Jump to
S1C2
S1C3
Energy calculated at HF/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -208.045583 |
| Energy at 298.15K | -208.051734 |
| HF Energy | -208.045583 |
| Nuclear repulsion energy | 120.677545 |
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/aug-cc-pVTZ
| 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' |
3837 |
3493 |
41.46 |
|
|
|
| 2 |
A' |
3250 |
2959 |
27.59 |
|
|
|
| 3 |
A' |
3168 |
2884 |
65.91 |
|
|
|
| 4 |
A' |
3139 |
2858 |
56.97 |
|
|
|
| 5 |
A' |
1935 |
1761 |
691.04 |
|
|
|
| 6 |
A' |
1659 |
1511 |
24.55 |
|
|
|
| 7 |
A' |
1621 |
1476 |
6.82 |
|
|
|
| 8 |
A' |
1600 |
1456 |
7.31 |
|
|
|
| 9 |
A' |
1522 |
1386 |
9.49 |
|
|
|
| 10 |
A' |
1399 |
1274 |
193.33 |
|
|
|
| 11 |
A' |
1257 |
1145 |
51.22 |
|
|
|
| 12 |
A' |
1085 |
988 |
46.59 |
|
|
|
| 13 |
A' |
658 |
599 |
16.67 |
|
|
|
| 14 |
A' |
374 |
341 |
9.63 |
|
|
|
| 15 |
A" |
3215 |
2927 |
37.57 |
|
|
|
| 16 |
A" |
1605 |
1461 |
5.64 |
|
|
|
| 17 |
A" |
1251 |
1139 |
1.67 |
|
|
|
| 18 |
A" |
1174 |
1069 |
0.01 |
|
|
|
| 19 |
A" |
643 |
585 |
139.34 |
|
|
|
| 20 |
A" |
198 |
180 |
0.12 |
|
|
|
| 21 |
A" |
77 |
70 |
0.85 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17333.8 cm
-1
Scaled (by 0.9104) Zero Point Vibrational Energy (zpe) 15780.7 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/aug-cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.291 |
-0.750 |
0.000 |
| O2 |
1.391 |
-1.205 |
0.000 |
| N3 |
0.000 |
0.561 |
0.000 |
| C4 |
-1.331 |
1.112 |
0.000 |
| H5 |
-0.597 |
-1.386 |
0.000 |
| H6 |
0.779 |
1.177 |
0.000 |
| H7 |
-2.052 |
0.307 |
0.000 |
| H8 |
-1.506 |
1.719 |
0.880 |
| H9 |
-1.506 |
1.719 |
-0.880 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.1907 | 1.3425 | 2.4692 | 1.0918 | 1.9879 | 2.5693 | 3.1774 | 3.1774 |
O2 | 1.1907 | | 2.2480 | 3.5749 | 1.9956 | 2.4596 | 3.7597 | 4.2090 | 4.2090 | N3 | 1.3425 | 2.2480 | | 1.4409 | 2.0364 | 0.9934 | 2.0674 | 2.0936 | 2.0936 | C4 | 2.4692 | 3.5749 | 1.4409 | | 2.6041 | 2.1114 | 1.0808 | 1.0829 | 1.0829 | H5 | 1.0918 | 1.9956 | 2.0364 | 2.6041 | | 2.9091 | 2.2320 | 3.3529 | 3.3529 | H6 | 1.9879 | 2.4596 | 0.9934 | 2.1114 | 2.9091 | | 2.9617 | 2.5079 | 2.5079 | H7 | 2.5693 | 3.7597 | 2.0674 | 1.0808 | 2.2320 | 2.9617 | | 1.7512 | 1.7512 | H8 | 3.1774 | 4.2090 | 2.0936 | 1.0829 | 3.3529 | 2.5079 | 1.7512 | | 1.7598 | H9 | 3.1774 | 4.2090 | 2.0936 | 1.0829 | 3.3529 | 2.5079 | 1.7512 | 1.7598 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
124.994 |
|
C1 |
N3 |
H6 |
115.842 |
| O2 |
C1 |
N3 |
124.987 |
|
O2 |
C1 |
H5 |
121.860 |
| N3 |
