Jump to
S1C2
Energy calculated at HSEh1PBE/6-311G*
| | hartrees |
| Energy at 0K | -247.047613 |
| Energy at 298.15K | -247.053228 |
| HF Energy | -247.047613 |
| Nuclear repulsion energy | 157.832845 |
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 HSEh1PBE/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' |
3169 |
3041 |
19.66 |
|
|
|
| 2 |
A' |
3006 |
2884 |
60.40 |
|
|
|
| 3 |
A' |
2996 |
2875 |
26.12 |
|
|
|
| 4 |
A' |
2401 |
2304 |
0.58 |
|
|
|
| 5 |
A' |
1531 |
1470 |
7.48 |
|
|
|
| 6 |
A' |
1508 |
1447 |
10.94 |
|
|
|
| 7 |
A' |
1491 |
1430 |
0.12 |
|
|
|
| 8 |
A' |
1430 |
1372 |
35.15 |
|
|
|
| 9 |
A' |
1244 |
1194 |
61.75 |
|
|
|
| 10 |
A' |
1188 |
1140 |
125.36 |
|
|
|
| 11 |
A' |
1025 |
983 |
37.49 |
|
|
|
| 12 |
A' |
968 |
929 |
6.19 |
|
|
|
| 13 |
A' |
559 |
537 |
1.63 |
|
|
|
| 14 |
A' |
384 |
368 |
1.86 |
|
|
|
| 15 |
A' |
183 |
176 |
2.29 |
|
|
|
| 16 |
A" |
3059 |
2935 |
56.34 |
|
|
|
| 17 |
A" |
3024 |
2902 |
37.89 |
|
|
|
| 18 |
A" |
1503 |
1443 |
11.63 |
|
|
|
| 19 |
A" |
1281 |
1230 |
4.13 |
|
|
|
| 20 |
A" |
1194 |
1146 |
3.07 |
|
|
|
| 21 |
A" |
1038 |
996 |
1.86 |
|
|
|
| 22 |
A" |
386 |
370 |
1.48 |
|
|
|
| 23 |
A" |
234 |
224 |
4.58 |
|
|
|
| 24 |
A" |
90 |
87 |
0.05 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17445.8 cm
-1
Scaled (by 0.9596) Zero Point Vibrational Energy (zpe) 16741.0 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 HSEh1PBE/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-2.117 |
-0.362 |
0.000 |
| O2 |
-0.732 |
-0.609 |
0.000 |
| C3 |
0.000 |
0.580 |
0.000 |
| C4 |
1.427 |
0.275 |
0.000 |
| N5 |
2.558 |
0.066 |
0.000 |
| H6 |
-2.610 |
-1.333 |
0.000 |
| H7 |
-2.427 |
0.197 |
0.893 |
| H8 |
-2.427 |
0.197 |
-0.893 |
| H9 |
-0.223 |
1.195 |
-0.886 |
| H10 |
-0.223 |
1.195 |
0.886 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
C3 |
C4 |
N5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.4063 | 2.3175 | 3.6011 | 4.6952 | 1.0888 | 1.0988 | 1.0988 | 2.6075 | 2.6075 |
O2 | 1.4063 | | 1.3964 | 2.3335 | 3.3595 | 2.0122 | 2.0783 | 2.0783 | 2.0732 | 2.0732 | C3 | 2.3175 | 1.3964 | | 1.4594 | 2.6096 | 3.2360 | 2.6144 | 2.6144 | 1.1014 | 1.1014 | C4 | 3.6011 | 2.3335 | 1.4594 | | 1.1504 | 4.3454 | 3.9572 | 3.9572 | 2.0866 | 2.0866 | N5 | 4.6952 | 3.3595 | 2.6096 | 1.1504 | | 5.3542 | 5.0667 | 5.0667 | 3.1297 | 3.1297 | H6 | 1.0888 | 2.0122 | 3.2360 | 4.3454 | 5.3542 | | 1.7818 | 1.7818 | 3.5882 | 3.5882 | H7 | 1.0988 | 2.0783 | 2.6144 | 3.9572 | 5.0667 | 1.7818 | | 1.7862 | 3.0033 | 2.4195 | H8 | 1.0988 | 2.0783 | 2.6144 | 3.9572 | 5.0667 | 1.7818 | 1.7862 | | 2.4195 | 3.0033 | H9 | 2.6075 | 2.0732 | 1.1014 | 2.0866 | 3.1297 | 3.5882 | 3.0033 | 2.4195 | | 1.7725 | H10 | 2.6075 | 2.0732 | 1.1014 | 2.0866 | 3.1297 | 3.5882 | 2.4195 | 3.0033 | 1.7725 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
