Jump to
S1C2
S1C3
Energy calculated at HF/6-311G**
| | hartrees |
| Energy at 0K | -224.055118 |
| Energy at 298.15K | -224.061537 |
| HF Energy | -224.055118 |
| Nuclear repulsion energy | 125.273610 |
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/6-311G**
| 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 |
3916 |
3558 |
52.87 |
|
|
|
| 2 |
A |
3805 |
3457 |
5.88 |
|
|
|
| 3 |
A |
1979 |
1798 |
572.86 |
|
|
|
| 4 |
A |
1778 |
1616 |
0.00 |
|
|
|
| 5 |
A |
1292 |
1174 |
6.85 |
|
|
|
| 6 |
A |
1026 |
932 |
9.81 |
|
|
|
| 7 |
A |
626 |
569 |
78.05 |
|
|
|
| 8 |
A |
516 |
468 |
2.18 |
|
|
|
| 9 |
A |
408 |
370 |
91.98 |
|
|
|
| 10 |
B |
3916 |
3558 |
28.10 |
|
|
|
| 11 |
B |
3800 |
3453 |
65.83 |
|
|
|
| 12 |
B |
1787 |
1623 |
226.15 |
|
|
|
| 13 |
B |
1531 |
1391 |
243.93 |
|
|
|
| 14 |
B |
1151 |
1045 |
28.51 |
|
|
|
| 15 |
B |
882 |
801 |
128.96 |
|
|
|
| 16 |
B |
631 |
573 |
65.97 |
|
|
|
| 17 |
B |
587 |
533 |
247.30 |
|
|
|
| 18 |
B |
478 |
434 |
111.98 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15053.8 cm
-1
Scaled (by 0.9085) Zero Point Vibrational Energy (zpe) 13676.4 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/6-311G**
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 |
1.338 |
| N3 |
0.000 |
1.151 |
-0.603 |
| N4 |
0.000 |
-1.151 |
-0.603 |
| H5 |
0.205 |
1.968 |
-0.074 |
| H6 |
0.429 |
1.117 |
-1.499 |
| H7 |
-0.205 |
-1.968 |
-0.074 |
| H8 |
-0.429 |
-1.117 |
-1.499 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.1915 | 1.3735 | 1.3735 | 1.9912 | 2.0345 | 1.9912 | 2.0345 |
O2 | 1.1915 | | 2.2563 | 2.2563 | 2.4309 | 3.0789 | 2.4309 | 3.0789 | N3 | 1.3735 | 2.2563 | | 2.3025 | 0.9946 | 0.9944 | 3.1708 | 2.4764 | N4 | 1.3735 | 2.2563 | 2.3025 | | 3.1708 | 2.4764 | 0.9946 | 0.9944 | H5 | 1.9912 | 2.4309 | 0.9946 | 3.1708 | | 1.6753 | 3.9580 | 3.4572 | H6 | 2.0345 | 3.0789 | 0.9944 | 2.4764 | 1.6753 | | 3.4572 | 2.3932 | H7 | 1.9912 | 2.4309 | 3.1708 | 0.9946 | 3.9580 | 3.4572 | | 1.6753 | H8 | 2.0345 | 3.0789 | 2.4764 | 0.9944 | 3.4572 | 2.3932 | 1.6753 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
113.495 |
|
C1 |
N3 |
H6 |
117.558 |
| C1 |
N4 |
H7 |
113.495 |
|
C1 |
N4 |
H8 |
117.558 |
| O2 |
C1 |
N3 |
123.049 |
|
O2 |
C1 |
N4 |
123.049 |
| N3 |
C1 |
N4 |
113.903 |
|
H5 |
N3 |
H6 |
114.759 |
| H7 |
N4 |
H8 |
114.759 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.624 |
|
|
|
| 2 |
O |
-0.497 |
|
|
|
| 3 |
N |
-0.518 |
|
|
|
| 4 |
N |
-0.518 |
|
|
|
| 5 |
H |
0.238 |
|
|
|
| 6 |
H |
0.218 |
|
|
|
| 7 |
H |
0.238 |
|
|
|
| 8 |
H |
0.218 |
|
|
|
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 |
-3.880 |
3.880 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.539 |
3.356 |
0.000 |
| y |
3.356 |
-17.742 |
0.000 |
| z |
0.000 |
0.000 |
-25.277 |
|
| Traceless |
| | x | y | z |
| x |
-3.030 |
3.356 |
0.000 |
| y |
3.356 |
7.166 |
0.000 |
| z |
0.000 |
0.000 |
-4.136 |
|
| Polar |
| 3z2-r2 | -8.273 |
| x2-y2 | -6.797 |
| xy | 3.356 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.385 |
0.136 |
0.000 |
| y |
0.136 |
4.111 |
0.000 |
| z |
0.000 |
0.000 |
4.470 |
<r2> (average value of r
2) Å
2
| <r2> |
67.355 |
| (<r2>)1/2 |
8.207 |
Jump to
S1C1
S1C3
