Jump to
S1C2
Energy calculated at B3PW91/3-21G
| | hartrees |
| Energy at 0K | -340.373246 |
| Energy at 298.15K | |
| HF Energy | -340.373246 |
| Nuclear repulsion energy | 240.787303 |
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 B3PW91/3-21G
| 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 |
3094 |
2974 |
35.38 |
|
|
|
| 2 |
A1 |
1924 |
1849 |
463.46 |
|
|
|
| 3 |
A1 |
1584 |
1523 |
1.39 |
|
|
|
| 4 |
A1 |
1377 |
1323 |
0.04 |
|
|
|
| 5 |
A1 |
1128 |
1084 |
182.07 |
|
|
|
| 6 |
A1 |
915 |
879 |
5.97 |
|
|
|
| 7 |
A1 |
776 |
746 |
29.84 |
|
|
|
| 8 |
A1 |
703 |
675 |
1.84 |
|
|
|
| 9 |
A2 |
3125 |
3004 |
0.00 |
|
|
|
| 10 |
A2 |
1268 |
1219 |
0.00 |
|
|
|
| 11 |
A2 |
1143 |
1099 |
0.00 |
|
|
|
| 12 |
A2 |
167i |
160i |
0.00 |
|
|
|
| 13 |
B1 |
3150 |
3027 |
36.99 |
|
|
|
| 14 |
B1 |
1257 |
1208 |
0.07 |
|
|
|
| 15 |
B1 |
873 |
839 |
0.18 |
|
|
|
| 16 |
B1 |
721 |
693 |
23.99 |
|
|
|
| 17 |
B1 |
124 |
119 |
4.22 |
|
|
|
| 18 |
B2 |
3086 |
2966 |
25.25 |
|
|
|
| 19 |
B2 |
1570 |
1509 |
2.25 |
|
|
|
| 20 |
B2 |
1405 |
1351 |
0.01 |
|
|
|
| 21 |
B2 |
1133 |
1089 |
5.89 |
|
|
|
| 22 |
B2 |
949 |
912 |
289.47 |
|
|
|
| 23 |
B2 |
732 |
704 |
2.16 |
|
|
|
| 24 |
B2 |
484 |
465 |
0.58 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16175.3 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 15547.7 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 B3PW91/3-21G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.894 |
| O2 |
0.000 |
0.000 |
2.091 |
| O3 |
0.000 |
1.158 |
0.059 |
| O4 |
0.000 |
-1.158 |
0.059 |
| C5 |
0.000 |
0.784 |
-1.318 |
| C6 |
0.000 |
-0.784 |
-1.318 |
| H7 |
-0.893 |
1.185 |
-1.803 |
| H8 |
0.893 |
1.185 |
-1.803 |
| H9 |
0.893 |
-1.185 |
-1.803 |
| H10 |
-0.893 |
-1.185 |
-1.803 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1979 | 1.4271 | 1.4271 | 2.3469 | 2.3469 | 3.0785 | 3.0785 | 3.0785 | 3.0785 |
O2 | 1.1979 | | 2.3391 | 2.3391 | 3.4989 | 3.4989 | 4.1681 | 4.1681 | 4.1681 | 4.1681 | O3 | 1.4271 | 2.3391 | | 2.3150 | 1.4271 | 2.3803 | 2.0656 | 2.0656 | 3.1234 | 3.1234 | O4 | 1.4271 | 2.3391 | 2.3150 | | 2.3803 | 1.4271 | 3.1234 | 3.1234 | 2.0656 | 2.0656 | C5 | 2.3469 | 3.4989 | 1.4271 | 2.3803 | | 1.5677 | 1.0930 | 1.0930 | 2.2162 | 2.2162 | C6 | 2.3469 | 3.4989 | 2.3803 | 1.4271 | 1.5677 | | 2.2162 | 2.2162 | 1.0930 | 1.0930 | H7 | 3.0785 | 4.1681 | 2.0656 | 3.1234 | 1.0930 | 2.2162 | | 1.7869 | 2.9689 | 2.3709 | H8 | 3.0785 | 4.1681 | 2.0656 | 3.1234 | 1.0930 | 2.2162 | 1.7869 | | 2.3709 | 2.9689 | H9 | 3.0785 | 4.1681 | 3.1234 | 2.0656 | 2.2162 | 1.0930 | 2.9689 | 2.3709 | | 1.7869 | H10 | 3.0785 | 4.1681 | 3.1234 | 2.0656 | 2.2162 | 1.0930 | 2.3709 | 2.9689 | 1.7869 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