C3 |
111.552 |
|
O2 |
C1 |
H6 |
106.808 |
| O2 |
C1 |
H7 |
111.535 |
|
O2 |
C1 |
H8 |
111.535 |
| O2 |
C3 |
C4 |
109.572 |
|
O2 |
C3 |
H9 |
111.660 |
| O2 |
C3 |
H10 |
111.660 |
|
C3 |
C4 |
N5 |
178.395 |
| C4 |
C3 |
H9 |
108.331 |
|
C4 |
C3 |
H10 |
108.331 |
| H6 |
C1 |
H7 |
109.078 |
|
H6 |
C1 |
H8 |
109.078 |
| H7 |
C1 |
H8 |
108.744 |
|
H9 |
C3 |
H10 |
107.160 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.477 |
|
|
|
| 2 |
O |
-0.312 |
|
|
|
| 3 |
C |
-0.230 |
|
|
|
| 4 |
C |
0.123 |
|
|
|
| 5 |
N |
-0.260 |
|
|
|
| 6 |
H |
0.245 |
|
|
|
| 7 |
H |
0.212 |
|
|
|
| 8 |
H |
0.212 |
|
|
|
| 9 |
H |
0.243 |
|
|
|
| 10 |
H |
0.243 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-4.367 |
1.748 |
0.000 |
4.704 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-36.064 |
0.694 |
0.000 |
| y |
0.694 |
-29.226 |
0.000 |
| z |
0.000 |
0.000 |
-29.193 |
|
| Traceless |
| | x | y | z |
| x |
-6.855 |
0.694 |
0.000 |
| y |
0.694 |
3.403 |
0.000 |
| z |
0.000 |
0.000 |
3.452 |
|
| Polar |
| 3z2-r2 | 6.904 |
| x2-y2 | -6.838 |
| xy | 0.694 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
8.140 |
0.006 |
0.000 |
| y |
0.006 |
4.850 |
0.000 |
| z |
0.000 |
0.000 |
4.559 |
<r2> (average value of r
2) Å
2
| <r2> |
141.723 |
| (<r2>)1/2 |
11.905 |
Jump to
S1C1
Energy calculated at HSEh1PBE/6-311G*
| | hartrees |
| Energy at 0K | -247.050141 |
| Energy at 298.15K | -247.055842 |
| HF Energy | -247.050141 |
| Nuclear repulsion energy | 160.639437 |
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 HSEh1PBE/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 |
3170 |
3042 |
20.90 |
|
|
|
| 2 |
A |
3130 |
3003 |
5.65 |
|
|
|
| 3 |
A |
3079 |
2954 |
42.50 |
|
|
|
| 4 |
A |
3016 |
2895 |
47.44 |
|
|
|
| 5 |
A |
3012 |
2891 |
32.20 |
|
|
|
| 6 |
A |
2382 |
2286 |
0.19 |
|
|
|
| 7 |
A |
1524 |
1462 |
11.74 |
|
|
|
| 8 |
A |
1506 |
1445 |
9.57 |
|
|
|
| 9 |
A |
1495 |
1435 |
3.77 |
|
|
|
| 10 |
A |
1481 |
1421 |
5.71 |
|
|
|
| 11 |
A |
1403 |
1346 |
13.74 |
|
|
|
| 12 |
A |
1330 |
1276 |
9.33 |
|
|
|
| 13 |
A |
1236 |
1187 |
55.75 |
|
|
|
| 14 |
A |
1194 |
1146 |
13.86 |
|
|
|
| 15 |
A |
1181 |
1134 |
87.10 |
|
|
|
| 16 |
A |
1040 |
998 |
8.20 |
|
|
|
| 17 |
A |
971 |
932 |
33.77 |
|
|
|
| 18 |
A |
915 |
879 |
18.51 |
|
|
|
| 19 |
A |
612 |
588 |
1.83 |
|
|
|
| 20 |
A |
395 |
379 |
2.41 |
|
|
|
| 21 |
A |
372 |
357 |
1.36 |
|
|
|
| 22 |
A |
259 |
248 |
11.09 |
|
|
|
| 23 |
A |
179 |
172 |
3.44 |
|
|
|
| 24 |
A |
118 |
114 |
8.68 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17500.1 cm
-1
Scaled (by 0.9596) Zero Point Vibrational Energy (zpe) 16793.1 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 HSEh1PBE/6-311G*
