Jump to
S1C2
Energy calculated at PBE1PBE/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -342.160087 |
| Energy at 298.15K | |
| HF Energy | -342.160087 |
| Nuclear repulsion energy | 246.825130 |
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/aug-cc-pVTZ
| 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 |
3066 |
2948 |
61.34 |
|
|
|
| 2 |
A1 |
1946 |
1871 |
666.91 |
|
|
|
| 3 |
A1 |
1547 |
1487 |
0.91 |
|
|
|
| 4 |
A1 |
1398 |
1345 |
0.00 |
|
|
|
| 5 |
A1 |
1234 |
1186 |
246.09 |
|
|
|
| 6 |
A1 |
967 |
930 |
8.66 |
|
|
|
| 7 |
A1 |
853 |
820 |
37.24 |
|
|
|
| 8 |
A1 |
733 |
705 |
0.89 |
|
|
|
| 9 |
A2 |
3089 |
2970 |
0.00 |
|
|
|
| 10 |
A2 |
1261 |
1213 |
0.00 |
|
|
|
| 11 |
A2 |
1170 |
1125 |
0.00 |
|
|
|
| 12 |
A2 |
170i |
163i |
0.00 |
|
|
|
| 13 |
B1 |
3113 |
2993 |
35.26 |
|
|
|
| 14 |
B1 |
1274 |
1225 |
2.29 |
|
|
|
| 15 |
B1 |
861 |
828 |
0.38 |
|
|
|
| 16 |
B1 |
777 |
747 |
21.95 |
|
|
|
| 17 |
B1 |
145 |
140 |
1.34 |
|
|
|
| 18 |
B2 |
3059 |
2941 |
20.38 |
|
|
|
| 19 |
B2 |
1534 |
1475 |
6.71 |
|
|
|
| 20 |
B2 |
1415 |
1361 |
13.01 |
|
|
|
| 21 |
B2 |
1219 |
1172 |
4.40 |
|
|
|
| 22 |
B2 |
1063 |
1022 |
299.24 |
|
|
|
| 23 |
B2 |
759 |
730 |
1.58 |
|
|
|
| 24 |
B2 |
513 |
493 |
0.05 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16413.3 cm
-1
Scaled (by 0.9615) Zero Point Vibrational Energy (zpe) 15781.4 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/aug-cc-pVTZ
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 |
1.124 |
0.057 |
| O4 |
0.000 |
-1.124 |
0.057 |
| C5 |
0.000 |
0.771 |
-1.279 |
| C6 |
0.000 |
-0.771 |
-1.279 |
| H7 |
-0.887 |
1.183 |
-1.765 |
| H8 |
0.887 |
1.183 |
-1.765 |
| H9 |
0.887 |
-1.183 |
-1.765 |
| H10 |
-0.887 |
-1.183 |
-1.765 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1787 | 1.3818 | 1.3818 | 2.2751 | 2.2751 | 3.0143 | 3.0143 | 3.0143 | 3.0143 |
O2 | 1.1787 | | 2.2793 | 2.2793 | 3.4075 | 3.4075 | 4.0826 | 4.0826 | 4.0826 | 4.0826 | O3 | 1.3818 | 2.2793 | | 2.2471 | 1.3818 | 2.3182 | 2.0275 | 2.0275 | 3.0704 | 3.0704 | O4 | 1.3818 | 2.2793 | 2.2471 | | 2.3182 | 1.3818 | 3.0704 | 3.0704 | 2.0275 | 2.0275 | C5 | 2.2751 | 3.4075 | 1.3818 | 2.3182 | | 1.5420 | 1.0919 | 1.0919 | 2.2002 | 2.2002 | C6 | 2.2751 | 3.4075 | 2.3182 | 1.3818 | 1.5420 | | 2.2002 | 2.2002 | 1.0919 | 1.0919 | H7 | 3.0143 | 4.0826 | 2.0275 | 3.0704 | 1.0919 | 2.2002 | | 1.7730 | 2.9567 | 2.3661 | H8 | 3.0143 | 4.0826 | 2.0275 | 3.0704 | 1.0919 | 2.2002 | 1.7730 | | 2.3661 | 2.9567 | H9 | 3.0143 | 4.0826 | 3.0704 | 2.0275 | 2.2002 | 1.0919 | 2.9567 | 2.3661 | | 1.7730 | H10 | 3.0143 | 4.0826 | 3.0704 | 2.0275 | 2.2002 | 1.0919 | 2.3661 | 2.9567 | 1.7730 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
