Jump to
S1C2
S1C3
Energy calculated at B1B95/6-311G*
| | hartrees |
| Energy at 0K | -209.156838 |
| Energy at 298.15K | -209.162921 |
| HF Energy | -209.156838 |
| Nuclear repulsion energy | 119.798395 |
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 B1B95/6-311G*
| 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' |
3650 |
3499 |
18.71 |
|
|
|
| 2 |
A' |
3150 |
3020 |
21.13 |
|
|
|
| 3 |
A' |
3054 |
2928 |
59.09 |
|
|
|
| 4 |
A' |
2954 |
2831 |
104.75 |
|
|
|
| 5 |
A' |
1852 |
1775 |
508.53 |
|
|
|
| 6 |
A' |
1557 |
1493 |
23.87 |
|
|
|
| 7 |
A' |
1511 |
1448 |
7.82 |
|
|
|
| 8 |
A' |
1484 |
1423 |
5.94 |
|
|
|
| 9 |
A' |
1415 |
1356 |
9.82 |
|
|
|
| 10 |
A' |
1322 |
1267 |
106.32 |
|
|
|
| 11 |
A' |
1187 |
1138 |
28.33 |
|
|
|
| 12 |
A' |
1026 |
983 |
47.07 |
|
|
|
| 13 |
A' |
621 |
595 |
15.40 |
|
|
|
| 14 |
A' |
351 |
336 |
8.64 |
|
|
|
| 15 |
A" |
3113 |
2984 |
36.67 |
|
|
|
| 16 |
A" |
1506 |
1443 |
7.45 |
|
|
|
| 17 |
A" |
1158 |
1110 |
0.44 |
|
|
|
| 18 |
A" |
1044 |
1001 |
0.35 |
|
|
|
| 19 |
A" |
641 |
614 |
136.59 |
|
|
|
| 20 |
A" |
205 |
197 |
1.09 |
|
|
|
| 21 |
A" |
100 |
96 |
0.88 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16449.5 cm
-1
Scaled (by 0.9586) Zero Point Vibrational Energy (zpe) 15768.5 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 B1B95/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.284 |
-0.754 |
0.000 |
| O2 |
1.393 |
-1.228 |
0.000 |
| N3 |
0.000 |
0.569 |
0.000 |
| C4 |
-1.325 |
1.128 |
0.000 |
| H5 |
-0.632 |
-1.374 |
0.000 |
| H6 |
0.796 |
1.185 |
0.000 |
| H7 |
-2.049 |
0.314 |
0.000 |
| H8 |
-1.507 |
1.738 |
0.887 |
| H9 |
-1.507 |
1.738 |
-0.887 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.2057 | 1.3533 | 2.4769 | 1.1068 | 2.0060 | 2.5662 | 3.1944 | 3.1944 |
O2 | 1.2057 | | 2.2738 | 3.5976 | 2.0307 | 2.4863 | 3.7717 | 4.2416 | 4.2416 | N3 | 1.3533 | 2.2738 | | 1.4386 | 2.0435 | 1.0070 | 2.0647 | 2.1030 | 2.1030 | C4 | 2.4769 | 3.5976 | 1.4386 | | 2.5966 | 2.1225 | 1.0891 | 1.0914 | 1.0914 | H5 | 1.1068 | 2.0307 | 2.0435 | 2.5966 | | 2.9313 | 2.2038 | 3.3518 | 3.3518 | H6 | 2.0060 | 2.4863 | 1.0070 | 2.1225 | 2.9313 | | 2.9756 | 2.5289 | 2.5289 | H7 | 2.5662 | 3.7717 | 2.0647 | 1.0891 | 2.2038 | 2.9756 | | 1.7628 | 1.7628 | H8 | 3.1944 | 4.2416 | 2.1030 | 1.0914 | 3.3518 | 2.5289 | 1.7628 | | 1.7741 | H9 | 3.1944 | 4.2416 | 2.1030 | 1.0914 | 3.3518 | 2.5289 | 1.7628 | 1.7741 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
125.007 |
|
C1 |
N3 |
H6 |
115.616 |
| O2 |
C1 |
N3 |
125.285 |
|
O2 |
C1 |
H5 |
122.777 |
