Jump to
S1C2
Energy calculated at PBE1PBE/3-21G
| | hartrees |
| Energy at 0K | -340.131227 |
| Energy at 298.15K | |
| HF Energy | -340.131227 |
| Nuclear repulsion energy | 241.363121 |
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/3-21G
| 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 |
3108 |
2985 |
32.71 |
|
|
|
| 2 |
A1 |
1944 |
1867 |
477.09 |
|
|
|
| 3 |
A1 |
1587 |
1525 |
1.17 |
|
|
|
| 4 |
A1 |
1382 |
1327 |
0.00 |
|
|
|
| 5 |
A1 |
1149 |
1104 |
187.34 |
|
|
|
| 6 |
A1 |
925 |
888 |
6.16 |
|
|
|
| 7 |
A1 |
789 |
758 |
30.17 |
|
|
|
| 8 |
A1 |
710 |
682 |
1.67 |
|
|
|
| 9 |
A2 |
3140 |
3016 |
0.00 |
|
|
|
| 10 |
A2 |
1273 |
1223 |
0.00 |
|
|
|
| 11 |
A2 |
1147 |
1102 |
0.00 |
|
|
|
| 12 |
A2 |
171i |
164i |
0.00 |
|
|
|
| 13 |
B1 |
3165 |
3039 |
33.31 |
|
|
|
| 14 |
B1 |
1263 |
1213 |
0.10 |
|
|
|
| 15 |
B1 |
874 |
840 |
0.27 |
|
|
|
| 16 |
B1 |
730 |
701 |
25.70 |
|
|
|
| 17 |
B1 |
122 |
118 |
4.27 |
|
|
|
| 18 |
B2 |
3100 |
2977 |
23.48 |
|
|
|
| 19 |
B2 |
1573 |
1510 |
2.66 |
|
|
|
| 20 |
B2 |
1411 |
1356 |
0.00 |
|
|
|
| 21 |
B2 |
1153 |
1107 |
7.44 |
|
|
|
| 22 |
B2 |
966 |
927 |
293.85 |
|
|
|
| 23 |
B2 |
741 |
711 |
1.15 |
|
|
|
| 24 |
B2 |
489 |
469 |
0.37 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16284.0 cm
-1
Scaled (by 0.9604) Zero Point Vibrational Energy (zpe) 15639.2 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/3-21G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.891 |
| O2 |
0.000 |
0.000 |
2.087 |
| O3 |
0.000 |
1.153 |
0.058 |
| O4 |
0.000 |
-1.153 |
0.058 |
| C5 |
0.000 |
0.783 |
-1.315 |
| C6 |
0.000 |
-0.783 |
-1.315 |
| H7 |
-0.893 |
1.184 |
-1.800 |
| H8 |
0.893 |
1.184 |
-1.800 |
| H9 |
0.893 |
-1.184 |
-1.800 |
| H10 |
-0.893 |
-1.184 |
-1.800 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1960 | 1.4226 | 1.4226 | 2.3409 | 2.3409 | 3.0728 | 3.0728 | 3.0728 | 3.0728 |
O2 | 1.1960 | | 2.3337 | 2.3337 | 3.4910 | 3.4910 | 4.1605 | 4.1605 | 4.1605 | 4.1605 | O3 | 1.4226 | 2.3337 | | 2.3069 | 1.4226 | 2.3739 | 2.0622 | 2.0622 | 3.1170 | 3.1170 | O4 | 1.4226 | 2.3337 | 2.3069 | | 2.3739 | 1.4226 | 3.1170 | 3.1170 | 2.0622 | 2.0622 | C5 | 2.3409 | 3.4910 | 1.4226 | 2.3739 | | 1.5655 | 1.0927 | 1.0927 | 2.2139 | 2.2139 | C6 | 2.3409 | 3.4910 | 2.3739 | 1.4226 | 1.5655 | | 2.2139 | 2.2139 | 1.0927 | 1.0927 | H7 | 3.0728 | 4.1605 | 2.0622 | 3.1170 | 1.0927 | 2.2139 | | 1.7864 | 2.9664 | 2.3682 | H8 | 3.0728 | 4.1605 | 2.0622 | 3.1170 | 1.0927 | 2.2139 | 1.7864 | | 2.3682 | 2.9664 | H9 | 3.0728 | 4.1605 | 3.1170 | 2.0622 | 2.2139 | 1.0927 | 2.9664 | 2.3682 | | 1.7864 | H10 | 3.0728 | 4.1605 | 3.1170 | 2.0622 | 2.2139 | 1.0927 | 2.3682 | 2.9664 | 1.7864 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