110.817 |
|
C1 |
O4 |
C6 |
110.817 |
| O2 |
C1 |
O3 |
125.600 |
|
O2 |
C1 |
O4 |
125.600 |
| O3 |
C1 |
O4 |
108.800 |
|
O3 |
C5 |
C6 |
104.783 |
| O3 |
C5 |
H7 |
109.537 |
|
O3 |
C5 |
H8 |
109.537 |
| O4 |
C6 |
C5 |
104.783 |
|
O4 |
C6 |
H9 |
109.537 |
| O4 |
C6 |
H10 |
109.537 |
|
C5 |
C6 |
H9 |
112.172 |
| C5 |
C6 |
H10 |
112.172 |
|
C6 |
C5 |
H7 |
112.172 |
| C6 |
C5 |
H8 |
112.172 |
|
H7 |
C5 |
H8 |
108.560 |
| H9 |
C6 |
H10 |
108.560 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.350 |
|
|
|
| 2 |
O |
-0.478 |
|
|
|
| 3 |
O |
-0.258 |
|
|
|
| 4 |
O |
-0.258 |
|
|
|
| 5 |
C |
-0.171 |
|
|
|
| 6 |
C |
-0.171 |
|
|
|
| 7 |
H |
0.246 |
|
|
|
| 8 |
H |
0.246 |
|
|
|
| 9 |
H |
0.246 |
|
|
|
| 10 |
H |
0.246 |
|
|
|
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 |
-4.858 |
4.858 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.153 |
0.000 |
0.000 |
| y |
0.000 |
-36.113 |
0.000 |
| z |
0.000 |
0.000 |
-36.415 |
|
| Traceless |
| | x | y | z |
| x |
4.110 |
0.000 |
0.000 |
| y |
0.000 |
-1.829 |
0.000 |
| z |
0.000 |
0.000 |
-2.281 |
|
| Polar |
| 3z2-r2 | -4.563 |
| x2-y2 | 3.960 |
| 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 |
5.143 |
0.000 |
0.000 |
| y |
0.000 |
6.410 |
0.000 |
| z |
0.000 |
0.000 |
8.384 |
<r2> (average value of r
2) Å
2
| <r2> |
127.766 |
| (<r2>)1/2 |
11.303 |
Jump to
S1C1
Energy calculated at PBE1PBE/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -342.160600 |
| Energy at 298.15K | -342.166986 |
| HF Energy | -342.160600 |
| Nuclear repulsion energy | 247.294302 |
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/aug-cc-pVTZ
| 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 |
3116 |
2996 |
18.44 |
|
|
|
| 2 |
A |
3043 |
2926 |
34.08 |
|
|
|
| 3 |
A |
1949 |
1874 |
653.16 |
|
|
|
| 4 |
A |
1535 |
1476 |
1.18 |
|
|
|
| 5 |
A |
1402 |
1348 |
2.05 |
|
|
|
| 6 |
A |
1265 |
1216 |
26.32 |
|
|
|
| 7 |
A |
1229 |
1181 |
187.97 |
|
|
|
| 8 |
A |
1159 |
1114 |
27.29 |
|
|
|
| 9 |
A |
968 |
931 |
3.64 |
|
|
|
| 10 |
A |
849 |
816 |
40.23 |
|
|
|
| 11 |
A |
731 |
702 |
1.09 |
|
|
|
| 12 |
A |
111 |
106 |
0.32 |
|
|
|
| 13 |
B |
3127 |
3007 |
20.90 |
|
|
|
| 14 |
B |
3048 |
2931 |
39.25 |
|
|
|
| 15 |
B |
1527 |
1468 |
7.81 |
|
|
|
| 16 |
B |
1408 |
1354 |
11.47 |
|
|
|
| 17 |
B |
1277 |
1228 |
5.26 |
|
|
|
| 18 |
B |
1197 |
1151 |
3.92 |
|
|
|
| 19 |
B |
1056 |
1016 |
282.92 |
|
|
|
| 20 |
B |
899 |
864 |
6.74 |
|
|
|
| 21 |
B |
783 |
753 |
22.17 |
|
|
|
| 22 |
B |
698 |
672 |
0.63 |
|
|
|
| 23 |
B |
513 |
494 |
0.12 |
|
|
|
| 24 |
B |
150 |
145 |
1.20 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16520.2 cm
-1
Scaled (by 0.9615) Zero Point Vibrational Energy (zpe) 15884.2 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/aug-cc-pVTZ
