Jump to
S1C2
S1C3
Energy calculated at PBE1PBE/cc-pVDZ
| | hartrees |
| Energy at 0K | -208.974812 |
| Energy at 298.15K | -208.980886 |
| HF Energy | -208.974812 |
| Nuclear repulsion energy | 119.377434 |
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 PBE1PBE/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' |
3629 |
3489 |
27.52 |
|
|
|
| 2 |
A' |
3154 |
3032 |
11.76 |
|
|
|
| 3 |
A' |
3043 |
2925 |
54.84 |
|
|
|
| 4 |
A' |
2937 |
2824 |
95.43 |
|
|
|
| 5 |
A' |
1858 |
1787 |
478.23 |
|
|
|
| 6 |
A' |
1528 |
1469 |
29.51 |
|
|
|
| 7 |
A' |
1479 |
1422 |
9.36 |
|
|
|
| 8 |
A' |
1444 |
1388 |
3.48 |
|
|
|
| 9 |
A' |
1379 |
1326 |
10.24 |
|
|
|
| 10 |
A' |
1314 |
1263 |
96.05 |
|
|
|
| 11 |
A' |
1184 |
1139 |
18.71 |
|
|
|
| 12 |
A' |
1017 |
978 |
44.65 |
|
|
|
| 13 |
A' |
621 |
597 |
15.15 |
|
|
|
| 14 |
A' |
340 |
327 |
8.08 |
|
|
|
| 15 |
A" |
3111 |
2991 |
26.70 |
|
|
|
| 16 |
A" |
1454 |
1398 |
6.67 |
|
|
|
| 17 |
A" |
1138 |
1094 |
0.10 |
|
|
|
| 18 |
A" |
1045 |
1004 |
0.41 |
|
|
|
| 19 |
A" |
625 |
601 |
110.09 |
|
|
|
| 20 |
A" |
213 |
205 |
0.84 |
|
|
|
| 21 |
A" |
102 |
98 |
0.73 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16306.3 cm
-1
Scaled (by 0.9615) Zero Point Vibrational Energy (zpe) 15678.5 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 PBE1PBE/cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.282 |
-0.757 |
0.000 |
| O2 |
1.397 |
-1.231 |
0.000 |
| N3 |
0.000 |
0.571 |
0.000 |
| C4 |
-1.324 |
1.130 |
0.000 |
| H5 |
-0.650 |
-1.375 |
0.000 |
| H6 |
0.805 |
1.188 |
0.000 |
| H7 |
-2.055 |
0.308 |
0.000 |
| H8 |
-1.512 |
1.747 |
0.894 |
| H9 |
-1.512 |
1.747 |
-0.894 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.2115 | 1.3570 | 2.4778 | 1.1188 | 2.0140 | 2.5679 | 3.2074 | 3.2074 |
O2 | 1.2115 | | 2.2798 | 3.6026 | 2.0524 | 2.4908 | 3.7791 | 4.2580 | 4.2580 | N3 | 1.3570 | 2.2798 | | 1.4374 | 2.0514 | 1.0144 | 2.0713 | 2.1141 | 2.1141 | C4 | 2.4778 | 3.6026 | 1.4374 | | 2.5940 | 2.1295 | 1.0998 | 1.1025 | 1.1025 | H5 | 1.1188 | 2.0524 | 2.0514 | 2.5940 | | 2.9474 | 2.1918 | 3.3600 | 3.3600 | H6 | 2.0140 | 2.4908 | 1.0144 | 2.1295 | 2.9474 | | 2.9917 | 2.5451 | 2.5451 | H7 | 2.5679 | 3.7791 | 2.0713 | 1.0998 | 2.1918 | 2.9917 | | 1.7792 | 1.7792 | H8 | 3.2074 | 4.2580 | 2.1141 | 1.1025 | 3.3600 | 2.5451 | 1.7792 | | 1.7880 | H9 | 3.2074 | 4.2580 | 2.1141 | 1.1025 | 3.3600 | 2.5451 | 1.7792 | 1.7880 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
124.905 |
|
C1 |
N3 |
H6 |
115.510 |
| O2 |
C1 |
N3 |
125.053 |
|
O2 |
C1 |
H5 |
123.405 |
