Jump to
S1C2
S1C3
Energy calculated at B1B95/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -209.139707 |
| Energy at 298.15K | -209.145793 |
| HF Energy | -209.139707 |
| Nuclear repulsion energy | 119.505964 |
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/aug-cc-pVDZ
| 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' |
3640 |
3487 |
29.83 |
|
|
|
| 2 |
A' |
3159 |
3026 |
13.59 |
|
|
|
| 3 |
A' |
3056 |
2927 |
54.86 |
|
|
|
| 4 |
A' |
2974 |
2848 |
77.91 |
|
|
|
| 5 |
A' |
1813 |
1736 |
556.62 |
|
|
|
| 6 |
A' |
1525 |
1461 |
25.89 |
|
|
|
| 7 |
A' |
1479 |
1416 |
5.34 |
|
|
|
| 8 |
A' |
1447 |
1386 |
5.92 |
|
|
|
| 9 |
A' |
1384 |
1325 |
13.77 |
|
|
|
| 10 |
A' |
1312 |
1256 |
100.84 |
|
|
|
| 11 |
A' |
1179 |
1129 |
21.54 |
|
|
|
| 12 |
A' |
1017 |
974 |
40.56 |
|
|
|
| 13 |
A' |
617 |
591 |
14.44 |
|
|
|
| 14 |
A' |
348 |
333 |
8.29 |
|
|
|
| 15 |
A" |
3123 |
2992 |
23.25 |
|
|
|
| 16 |
A" |
1458 |
1397 |
6.46 |
|
|
|
| 17 |
A" |
1140 |
1092 |
0.41 |
|
|
|
| 18 |
A" |
1036 |
992 |
2.09 |
|
|
|
| 19 |
A" |
623 |
597 |
111.29 |
|
|
|
| 20 |
A" |
210 |
202 |
0.25 |
|
|
|
| 21 |
A" |
104 |
100 |
0.45 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16320.2 cm
-1
Scaled (by 0.9579) Zero Point Vibrational Energy (zpe) 15633.1 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/aug-cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.282 |
-0.753 |
0.000 |
| O2 |
1.400 |
-1.226 |
0.000 |
| N3 |
0.000 |
0.571 |
0.000 |
| C4 |
-1.330 |
1.125 |
0.000 |
| H5 |
-0.634 |
-1.380 |
0.000 |
| H6 |
0.798 |
1.189 |
0.000 |
| H7 |
-2.050 |
0.301 |
0.000 |
| H8 |
-1.512 |
1.737 |
0.891 |
| H9 |
-1.512 |
1.737 |
-0.891 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.2144 | 1.3530 | 2.4742 | 1.1100 | 2.0089 | 2.5589 | 3.1949 | 3.1949 |
O2 | 1.2144 | | 2.2779 | 3.6026 | 2.0398 | 2.4889 | 3.7730 | 4.2487 | 4.2487 | N3 | 1.3530 | 2.2779 | | 1.4406 | 2.0510 | 1.0095 | 2.0678 | 2.1069 | 2.1069 | C4 | 2.4742 | 3.6026 | 1.4406 | | 2.5994 | 2.1289 | 1.0942 | 1.0963 | 1.0963 | H5 | 1.1100 | 2.0398 | 2.0510 | 2.5994 | | 2.9410 | 2.1979 | 3.3581 | 3.3581 | H6 | 2.0089 | 2.4889 | 1.0095 | 2.1289 | 2.9410 | | 2.9834 | 2.5359 | 2.5359 | H7 | 2.5589 | 3.7730 | 2.0678 | 1.0942 | 2.1979 | 2.9834 | | 1.7733 | 1.7733 | H8 | 3.1949 | 4.2487 | 2.1069 | 1.0963 | 3.3581 | 2.5359 | 1.7733 | | 1.7826 | H9 | 3.1949 | 4.2487 | 2.1069 | 1.0963 | 3.3581 | 2.5359 | 1.7733 | 1.7826 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
124.640 |
|
C1 |
N3 |
H6 |
115.734 |
| O2 |
C1 |
N3 |
124.977 |
|
O2 |
C1 |
H5 |
122.635 |
| N3 |