110.725 |
|
C1 |
O4 |
C6 |
110.725 |
| O2 |
C1 |
O3 |
125.827 |
|
O2 |
C1 |
O4 |
125.827 |
| O3 |
C1 |
O4 |
108.345 |
|
O3 |
C5 |
C6 |
105.103 |
| O3 |
C5 |
H7 |
109.440 |
|
O3 |
C5 |
H8 |
109.440 |
| O4 |
C6 |
C5 |
105.103 |
|
O4 |
C6 |
H9 |
109.440 |
| O4 |
C6 |
H10 |
109.440 |
|
C5 |
C6 |
H9 |
111.546 |
| C5 |
C6 |
H10 |
111.546 |
|
C6 |
C5 |
H7 |
111.546 |
| C6 |
C5 |
H8 |
111.546 |
|
H7 |
C5 |
H8 |
109.651 |
| H9 |
C6 |
H10 |
109.651 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.887 |
|
|
|
| 2 |
O |
-0.470 |
|
|
|
| 3 |
O |
-0.505 |
|
|
|
| 4 |
O |
-0.505 |
|
|
|
| 5 |
C |
-0.209 |
|
|
|
| 6 |
C |
-0.209 |
|
|
|
| 7 |
H |
0.253 |
|
|
|
| 8 |
H |
0.253 |
|
|
|
| 9 |
H |
0.253 |
|
|
|
| 10 |
H |
0.253 |
|
|
|
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 |
-5.027 |
5.027 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.995 |
0.000 |
0.000 |
| y |
0.000 |
-37.132 |
0.000 |
| z |
0.000 |
0.000 |
-34.754 |
|
| Traceless |
| | x | y | z |
| x |
3.949 |
0.000 |
0.000 |
| y |
0.000 |
-3.758 |
0.000 |
| z |
0.000 |
0.000 |
-0.191 |
|
| Polar |
| 3z2-r2 | -0.382 |
| x2-y2 | 5.138 |
| 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 |
3.575 |
0.000 |
0.000 |
| y |
0.000 |
4.539 |
0.000 |
| z |
0.000 |
0.000 |
6.950 |
<r2> (average value of r
2) Å
2
| <r2> |
132.446 |
| (<r2>)1/2 |
11.509 |
Jump to
S1C1
Energy calculated at PBE1PBE/3-21G
| | hartrees |
| Energy at 0K | -340.132113 |
| Energy at 298.15K | -340.138374 |
| HF Energy | -340.132113 |
| Nuclear repulsion energy | 241.991237 |
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/3-21G
| 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 |
3171 |
3045 |
7.86 |
|
|
|
| 2 |
A |
3088 |
2966 |
17.53 |
|
|
|
| 3 |
A |
1949 |
1872 |
457.49 |
|
|
|
| 4 |
A |
1573 |
1511 |
1.26 |
|
|
|
| 5 |
A |
1397 |
1341 |
4.76 |
|
|
|
| 6 |
A |
1269 |
1219 |
18.03 |
|
|
|
| 7 |
A |
1166 |
1120 |
35.69 |
|
|
|
| 8 |
A |
1124 |
1079 |
123.35 |
|
|
|
| 9 |
A |
939 |
901 |
2.88 |
|
|
|
| 10 |
A |
784 |
753 |
31.66 |
|
|
|
| 11 |
A |
706 |
678 |
2.27 |
|
|
|
| 12 |
A |
128 |
123 |
0.72 |
|
|
|
| 13 |
B |
3182 |
3056 |
19.42 |
|
|
|
| 14 |
B |
3093 |
2970 |
38.44 |
|
|
|
| 15 |
B |
1565 |
1503 |
4.20 |
|
|
|
| 16 |
B |
1411 |
1355 |
0.34 |
|
|
|
| 17 |
B |
1264 |
1214 |
1.07 |
|
|
|
| 18 |
B |
1130 |
1085 |
6.80 |
|
|
|
| 19 |
B |
972 |
934 |
216.79 |
|
|
|
| 20 |
B |
909 |
873 |
59.75 |
|
|
|
| 21 |
B |
741 |
711 |
27.51 |
|
|
|
| 22 |
B |
666 |
640 |
0.62 |
|
|
|
| 23 |
B |
489 |
469 |
0.52 |
|
|
|
| 24 |
B |
137 |
131 |
4.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16424.4 cm
-1
Scaled (by 0.9604) Zero Point Vibrational Energy (zpe) 15774.0 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 PBE1PBE/3-21G
