Jump to
S1C2
Energy calculated at HF/LANL2DZ
| | hartrees |
| Energy at 0K | -340.406768 |
| Energy at 298.15K | |
| HF Energy | -340.406768 |
| Nuclear repulsion energy | 243.868432 |
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/LANL2DZ
| 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 |
3307 |
2976 |
68.47 |
|
|
|
| 2 |
A1 |
1985 |
1786 |
814.89 |
|
|
|
| 3 |
A1 |
1699 |
1529 |
0.32 |
|
|
|
| 4 |
A1 |
1521 |
1369 |
0.18 |
|
|
|
| 5 |
A1 |
1280 |
1152 |
296.85 |
|
|
|
| 6 |
A1 |
1012 |
910 |
21.39 |
|
|
|
| 7 |
A1 |
845 |
760 |
35.85 |
|
|
|
| 8 |
A1 |
753 |
678 |
1.51 |
|
|
|
| 9 |
A2 |
3351 |
3016 |
0.00 |
|
|
|
| 10 |
A2 |
1371 |
1234 |
0.00 |
|
|
|
| 11 |
A2 |
1272 |
1145 |
0.00 |
|
|
|
| 12 |
A2 |
161i |
145i |
0.00 |
|
|
|
| 13 |
B1 |
3372 |
3034 |
57.66 |
|
|
|
| 14 |
B1 |
1366 |
1229 |
3.80 |
|
|
|
| 15 |
B1 |
937 |
844 |
1.31 |
|
|
|
| 16 |
B1 |
805 |
725 |
72.98 |
|
|
|
| 17 |
B1 |
129 |
116 |
6.20 |
|
|
|
| 18 |
B2 |
3294 |
2964 |
31.45 |
|
|
|
| 19 |
B2 |
1687 |
1518 |
5.98 |
|
|
|
| 20 |
B2 |
1541 |
1386 |
4.02 |
|
|
|
| 21 |
B2 |
1260 |
1134 |
3.82 |
|
|
|
| 22 |
B2 |
1055 |
950 |
384.77 |
|
|
|
| 23 |
B2 |
808 |
727 |
0.81 |
|
|
|
| 24 |
B2 |
515 |
464 |
0.23 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17502.1 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 15750.2 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 HF/LANL2DZ
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 |
2.078 |
| O3 |
0.000 |
1.128 |
0.053 |
| O4 |
0.000 |
-1.128 |
0.053 |
| C5 |
0.000 |
0.779 |
-1.309 |
| C6 |
0.000 |
-0.779 |
-1.309 |
| H7 |
-0.879 |
1.190 |
-1.776 |
| H8 |
0.879 |
1.190 |
-1.776 |
| H9 |
0.879 |
-1.190 |
-1.776 |
| H10 |
-0.879 |
-1.190 |
-1.776 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1863 | 1.4053 | 1.4053 | 2.3340 | 2.3340 | 3.0499 | 3.0499 | 3.0499 | 3.0499 |
O2 | 1.1863 | | 2.3178 | 2.3178 | 3.4749 | 3.4749 | 4.1276 | 4.1276 | 4.1276 | 4.1276 | O3 | 1.4053 | 2.3178 | | 2.2552 | 1.4053 | 2.3428 | 2.0297 | 2.0297 | 3.0799 | 3.0799 | O4 | 1.4053 | 2.3178 | 2.2552 | | 2.3428 | 1.4053 | 3.0799 | 3.0799 | 2.0297 | 2.0297 | C5 | 2.3340 | 3.4749 | 1.4053 | 2.3428 | | 1.5581 | 1.0767 | 1.0767 | 2.2061 | 2.2061 | C6 | 2.3340 | 3.4749 | 2.3428 | 1.4053 | 1.5581 | | 2.2061 | 2.2061 | 1.0767 | 1.0767 | H7 | 3.0499 | 4.1276 | 2.0297 | 3.0799 | 1.0767 | 2.2061 | | 1.7579 | 2.9583 | 2.3794 | H8 | 3.0499 | 4.1276 | 2.0297 | 3.0799 | 1.0767 | 2.2061 | 1.7579 | | 2.3794 | 2.9583 | H9 | 3.0499 | 4.1276 | 3.0799 | 2.0297 | 2.2061 | 1.0767 | 2.9583 | 2.3794 | | 1.7579 | H10 | 3.0499 | 4.1276 | 3.0799 | 2.0297 | 2.2061 | 1.0767 | 2.3794 | 2.9583 | 1.7579 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