| N3 |
C1 |
H5 |
111.541 |
|
N3 |
C4 |
H7 |
108.721 |
| N3 |
C4 |
H8 |
112.009 |
|
N3 |
C4 |
H9 |
112.009 |
| C4 |
N3 |
H6 |
119.585 |
|
H7 |
C4 |
H8 |
107.782 |
| H7 |
C4 |
H9 |
107.782 |
|
H8 |
C4 |
H9 |
108.367 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.193 |
|
|
|
| 2 |
O |
-0.282 |
|
|
|
| 3 |
N |
-0.198 |
|
|
|
| 4 |
C |
0.008 |
|
|
|
| 5 |
H |
0.000 |
|
|
|
| 6 |
H |
0.104 |
|
|
|
| 7 |
H |
0.058 |
|
|
|
| 8 |
H |
0.059 |
|
|
|
| 9 |
H |
0.059 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.823 |
2.719 |
0.000 |
3.919 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.930 |
3.798 |
0.000 |
| y |
3.798 |
-24.092 |
0.000 |
| z |
0.000 |
0.000 |
-24.413 |
|
| Traceless |
| | x | y | z |
| x |
-1.678 |
3.798 |
0.000 |
| y |
3.798 |
1.080 |
0.000 |
| z |
0.000 |
0.000 |
0.598 |
|
| Polar |
| 3z2-r2 | 1.196 |
| x2-y2 | -1.838 |
| xy | 3.798 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.615 |
-1.008 |
0.000 |
| y |
-1.008 |
5.652 |
0.000 |
| z |
0.000 |
0.000 |
3.123 |
<r2> (average value of r
2) Å
2
| <r2> |
88.571 |
| (<r2>)1/2 |
9.411 |
Jump to
S1C1
S1C3
Energy calculated at PBE1PBE/cc-pVDZ
| | hartrees |
| Energy at 0K | -208.974812 |
| Energy at 298.15K | -208.980886 |
| HF Energy | -208.974812 |
| Nuclear repulsion energy | 119.377434 |
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 PBE1PBE/cc-pVDZ
Geometric Data calculated at PBE1PBE/cc-pVDZ
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
Energy calculated at PBE1PBE/cc-pVDZ
| | hartrees |
| Energy at 0K | -208.976566 |
| Energy at 298.15K | -208.982688 |
| HF Energy | -208.976566 |
| Nuclear repulsion energy | 121.606139 |
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 PBE1PBE/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 |
3666 |
3525 |
28.51 |
|
|
|
| 2 |
A |
3186 |
3064 |
0.12 |
|
|
|
| 3 |
A |
3123 |
3003 |
26.57 |
|
|
|
| 4 |
A |
3052 |
2934 |
44.80 |
|
|
|
| 5 |
A |
2963 |
2849 |
122.48 |
|
|
|
| 6 |
A |
1842 |
1771 |
339.54 |
|
|
|
| 7 |
A |
1566 |
1505 |
106.48 |
|
|
|
| 8 |
A |
1473 |
1416 |
7.97 |
|
|
|
| 9 |
A |
1471 |
1414 |
22.79 |
|
|
|
| 10 |
A |
1417 |
1362 |
18.50 |
|
|
|
| 11 |
A |
1406 |
1352 |
2.06 |
|
|
|
| 12 |
A |
1239 |
1191 |
65.47 |
|
|
|
| 13 |
A |
1152 |
1107 |
19.94 |
|
|
|
| 14 |
A |
1142 |
1098 |
0.32 |
|
|
|
| 15 |
A |
1025 |
985 |
0.16 |
|
|
|
| 16 |
A |
994 |
956 |
23.18 |
|
|
|
| 17 |
A |
772 |
742 |
0.56 |
|
|
|
| 18 |
A |
538 |
518 |
38.57 |
|
|
|
| 19 |
A |
302 |
291 |
13.95 |
|
|
|
| 20 |
A |
264 |
254 |
68.42 |
|
|
|
| 21 |
A |
113 |
108 |
