Jump to
S1C2
S1C3
Energy calculated at HF/6-31G**
| | hartrees |
| Energy at 0K | -207.969928 |
| Energy at 298.15K | -207.976061 |
| HF Energy | -207.969928 |
| Nuclear repulsion energy | 120.386615 |
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/6-31G**
| 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' |
3867 |
3491 |
42.94 |
|
|
|
| 2 |
A' |
3279 |
2959 |
32.66 |
|
|
|
| 3 |
A' |
3190 |
2880 |
64.93 |
|
|
|
| 4 |
A' |
3169 |
2860 |
71.19 |
|
|
|
| 5 |
A' |
1987 |
1793 |
626.15 |
|
|
|
| 6 |
A' |
1670 |
1508 |
28.81 |
|
|
|
| 7 |
A' |
1634 |
1474 |
15.50 |
|
|
|
| 8 |
A' |
1610 |
1453 |
7.65 |
|
|
|
| 9 |
A' |
1534 |
1385 |
10.77 |
|
|
|
| 10 |
A' |
1407 |
1270 |
175.19 |
|
|
|
| 11 |
A' |
1266 |
1143 |
48.25 |
|
|
|
| 12 |
A' |
1093 |
987 |
48.42 |
|
|
|
| 13 |
A' |
660 |
596 |
19.34 |
|
|
|
| 14 |
A' |
375 |
338 |
10.21 |
|
|
|
| 15 |
A" |
3248 |
2931 |
47.50 |
|
|
|
| 16 |
A" |
1614 |
1457 |
4.27 |
|
|
|
| 17 |
A" |
1253 |
1131 |
1.98 |
|
|
|
| 18 |
A" |
1179 |
1065 |
2.33 |
|
|
|
| 19 |
A" |
652 |
588 |
175.66 |
|
|
|
| 20 |
A" |
197 |
177 |
0.69 |
|
|
|
| 21 |
A" |
72 |
65 |
1.17 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17477.2 cm
-1
Scaled (by 0.9026) Zero Point Vibrational Energy (zpe) 15774.9 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/6-31G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.287 |
-0.755 |
0.000 |
| O2 |
1.390 |
-1.213 |
0.000 |
| N3 |
0.000 |
0.561 |
0.000 |
| C4 |
-1.328 |
1.123 |
0.000 |
| H5 |
-0.606 |
-1.387 |
0.000 |
| H6 |
0.787 |
1.171 |
0.000 |
| H7 |
-2.056 |
0.321 |
0.000 |
| H8 |
-1.500 |
1.732 |
0.881 |
| H9 |
-1.500 |
1.732 |
-0.881 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.1949 | 1.3467 | 2.4766 | 1.0932 | 1.9900 | 2.5780 | 3.1862 | 3.1862 |
O2 | 1.1949 | | 2.2537 | 3.5841 | 2.0035 | 2.4593 | 3.7723 | 4.2191 | 4.2191 | N3 | 1.3467 | 2.2537 | | 1.4421 | 2.0394 | 0.9958 | 2.0699 | 2.0969 | 2.0969 | C4 | 2.4766 | 3.5841 | 1.4421 | | 2.6114 | 2.1155 | 1.0829 | 1.0849 | 1.0849 | H5 | 1.0932 | 2.0035 | 2.0394 | 2.6114 | | 2.9123 | 2.2405 | 3.3616 | 3.3616 | H6 | 1.9900 | 2.4593 | 0.9958 | 2.1155 | 2.9123 | | 2.9672 | 2.5139 | 2.5139 | H7 | 2.5780 | 3.7723 | 2.0699 | 1.0829 | 2.2405 | 2.9672 | | 1.7538 | 1.7538 | H8 | 3.1862 | 4.2191 | 2.0969 | 1.0849 | 3.3616 | 2.5139 | 1.7538 | | 1.7626 | H9 | 3.1862 | 4.2191 | 2.0969 | 1.0849 | 3.3616 | 2.5139 | 1.7538 | 1.7626 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
125.229 |
|
C1 |
N3 |
H6 |
115.507 |
| O2 |
C1 |
N3 |
124.828 |
|
O2 |
C1 |
H5 |
122.168 |