112.282 |
|
C1 |
O4 |
C6 |
112.282 |
| O2 |
C1 |
O3 |
126.642 |
|
O2 |
C1 |
O4 |
126.642 |
| O3 |
C1 |
O4 |
106.715 |
|
O3 |
C5 |
C6 |
104.360 |
| O3 |
C5 |
H7 |
109.004 |
|
O3 |
C5 |
H8 |
109.004 |
| O4 |
C6 |
C5 |
104.360 |
|
O4 |
C6 |
H9 |
109.004 |
| O4 |
C6 |
H10 |
109.004 |
|
C5 |
C6 |
H9 |
112.419 |
| C5 |
C6 |
H10 |
112.419 |
|
C6 |
C5 |
H7 |
112.419 |
| C6 |
C5 |
H8 |
112.419 |
|
H7 |
C5 |
H8 |
109.439 |
| H9 |
C6 |
H10 |
109.439 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.667 |
|
|
|
| 2 |
O |
-0.311 |
|
|
|
| 3 |
O |
-0.461 |
|
|
|
| 4 |
O |
-0.461 |
|
|
|
| 5 |
C |
-0.131 |
|
|
|
| 6 |
C |
-0.131 |
|
|
|
| 7 |
H |
0.207 |
|
|
|
| 8 |
H |
0.207 |
|
|
|
| 9 |
H |
0.207 |
|
|
|
| 10 |
H |
0.207 |
|
|
|
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 |
-6.226 |
6.226 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.389 |
0.000 |
0.000 |
| y |
0.000 |
-39.410 |
0.000 |
| z |
0.000 |
0.000 |
-37.136 |
|
| Traceless |
| | x | y | z |
| x |
5.884 |
0.000 |
0.000 |
| y |
0.000 |
-4.647 |
0.000 |
| z |
0.000 |
0.000 |
-1.237 |
|
| Polar |
| 3z2-r2 | -2.473 |
| x2-y2 | 7.021 |
| 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 |
3.637 |
0.000 |
0.000 |
| y |
0.000 |
4.474 |
0.000 |
| z |
0.000 |
0.000 |
6.774 |
<r2> (average value of r
2) Å
2
| <r2> |
131.573 |
| (<r2>)1/2 |
11.471 |
Jump to
S1C1
Energy calculated at HF/LANL2DZ
| | hartrees |
| Energy at 0K | -340.406872 |
| Energy at 298.15K | |
| HF Energy | -340.406872 |
| Nuclear repulsion energy | 244.040668 |
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/LANL2DZ
| 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 |
3359 |
3023 |
9.54 |
|
|
|
| 2 |
A |
3300 |
2969 |
54.11 |
|
|
|
| 3 |
A |
1986 |
1787 |
806.81 |
|
|
|
| 4 |
A |
1695 |
1525 |
0.37 |
|
|
|
| 5 |
A |
1523 |
1371 |
0.17 |
|
|
|
| 6 |
A |
1369 |
1232 |
13.09 |
|
|
|
| 7 |
A |
1288 |
1159 |
138.50 |
|
|
|
| 8 |
A |
1259 |
1133 |
145.01 |
|
|
|
| 9 |
A |
1013 |
912 |
17.56 |
|
|
|
| 10 |
A |
844 |
759 |
36.65 |
|
|
|
| 11 |
A |
751 |
676 |
1.66 |
|
|
|
| 12 |
A |
83i |
75i |
0.40 |
|
|
|
| 13 |
B |
3375 |
3037 |
49.58 |
|
|
|
| 14 |
B |
3291 |
2961 |
41.47 |
|
|
|
| 15 |
B |
1685 |
1516 |
6.66 |
|
|
|
| 16 |
B |
1539 |
1385 |
3.72 |
|
|
|
| 17 |
B |
1365 |
1229 |
5.00 |
|
|
|
| 18 |
B |
1253 |
1128 |
5.00 |
|
|
|
| 19 |
B |
1057 |
951 |
369.15 |
|
|
|
| 20 |
B |
954 |
859 |
11.20 |
|
|
|
| 21 |
B |
808 |
727 |
72.23 |
|
|
|
| 22 |
B |
781 |
703 |
1.43 |
|
|
|
| 23 |
B |
516 |
464 |
0.21 |
|
|
|
| 24 |
B |
134 |
121 |
5.94 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17529.8 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 15775.1 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 HF/LANL2DZ