0.21 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16351.8 cm
-1
Scaled (by 0.9615) Zero Point Vibrational Energy (zpe) 15722.2 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 PBE1PBE/cc-pVDZ
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.862 |
0.435 |
0.005 |
| O2 |
1.366 |
-0.672 |
-0.000 |
| N3 |
-0.471 |
0.658 |
-0.021 |
| C4 |
-1.413 |
-0.440 |
0.005 |
| H5 |
1.457 |
1.377 |
0.019 |
| H6 |
-0.805 |
1.609 |
0.057 |
| H7 |
-2.417 |
-0.059 |
-0.222 |
| H8 |
-1.128 |
-1.186 |
-0.750 |
| H9 |
-1.427 |
-0.939 |
0.988 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.2166 | 1.3520 | 2.4377 | 1.1138 | 2.0392 | 3.3237 | 2.6756 | 2.8453 |
O2 | 1.2166 | | 2.2681 | 2.7884 | 2.0513 | 3.1492 | 3.8385 | 2.6541 | 2.9745 | N3 | 1.3520 | 2.2681 | | 1.4470 | 2.0579 | 1.0107 | 2.0833 | 2.0892 | 2.1171 | C4 | 2.4377 | 2.7884 | 1.4470 | | 3.3966 | 2.1383 | 1.0977 | 1.0992 | 1.1021 | H5 | 1.1138 | 2.0513 | 2.0579 | 3.3966 | | 2.2734 | 4.1381 | 3.7205 | 3.8234 | H6 | 2.0392 | 3.1492 | 1.0107 | 2.1383 | 2.2734 | | 2.3365 | 2.9276 | 2.7833 | H7 | 3.3237 | 3.8385 | 2.0833 | 1.0977 | 4.1381 | 2.3365 | | 1.7924 | 1.7937 | H8 | 2.6756 | 2.6541 | 2.0892 | 1.0992 | 3.7205 | 2.9276 | 1.7924 | | 1.7806 | H9 | 2.8453 | 2.9745 | 2.1171 | 1.1021 | 3.8234 | 2.7833 | 1.7937 | 1.7806 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
121.091 |
|
C1 |
N3 |
H6 |
118.608 |
| O2 |
C1 |
N3 |
123.930 |
|
O2 |
C1 |
H5 |
123.277 |
| N3 |
C1 |
H5 |
112.790 |
|
N3 |
C4 |
H7 |
109.135 |
| N3 |
C4 |
H8 |
109.518 |
|
N3 |
C4 |
H9 |
111.588 |
| C4 |
N3 |
H6 |
119.876 |
|
H7 |
C4 |
H8 |
109.346 |
| H7 |
C4 |
H9 |
109.250 |
|
H8 |
C4 |
H9 |
107.972 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.203 |
|
|
|
| 2 |
O |
-0.288 |
|
|
|
| 3 |
N |
-0.209 |
|
|
|
| 4 |
C |
-0.001 |
|
|
|
| 5 |
H |
0.007 |
|
|
|
| 6 |
H |
0.100 |
|
|
|
| 7 |
H |
0.055 |
|
|
|
| 8 |
H |
0.077 |
|
|
|
| 9 |
H |
0.055 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.794 |
2.505 |
-0.000 |
3.752 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.233 |
2.293 |
0.000 |
| y |
2.293 |
-21.869 |
-0.000 |
| z |
0.000 |
-0.000 |
-24.415 |
|
| Traceless |
| | x | y | z |
| x |
-2.091 |
2.293 |
0.000 |
| y |
2.293 |
2.954 |
-0.000 |
| z |
0.000 |
-0.000 |
-0.864 |
|
| Polar |
| 3z2-r2 | -1.727 |
| x2-y2 | -3.363 |
| xy | 2.293 |
| xz | 0.000 |
| yz | -0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.017 |
0.016 |
0.000 |
| y |
0.016 |
5.023 |
0.000 |
| z |
0.000 |
0.000 |
3.114 |
<r2> (average value of r
2) Å
2
| <r2> |
77.920 |
| (<r2>)1/2 |
8.827 |