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.886 |
| O2 |
0.000 |
0.000 |
2.081 |
| O3 |
0.000 |
1.154 |
0.046 |
| O4 |
0.000 |
-1.154 |
0.046 |
| C5 |
0.219 |
0.742 |
-1.303 |
| C6 |
-0.219 |
-0.742 |
-1.303 |
| H7 |
-0.384 |
1.358 |
-1.971 |
| H8 |
1.280 |
0.839 |
-1.554 |
| H9 |
0.384 |
-1.358 |
-1.971 |
| H10 |
-1.280 |
-0.839 |
-1.554 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1955 | 1.4276 | 1.4276 | 2.3215 | 2.3215 | 3.1860 | 2.8799 | 3.1860 | 2.8799 |
O2 | 1.1955 | | 2.3400 | 2.3400 | 3.4717 | 3.4717 | 4.2907 | 3.9441 | 4.2907 | 3.9441 | O3 | 1.4276 | 2.3400 | | 2.3088 | 1.4276 | 2.3373 | 2.0628 | 2.0731 | 3.2443 | 2.8584 | O4 | 1.4276 | 2.3400 | 2.3088 | | 2.3373 | 1.4276 | 3.2443 | 2.8584 | 2.0628 | 2.0731 | C5 | 2.3215 | 3.4717 | 1.4276 | 2.3373 | | 1.5466 | 1.0901 | 1.0953 | 2.2095 | 2.1926 | C6 | 2.3215 | 3.4717 | 2.3373 | 1.4276 | 1.5466 | | 2.2095 | 2.1926 | 1.0901 | 1.0953 | H7 | 3.1860 | 4.2907 | 2.0628 | 3.2443 | 1.0901 | 2.2095 | | 1.7927 | 2.8224 | 2.4089 | H8 | 2.8799 | 3.9441 | 2.0731 | 2.8584 | 1.0953 | 2.1926 | 1.7927 | | 2.4089 | 3.0613 | H9 | 3.1860 | 4.2907 | 3.2443 | 2.0628 | 2.2095 | 1.0901 | 2.8224 | 2.4089 | | 1.7927 | H10 | 2.8799 | 3.9441 | 2.8584 | 2.0731 | 2.1926 | 1.0953 | 2.4089 | 3.0613 | 1.7927 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
108.799 |
|
C1 |
O4 |
C6 |
108.799 |
| O2 |
C1 |
O3 |
126.039 |
|
O2 |
C1 |
O4 |
126.039 |
| O3 |
C1 |
O4 |
107.923 |
|
O3 |
C5 |
C6 |
103.529 |
| O3 |
C5 |
H7 |
109.304 |
|
O3 |
C5 |
H8 |
109.817 |
| O4 |
C6 |
C5 |
103.529 |
|
O4 |
C6 |
H9 |
109.304 |
| O4 |
C6 |
H10 |
109.817 |
|
C5 |
C6 |
H9 |
112.703 |
| C5 |
C6 |
H10 |
111.032 |
|
C6 |
C5 |
H7 |
112.703 |
| C6 |
C5 |
H8 |
111.032 |
|
H7 |
C5 |
H8 |
110.235 |
| H9 |
C6 |
H10 |
110.235 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.884 |
|
|
|
| 2 |
O |
-0.470 |
|
|
|
| 3 |
O |
-0.502 |
|
|
|
| 4 |
O |
-0.502 |
|
|
|
| 5 |
C |
-0.211 |
|
|
|
| 6 |
C |
-0.211 |
|
|
|
| 7 |
H |
0.256 |
|
|
|
| 8 |
H |
0.250 |
|
|
|
| 9 |
H |
0.256 |
|
|
|
| 10 |
H |
0.250 |
|
|
|
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 |
-4.950 |
4.950 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.039 |
0.261 |
0.000 |
| y |
0.261 |
-37.182 |
0.000 |
| z |
0.000 |
0.000 |
-34.562 |
|
| Traceless |
| | x | y | z |
| x |
3.833 |
0.261 |
0.000 |
| y |
0.261 |
-3.882 |
0.000 |
| z |
0.000 |
0.000 |
0.049 |
|
| Polar |
| 3z2-r2 | 0.098 |
| x2-y2 | 5.143 |
| xy | 0.261 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.665 |
0.128 |
0.000 |
| y |
0.128 |
4.467 |
0.000 |
| z |
0.000 |
0.000 |
6.917 |
<r2> (average value of r
2) Å
2
| <r2> |
131.143 |
| (<r2>)1/2 |
11.452 |