C1 |
H5 |
112.388 |
|
N3 |
C4 |
H7 |
108.553 |
| N3 |
C4 |
H8 |
111.589 |
|
N3 |
C4 |
H9 |
111.589 |
| C4 |
N3 |
H6 |
119.626 |
|
H7 |
C4 |
H8 |
108.101 |
| H7 |
C4 |
H9 |
108.101 |
|
H8 |
C4 |
H9 |
108.786 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.795 |
|
|
|
| 2 |
O |
-0.506 |
|
|
|
| 3 |
N |
-0.049 |
|
|
|
| 4 |
C |
0.918 |
|
|
|
| 5 |
H |
-0.315 |
|
|
|
| 6 |
H |
-0.205 |
|
|
|
| 7 |
H |
-0.254 |
|
|
|
| 8 |
H |
-0.192 |
|
|
|
| 9 |
H |
-0.192 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.195 |
2.869 |
0.000 |
4.294 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-27.034 |
4.266 |
0.000 |
| y |
4.266 |
-24.570 |
0.000 |
| z |
0.000 |
0.000 |
-24.900 |
|
| Traceless |
| | x | y | z |
| x |
-2.299 |
4.266 |
0.000 |
| y |
4.266 |
1.397 |
0.000 |
| z |
0.000 |
0.000 |
0.902 |
|
| Polar |
| 3z2-r2 | 1.805 |
| x2-y2 | -2.464 |
| xy | 4.266 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.744 |
-1.206 |
0.000 |
| y |
-1.206 |
6.632 |
0.000 |
| z |
0.000 |
0.000 |
4.304 |
<r2> (average value of r
2) Å
2
| <r2> |
88.832 |
| (<r2>)1/2 |
9.425 |
Jump to
S1C1
S1C3
Energy calculated at B1B95/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -209.139707 |
| Energy at 298.15K | -209.145793 |
| HF Energy | -209.139707 |
| Nuclear repulsion energy | 119.505964 |
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/aug-cc-pVDZ
Geometric Data calculated at B1B95/aug-cc-pVDZ
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
Energy calculated at B1B95/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -209.141639 |
| Energy at 298.15K | -209.147715 |
| HF Energy | -209.141639 |
| Nuclear repulsion energy | 121.702841 |
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/aug-cc-pVDZ
| 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 |
3679 |
3524 |
29.59 |
|
|
|
| 2 |
A |
3192 |
3057 |
0.27 |
|
|
|
| 3 |
A |
3135 |
3003 |
23.61 |
|
|
|
| 4 |
A |
3067 |
2937 |
45.49 |
|
|
|
| 5 |
A |
2993 |
2867 |
99.27 |
|
|
|
| 6 |
A |
1801 |
1725 |
387.55 |
|
|
|
| 7 |
A |
1568 |
1502 |
114.41 |
|
|
|
| 8 |
A |
1475 |
1413 |
9.06 |
|
|
|
| 9 |
A |
1475 |
1412 |
16.96 |
|
|
|
| 10 |
A |
1426 |
1366 |
15.74 |
|
|
|
| 11 |
A |
1409 |
1350 |
4.26 |
|
|
|
| 12 |
A |
1238 |
1186 |
62.74 |
|
|
|
| 13 |
A |
1157 |
1109 |
19.95 |
|
|
|
| 14 |
A |
1143 |
1094 |
0.86 |
|
|
|
| 15 |
A |
1022 |
979 |
0.10 |
|
|
|
| 16 |
A |
984 |
942 |
24.13 |
|
|
|
| 17 |
A |
768 |
735 |
1.03 |
|
|
|
| 18 |
A |
551 |
527 |
43.33 |
|
|
|
| 19 |
A |
310 |
297 |
13.97 |
|
|
|
| 20 |
A |
281 |
269 |
64.61 |
|
|
|
| 21 |
A |
63 |
