Jump to
S1C2
Energy calculated at HSEh1PBE/6-311G*
| | hartrees |
| Energy at 0K | -342.140563 |
| Energy at 298.15K | |
| HF Energy | -342.140563 |
| Nuclear repulsion energy | 246.663207 |
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 |
A1 |
3080 |
2955 |
64.44 |
|
|
|
| 2 |
A1 |
1973 |
1893 |
644.31 |
|
|
|
| 3 |
A1 |
1566 |
1503 |
1.35 |
|
|
|
| 4 |
A1 |
1413 |
1355 |
0.91 |
|
|
|
| 5 |
A1 |
1234 |
1185 |
247.07 |
|
|
|
| 6 |
A1 |
968 |
928 |
9.72 |
|
|
|
| 7 |
A1 |
853 |
818 |
34.24 |
|
|
|
| 8 |
A1 |
734 |
704 |
0.96 |
|
|
|
| 9 |
A2 |
3105 |
2980 |
0.00 |
|
|
|
| 10 |
A2 |
1268 |
1217 |
0.00 |
|
|
|
| 11 |
A2 |
1180 |
1132 |
0.00 |
|
|
|
| 12 |
A2 |
177i |
170i |
0.00 |
|
|
|
| 13 |
B1 |
3129 |
3002 |
57.22 |
|
|
|
| 14 |
B1 |
1288 |
1236 |
1.39 |
|
|
|
| 15 |
B1 |
868 |
833 |
0.68 |
|
|
|
| 16 |
B1 |
774 |
742 |
23.60 |
|
|
|
| 17 |
B1 |
141 |
136 |
1.78 |
|
|
|
| 18 |
B2 |
3072 |
2948 |
32.41 |
|
|
|
| 19 |
B2 |
1553 |
1490 |
5.20 |
|
|
|
| 20 |
B2 |
1422 |
1365 |
15.85 |
|
|
|
| 21 |
B2 |
1219 |
1170 |
2.36 |
|
|
|
| 22 |
B2 |
1057 |
1014 |
332.65 |
|
|
|
| 23 |
B2 |
762 |
732 |
2.74 |
|
|
|
| 24 |
B2 |
517 |
496 |
0.03 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16498.5 cm
-1
Scaled (by 0.9596) Zero Point Vibrational Energy (zpe) 15831.9 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 HSEh1PBE/6-311G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.862 |
| O2 |
0.000 |
0.000 |
2.040 |
| O3 |
0.000 |
1.125 |
0.058 |
| O4 |
0.000 |
-1.125 |
0.058 |
| C5 |
0.000 |
0.772 |
-1.280 |
| C6 |
0.000 |
-0.772 |
-1.280 |
| H7 |
-0.887 |
1.188 |
-1.764 |
| H8 |
0.887 |
1.188 |
-1.764 |
| H9 |
0.887 |
-1.188 |
-1.764 |
| H10 |
-0.887 |
-1.188 |
-1.764 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1776 | 1.3831 | 1.3831 | 2.2769 | 2.2769 | 3.0162 | 3.0162 | 3.0162 | 3.0162 |
O2 | 1.1776 | | 2.2792 | 2.2792 | 3.4082 | 3.4082 | 4.0829 | 4.0829 | 4.0829 | 4.0829 | O3 | 1.3831 | 2.2792 | | 2.2498 | 1.3831 | 2.3210 | 2.0275 | 2.0275 | 3.0749 | 3.0749 | O4 | 1.3831 | 2.2792 | 2.2498 | | 2.3210 | 1.3831 | 3.0749 | 3.0749 | 2.0275 | 2.0275 | C5 | 2.2769 | 3.4082 | 1.3831 | 2.3210 | | 1.5442 | 1.0930 | 1.0930 | 2.2053 | 2.2053 | C6 | 2.2769 | 3.4082 | 2.3210 | 1.3831 | 1.5442 | | 2.2053 | 2.2053 | 1.0930 | 1.0930 | H7 | 3.0162 | 4.0829 | 2.0275 | 3.0749 | 1.0930 | 2.2053 | | 1.7742 | 2.9650 | 2.3756 | H8 | 3.0162 | 4.0829 | 2.0275 | 3.0749 | 1.0930 | 2.2053 | 1.7742 | | 2.3756 | 2.9650 | H9 | 3.0162 | 4.0829 | 3.0749 | 2.0275 | 2.2053 | 1.0930 | 2.9650 | 2.3756 | | 1.7742 | H10 | 3.0162 | 4.0829 | 3.0749 | 2.0275 | 2.2053 | 1.0930 | 2.3756 | 2.9650 | 1.7742 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
