Jump to
S1C2
Energy calculated at B97D3/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -342.324866 |
| Energy at 298.15K | |
| HF Energy | -342.324866 |
| Nuclear repulsion energy | 244.726572 |
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 B97D3/6-311+G(3df,2p)
| 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 |
3009 |
2970 |
57.54 |
|
|
|
| 2 |
A1 |
1848 |
1824 |
611.22 |
|
|
|
| 3 |
A1 |
1507 |
1487 |
0.37 |
|
|
|
| 4 |
A1 |
1352 |
1334 |
0.49 |
|
|
|
| 5 |
A1 |
1056 |
1043 |
206.90 |
|
|
|
| 6 |
A1 |
944 |
932 |
24.38 |
|
|
|
| 7 |
A1 |
858 |
847 |
2.72 |
|
|
|
| 8 |
A1 |
707 |
698 |
4.26 |
|
|
|
| 9 |
A2 |
3041 |
3001 |
0.00 |
|
|
|
| 10 |
A2 |
1218 |
1202 |
0.00 |
|
|
|
| 11 |
A2 |
1131 |
1116 |
0.00 |
|
|
|
| 12 |
A2 |
108i |
106i |
0.00 |
|
|
|
| 13 |
B1 |
3064 |
3024 |
36.65 |
|
|
|
| 14 |
B1 |
1216 |
1200 |
1.86 |
|
|
|
| 15 |
B1 |
839 |
828 |
0.28 |
|
|
|
| 16 |
B1 |
740 |
730 |
17.63 |
|
|
|
| 17 |
B1 |
181 |
179 |
1.39 |
|
|
|
| 18 |
B2 |
3004 |
2965 |
22.73 |
|
|
|
| 19 |
B2 |
1496 |
1477 |
5.39 |
|
|
|
| 20 |
B2 |
1377 |
1359 |
30.93 |
|
|
|
| 21 |
B2 |
1084 |
1070 |
272.64 |
|
|
|
| 22 |
B2 |
1022 |
1009 |
2.32 |
|
|
|
| 23 |
B2 |
728 |
718 |
0.04 |
|
|
|
| 24 |
B2 |
506 |
499 |
0.04 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15909.4 cm
-1
Scaled (by 0.987) Zero Point Vibrational Energy (zpe) 15702.6 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 B97D3/6-311+G(3df,2p)
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.858 |
| O2 |
0.000 |
0.000 |
2.051 |
| O3 |
0.000 |
1.122 |
0.081 |
| O4 |
0.000 |
-1.122 |
0.081 |
| C5 |
0.000 |
0.773 |
-1.313 |
| C6 |
0.000 |
-0.773 |
-1.313 |
| H7 |
-0.893 |
1.199 |
-1.777 |
| H8 |
0.893 |
1.199 |
-1.777 |
| H9 |
0.893 |
-1.199 |
-1.777 |
| H10 |
-0.893 |
-1.199 |
-1.777 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1930 | 1.3648 | 1.3648 | 2.3042 | 2.3042 | 3.0298 | 3.0298 | 3.0298 | 3.0298 |
O2 | 1.1930 | | 2.2671 | 2.2671 | 3.4514 | 3.4514 | 4.1098 | 4.1098 | 4.1098 | 4.1098 | O3 | 1.3648 | 2.2671 | | 2.2443 | 1.4371 | 2.3522 | 2.0631 | 2.0631 | 3.1047 | 3.1047 | O4 | 1.3648 | 2.2671 | 2.2443 | | 2.3522 | 1.4371 | 3.1047 | 3.1047 | 2.0631 | 2.0631 | C5 | 2.3042 | 3.4514 | 1.4371 | 2.3522 | | 1.5450 | 1.0933 | 1.0933 | 2.2138 | 2.2138 | C6 | 2.3042 | 3.4514 | 2.3522 | 1.4371 | 1.5450 | | 2.2138 | 2.2138 | 1.0933 | 1.0933 | H7 | 3.0298 | 4.1098 | 2.0631 | 3.1047 | 1.0933 | 2.2138 | | 1.7861 | 2.9904 | 2.3984 | H8 | 3.0298 | 4.1098 | 2.0631 | 3.1047 | 1.0933 | 2.2138 | 1.7861 | | 2.3984 | 2.9904 | H9 | 3.0298 | 4.1098 | 3.1047 | 2.0631 | 2.2138 | 1.0933 | 2.9904 | 2.3984 | | 1.7861 | H10 | 3.0298 | 4.1098 | 3.1047 | 2.0631 | 2.2138 | 1.0933 | 2.3984 | 2.9904 | 1.7861 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