60 |
0.10 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16366.9 cm
-1
Scaled (by 0.9579) Zero Point Vibrational Energy (zpe) 15677.9 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/aug-cc-pVDZ
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.861 |
0.437 |
0.003 |
| O2 |
1.365 |
-0.672 |
0.000 |
| N3 |
-0.470 |
0.657 |
-0.020 |
| C4 |
-1.415 |
-0.440 |
0.005 |
| H5 |
1.460 |
1.366 |
0.018 |
| H6 |
-0.797 |
1.605 |
0.057 |
| H7 |
-2.413 |
-0.053 |
-0.213 |
| H8 |
-1.136 |
-1.176 |
-0.754 |
| H9 |
-1.421 |
-0.939 |
0.981 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.2179 | 1.3497 | 2.4390 | 1.1058 | 2.0295 | 3.3176 | 2.6766 | 2.8380 |
O2 | 1.2179 | | 2.2658 | 2.7893 | 2.0408 | 3.1407 | 3.8341 | 2.6603 | 2.9652 | N3 | 1.3497 | 2.2658 | | 1.4475 | 2.0568 | 1.0059 | 2.0773 | 2.0838 | 2.1092 | C4 | 2.4390 | 2.7893 | 1.4475 | | 3.3951 | 2.1364 | 1.0923 | 1.0935 | 1.0961 | H5 | 1.1058 | 2.0408 | 2.0568 | 3.3951 | | 2.2704 | 4.1311 | 3.7146 | 3.8130 | H6 | 2.0295 | 3.1407 | 1.0059 | 2.1364 | 2.2704 | | 2.3302 | 2.9164 | 2.7768 | H7 | 3.3176 | 3.8341 | 2.0773 | 1.0923 | 4.1311 | 2.3302 | | 1.7847 | 1.7868 | H8 | 2.6766 | 2.6603 | 2.0838 | 1.0935 | 3.7146 | 2.9164 | 1.7847 | | 1.7743 | H9 | 2.8380 | 2.9652 | 2.1092 | 1.0961 | 3.8130 | 2.7768 | 1.7868 | 1.7743 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
121.333 |
|
C1 |
N3 |
H6 |
118.255 |
| O2 |
C1 |
N3 |
123.795 |
|
O2 |
C1 |
H5 |
122.795 |
| N3 |
C1 |
H5 |
113.408 |
|
N3 |
C4 |
H7 |
108.942 |
| N3 |
C4 |
H8 |
109.391 |
|
N3 |
C4 |
H9 |
111.290 |
| C4 |
N3 |
H6 |
120.021 |
|
H7 |
C4 |
H8 |
109.472 |
| H7 |
C4 |
H9 |
109.470 |
|
H8 |
C4 |
H9 |
108.255 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.750 |
|
|
|
| 2 |
O |
-0.486 |
|
|
|
| 3 |
N |
-0.081 |
|
|
|
| 4 |
C |
0.915 |
|
|
|
| 5 |
H |
-0.289 |
|
|
|
| 6 |
H |
-0.161 |
|
|
|
| 7 |
H |
-0.193 |
|
|
|
| 8 |
H |
-0.262 |
|
|
|
| 9 |
H |
-0.193 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.983 |
2.635 |
-0.000 |
3.980 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.896 |
2.781 |
0.000 |
| y |
2.781 |
-22.538 |
-0.000 |
| z |
0.000 |
-0.000 |
-24.973 |
|
| Traceless |
| | x | y | z |
| x |
-2.141 |
2.781 |
0.000 |
| y |
2.781 |
2.897 |
-0.000 |
| z |
0.000 |
-0.000 |
-0.756 |
|
| Polar |
| 3z2-r2 | -1.512 |
| x2-y2 | -3.358 |
| xy | 2.781 |
| xz | 0.000 |
| yz | -0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.146 |
-0.094 |
0.000 |
| y |
-0.094 |
6.011 |
0.000 |
| z |
0.000 |
0.000 |
4.351 |
<r2> (average value of r
2) Å
2
| <r2> |
78.285 |
| (<r2>)1/2 |
8.848 |