656 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.144 |
0.000 |
0.000 |
| y |
0.000 |
-16.350 |
0.000 |
| z |
0.000 |
0.000 |
-24.305 |
|
| Traceless |
| | x | y | z |
| x |
-4.816 |
0.000 |
0.000 |
| y |
0.000 |
8.374 |
0.000 |
| z |
0.000 |
0.000 |
-3.558 |
|
| Polar |
| 3z2-r2 | -7.116 |
| x2-y2 | -8.794 |
| 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 |
0.994 |
0.000 |
0.000 |
| y |
0.000 |
3.465 |
0.000 |
| z |
0.000 |
0.000 |
3.933 |
<r2> (average value of r
2) Å
2
| <r2> |
67.962 |
| (<r2>)1/2 |
8.244 |