| N3 |
C1 |
H5 |
111.938 |
|
N3 |
C4 |
H7 |
108.752 |
| N3 |
C4 |
H8 |
111.720 |
|
N3 |
C4 |
H9 |
111.720 |
| C4 |
N3 |
H6 |
119.378 |
|
H7 |
C4 |
H8 |
107.887 |
| H7 |
C4 |
H9 |
107.887 |
|
H8 |
C4 |
H9 |
108.730 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.215 |
|
|
|
| 2 |
O |
-0.368 |
|
|
|
| 3 |
N |
-0.526 |
|
|
|
| 4 |
C |
-0.499 |
|
|
|
| 5 |
H |
0.145 |
|
|
|
| 6 |
H |
0.345 |
|
|
|
| 7 |
H |
0.225 |
|
|
|
| 8 |
H |
0.232 |
|
|
|
| 9 |
H |
0.232 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.962 |
2.789 |
0.000 |
4.069 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.181 |
4.011 |
0.000 |
| y |
4.011 |
-24.170 |
0.000 |
| z |
0.000 |
0.000 |
-24.670 |
|
| Traceless |
| | x | y | z |
| x |
-1.761 |
4.011 |
0.000 |
| y |
4.011 |
1.256 |
0.000 |
| z |
0.000 |
0.000 |
0.505 |
|
| Polar |
| 3z2-r2 | 1.010 |
| x2-y2 | -2.011 |
| xy | 4.011 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.594 |
-1.022 |
0.000 |
| y |
-1.022 |
5.629 |
0.000 |
| z |
0.000 |
0.000 |
3.226 |
<r2> (average value of r
2) Å
2
| <r2> |
88.329 |
| (<r2>)1/2 |
9.398 |
Jump to
S1C1
S1C3
Energy calculated at B1B95/6-311G*
| | hartrees |
| Energy at 0K | -209.156838 |
| Energy at 298.15K | -209.162921 |
| HF Energy | -209.156838 |
| Nuclear repulsion energy | 119.798395 |
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 B1B95/6-311G*
Geometric Data calculated at B1B95/6-311G*
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
Energy calculated at B1B95/6-311G*
| | hartrees |
| Energy at 0K | -209.158763 |
| Energy at 298.15K | -209.164894 |
| HF Energy | -209.158763 |
| Nuclear repulsion energy | 122.041516 |
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 B1B95/6-311G*
| 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 |
3685 |
3532 |
19.25 |
|
|
|
| 2 |
A |
3190 |
3058 |
1.63 |
|
|
|
| 3 |
A |
3121 |
2992 |
37.71 |
|
|
|
| 4 |
A |
3062 |
2935 |
48.38 |
|
|
|
| 5 |
A |
2972 |
2849 |
135.92 |
|
|
|
| 6 |
A |
1838 |
1762 |
351.15 |
|
|
|
| 7 |
A |
1588 |
1522 |
112.41 |
|
|
|
| 8 |
A |
1521 |
1458 |
8.99 |
|
|
|
| 9 |
A |
1513 |
1450 |
34.41 |
|
|
|
| 10 |
A |
1459 |
1399 |
20.08 |
|
|
|
| 11 |
A |
1433 |
1374 |
3.15 |
|
|
|
| 12 |
A |
1242 |
1191 |
75.32 |
|
|
|
| 13 |
A |
1175 |
1126 |
21.29 |
|
|
|
| 14 |
A |
1161 |
1113 |
0.80 |
|
|
|
| 15 |
A |
1025 |
982 |
0.36 |
|
|
|
| 16 |
A |
987 |
946 |
21.73 |
|
|
|
| 17 |
A |
781 |
749 |
0.85 |
|
|
|
| 18 |
A |
551 |
528 |
54.79 |
|
|
|
| 19 |
A |
317 |
304 |
13.12 |
|
|
|
| 20 |
A |
280 |
269 |
79.74 |
|
|
|
| 21 |
A |
89 |
86 |