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
1.562 |
-0.763 |
0.135 |
| O2 |
1.074 |
0.433 |
-0.434 |
| C3 |
-0.064 |
0.921 |
0.206 |
| C4 |
-1.241 |
0.054 |
0.036 |
| N5 |
-2.152 |
-0.637 |
-0.096 |
| H6 |
2.466 |
-1.023 |
-0.414 |
| H7 |
0.836 |
-1.580 |
0.041 |
| H8 |
1.809 |
-0.626 |
1.196 |
| H9 |
-0.283 |
1.898 |
-0.229 |
| H10 |
0.102 |
1.061 |
1.285 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
C3 |
C4 |
N5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.4111 | 2.3414 | 2.9212 | 3.7232 | 1.0888 | 1.0967 | 1.0984 | 3.2584 | 2.6041 |
O2 | 1.4111 | | 1.3938 | 2.3925 | 3.4159 | 2.0140 | 2.0817 | 2.0775 | 2.0078 | 2.0725 | C3 | 2.3414 | 1.3938 | | 1.4717 | 2.6230 | 3.2496 | 2.6630 | 2.6223 | 1.0920 | 1.1006 | C4 | 2.9212 | 2.3925 | 1.4717 | | 1.1514 | 3.8863 | 2.6433 | 3.3331 | 2.0941 | 2.0924 | N5 | 3.7232 | 3.4159 | 2.6230 | 1.1514 | | 4.6451 | 3.1368 | 4.1666 | 3.1520 | 3.1422 | H6 | 1.0888 | 2.0140 | 3.2496 | 3.8863 | 4.6451 | | 1.7811 | 1.7831 | 4.0153 | 3.5798 | H7 | 1.0967 | 2.0817 | 2.6630 | 2.6433 | 3.1368 | 1.7811 | | 1.7868 | 3.6636 | 3.0106 | H8 | 1.0984 | 2.0775 | 2.6223 | 3.3331 | 4.1666 | 1.7831 | 1.7868 | | 3.5742 | 2.4010 | H9 | 3.2584 | 2.0078 | 1.0920 | 2.0941 | 3.1520 | 4.0153 | 3.6636 | 3.5742 | | 1.7727 | H10 | 2.6041 | 2.0725 | 1.1006 | 2.0924 | 3.1422 | 3.5798 | 3.0106 | 2.4010 | 1.7727 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
C3 |
113.180 |
|
O2 |
C1 |
H6 |
106.634 |
| O2 |
C1 |
H7 |
111.611 |
|
O2 |
C1 |
H8 |
111.152 |
| O2 |
C3 |
C4 |
113.191 |
|
O2 |
C3 |
H9 |
107.123 |
| O2 |
C3 |
H10 |
111.838 |
|
C3 |
C4 |
N5 |
179.160 |
| C4 |
C3 |
H9 |
108.630 |
|
C4 |
C3 |
H10 |
107.997 |
| H6 |
C1 |
H7 |
109.171 |
|
H6 |
C1 |
H8 |
109.231 |
| H7 |
C1 |
H8 |
108.981 |
|
H9 |
C3 |
H10 |
107.896 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.486 |
|
|
|
| 2 |
O |
-0.304 |
|
|
|
| 3 |
C |
-0.280 |
|
|
|
| 4 |
C |
0.127 |
|
|
|
| 5 |
N |
-0.265 |
|
|
|
| 6 |
H |
0.239 |
|
|
|
| 7 |
H |
0.236 |
|
|
|
| 8 |
H |
0.209 |
|
|
|
| 9 |
H |
0.272 |
|
|
|
| 10 |
H |
0.251 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.536 |
1.239 |
1.404 |
3.153 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-36.178 |
-5.554 |
0.601 |
| y |
-5.554 |
-27.986 |
0.591 |
| z |
0.601 |
0.591 |
-29.731 |
|
| Traceless |
| | x | y | z |
| x |
-7.319 |
-5.554 |
0.601 |
| y |
-5.554 |
4.968 |
0.591 |
| z |
0.601 |
0.591 |
2.351 |
|
| Polar |
| 3z2-r2 | 4.702 |
| x2-y2 | -8.192 |
| xy | -5.554 |
| xz | 0.601 |
| yz | 0.591 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.943 |
0.448 |
0.173 |
| y |
0.448 |
5.639 |
0.229 |
| z |
0.173 |
0.229 |
4.570 |
<r2> (average value of r
2) Å
2
| <r2> |
122.095 |
| (<r2>)1/2 |
11.050 |