| N3 |
C1 |
H5 |
113.004 |
|
N3 |
C4 |
H7 |
109.300 |
| N3 |
C4 |
H8 |
111.380 |
|
N3 |
C4 |
H9 |
111.380 |
| C4 |
N3 |
H6 |
119.264 |
|
H7 |
C4 |
H8 |
108.005 |
| H7 |
C4 |
H9 |
108.005 |
|
H8 |
C4 |
H9 |
108.653 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.580 |
|
|
|
| 2 |
O |
-0.578 |
|
|
|
| 3 |
N |
-0.676 |
|
|
|
| 4 |
C |
-0.130 |
|
|
|
| 5 |
H |
0.091 |
|
|
|
| 6 |
H |
0.315 |
|
|
|
| 7 |
H |
0.132 |
|
|
|
| 8 |
H |
0.133 |
|
|
|
| 9 |
H |
0.133 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.364 |
2.675 |
0.000 |
4.297 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.711 |
4.473 |
0.000 |
| y |
4.473 |
-24.303 |
0.000 |
| z |
0.000 |
0.000 |
-24.637 |
|
| Traceless |
| | x | y | z |
| x |
-2.241 |
4.473 |
0.000 |
| y |
4.473 |
1.371 |
0.000 |
| z |
0.000 |
0.000 |
0.870 |
|
| Polar |
| 3z2-r2 | 1.740 |
| x2-y2 | -2.408 |
| xy | 4.473 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.001 |
-0.866 |
0.000 |
| y |
-0.866 |
4.962 |
0.000 |
| z |
0.000 |
0.000 |
2.916 |
<r2> (average value of r
2) Å
2
| <r2> |
87.906 |
| (<r2>)1/2 |
9.376 |
Jump to
S1C1
S1C3
Energy calculated at HF/6-31G**
| | hartrees |
| Energy at 0K | -207.969928 |
| Energy at 298.15K | -207.976061 |
| HF Energy | -207.969928 |
| Nuclear repulsion energy | 120.386615 |
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/6-31G**
Geometric Data calculated at HF/6-31G**
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
Energy calculated at HF/6-31G**
| | hartrees |
| Energy at 0K | -207.971691 |
| Energy at 298.15K | -207.977787 |
| HF Energy | -207.971691 |
| Nuclear repulsion energy | 122.649644 |
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/6-31G**
| 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 |
3905 |
3525 |
44.25 |
|
|
|
| 2 |
A |
3313 |
2990 |
13.13 |
|
|
|
| 3 |
A |
3265 |
2947 |
42.54 |
|
|
|
| 4 |
A |
3196 |
2885 |
38.80 |
|
|
|
| 5 |
A |
3176 |
2867 |
125.31 |
|
|
|
| 6 |
A |
1976 |
1784 |
420.03 |
|
|
|
| 7 |
A |
1696 |
1531 |
194.06 |
|
|
|
| 8 |
A |
1639 |
1479 |
10.37 |
|
|
|
| 9 |
A |
1620 |
1462 |
19.44 |
|
|
|
| 10 |
A |
1588 |
1433 |
12.09 |
|
|
|
| 11 |
A |
1556 |
1405 |
9.63 |
|
|
|
| 12 |
A |
1336 |
1206 |
109.58 |
|
|
|
| 13 |
A |
1276 |
1152 |
2.19 |
|
|
|
| 14 |
A |
1253 |
1131 |
9.05 |
|
|
|
| 15 |
A |
1169 |
1055 |
7.66 |
|
|
|
| 16 |
A |
1031 |
931 |
18.12 |
|
|
|
| 17 |
A |
836 |
755 |
9.46 |
|
|
|
| 18 |
A |
515 |
465 |
39.67 |
|
|
|
| 19 |
A |
310 |
279 |
17.57 |
|
|
|
| 20 |
A |
271 |
245 |
118.66 |
|
|
|
| 21 |
A |
51 |
46 |