110.620 |
|
C1 |
O4 |
C6 |
110.620 |
| O2 |
C1 |
O3 |
125.798 |
|
O2 |
C1 |
O4 |
125.798 |
| O3 |
C1 |
O4 |
108.404 |
|
O3 |
C5 |
C6 |
105.178 |
| O3 |
C5 |
H7 |
109.387 |
|
O3 |
C5 |
H8 |
109.387 |
| O4 |
C6 |
C5 |
105.178 |
|
O4 |
C6 |
H9 |
109.387 |
| O4 |
C6 |
H10 |
109.387 |
|
C5 |
C6 |
H9 |
111.557 |
| C5 |
C6 |
H10 |
111.557 |
|
C6 |
C5 |
H7 |
111.557 |
| C6 |
C5 |
H8 |
111.557 |
|
H7 |
C5 |
H8 |
109.659 |
| H9 |
C6 |
H10 |
109.659 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.867 |
|
|
|
| 2 |
O |
-0.464 |
|
|
|
| 3 |
O |
-0.494 |
|
|
|
| 4 |
O |
-0.494 |
|
|
|
| 5 |
C |
-0.204 |
|
|
|
| 6 |
C |
-0.204 |
|
|
|
| 7 |
H |
0.248 |
|
|
|
| 8 |
H |
0.248 |
|
|
|
| 9 |
H |
0.248 |
|
|
|
| 10 |
H |
0.248 |
|
|
|
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 |
-5.009 |
5.009 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.938 |
0.000 |
0.000 |
| y |
0.000 |
-37.011 |
0.000 |
| z |
0.000 |
0.000 |
-34.657 |
|
| Traceless |
| | x | y | z |
| x |
3.896 |
0.000 |
0.000 |
| y |
0.000 |
-3.714 |
0.000 |
| z |
0.000 |
0.000 |
-0.183 |
|
| Polar |
| 3z2-r2 | -0.365 |
| x2-y2 | 5.073 |
| 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 |
3.589 |
0.000 |
0.000 |
| y |
0.000 |
4.584 |
0.000 |
| z |
0.000 |
0.000 |
7.022 |
<r2> (average value of r
2) Å
2
| <r2> |
132.904 |
| (<r2>)1/2 |
11.528 |
Jump to
S1C1
Energy calculated at B3PW91/3-21G
| | hartrees |
| Energy at 0K | -340.374060 |
| Energy at 298.15K | -340.380284 |
| HF Energy | -340.374060 |
| Nuclear repulsion energy | 241.386682 |
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 B3PW91/3-21G
| 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 |
3155 |
3033 |
9.04 |
|
|
|
| 2 |
A |
3075 |
2955 |
18.98 |
|
|
|
| 3 |
A |
1929 |
1854 |
445.18 |
|
|
|
| 4 |
A |
1570 |
1509 |
1.44 |
|
|
|
| 5 |
A |
1391 |
1337 |
4.72 |
|
|
|
| 6 |
A |
1263 |
1214 |
15.83 |
|
|
|
| 7 |
A |
1157 |
1112 |
16.57 |
|
|
|
| 8 |
A |
1108 |
1065 |
139.79 |
|
|
|
| 9 |
A |
929 |
893 |
3.08 |
|
|
|
| 10 |
A |
770 |
740 |
31.28 |
|
|
|
| 11 |
A |
699 |
672 |
2.52 |
|
|
|
| 12 |
A |
124 |
120 |
0.67 |
|
|
|
| 13 |
B |
3166 |
3044 |
22.18 |
|
|
|
| 14 |
B |
3079 |
2960 |
41.24 |
|
|
|
| 15 |
B |
1563 |
1502 |
3.61 |
|
|
|
| 16 |
B |
1405 |
1350 |
0.33 |
|
|
|
| 17 |
B |
1257 |
1208 |
0.82 |
|
|
|
| 18 |
B |
1112 |
1069 |
6.04 |
|
|
|
| 19 |
B |
959 |
922 |
191.22 |
|
|
|
| 20 |
B |
898 |
864 |
81.93 |
|
|
|
| 21 |
B |
732 |
703 |
25.68 |
|
|
|
| 22 |
B |
663 |
637 |
0.74 |
|
|
|
| 23 |
B |
484 |
465 |
0.75 |
|
|
|
| 24 |
B |
137 |
132 |
3.97 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16312.6 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 15679.7 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 B3PW91/3-21G