Energy calculated at HF/6-311G**
| | hartrees |
| Energy at 0K | -224.053342 |
| Energy at 298.15K | -224.058991 |
| HF Energy | -224.053342 |
| Nuclear repulsion energy | 125.356612 |
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/6-311G**
| 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' |
3954 |
3592 |
63.44 |
|
|
|
| 2 |
A' |
3832 |
3482 |
13.19 |
|
|
|
| 3 |
A' |
1962 |
1782 |
612.47 |
|
|
|
| 4 |
A' |
1785 |
1621 |
9.26 |
|
|
|
| 5 |
A' |
1279 |
1162 |
6.22 |
|
|
|
| 6 |
A' |
1036 |
941 |
13.21 |
|
|
|
| 7 |
A' |
865 |
786 |
56.52 |
|
|
|
| 8 |
A' |
578 |
525 |
26.64 |
|
|
|
| 9 |
A' |
521 |
473 |
13.20 |
|
|
|
| 10 |
A' |
373 |
339 |
462.43 |
|
|
|
| 11 |
A" |
3951 |
3589 |
31.55 |
|
|
|
| 12 |
A" |
3824 |
3474 |
71.54 |
|
|
|
| 13 |
A" |
1776 |
1613 |
254.11 |
|
|
|
| 14 |
A" |
1533 |
1392 |
258.06 |
|
|
|
| 15 |
A" |
1111 |
1009 |
20.85 |
|
|
|
| 16 |
A" |
626 |
568 |
26.69 |
|
|
|
| 17 |
A" |
445 |
404 |
41.87 |
|
|
|
| 18 |
A" |
36 |
33 |
43.51 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14741.8 cm
-1
Scaled (by 0.9085) Zero Point Vibrational Energy (zpe) 13392.9 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/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.011 |
0.143 |
0.000 |
| O2 |
0.031 |
1.337 |
0.000 |
| N3 |
0.031 |
-0.593 |
1.152 |
| N4 |
0.031 |
-0.593 |
-1.152 |
| H5 |
-0.140 |
-0.080 |
1.984 |
| H6 |
-0.232 |
-1.549 |
1.152 |
| H7 |
-0.140 |
-0.080 |
-1.984 |
| H8 |
-0.232 |
-1.549 |
-1.152 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.1938 | 1.3672 | 1.3672 | 2.0026 | 2.0617 | 2.0026 | 2.0617 |
O2 | 1.1938 | | 2.2473 | 2.2473 | 2.4441 | 3.1186 | 2.4441 | 3.1186 | N3 | 1.3672 | 2.2473 | | 2.3039 | 0.9927 | 0.9917 | 3.1827 | 2.5085 | N4 | 1.3672 | 2.2473 | 2.3039 | | 3.1827 | 2.5085 | 0.9927 | 0.9917 | H5 | 2.0026 | 2.4441 | 0.9927 | 3.1827 | | 1.6913 | 3.9689 | 3.4651 | H6 | 2.0617 | 3.1186 | 0.9917 | 2.5085 | 1.6913 | | 3.4651 | 2.3044 | H7 | 2.0026 | 2.4441 | 3.1827 | 0.9927 | 3.9689 | 3.4651 | | 1.6913 | H8 | 2.0617 | 3.1186 | 2.5085 | 0.9917 | 3.4651 | 2.3044 | 1.6913 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
115.199 |
|
C1 |
N3 |
H6 |
121.034 |
| C1 |
N4 |
H7 |
115.199 |
|
C1 |
N4 |
H8 |
121.034 |
| O2 |
C1 |
N3 |
122.552 |
|
O2 |
C1 |
N4 |
122.552 |
| N3 |
C1 |
N4 |
114.826 |
|
H5 |
N3 |
H6 |
116.932 |
| H7 |
N4 |
H8 |
116.932 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.643 |
|
|
|
| 2 |
O |
-0.510 |
|
|
|
| 3 |
N |
-0.523 |
|
|
|
| 4 |
N |
-0.523 |
|
|
|
| 5 |
H |
0.244 |
|
|
|
| 6 |
H |
0.212 |
|
|
|
| 7 |
H |
0.244 |
|
|
|
| 8 |
H |
0.212 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.508 |
-4.290 |
0.000 |
4.547 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.177 |
1.531 |
0.000 |
| y |
1.531 |
-24.592 |
0.000 |
| z |
0.000 |
0.000 |
-17.080 |
|
| Traceless |
| | x | y | z |
| x |
-4.340 |
1.531 |
0.000 |
| y |
1.531 |
-3.464 |
0.000 |
| z |
0.000 |
0.000 |
7.804 |
|
| Polar |
| 3z2-r2 | 15.608 |
| x2-y2 | -0.584 |
| xy | 1.531 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.318 |
0.095 |
0.000 |
| y |
0.095 |
4.430 |
0.000 |
| z |
0.000 |
0.000 |
4.107 |
<r2> (average value of r
2) Å
2
| <r2> |
67.347 |
| (<r2>)1/2 |