111.610 |
|
C1 |
O4 |
C6 |
111.610 |
| O2 |
C1 |
O3 |
125.498 |
|
O2 |
C1 |
O4 |
125.498 |
| O3 |
C1 |
O4 |
109.005 |
|
O3 |
C5 |
C6 |
103.888 |
| O3 |
C5 |
H7 |
109.997 |
|
O3 |
C5 |
H8 |
109.997 |
| O4 |
C6 |
C5 |
103.888 |
|
O4 |
C6 |
H9 |
109.997 |
| O4 |
C6 |
H10 |
109.997 |
|
C5 |
C6 |
H9 |
112.212 |
| C5 |
C6 |
H10 |
112.212 |
|
C6 |
C5 |
H7 |
112.212 |
| C6 |
C5 |
H8 |
112.212 |
|
H7 |
C5 |
H8 |
108.469 |
| H9 |
C6 |
H10 |
108.469 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
1.252 |
|
|
|
| 2 |
O |
-0.757 |
|
|
|
| 3 |
O |
-0.626 |
|
|
|
| 4 |
O |
-0.626 |
|
|
|
| 5 |
C |
0.145 |
|
|
|
| 6 |
C |
0.145 |
|
|
|
| 7 |
H |
0.117 |
|
|
|
| 8 |
H |
0.117 |
|
|
|
| 9 |
H |
0.117 |
|
|
|
| 10 |
H |
0.117 |
|
|
|
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 |
-5.352 |
5.352 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.211 |
0.000 |
0.000 |
| y |
0.000 |
-36.030 |
0.000 |
| z |
0.000 |
0.000 |
-36.505 |
|
| Traceless |
| | x | y | z |
| x |
4.056 |
0.000 |
0.000 |
| y |
0.000 |
-1.672 |
0.000 |
| z |
0.000 |
0.000 |
-2.384 |
|
| Polar |
| 3z2-r2 | -4.768 |
| x2-y2 | 3.818 |
| 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 |
5.240 |
0.000 |
0.000 |
| y |
0.000 |
6.642 |
0.000 |
| z |
0.000 |
0.000 |
8.816 |
<r2> (average value of r
2) Å
2
| <r2> |
129.550 |
| (<r2>)1/2 |
11.382 |
Jump to
S1C1
Energy calculated at B97D3/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -342.325314 |
| Energy at 298.15K | -342.331695 |
| HF Energy | -342.325314 |
| Nuclear repulsion energy | 245.180446 |
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 B97D3/6-311+G(3df,2p)
| 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 |
3060 |
3021 |
15.33 |
|
|
|
| 2 |
A |
2993 |
2954 |
35.36 |
|
|
|
| 3 |
A |
1851 |
1827 |
600.90 |
|
|
|
| 4 |
A |
1497 |
1477 |
0.39 |
|
|
|
| 5 |
A |
1354 |
1337 |
0.14 |
|
|
|
| 6 |
A |
1220 |
1204 |
11.58 |
|
|
|
| 7 |
A |
1130 |
1115 |
1.58 |
|
|
|
| 8 |
A |
1046 |
1033 |
193.42 |
|
|
|
| 9 |
A |
941 |
929 |
22.94 |
|
|
|
| 10 |
A |
859 |
848 |
4.95 |
|
|
|
| 11 |
A |
705 |
696 |
4.44 |
|
|
|
| 12 |
A |
146 |
144 |
0.24 |
|
|
|
| 13 |
B |
3074 |
3034 |
25.67 |
|
|
|
| 14 |
B |
2997 |
2958 |
37.20 |
|
|
|
| 15 |
B |
1488 |
1469 |
6.32 |
|
|
|
| 16 |
B |
1370 |
1352 |
26.58 |
|
|
|
| 17 |
B |
1214 |
1198 |
5.87 |
|
|
|
| 18 |
B |
1074 |
1060 |
261.07 |
|
|
|
| 19 |
B |
1015 |
1002 |
2.66 |
|
|
|
| 20 |
B |
864 |
853 |
1.43 |
|
|
|
| 21 |
B |
746 |
736 |
17.25 |
|
|
|
| 22 |
B |
679 |
670 |
0.37 |
|
|
|
| 23 |
B |
506 |
500 |
0.06 |
|
|
|
| 24 |
