Jump to
S1C2
Energy calculated at B1B95/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -342.328322 |
| Energy at 298.15K | |
| HF Energy | -342.328322 |
| Nuclear repulsion energy | 246.345216 |
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 B1B95/aug-cc-pVDZ
| 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 |
3088 |
2958 |
64.39 |
|
|
|
| 2 |
A1 |
1941 |
1859 |
665.13 |
|
|
|
| 3 |
A1 |
1535 |
1470 |
0.84 |
|
|
|
| 4 |
A1 |
1395 |
1336 |
0.07 |
|
|
|
| 5 |
A1 |
1235 |
1183 |
239.63 |
|
|
|
| 6 |
A1 |
972 |
931 |
9.93 |
|
|
|
| 7 |
A1 |
849 |
813 |
38.45 |
|
|
|
| 8 |
A1 |
725 |
695 |
0.69 |
|
|
|
| 9 |
A2 |
3120 |
2988 |
0.00 |
|
|
|
| 10 |
A2 |
1251 |
1198 |
0.00 |
|
|
|
| 11 |
A2 |
1164 |
1115 |
0.00 |
|
|
|
| 12 |
A2 |
177i |
170i |
0.00 |
|
|
|
| 13 |
B1 |
3142 |
3010 |
37.90 |
|
|
|
| 14 |
B1 |
1267 |
1213 |
2.24 |
|
|
|
| 15 |
B1 |
861 |
824 |
0.47 |
|
|
|
| 16 |
B1 |
768 |
735 |
22.06 |
|
|
|
| 17 |
B1 |
140 |
134 |
1.46 |
|
|
|
| 18 |
B2 |
3080 |
2951 |
21.81 |
|
|
|
| 19 |
B2 |
1524 |
1460 |
5.93 |
|
|
|
| 20 |
B2 |
1396 |
1338 |
16.94 |
|
|
|
| 21 |
B2 |
1217 |
1166 |
4.90 |
|
|
|
| 22 |
B2 |
1060 |
1016 |
296.07 |
|
|
|
| 23 |
B2 |
752 |
721 |
1.36 |
|
|
|
| 24 |
B2 |
504 |
483 |
0.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16403.5 cm
-1
Scaled (by 0.9579) Zero Point Vibrational Energy (zpe) 15712.9 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 B1B95/aug-cc-pVDZ
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 |
2.046 |
| O3 |
0.000 |
1.126 |
0.056 |
| O4 |
0.000 |
-1.126 |
0.056 |
| C5 |
0.000 |
0.770 |
-1.282 |
| C6 |
0.000 |
-0.770 |
-1.282 |
| H7 |
-0.890 |
1.186 |
-1.766 |
| H8 |
0.890 |
1.186 |
-1.766 |
| H9 |
0.890 |
-1.186 |
-1.766 |
| H10 |
-0.890 |
-1.186 |
-1.766 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1833 | 1.3845 | 1.3845 | 2.2780 | 2.2780 | 3.0179 | 3.0179 | 3.0179 | 3.0179 |
O2 | 1.1833 | | 2.2857 | 2.2857 | 3.4152 | 3.4152 | 4.0901 | 4.0901 | 4.0901 | 4.0901 | O3 | 1.3845 | 2.2857 | | 2.2515 | 1.3845 | 2.3205 | 2.0294 | 2.0294 | 3.0753 | 3.0753 | O4 | 1.3845 | 2.2857 | 2.2515 | | 2.3205 | 1.3845 | 3.0753 | 3.0753 | 2.0294 | 2.0294 | C5 | 2.2780 | 3.4152 | 1.3845 | 2.3205 | | 1.5404 | 1.0954 | 1.0954 | 2.2028 | 2.2028 | C6 | 2.2780 | 3.4152 | 2.3205 | 1.3845 | 1.5404 | | 2.2028 | 2.2028 | 1.0954 | 1.0954 | H7 | 3.0179 | 4.0901 | 2.0294 | 3.0753 | 1.0954 | 2.2028 | | 1.7802 | 2.9652 | 2.3713 | H8 | 3.0179 | 4.0901 | 2.0294 | 3.0753 | 1.0954 | 2.2028 | 1.7802 | | 2.3713 | 2.9652 | H9 | 3.0179 | 4.0901 | 3.0753 | 2.0294 | 2.2028 | 1.0954 | 2.9652 | 2.3713 | | 1.7802 | H10 | 3.0179 | 4.0901 | 3.0753 | 2.0294 | 2.2028 | 1.0954 | 2.3713 | 2.9652 | 1.7802 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