8.207 |
Jump to
S1C1
S1C2
Energy calculated at HF/6-311G**
| | hartrees |
| Energy at 0K | -224.052923 |
| Energy at 298.15K | |
| HF Energy | -224.052923 |
| Nuclear repulsion energy | 125.463860 |
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/6-311G**
| 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 |
3987 |
3622 |
83.24 |
|
|
|
| 2 |
A1 |
3854 |
3501 |
10.11 |
|
|
|
| 3 |
A1 |
1950 |
1771 |
652.83 |
|
|
|
| 4 |
A1 |
1775 |
1612 |
0.82 |
|
|
|
| 5 |
A1 |
1255 |
1140 |
2.40 |
|
|
|
| 6 |
A1 |
1044 |
948 |
12.52 |
|
|
|
| 7 |
A1 |
521 |
473 |
2.58 |
|
|
|
| 8 |
A2 |
425 |
386 |
0.00 |
|
|
|
| 9 |
A2 |
416i |
378i |
0.00 |
|
|
|
| 10 |
B1 |
864 |
785 |
28.40 |
|
|
|
| 11 |
B1 |
599 |
545 |
8.82 |
|
|
|
| 12 |
B1 |
274i |
249i |
554.72 |
|
|
|
| 13 |
B2 |
3984 |
3619 |
37.29 |
|
|
|
| 14 |
B2 |
3845 |
3494 |
94.60 |
|
|
|
| 15 |
B2 |
1770 |
1608 |
301.08 |
|
|
|
| 16 |
B2 |
1535 |
1394 |
279.08 |
|
|
|
| 17 |
B2 |
1089 |
989 |
14.19 |
|
|
|
| 18 |
B2 |
620 |
563 |
19.87 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14212.3 cm
-1
Scaled (by 0.9085) Zero Point Vibrational Energy (zpe) 12911.9 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/6-311G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.144 |
| O2 |
0.000 |
0.000 |
1.339 |
| N3 |
0.000 |
1.148 |
-0.589 |
| N4 |
0.000 |
-1.148 |
-0.589 |
| H5 |
0.000 |
2.004 |
-0.090 |
| H6 |
0.000 |
1.164 |
-1.578 |
| H7 |
0.000 |
-2.004 |
-0.090 |
| H8 |
0.000 |
-1.164 |
-1.578 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.1956 | 1.3613 | 1.3613 | 2.0172 | 2.0784 | 2.0172 | 2.0784 |
O2 | 1.1956 | | 2.2437 | 2.2437 | 2.4611 | 3.1411 | 2.4611 | 3.1411 | N3 | 1.3613 | 2.2437 | | 2.2950 | 0.9908 | 0.9896 | 3.1903 | 2.5144 | N4 | 1.3613 | 2.2437 | 2.2950 | | 3.1903 | 2.5144 | 0.9908 | 0.9896 | H5 | 2.0172 | 2.4611 | 0.9908 | 3.1903 | | 1.7087 | 4.0072 | 3.4998 | H6 | 2.0784 | 3.1411 | 0.9896 | 2.5144 | 1.7087 | | 3.4998 | 2.3280 | H7 | 2.0172 | 2.4611 | 3.1903 | 0.9908 | 4.0072 | 3.4998 | | 1.7087 | H8 | 2.0784 | 3.1411 | 2.5144 | 0.9896 | 3.4998 | 2.3280 | 1.7087 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
117.229 |
|
C1 |
N3 |
H6 |
123.502 |
| C1 |
N4 |
H7 |
117.229 |
|
C1 |
N4 |
H8 |
123.502 |
| O2 |
C1 |
N3 |
122.547 |
|
O2 |
C1 |
N4 |
122.547 |
| N3 |
C1 |
N4 |
114.905 |
|
H5 |
N3 |
H6 |
119.269 |
| H7 |
N4 |
H8 |
119.269 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.672 |
|
|
|
| 2 |
O |
-0.520 |
|
|
|
| 3 |
N |
-0.551 |
|
|
|
| 4 |
N |
-0.551 |
|
|
|
| 5 |
H |
0.253 |
|
|
|
| 6 |
H |
0.222 |
|
|
|
| 7 |
H |
0.253 |
|
|
|
| 8 |
H |
0.222 |
|
|
|
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 |
-4.579 |
4.579 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.490 |
0.000 |
0.000 |
| y |
0.000 |
-16.458 |
0.000 |
| z |
0.000 |
0.000 |
-24.183 |
|
| Traceless |
| | x | y | z |
| x |
-5.170 |
0.000 |
0.000 |
| y |
0.000 |
8.379 |
0.000 |
| z |
0.000 |
0.000 |
-3.209 |
|
| Polar |
| 3z2-r2 | -6.418 |
| x2-y2 | -9.033 |
| 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 |
2.269 |
0.000 |
0.000 |
| y |
0.000 |
4.083 |
0.000 |
| z |
0.000 |
0.000 |
4.364 |
<r2> (average value of r
2) Å
2
| <r2> |
67.265 |
| (<r2>)1/2 |
8.202 |