Jump to
S1C2
S1C3
Energy calculated at B3PW91/6-31G(2df,p)
| hartrees |
Energy at 0K | -225.201963 |
Energy at 298.15K | -225.208136 |
HF Energy | -225.201963 |
Nuclear repulsion energy | 123.873251 |
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 B3PW91/6-31G(2df,p)
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 |
3720 |
3577 |
33.33 |
|
|
|
2 |
A |
3603 |
3464 |
2.58 |
|
|
|
3 |
A |
1844 |
1773 |
353.32 |
|
|
|
4 |
A |
1626 |
1563 |
0.73 |
|
|
|
5 |
A |
1180 |
1135 |
2.55 |
|
|
|
6 |
A |
961 |
924 |
6.17 |
|
|
|
7 |
A |
583 |
561 |
73.52 |
|
|
|
8 |
A |
469 |
451 |
2.16 |
|
|
|
9 |
A |
389 |
374 |
62.53 |
|
|
|
10 |
B |
3720 |
3576 |
28.30 |
|
|
|
11 |
B |
3599 |
3460 |
43.06 |
|
|
|
12 |
B |
1628 |
1565 |
186.76 |
|
|
|
13 |
B |
1423 |
1368 |
179.62 |
|
|
|
14 |
B |
1048 |
1007 |
19.32 |
|
|
|
15 |
B |
791 |
761 |
68.22 |
|
|
|
16 |
B |
580 |
558 |
111.54 |
|
|
|
17 |
B |
541 |
520 |
150.98 |
|
|
|
18 |
B |
448 |
430 |
116.92 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14075.8 cm
-1
Scaled (by 0.9614) Zero Point Vibrational Energy (zpe) 13532.5 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 B3PW91/6-31G(2df,p)
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 |
1.358 |
N3 |
-0.134 |
1.151 |
-0.612 |
N4 |
0.134 |
-1.151 |
-0.612 |
H5 |
0.000 |
1.989 |
-0.069 |
H6 |
0.315 |
1.169 |
-1.515 |
H7 |
0.000 |
-1.989 |
-0.069 |
H8 |
-0.315 |
-1.169 |
-1.515 |
Atom - Atom Distances (Å)
|
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.2126 | 1.3847 | 1.3847 | 2.0005 | 2.0550 | 2.0005 | 2.0550 |
O2 | 1.2126 | | 2.2861 | 2.2861 | 2.4478 | 3.1178 | 2.4478 | 3.1178 | N3 | 1.3847 | 2.2861 | | 2.3177 | 1.0078 | 1.0080 | 3.1896 | 2.4961 | N4 | 1.3847 | 2.2861 | 2.3177 | | 3.1896 | 2.4961 | 1.0078 | 1.0080 | H5 | 2.0005 | 2.4478 | 1.0078 | 3.1896 | | 1.6922 | 3.9780 | 3.4877 | H6 | 2.0550 | 3.1178 | 1.0080 | 2.4961 | 1.6922 | | 3.4877 | 2.4212 | H7 | 2.0005 | 2.4478 | 3.1896 | 1.0078 | 3.9780 | 3.4877 | | 1.6922 | H8 | 2.0550 | 3.1178 | 2.4961 | 1.0080 | 3.4877 | 2.4212 | 1.6922 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
N3 |
H5 |
112.522 |
|
C1 |
N3 |
H6 |
117.515 |
C1 |
N4 |
H7 |
112.522 |
|
C1 |
N4 |
H8 |
117.515 |
O2 |
C1 |
N3 |
123.186 |
|
O2 |
C1 |
N4 |
123.186 |
N3 |
C1 |
N4 |
113.628 |
|
H5 |
N3 |
H6 |
114.169 |
H7 |
N4 |
H8 |
114.169 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-31G(2df,p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.460 |
|
|
|
2 |
O |
-0.390 |
|
|
|
3 |
N |
-0.591 |
|
|
|
4 |
N |
-0.591 |
|
|
|
5 |
H |
0.283 |
|
|
|
6 |
H |
0.272 |
|
|
|
7 |
H |
0.283 |
|
|
|
8 |
H |
0.272 |
|
|
|
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 |
-3.523 |
3.523 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-24.731 |
2.389 |
0.000 |
y |
2.389 |
-16.800 |
0.000 |
z |
0.000 |
0.000 |
-24.229 |
|
Traceless |
| x | y | z |
x |
-4.216 |
2.389 |
0.000 |
y |
2.389 |
7.680 |
0.000 |
z |
0.000 |
0.000 |
-3.463 |
|
Polar |
3z2-r2 | -6.927 |
x2-y2 | -7.931 |
xy | 2.389 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.568 |
-0.083 |
0.000 |
y |
-0.083 |
4.944 |
0.000 |
z |
0.000 |
0.000 |
4.930 |
<r2> (average value of r
2) Å
2
<r2> |
68.069 |
(<r2>)1/2 |
8.250 |
Jump to
S1C1