1.43 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17488.3 cm
-1
Scaled (by 0.9026) Zero Point Vibrational Energy (zpe) 15785.0 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/6-31G**
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.863 |
0.420 |
0.005 |
| O2 |
1.376 |
-0.660 |
-0.000 |
| N3 |
-0.464 |
0.647 |
-0.024 |
| C4 |
-1.429 |
-0.430 |
0.006 |
| H5 |
1.449 |
1.342 |
0.022 |
| H6 |
-0.780 |
1.583 |
0.069 |
| H7 |
-2.366 |
-0.080 |
-0.410 |
| H8 |
-1.064 |
-1.252 |
-0.592 |
| H9 |
-1.606 |
-0.790 |
1.015 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.1956 | 1.3460 | 2.4448 | 1.0927 | 2.0138 | 3.2932 | 2.6200 | 2.9288 |
O2 | 1.1956 | | 2.2567 | 2.8150 | 2.0035 | 3.1119 | 3.8085 | 2.5796 | 3.1524 | N3 | 1.3460 | 2.2567 | | 1.4469 | 2.0351 | 0.9925 | 2.0726 | 2.0712 | 2.1091 | C4 | 2.4448 | 2.8150 | 1.4469 | | 3.3799 | 2.1164 | 1.0825 | 1.0801 | 1.0856 | H5 | 1.0927 | 2.0035 | 2.0351 | 3.3799 | | 2.2418 | 4.0935 | 3.6633 | 3.8551 | H6 | 2.0138 | 3.1119 | 0.9925 | 2.1164 | 2.2418 | | 2.3475 | 2.9251 | 2.6852 | H7 | 3.2932 | 3.8085 | 2.0726 | 1.0825 | 4.0935 | 2.3475 | | 1.7611 | 1.7641 | H8 | 2.6200 | 2.5796 | 2.0712 | 1.0801 | 3.6633 | 2.9251 | 1.7611 | | 1.7570 | H9 | 2.9288 | 3.1524 | 2.1091 | 1.0856 | 3.8551 | 2.6852 | 1.7641 | 1.7570 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
122.129 |
|
C1 |
N3 |
H6 |
118.102 |
| O2 |
C1 |
N3 |
125.121 |
|
O2 |
C1 |
H5 |
122.157 |
| N3 |
C1 |
H5 |
112.719 |
|
N3 |
C4 |
H7 |
109.194 |
| N3 |
C4 |
H8 |
109.230 |
|
N3 |
C4 |
H9 |
111.983 |
| C4 |
N3 |
H6 |
119.181 |
|
H7 |
C4 |
H8 |
109.040 |
| H7 |
C4 |
H9 |
108.903 |
|
H8 |
C4 |
H9 |
108.446 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.563 |
|
|
|
| 2 |
O |
-0.574 |
|
|
|
| 3 |
N |
-0.681 |
|
|
|
| 4 |
C |
-0.127 |
|
|
|
| 5 |
H |
0.099 |
|
|
|
| 6 |
H |
0.306 |
|
|
|
| 7 |
H |
0.121 |
|
|
|
| 8 |
H |
0.163 |
|
|
|
| 9 |
H |
0.130 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.813 |
2.931 |
0.152 |
4.065 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.340 |
3.163 |
-0.038 |
| y |
3.163 |
-22.081 |
0.410 |
| z |
-0.038 |
0.410 |
-24.632 |
|
| Traceless |
| | x | y | z |
| x |
-1.984 |
3.163 |
-0.038 |
| y |
3.163 |
2.905 |
0.410 |
| z |
-0.038 |
0.410 |
-0.921 |
|
| Polar |
| 3z2-r2 | -1.843 |
| x2-y2 | -3.259 |
| xy | 3.163 |
| xz | -0.038 |
| yz | 0.410 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.150 |
-0.198 |
-0.016 |
| y |
-0.198 |
4.567 |
-0.013 |
| z |
-0.016 |
-0.013 |
2.890 |
<r2> (average value of r
2) Å
2
| <r2> |
77.039 |
| (<r2>)1/2 |
8.777 |