C1 |
H5 |
113.153 |
|
N3 |
C4 |
H7 |
109.304 |
| N3 |
C4 |
H8 |
111.309 |
|
N3 |
C4 |
H9 |
111.309 |
| C4 |
N3 |
H6 |
119.164 |
|
H7 |
C4 |
H8 |
108.059 |
| H7 |
C4 |
H9 |
108.059 |
|
H8 |
C4 |
H9 |
108.690 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.187 |
|
|
|
| 2 |
O |
-0.683 |
|
|
|
| 3 |
N |
-0.084 |
|
|
|
| 4 |
C |
-0.855 |
|
|
|
| 5 |
H |
0.621 |
|
|
|
| 6 |
H |
0.153 |
|
|
|
| 7 |
H |
0.368 |
|
|
|
| 8 |
H |
0.333 |
|
|
|
| 9 |
H |
0.333 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.477 |
2.756 |
0.000 |
4.437 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-27.356 |
4.662 |
0.000 |
| y |
4.662 |
-24.502 |
0.000 |
| z |
0.000 |
0.000 |
-24.803 |
|
| Traceless |
| | x | y | z |
| x |
-2.704 |
4.662 |
0.000 |
| y |
4.662 |
1.578 |
0.000 |
| z |
0.000 |
0.000 |
1.126 |
|
| Polar |
| 3z2-r2 | 2.252 |
| x2-y2 | -2.854 |
| xy | 4.662 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.986 |
-0.970 |
0.000 |
| y |
-0.970 |
5.827 |
0.000 |
| z |
0.000 |
0.000 |
4.049 |
<r2> (average value of r
2) Å
2
| <r2> |
87.758 |
| (<r2>)1/2 |
9.368 |
Jump to
S1C1
S1C3
Energy calculated at HF/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -208.045583 |
| Energy at 298.15K | -208.051734 |
| HF Energy | -208.045583 |
| Nuclear repulsion energy | 120.677545 |
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/aug-cc-pVTZ
Geometric Data calculated at HF/aug-cc-pVTZ
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
Energy calculated at HF/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -208.047540 |
| Energy at 298.15K | -208.053564 |
| HF Energy | -208.047540 |
| Nuclear repulsion energy | 122.925985 |
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/aug-cc-pVTZ
| 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 |
3892 |
3543 |
47.89 |
|
|
|
| 2 |
A |
3260 |
2968 |
26.02 |
|
|
|
| 3 |
A |
3241 |
2951 |
28.22 |
|
|
|
| 4 |
A |
3183 |
2898 |
34.04 |
|
|
|
| 5 |
A |
3146 |
2865 |
97.10 |
|
|
|
| 6 |
A |
1927 |
1755 |
459.69 |
|
|
|
| 7 |
A |
1674 |
1524 |
206.98 |
|
|
|
| 8 |
A |
1630 |
1484 |
9.16 |
|
|
|
| 9 |
A |
1599 |
1456 |
7.93 |
|
|
|
| 10 |
A |
1585 |
1443 |
16.33 |
|
|
|
| 11 |
A |
1543 |
1405 |
12.26 |
|
|
|
| 12 |
A |
1333 |
1213 |
95.56 |
|
|
|
| 13 |
A |
1272 |
1158 |
11.38 |
|
|
|
| 14 |
A |
1255 |
1143 |
0.13 |
|
|
|
| 15 |
A |
1170 |
1065 |
1.34 |
|
|
|
| 16 |
A |
1018 |
926 |
19.81 |
|
|
|
| 17 |
A |
833 |
758 |
9.43 |
|
|
|
| 18 |
A |
497 |
453 |
16.63 |
|
|
|
| 19 |
A |
289 |
263 |
12.76 |
|
|
|
| 20 |
A |
245 |
223 |
96.73 |
|
|
|
| 21 |
A |
44 |
40 |