S1C3
Energy calculated at B3PW91/6-31G(2df,p)
| hartrees |
Energy at 0K | -225.200346 |
Energy at 298.15K | -225.206063 |
HF Energy | -225.200346 |
Nuclear repulsion energy | 123.931910 |
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 B3PW91/6-31G(2df,p)
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' |
3751 |
3606 |
35.80 |
|
|
|
2 |
A' |
3628 |
3488 |
8.36 |
|
|
|
3 |
A' |
1834 |
1763 |
369.57 |
|
|
|
4 |
A' |
1634 |
1571 |
14.13 |
|
|
|
5 |
A' |
1175 |
1129 |
2.63 |
|
|
|
6 |
A' |
968 |
931 |
8.11 |
|
|
|
7 |
A' |
781 |
751 |
26.64 |
|
|
|
8 |
A' |
549 |
527 |
31.90 |
|
|
|
9 |
A' |
477 |
459 |
23.11 |
|
|
|
10 |
A' |
403 |
387 |
325.30 |
|
|
|
11 |
A" |
3748 |
3603 |
33.75 |
|
|
|
12 |
A" |
3618 |
3479 |
42.53 |
|
|
|
13 |
A" |
1619 |
1557 |
209.13 |
|
|
|
14 |
A" |
1427 |
1372 |
177.52 |
|
|
|
15 |
A" |
1013 |
974 |
16.61 |
|
|
|
16 |
A" |
569 |
547 |
26.09 |
|
|
|
17 |
A" |
418 |
402 |
63.92 |
|
|
|
18 |
A" |
166 |
160 |
44.35 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13888.0 cm
-1
Scaled (by 0.9614) Zero Point Vibrational Energy (zpe) 13352.0 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 B3PW91/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.009 |
0.142 |
0.000 |
O2 |
0.038 |
1.356 |
0.000 |
N3 |
0.038 |
-0.603 |
1.161 |
N4 |
0.038 |
-0.603 |
-1.161 |
H5 |
-0.162 |
-0.070 |
1.991 |
H6 |
-0.278 |
-1.558 |
1.166 |
H7 |
-0.162 |
-0.070 |
-1.991 |
H8 |
-0.278 |
-1.558 |
-1.166 |
Atom - Atom Distances (Å)
|
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.2144 | 1.3795 | 1.3795 | 2.0090 | 2.0809 | 2.0090 | 2.0809 |
O2 | 1.2144 | | 2.2768 | 2.2768 | 2.4565 | 3.1539 | 2.4565 | 3.1539 | N3 | 1.3795 | 2.2768 | | 2.3221 | 1.0058 | 1.0056 | 3.2025 | 2.5353 | N4 | 1.3795 | 2.2768 | 2.3221 | | 3.2025 | 2.5353 | 1.0058 | 1.0056 | H5 | 2.0090 | 2.4565 | 1.0058 | 3.2025 | | 1.7047 | 3.9811 | 3.4918 | H6 | 2.0809 | 3.1539 | 1.0056 | 2.5353 | 1.7047 | | 3.4918 | 2.3326 | H7 | 2.0090 | 2.4565 | 3.2025 | 1.0058 | 3.9811 | 3.4918 | | 1.7047 | H8 | 2.0809 | 3.1539 | 2.5353 | 1.0056 | 3.4918 | 2.3326 | 1.7047 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
N3 |
H5 |
113.836 |
|
C1 |
N3 |
H6 |
120.684 |
C1 |
N4 |
H7 |
113.836 |
|
C1 |
N4 |
H8 |
120.684 |
O2 |
C1 |
N3 |
122.616 |
|
O2 |
C1 |
N4 |
122.616 |
N3 |
C1 |
N4 |
114.626 |
|
H5 |
N3 |
H6 |
115.888 |
H7 |
N4 |
H8 |
115.888 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-31G(2df,p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.475 |
|
|
|
2 |
O |
-0.400 |
|
|
|
3 |
N |
-0.589 |
|
|
|
4 |
N |
-0.589 |
|
|
|
5 |
H |
0.285 |
|
|
|
6 |
H |
0.267 |
|
|
|
7 |
H |
0.285 |
|
|
|
8 |
H |
0.267 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-1.574 |
-3.814 |
0.000 |
4.126 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-24.650 |
1.641 |
0.000 |
y |
1.641 |
-23.699 |
0.000 |
z |
0.000 |
0.000 |
-16.843 |
|
Traceless |
| x | y | z |
x |
-4.379 |
1.641 |
0.000 |
y |
1.641 |
-2.953 |
0.000 |
z |
0.000 |
0.000 |
7.332 |
|
Polar |
3z2-r2 | 14.664 |
x2-y2 | -0.951 |
xy | 1.641 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.500 |
0.143 |
0.000 |
y |
0.143 |
4.956 |
0.000 |
z |
0.000 |
0.000 |
4.966 |
<r2> (average value of r
2) Å
2
<r2> |
68.102 |