110.800 |
|
C1 |
O4 |
C6 |
110.800 |
| O2 |
C1 |
O3 |
125.577 |
|
O2 |
C1 |
O4 |
125.577 |
| O3 |
C1 |
O4 |
108.845 |
|
O3 |
C5 |
C6 |
104.778 |
| O3 |
C5 |
H7 |
109.377 |
|
O3 |
C5 |
H8 |
109.377 |
| O4 |
C6 |
C5 |
104.778 |
|
O4 |
C6 |
H9 |
109.377 |
| O4 |
C6 |
H10 |
109.377 |
|
C5 |
C6 |
H9 |
112.353 |
| C5 |
C6 |
H10 |
112.353 |
|
C6 |
C5 |
H7 |
112.353 |
| C6 |
C5 |
H8 |
112.353 |
|
H7 |
C5 |
H8 |
108.507 |
| H9 |
C6 |
H10 |
108.507 |
|
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 |
0.510 |
|
|
|
| 2 |
O |
-0.310 |
|
|
|
| 3 |
O |
-0.289 |
|
|
|
| 4 |
O |
-0.289 |
|
|
|
| 5 |
C |
-0.281 |
|
|
|
| 6 |
C |
-0.281 |
|
|
|
| 7 |
H |
0.235 |
|
|
|
| 8 |
H |
0.235 |
|
|
|
| 9 |
H |
0.235 |
|
|
|
| 10 |
H |
0.235 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
-4.861 |
4.861 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.905 |
0.000 |
0.000 |
| y |
0.000 |
-36.311 |
0.000 |
| z |
0.000 |
0.000 |
-35.614 |
|
| Traceless |
| | x | y | z |
| x |
4.058 |
0.000 |
0.000 |
| y |
0.000 |
-2.552 |
0.000 |
| z |
0.000 |
0.000 |
-1.506 |
|
| Polar |
| 3z2-r2 | -3.013 |
| x2-y2 | 4.406 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.252 |
0.000 |
0.000 |
| y |
0.000 |
5.172 |
0.000 |
| z |
0.000 |
0.000 |
7.300 |
<r2> (average value of r
2) Å
2
| <r2> |
127.714 |
| (<r2>)1/2 |
11.301 |
Jump to
S1C1
Energy calculated at HSEh1PBE/6-311G*
| | hartrees |
| Energy at 0K | -342.141315 |
| Energy at 298.15K | -342.147729 |
| HF Energy | -342.141315 |
| Nuclear repulsion energy | 247.232848 |
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 |
3134 |
3007 |
22.46 |
|
|
|
| 2 |
A |
3054 |
2930 |
32.77 |
|
|
|
| 3 |
A |
1975 |
1895 |
627.50 |
|
|
|
| 4 |
A |
1552 |
1489 |
1.73 |
|
|
|
| 5 |
A |
1418 |
1360 |
6.43 |
|
|
|
| 6 |
A |
1274 |
1222 |
19.98 |
|
|
|
| 7 |
A |
1231 |
1181 |
179.64 |
|
|
|
| 8 |
A |
1166 |
1119 |
38.25 |
|
|
|
| 9 |
A |
969 |
930 |
3.80 |
|
|
|
| 10 |
A |
848 |
814 |
37.88 |
|
|
|
| 11 |
A |
732 |
702 |
1.19 |
|
|
|
| 12 |
A |
136 |
130 |
0.57 |
|
|
|
| 13 |
B |
3144 |
3017 |
34.95 |
|
|
|
| 14 |
B |
3059 |
2936 |
58.86 |
|
|
|
| 15 |
B |
1543 |
1481 |
6.95 |
|
|
|
| 16 |
B |
1415 |
1358 |
14.02 |
|
|
|
| 17 |
B |
1290 |
1238 |
4.94 |
|
|
|
| 18 |
B |
1196 |
1147 |
3.75 |
|
|
|
| 19 |
B |
1052 |
1010 |
303.09 |
|
|
|
| 20 |
B |
908 |
871 |
12.49 |
|
|
|
| 21 |
B |
783 |
751 |
24.88 |
|
|
|
| 22 |
B |
695 |
667 |
1.22 |
|
|
|
| 23 |
B |
517 |
496 |
0.10 |
|
|
|
| 24 |
B |
150 |
144 |
1.63 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16619.3 cm
-1
Scaled (by 0.9596) Zero Point Vibrational Energy (zpe) 15947.8 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 C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.857 |