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.888 |
| O2 |
0.000 |
0.000 |
2.086 |
| O3 |
0.000 |
1.158 |
0.046 |
| O4 |
0.000 |
-1.158 |
0.046 |
| C5 |
0.215 |
0.744 |
-1.307 |
| C6 |
-0.215 |
-0.744 |
-1.307 |
| H7 |
-0.394 |
1.358 |
-1.972 |
| H8 |
1.275 |
0.848 |
-1.563 |
| H9 |
0.394 |
-1.358 |
-1.972 |
| H10 |
-1.275 |
-0.848 |
-1.563 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1974 | 1.4320 | 1.4320 | 2.3282 | 2.3282 | 3.1903 | 2.8901 | 3.1903 | 2.8901 |
O2 | 1.1974 | | 2.3453 | 2.3453 | 3.4802 | 3.4802 | 4.2966 | 3.9567 | 4.2966 | 3.9567 | O3 | 1.4320 | 2.3453 | | 2.3170 | 1.4320 | 2.3449 | 2.0659 | 2.0766 | 3.2494 | 2.8709 | O4 | 1.4320 | 2.3453 | 2.3170 | | 2.3449 | 1.4320 | 3.2494 | 2.8709 | 2.0659 | 2.0766 | C5 | 2.3282 | 3.4802 | 1.4320 | 2.3449 | | 1.5492 | 1.0904 | 1.0955 | 2.2114 | 2.1958 | C6 | 2.3282 | 3.4802 | 2.3449 | 1.4320 | 1.5492 | | 2.2114 | 2.1958 | 1.0904 | 1.0955 | H7 | 3.1903 | 4.2966 | 2.0659 | 3.2494 | 1.0904 | 2.2114 | | 1.7929 | 2.8272 | 2.4100 | H8 | 2.8901 | 3.9567 | 2.0766 | 2.8709 | 1.0955 | 2.1958 | 1.7929 | | 2.4100 | 3.0631 | H9 | 3.1903 | 4.2966 | 3.2494 | 2.0659 | 2.2114 | 1.0904 | 2.8272 | 2.4100 | | 1.7929 | H10 | 2.8901 | 3.9567 | 2.8709 | 2.0766 | 2.1958 | 1.0955 | 2.4100 | 3.0631 | 1.7929 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
108.760 |
|
C1 |
O4 |
C6 |
108.760 |
| O2 |
C1 |
O3 |
126.003 |
|
O2 |
C1 |
O4 |
126.003 |
| O3 |
C1 |
O4 |
107.994 |
|
O3 |
C5 |
C6 |
103.666 |
| O3 |
C5 |
H7 |
109.226 |
|
O3 |
C5 |
H8 |
109.774 |
| O4 |
C6 |
C5 |
103.666 |
|
O4 |
C6 |
H9 |
109.226 |
| O4 |
C6 |
H10 |
109.774 |
|
C5 |
C6 |
H9 |
112.659 |
| C5 |
C6 |
H10 |
111.095 |
|
C6 |
C5 |
H7 |
112.659 |
| C6 |
C5 |
H8 |
111.095 |
|
H7 |
C5 |
H8 |
110.206 |
| H9 |
C6 |
H10 |
110.206 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.865 |
|
|
|
| 2 |
O |
-0.464 |
|
|
|
| 3 |
O |
-0.491 |
|
|
|
| 4 |
O |
-0.491 |
|
|
|
| 5 |
C |
-0.206 |
|
|
|
| 6 |
C |
-0.206 |
|
|
|
| 7 |
H |
0.251 |
|
|
|
| 8 |
H |
0.246 |
|
|
|
| 9 |
H |
0.251 |
|
|
|
| 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 |
-4.935 |
4.935 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.978 |
0.257 |
0.000 |
| y |
0.257 |
-37.062 |
0.000 |
| z |
0.000 |
0.000 |
-34.472 |
|
| Traceless |
| | x | y | z |
| x |
3.789 |
0.257 |
0.000 |
| y |
0.257 |
-3.836 |
0.000 |
| z |
0.000 |
0.000 |
0.047 |
|
| Polar |
| 3z2-r2 | 0.095 |
| x2-y2 | 5.084 |
| xy | 0.257 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.678 |
0.130 |
0.000 |
| y |
0.130 |
4.513 |
0.000 |
| z |
0.000 |
0.000 |
6.989 |
<r2> (average value of r
2) Å
2
| <r2> |
131.647 |
| (<r2>)1/2 |
11.474 |