0.05 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16494.8 cm
-1
Scaled (by 0.9586) Zero Point Vibrational Energy (zpe) 15811.9 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 B1B95/6-311G*
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.859 |
0.433 |
0.004 |
| O2 |
1.362 |
-0.669 |
-0.000 |
| N3 |
-0.470 |
0.658 |
-0.020 |
| C4 |
-1.410 |
-0.440 |
0.005 |
| H5 |
1.455 |
1.359 |
0.018 |
| H6 |
-0.801 |
1.602 |
0.057 |
| H7 |
-2.405 |
-0.062 |
-0.215 |
| H8 |
-1.131 |
-1.174 |
-0.747 |
| H9 |
-1.418 |
-0.935 |
0.977 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.2109 | 1.3480 | 2.4310 | 1.1017 | 2.0312 | 3.3088 | 2.6660 | 2.8289 |
O2 | 1.2109 | | 2.2617 | 2.7809 | 2.0303 | 3.1365 | 3.8215 | 2.6506 | 2.9583 | N3 | 1.3480 | 2.2617 | | 1.4458 | 2.0490 | 1.0036 | 2.0742 | 2.0794 | 2.1052 | C4 | 2.4310 | 2.7809 | 1.4458 | | 3.3832 | 2.1319 | 1.0872 | 1.0878 | 1.0908 | H5 | 1.1017 | 2.0303 | 2.0490 | 3.3832 | | 2.2694 | 4.1203 | 3.7003 | 3.8000 | H6 | 2.0312 | 3.1365 | 1.0036 | 2.1319 | 2.2694 | | 2.3277 | 2.9099 | 2.7687 | H7 | 3.3088 | 3.8215 | 2.0742 | 1.0872 | 4.1203 | 2.3277 | | 1.7736 | 1.7768 | H8 | 2.6660 | 2.6506 | 2.0794 | 1.0878 | 3.7003 | 2.9099 | 1.7736 | | 1.7642 | H9 | 2.8289 | 2.9583 | 2.1052 | 1.0908 | 3.8000 | 2.7687 | 1.7768 | 1.7642 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
120.911 |
|
C1 |
N3 |
H6 |
118.750 |
| O2 |
C1 |
N3 |
124.135 |
|
O2 |
C1 |
H5 |
122.714 |
| N3 |
C1 |
H5 |
113.147 |
|
N3 |
C4 |
H7 |
109.125 |
| N3 |
C4 |
H8 |
109.506 |
|
N3 |
C4 |
H9 |
111.418 |
| C4 |
N3 |
H6 |
119.921 |
|
H7 |
C4 |
H8 |
109.268 |
| H7 |
C4 |
H9 |
109.338 |
|
H8 |
C4 |
H9 |
108.156 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.206 |
|
|
|
| 2 |
O |
-0.370 |
|
|
|
| 3 |
N |
-0.533 |
|
|
|
| 4 |
C |
-0.517 |
|
|
|
| 5 |
H |
0.157 |
|
|
|
| 6 |
H |
0.346 |
|
|
|
| 7 |
H |
0.227 |
|
|
|
| 8 |
H |
0.258 |
|
|
|
| 9 |
H |
0.227 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.895 |
2.613 |
0.000 |
3.900 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.378 |
2.523 |
0.000 |
| y |
2.523 |
-21.917 |
0.001 |
| z |
0.000 |
0.001 |
-24.699 |
|
| Traceless |
| | x | y | z |
| x |
-2.070 |
2.523 |
0.000 |
| y |
2.523 |
3.122 |
0.001 |
| z |
0.000 |
0.001 |
-1.051 |
|
| Polar |
| 3z2-r2 | -2.103 |
| x2-y2 | -3.461 |
| xy | 2.523 |
| xz | 0.000 |
| yz | 0.001 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.985 |
-0.088 |
-0.000 |
| y |
-0.088 |
5.001 |
-0.000 |
| z |
-0.000 |
-0.000 |
3.217 |
<r2> (average value of r
2) Å
2
| <r2> |
77.707 |
| (<r2>)1/2 |
8.815 |