| O2 |
0.000 |
0.000 |
2.035 |
| O3 |
0.000 |
1.125 |
0.047 |
| O4 |
0.000 |
-1.125 |
0.047 |
| C5 |
0.193 |
0.740 |
-1.270 |
| C6 |
-0.193 |
-0.740 |
-1.270 |
| H7 |
-0.434 |
1.349 |
-1.923 |
| H8 |
1.244 |
0.888 |
-1.546 |
| H9 |
0.434 |
-1.349 |
-1.923 |
| H10 |
-1.244 |
-0.888 |
-1.546 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1774 | 1.3862 | 1.3862 | 2.2610 | 2.2610 | 3.1203 | 2.8484 | 3.1203 | 2.8484 |
O2 | 1.1774 | | 2.2837 | 2.2837 | 3.3924 | 3.3924 | 4.2035 | 3.8935 | 4.2035 | 3.8935 | O3 | 1.3862 | 2.2837 | | 2.2497 | 1.3862 | 2.2915 | 2.0296 | 2.0354 | 3.1918 | 2.8526 | O4 | 1.3862 | 2.2837 | 2.2497 | | 2.2915 | 1.3862 | 3.1918 | 2.8526 | 2.0296 | 2.0354 | C5 | 2.2610 | 3.3924 | 1.3862 | 2.2915 | | 1.5298 | 1.0906 | 1.0961 | 2.2014 | 2.1890 | C6 | 2.2610 | 3.3924 | 2.2915 | 1.3862 | 1.5298 | | 2.2014 | 2.1890 | 1.0906 | 1.0961 | H7 | 3.1203 | 4.2035 | 2.0296 | 3.1918 | 1.0906 | 2.2014 | | 1.7799 | 2.8334 | 2.4083 | H8 | 2.8484 | 3.8935 | 2.0354 | 2.8526 | 1.0961 | 2.1890 | 1.7799 | | 2.4083 | 3.0563 | H9 | 3.1203 | 4.2035 | 3.1918 | 2.0296 | 2.2014 | 1.0906 | 2.8334 | 2.4083 | | 1.7799 | H10 | 2.8484 | 3.8935 | 2.8526 | 2.0354 | 2.1890 | 1.0961 | 2.4083 | 3.0563 | 1.7799 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
109.282 |
|
C1 |
O4 |
C6 |
109.282 |
| O2 |
C1 |
O3 |
125.761 |
|
O2 |
C1 |
O4 |
125.761 |
| O3 |
C1 |
O4 |
108.478 |
|
O3 |
C5 |
C6 |
103.491 |
| O3 |
C5 |
H7 |
109.481 |
|
O3 |
C5 |
H8 |
109.614 |
| O4 |
C6 |
C5 |
103.491 |
|
O4 |
C6 |
H9 |
109.481 |
| O4 |
C6 |
H10 |
109.614 |
|
C5 |
C6 |
H9 |
113.236 |
| C5 |
C6 |
H10 |
111.888 |
|
C6 |
C5 |
H7 |
113.236 |
| C6 |
C5 |
H8 |
111.888 |
|
H7 |
C5 |
H8 |
108.973 |
| H9 |
C6 |
H10 |
108.973 |
|
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 |
0.511 |
|
|
|
| 2 |
O |
-0.307 |
|
|
|
| 3 |
O |
-0.290 |
|
|
|
| 4 |
O |
-0.290 |
|
|
|
| 5 |
C |
-0.283 |
|
|
|
| 6 |
C |
-0.283 |
|
|
|
| 7 |
H |
0.238 |
|
|
|
| 8 |
H |
0.232 |
|
|
|
| 9 |
H |
0.238 |
|
|
|
| 10 |
H |
0.232 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
-4.803 |
4.803 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.001 |
0.170 |
0.000 |
| y |
0.170 |
-36.311 |
0.000 |
| z |
0.000 |
0.000 |
-35.423 |
|
| Traceless |
| | x | y | z |
| x |
3.865 |
0.170 |
0.000 |
| y |
0.170 |
-2.598 |
0.000 |
| z |
0.000 |
0.000 |
-1.267 |
|
| Polar |
| 3z2-r2 | -2.534 |
| x2-y2 | 4.309 |
| xy | 0.170 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.354 |
0.155 |
0.000 |
| y |
0.155 |
5.125 |
0.000 |
| z |
0.000 |
0.000 |
7.264 |
<r2> (average value of r
2) Å
2
| <r2> |
126.656 |
| (<r2>)1/2 |
11.254 |