110.714 |
|
C1 |
O4 |
C6 |
110.714 |
| O2 |
C1 |
O3 |
125.597 |
|
O2 |
C1 |
O4 |
125.597 |
| O3 |
C1 |
O4 |
108.806 |
|
O3 |
C5 |
C6 |
104.882 |
| O3 |
C5 |
H7 |
109.285 |
|
O3 |
C5 |
H8 |
109.285 |
| O4 |
C6 |
C5 |
104.882 |
|
O4 |
C6 |
H9 |
109.285 |
| O4 |
C6 |
H10 |
109.285 |
|
C5 |
C6 |
H9 |
112.289 |
| C5 |
C6 |
H10 |
112.289 |
|
C6 |
C5 |
H7 |
112.289 |
| C6 |
C5 |
H8 |
112.289 |
|
H7 |
C5 |
H8 |
108.701 |
| H9 |
C6 |
H10 |
108.701 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.845 |
|
|
|
| 2 |
O |
-0.455 |
|
|
|
| 3 |
O |
-0.528 |
|
|
|
| 4 |
O |
-0.528 |
|
|
|
| 5 |
C |
1.018 |
|
|
|
| 6 |
C |
1.018 |
|
|
|
| 7 |
H |
-0.343 |
|
|
|
| 8 |
H |
-0.343 |
|
|
|
| 9 |
H |
-0.343 |
|
|
|
| 10 |
H |
-0.343 |
|
|
|
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 |
-4.900 |
4.900 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.201 |
0.000 |
0.000 |
| y |
0.000 |
-36.158 |
0.000 |
| z |
0.000 |
0.000 |
-36.419 |
|
| Traceless |
| | x | y | z |
| x |
4.087 |
0.000 |
0.000 |
| y |
0.000 |
-1.847 |
0.000 |
| z |
0.000 |
0.000 |
-2.240 |
|
| Polar |
| 3z2-r2 | -4.480 |
| x2-y2 | 3.956 |
| 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 |
5.109 |
0.000 |
0.000 |
| y |
0.000 |
6.377 |
0.000 |
| z |
0.000 |
0.000 |
8.434 |
<r2> (average value of r
2) Å
2
| <r2> |
128.180 |
| (<r2>)1/2 |
11.322 |
Jump to
S1C1
Energy calculated at B1B95/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -342.329034 |
| Energy at 298.15K | -342.335426 |
| HF Energy | -342.329034 |
| Nuclear repulsion energy | 246.889047 |
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 B1B95/aug-cc-pVDZ
| 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 |
3149 |
3017 |
17.78 |
|
|
|
| 2 |
A |
3066 |
2937 |
36.38 |
|
|
|
| 3 |
A |
1944 |
1862 |
649.56 |
|
|
|
| 4 |
A |
1523 |
1459 |
1.14 |
|
|
|
| 5 |
A |
1399 |
1340 |
3.87 |
|
|
|
| 6 |
A |
1254 |
1202 |
28.81 |
|
|
|
| 7 |
A |
1228 |
1177 |
181.94 |
|
|
|
| 8 |
A |
1150 |
1101 |
22.96 |
|
|
|
| 9 |
A |
974 |
933 |
4.02 |
|
|
|
| 10 |
A |
844 |
808 |
41.41 |
|
|
|
| 11 |
A |
722 |
692 |
0.92 |
|
|
|
| 12 |
A |
129 |
124 |
0.38 |
|
|
|
| 13 |
B |
3160 |
3026 |
22.28 |
|
|
|
| 14 |
B |
3070 |
2941 |
42.49 |
|
|
|
| 15 |
B |
1514 |
1450 |
7.34 |
|
|
|
| 16 |
B |
1389 |
1330 |
14.53 |
|
|
|
| 17 |
B |
1269 |
1216 |
5.76 |
|
|
|
| 18 |
B |
1192 |
1142 |
4.19 |
|
|
|
| 19 |
B |
1053 |
1008 |
277.85 |
|
|
|
| 20 |
B |
899 |
861 |
7.13 |
|
|
|
| 21 |
B |
775 |
743 |
22.41 |
|
|
|
| 22 |
B |
689 |
660 |
0.65 |
|
|
|
| 23 |
B |
506 |
484 |
0.07 |
|
|
|
| 24 |
B |
147 |
141 |
1.26 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16521.8 cm
-1