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.858 |
| O2 |
0.000 |
0.000 |
2.036 |
| O3 |
0.000 |
1.124 |
0.049 |
| O4 |
0.000 |
-1.124 |
0.049 |
| C5 |
0.177 |
0.744 |
-1.271 |
| C6 |
-0.177 |
-0.744 |
-1.271 |
| H7 |
-0.477 |
1.335 |
-1.913 |
| H8 |
1.216 |
0.916 |
-1.568 |
| H9 |
0.477 |
-1.335 |
-1.913 |
| H10 |
-1.216 |
-0.916 |
-1.568 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1783 | 1.3846 | 1.3846 | 2.2619 | 2.2619 | 3.1117 | 2.8641 | 3.1117 | 2.8641 |
O2 | 1.1783 | | 2.2829 | 2.2829 | 3.3942 | 3.3942 | 4.1951 | 3.9125 | 4.1951 | 3.9125 | O3 | 1.3846 | 2.2829 | | 2.2475 | 1.3846 | 2.2938 | 2.0294 | 2.0338 | 3.1807 | 2.8733 | O4 | 1.3846 | 2.2829 | 2.2475 | | 2.2938 | 1.3846 | 3.1807 | 2.8733 | 2.0294 | 2.0338 | C5 | 2.2619 | 3.3942 | 1.3846 | 2.2938 | | 1.5296 | 1.0897 | 1.0946 | 2.1959 | 2.1878 | C6 | 2.2619 | 3.3942 | 2.2938 | 1.3846 | 1.5296 | | 2.1959 | 2.1878 | 1.0897 | 1.0946 | H7 | 3.1117 | 4.1951 | 2.0294 | 3.1807 | 1.0897 | 2.1959 | | 1.7774 | 2.8341 | 2.3943 | H8 | 2.8641 | 3.9125 | 2.0338 | 2.8733 | 1.0946 | 2.1878 | 1.7774 | | 2.3943 | 3.0457 | H9 | 3.1117 | 4.1951 | 3.1807 | 2.0294 | 2.1959 | 1.0897 | 2.8341 | 2.3943 | | 1.7774 | H10 | 2.8641 | 3.9125 | 2.8733 | 2.0338 | 2.1878 | 1.0946 | 2.3943 | 3.0457 | 1.7774 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
109.529 |
|
C1 |
O4 |
C6 |
109.529 |
| O2 |
C1 |
O3 |
125.748 |
|
O2 |
C1 |
O4 |
125.748 |
| O3 |
C1 |
O4 |
108.505 |
|
O3 |
C5 |
C6 |
103.722 |
| O3 |
C5 |
H7 |
109.634 |
|
O3 |
C5 |
H8 |
109.683 |
| O4 |
C6 |
C5 |
103.722 |
|
O4 |
C6 |
H9 |
109.634 |
| O4 |
C6 |
H10 |
109.683 |
|
C5 |
C6 |
H9 |
112.855 |
| C5 |
C6 |
H10 |
111.894 |
|
C6 |
C5 |
H7 |
112.855 |
| C6 |
C5 |
H8 |
111.894 |
|
H7 |
C5 |
H8 |
108.923 |
| H9 |
C6 |
H10 |
108.923 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.380 |
|
|
|
| 2 |
O |
-0.489 |
|
|
|
| 3 |
O |
-0.273 |
|
|
|
| 4 |
O |
-0.273 |
|
|
|
| 5 |
C |
-0.184 |
|
|
|
| 6 |
C |
-0.184 |
|
|
|
| 7 |
H |
0.275 |
|
|
|
| 8 |
H |
0.236 |
|
|
|
| 9 |
H |
0.275 |
|
|
|
| 10 |
H |
0.236 |
|
|
|
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 |
-4.823 |
4.823 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.247 |
0.224 |
0.000 |
| y |
0.224 |
-36.138 |
0.000 |
| z |
0.000 |
0.000 |
-36.221 |
|
| Traceless |
| | x | y | z |
| x |
3.932 |
0.224 |
0.000 |
| y |
0.224 |
-1.903 |
0.000 |
| z |
0.000 |
0.000 |
-2.029 |
|
| Polar |
| 3z2-r2 | -4.058 |
| x2-y2 | 3.891 |
| xy | 0.224 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.251 |
0.158 |
0.000 |
| y |
0.158 |
6.349 |
0.000 |
| z |
0.000 |
0.000 |
8.350 |
<r2> (average value of r
2) Å
2
| <r2> |
126.887 |
| (<r2>)1/2 |
11.264 |