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.890 |
| O2 |
0.000 |
0.000 |
2.076 |
| O3 |
0.000 |
1.128 |
0.049 |
| O4 |
0.000 |
-1.128 |
0.049 |
| C5 |
0.121 |
0.767 |
-1.305 |
| C6 |
-0.121 |
-0.767 |
-1.305 |
| H7 |
-0.614 |
1.305 |
-1.878 |
| H8 |
1.108 |
1.025 |
-1.653 |
| H9 |
0.614 |
-1.305 |
-1.878 |
| H10 |
-1.108 |
-1.025 |
-1.653 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1862 | 1.4067 | 1.4067 | 2.3284 | 2.3284 | 3.1205 | 2.9574 | 3.1205 | 2.9574 |
O2 | 1.1862 | | 2.3195 | 2.3195 | 3.4692 | 3.4692 | 4.2082 | 4.0232 | 4.2082 | 4.0232 | O3 | 1.4067 | 2.3195 | | 2.2556 | 1.4067 | 2.3324 | 2.0299 | 2.0338 | 3.1632 | 2.9600 | O4 | 1.4067 | 2.3195 | 2.2556 | | 2.3324 | 1.4067 | 3.1632 | 2.9600 | 2.0299 | 2.0338 | C5 | 2.3284 | 3.4692 | 1.4067 | 2.3324 | | 1.5536 | 1.0756 | 1.0782 | 2.2055 | 2.2013 | C6 | 2.3284 | 3.4692 | 2.3324 | 1.4067 | 1.5536 | | 2.2055 | 2.2013 | 1.0756 | 1.0782 | H7 | 3.1205 | 4.2082 | 2.0299 | 3.1632 | 1.0756 | 2.2055 | | 1.7595 | 2.8842 | 2.3923 | H8 | 2.9574 | 4.0232 | 2.0338 | 2.9600 | 1.0782 | 2.2013 | 1.7595 | | 2.3923 | 3.0196 | H9 | 3.1205 | 4.2082 | 3.1632 | 2.0299 | 2.2055 | 1.0756 | 2.8842 | 2.3923 | | 1.7595 | H10 | 2.9574 | 4.0232 | 2.9600 | 2.0338 | 2.2013 | 1.0782 | 2.3923 | 3.0196 | 1.7595 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
111.711 |
|
C1 |
O4 |
C6 |
111.711 |
| O2 |
C1 |
O3 |
126.701 |
|
O2 |
C1 |
O4 |
126.701 |
| O3 |
C1 |
O4 |
106.598 |
|
O3 |
C5 |
C6 |
103.872 |
| O3 |
C5 |
H7 |
108.993 |
|
O3 |
C5 |
H8 |
109.157 |
| O4 |
C6 |
C5 |
103.872 |
|
O4 |
C6 |
H9 |
108.993 |
| O4 |
C6 |
H10 |
109.157 |
|
C5 |
C6 |
H9 |
112.771 |
| C5 |
C6 |
H10 |
112.271 |
|
C6 |
C5 |
H7 |
112.771 |
| C6 |
C5 |
H8 |
112.271 |
|
H7 |
C5 |
H8 |
109.555 |
| H9 |
C6 |
H10 |
109.555 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.665 |
|
|
|
| 2 |
O |
-0.309 |
|
|
|
| 3 |
O |
-0.462 |
|
|
|
| 4 |
O |
-0.462 |
|
|
|
| 5 |
C |
-0.131 |
|
|
|
| 6 |
C |
-0.131 |
|
|
|
| 7 |
H |
0.209 |
|
|
|
| 8 |
H |
0.205 |
|
|
|
| 9 |
H |
0.209 |
|
|
|
| 10 |
H |
0.205 |
|
|
|
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 |
-6.200 |
6.200 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.412 |
0.275 |
0.000 |
| y |
0.275 |
-39.426 |
0.000 |
| z |
0.000 |
0.000 |
-37.051 |
|
| Traceless |
| | x | y | z |
| x |
5.826 |
0.275 |
0.000 |
| y |
0.275 |
-4.694 |
0.000 |
| z |
0.000 |
0.000 |
-1.132 |
|
| Polar |
| 3z2-r2 | -2.264 |
| x2-y2 | 7.014 |
| xy | 0.275 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.662 |
0.064 |
0.000 |
| y |
0.064 |
4.460 |
0.000 |
| z |
0.000 |
0.000 |
6.778 |
<r2> (average value of r
2) Å
2
| <r2> |
131.203 |
| (<r2>)1/2 |
11.454 |