(<r2>)1/2 |
8.252 |
Jump to
S1C1
S1C2
Energy calculated at B3PW91/6-31G(2df,p)
| hartrees |
Energy at 0K | -225.199603 |
Energy at 298.15K | |
HF Energy | -225.199603 |
Nuclear repulsion energy | 124.101819 |
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 B3PW91/6-31G(2df,p)
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 |
3798 |
3651 |
49.91 |
|
|
|
2 |
A1 |
3662 |
3521 |
6.32 |
|
|
|
3 |
A1 |
1828 |
1758 |
400.05 |
|
|
|
4 |
A1 |
1621 |
1558 |
4.20 |
|
|
|
5 |
A1 |
1144 |
1099 |
0.24 |
|
|
|
6 |
A1 |
977 |
939 |
6.97 |
|
|
|
7 |
A1 |
474 |
456 |
3.56 |
|
|
|
8 |
A2 |
379 |
364 |
0.00 |
|
|
|
9 |
A2 |
403i |
387i |
0.00 |
|
|
|
10 |
B1 |
783 |
752 |
8.02 |
|
|
|
11 |
B1 |
572 |
550 |
8.67 |
|
|
|
12 |
B1 |
303i |
291i |
431.99 |
|
|
|
13 |
B2 |
3795 |
3649 |
42.33 |
|
|
|
14 |
B2 |
3653 |
3512 |
63.80 |
|
|
|
15 |
B2 |
1616 |
1553 |
277.54 |
|
|
|
16 |
B2 |
1432 |
1377 |
181.30 |
|
|
|
17 |
B2 |
982 |
944 |
10.42 |
|
|
|
18 |
B2 |
559 |
538 |
14.63 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13284.0 cm
-1
Scaled (by 0.9614) Zero Point Vibrational Energy (zpe) 12771.2 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 B3PW91/6-31G(2df,p)
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 |
1.359 |
N3 |
0.000 |
1.155 |
-0.597 |
N4 |
0.000 |
-1.155 |
-0.597 |
H5 |
0.000 |
2.018 |
-0.086 |
H6 |
0.000 |
1.183 |
-1.599 |
H7 |
0.000 |
-2.018 |
-0.086 |
H8 |
0.000 |
-1.183 |
-1.599 |
Atom - Atom Distances (Å)
|
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.2159 | 1.3715 | 1.3715 | 2.0306 | 2.1052 | 2.0306 | 2.1052 |
O2 | 1.2159 | | 2.2710 | 2.2710 | 2.4814 | 3.1851 | 2.4814 | 3.1851 | N3 | 1.3715 | 2.2710 | | 2.3101 | 1.0026 | 1.0023 | 3.2137 | 2.5438 | N4 | 1.3715 | 2.2710 | 2.3101 | | 3.2137 | 2.5438 | 1.0026 | 1.0023 | H5 | 2.0306 | 2.4814 | 1.0026 | 3.2137 | | 1.7277 | 4.0354 | 3.5404 | H6 | 2.1052 | 3.1851 | 1.0023 | 2.5438 | 1.7277 | | 3.5404 | 2.3664 | H7 | 2.0306 | 2.4814 | 3.2137 | 1.0026 | 4.0354 | 3.5404 | | 1.7277 | H8 | 2.1052 | 3.1851 | 2.5438 | 1.0023 | 3.5404 | 2.3664 | 1.7277 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
N3 |
H5 |
116.738 |
|
C1 |
N3 |
H6 |
124.232 |
C1 |
N4 |
H7 |
116.738 |
|
C1 |
N4 |
H8 |
124.232 |
O2 |
C1 |
N3 |
122.625 |
|
O2 |
C1 |
N4 |
122.625 |
N3 |
C1 |
N4 |
114.751 |
|
H5 |
N3 |
H6 |
119.030 |
H7 |
N4 |
H8 |
119.030 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-31G(2df,p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.499 |
|
|
|
2 |
O |
-0.414 |
|
|
|
3 |
N |
-0.599 |
|
|
|
4 |
N |
-0.599 |
|
|
|
5 |
H |
0.286 |
|
|
|
6 |
H |
0.270 |
|
|
|
7 |
H |
0.286 |
|
|
|
8 |
H |
0.270 |
|
|
|
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 |
-4.165 |
4.165 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-25.057 |
0.000 |
0.000 |
y |
0.000 |
-16.016 |
0.000 |
z |
0.000 |
0.000 |
-23.156 |
|
Traceless |
| x | y | z |
x |
-5.471 |
0.000 |
0.000 |
y |
0.000 |
8.090 |
0.000 |
z |
0.000 |
0.000 |
-2.620 |
|
Polar |
3z2-r2 | -5.239 |
x2-y2 | -9.041 |
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 |
2.416 |
0.000 |
0.000 |
y |
0.000 |
4.964 |
0.000 |
z |
0.000 |
0.000 |
4.949 |
<r2> (average value of r
2) Å
2
<r2> |
67.992 |
(<r2>)1/2 |
8.246 |