Scaled (by 0.9579) Zero Point Vibrational Energy (zpe) 15826.2 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 B1B95/aug-cc-pVDZ
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 |
2.041 |
| O3 |
0.000 |
1.126 |
0.047 |
| O4 |
0.000 |
-1.126 |
0.047 |
| C5 |
0.192 |
0.739 |
-1.272 |
| C6 |
-0.192 |
-0.739 |
-1.272 |
| H7 |
-0.443 |
1.345 |
-1.924 |
| H8 |
1.243 |
0.891 |
-1.550 |
| H9 |
0.443 |
-1.345 |
-1.924 |
| H10 |
-1.243 |
-0.891 |
-1.550 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1830 | 1.3877 | 1.3877 | 2.2627 | 2.2627 | 3.1217 | 2.8527 | 3.1217 | 2.8527 |
O2 | 1.1830 | | 2.2901 | 2.2901 | 3.3998 | 3.3998 | 4.2103 | 3.9032 | 4.2103 | 3.9032 | O3 | 1.3877 | 2.2901 | | 2.2516 | 1.3877 | 2.2919 | 2.0318 | 2.0373 | 3.1913 | 2.8568 | O4 | 1.3877 | 2.2901 | 2.2516 | | 2.2919 | 1.3877 | 3.1913 | 2.8568 | 2.0318 | 2.0373 | C5 | 2.2627 | 3.3998 | 1.3877 | 2.2919 | | 1.5267 | 1.0931 | 1.0981 | 2.1978 | 2.1889 | C6 | 2.2627 | 3.3998 | 2.2919 | 1.3877 | 1.5267 | | 2.1978 | 2.1889 | 1.0931 | 1.0981 | H7 | 3.1217 | 4.2103 | 2.0318 | 3.1913 | 1.0931 | 2.1978 | | 1.7856 | 2.8317 | 2.4037 | H8 | 2.8527 | 3.9032 | 2.0373 | 2.8568 | 1.0981 | 2.1889 | 1.7856 | | 2.4037 | 3.0584 | H9 | 3.1217 | 4.2103 | 3.1913 | 2.0318 | 2.1978 | 1.0931 | 2.8317 | 2.4037 | | 1.7856 | H10 | 2.8527 | 3.9032 | 2.8568 | 2.0373 | 2.1889 | 1.0981 | 2.4037 | 3.0584 | 1.7856 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
109.233 |
|
C1 |
O4 |
C6 |
109.233 |
| O2 |
C1 |
O3 |
125.777 |
|
O2 |
C1 |
O4 |
125.777 |
| O3 |
C1 |
O4 |
108.446 |
|
O3 |
C5 |
C6 |
103.602 |
| O3 |
C5 |
H7 |
109.403 |
|
O3 |
C5 |
H8 |
109.542 |
| O4 |
C6 |
C5 |
103.602 |
|
O4 |
C6 |
H9 |
109.403 |
| O4 |
C6 |
H10 |
109.542 |
|
C5 |
C6 |
H9 |
113.005 |
| C5 |
C6 |
H10 |
111.973 |
|
C6 |
C5 |
H7 |
113.005 |
| C6 |
C5 |
H8 |
111.973 |
|
H7 |
C5 |
H8 |
109.148 |
| H9 |
C6 |
H10 |
109.148 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.854 |
|
|
|
| 2 |
O |
-0.467 |
|
|
|
| 3 |
O |
-0.536 |
|
|
|
| 4 |
O |
-0.536 |
|
|
|
| 5 |
C |
1.030 |
|
|
|
| 6 |
C |
1.030 |
|
|
|
| 7 |
H |
-0.314 |
|
|
|
| 8 |
H |
-0.373 |
|
|
|
| 9 |
H |
-0.314 |
|
|
|
| 10 |
H |
-0.373 |
|
|
|
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 |
-4.859 |
4.859 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.298 |
0.251 |
0.000 |
| y |
0.251 |
-36.185 |
0.000 |
| z |
0.000 |
0.000 |
-36.201 |
|
| Traceless |
| | x | y | z |
| x |
3.895 |
0.251 |
0.000 |
| y |
0.251 |
-1.935 |
0.000 |
| z |
0.000 |
0.000 |
-1.959 |
|
| Polar |
| 3z2-r2 | -3.919 |
| x2-y2 | 3.887 |
| xy | 0.251 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.231 |
0.166 |
0.000 |
| y |
0.166 |
6.308 |
0.000 |
| z |
0.000 |
0.000 |
8.396 |
<r2> (average value of r
2) Å
2
| <r2> |
127.156 |
| (<r2>)1/2 |
11.276 |