10.36 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17318.0 cm
-1
Scaled (by 0.9104) Zero Point Vibrational Energy (zpe) 15766.3 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/aug-cc-pVTZ
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.864 |
0.418 |
0.000 |
| O2 |
1.368 |
-0.661 |
-0.000 |
| N3 |
-0.458 |
0.646 |
-0.000 |
| C4 |
-1.427 |
-0.428 |
0.000 |
| H5 |
1.455 |
1.335 |
0.000 |
| H6 |
-0.770 |
1.585 |
0.000 |
| H7 |
-2.418 |
0.001 |
-0.002 |
| H8 |
-1.312 |
-1.051 |
-0.876 |
| H9 |
-1.314 |
-1.050 |
0.877 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.1914 | 1.3411 | 2.4418 | 1.0911 | 2.0074 | 3.3083 | 2.7674 | 2.7686 |
O2 | 1.1914 | | 2.2459 | 2.8050 | 1.9981 | 3.1009 | 3.8441 | 2.8463 | 2.8485 | N3 | 1.3411 | 2.2459 | | 1.4465 | 2.0330 | 0.9890 | 2.0638 | 2.0923 | 2.0924 | C4 | 2.4418 | 2.8050 | 1.4465 | | 3.3782 | 2.1169 | 1.0801 | 1.0813 | 1.0813 | H5 | 1.0911 | 1.9981 | 2.0330 | 3.3782 | | 2.2388 | 4.0964 | 3.7572 | 3.7580 | H6 | 2.0074 | 3.1009 | 0.9890 | 2.1169 | 2.2388 | | 2.2857 | 2.8302 | 2.8293 | H7 | 3.3083 | 3.8441 | 2.0638 | 1.0801 | 4.0964 | 2.2857 | | 1.7597 | 1.7597 | H8 | 2.7674 | 2.8463 | 2.0923 | 1.0813 | 3.7572 | 2.8302 | 1.7597 | | 1.7528 | H9 | 2.7686 | 2.8485 | 2.0924 | 1.0813 | 3.7580 | 2.8293 | 1.7597 | 1.7528 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
122.271 |
|
C1 |
N3 |
H6 |
118.186 |
| O2 |
C1 |
N3 |
124.853 |
|
O2 |
C1 |
H5 |
122.131 |
| N3 |
C1 |
H5 |
113.016 |
|
N3 |
C4 |
H7 |
108.671 |
| N3 |
C4 |
H8 |
110.908 |
|
N3 |
C4 |
H9 |
110.915 |
| C4 |
N3 |
H6 |
119.542 |
|
H7 |
C4 |
H8 |
109.007 |
| H7 |
C4 |
H9 |
109.006 |
|
H8 |
C4 |
H9 |
108.295 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.238 |
|
|
|
| 2 |
O |
-0.663 |
|
|
|
| 3 |
N |
-0.071 |
|
|
|
| 4 |
C |
-0.769 |
|
|
|
| 5 |
H |
0.596 |
|
|
|
| 6 |
H |
0.133 |
|
|
|
| 7 |
H |
0.377 |
|
|
|
| 8 |
H |
0.318 |
|
|
|
| 9 |
H |
0.318 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.918 |
2.968 |
0.000 |
4.162 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.531 |
3.225 |
0.000 |
| y |
3.225 |
-22.623 |
0.001 |
| z |
0.000 |
0.001 |
-24.886 |
|
| Traceless |
| | x | y | z |
| x |
-1.777 |
3.225 |
0.000 |
| y |
3.225 |
2.586 |
0.001 |
| z |
0.000 |
0.001 |
-0.809 |
|
| Polar |
| 3z2-r2 | -1.618 |
| x2-y2 | -2.908 |
| xy | 3.225 |
| xz | 0.000 |
| yz | 0.001 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.128 |
-0.107 |
-0.000 |
| y |
-0.107 |
5.489 |
-0.000 |
| z |
-0.000 |
-0.000 |
4.093 |
<r2> (average value of r
2) Å
2
| <r2> |
76.952 |
| (<r2>)1/2 |
8.772 |