B |
184 |
182 |
1.22 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16006.8 cm
-1
Scaled (by 0.987) Zero Point Vibrational Energy (zpe) 15798.7 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 B97D3/6-311+G(3df,2p)
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.854 |
| O2 |
0.000 |
0.000 |
2.047 |
| O3 |
0.000 |
1.122 |
0.073 |
| O4 |
0.000 |
-1.122 |
0.073 |
| C5 |
0.179 |
0.745 |
-1.305 |
| C6 |
-0.179 |
-0.745 |
-1.305 |
| H7 |
-0.483 |
1.355 |
-1.922 |
| H8 |
1.222 |
0.929 |
-1.584 |
| H9 |
0.483 |
-1.355 |
-1.922 |
| H10 |
-1.222 |
-0.929 |
-1.584 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1926 | 1.3674 | 1.3674 | 2.2915 | 2.2915 | 3.1273 | 2.8817 | 3.1273 | 2.8817 |
O2 | 1.1926 | | 2.2706 | 2.2706 | 3.4386 | 3.4386 | 4.2220 | 3.9424 | 4.2220 | 3.9424 | O3 | 1.3674 | 2.2706 | | 2.2443 | 1.4399 | 2.3279 | 2.0661 | 2.0682 | 3.2175 | 2.9068 | O4 | 1.3674 | 2.2706 | 2.2443 | | 2.3279 | 1.4399 | 3.2175 | 2.9068 | 2.0661 | 2.0682 | C5 | 2.2915 | 3.4386 | 1.4399 | 2.3279 | | 1.5332 | 1.0914 | 1.0955 | 2.2104 | 2.2016 | C6 | 2.2915 | 3.4386 | 2.3279 | 1.4399 | 1.5332 | | 2.2104 | 2.2016 | 1.0914 | 1.0955 | H7 | 3.1273 | 4.2220 | 2.0661 | 3.2175 | 1.0914 | 2.2104 | | 1.7898 | 2.8774 | 2.4252 | H8 | 2.8817 | 3.9424 | 2.0682 | 2.9068 | 1.0955 | 2.2016 | 1.7898 | | 2.4252 | 3.0713 | H9 | 3.1273 | 4.2220 | 3.2175 | 2.0661 | 2.2104 | 1.0914 | 2.8774 | 2.4252 | | 1.7898 | H10 | 2.8817 | 3.9424 | 2.9068 | 2.0682 | 2.2016 | 1.0955 | 2.4252 | 3.0713 | 1.7898 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
108.994 |
|
C1 |
O4 |
C6 |
108.994 |
| O2 |
C1 |
O3 |
125.428 |
|
O2 |
C1 |
O4 |
125.428 |
| O3 |
C1 |
O4 |
109.143 |
|
O3 |
C5 |
C6 |
102.640 |
| O3 |
C5 |
H7 |
109.551 |
|
O3 |
C5 |
H8 |
109.275 |
| O4 |
C6 |
C5 |
102.640 |
|
O4 |
C6 |
H9 |
109.551 |
| O4 |
C6 |
H10 |
109.275 |
|
C5 |
C6 |
H9 |
113.677 |
| C5 |
C6 |
H10 |
111.795 |
|
C6 |
C5 |
H7 |
113.677 |
| C6 |
C5 |
H8 |
111.795 |
|
H7 |
C5 |
H8 |
109.632 |
| H9 |
C6 |
H10 |
109.632 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
1.244 |
|
|
|
| 2 |
O |
-0.754 |
|
|
|
| 3 |
O |
-0.617 |
|
|
|
| 4 |
O |
-0.617 |
|
|
|
| 5 |
C |
0.135 |
|
|
|
| 6 |
C |
0.135 |
|
|
|
| 7 |
H |
0.121 |
|
|
|
| 8 |
H |
0.116 |
|
|
|
| 9 |
H |
0.121 |
|
|
|
| 10 |
H |
0.116 |
|
|
|
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 |
-5.312 |
5.312 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.270 |
0.267 |
0.000 |
| y |
0.267 |
-36.078 |
0.000 |
| z |
0.000 |
0.000 |
-36.346 |
|
| Traceless |
| | x | y | z |
| x |
3.942 |
0.267 |
0.000 |
| y |
0.267 |
-1.770 |
0.000 |
| z |
0.000 |
0.000 |
-2.172 |
|
| Polar |
| 3z2-r2 | -4.344 |
| x2-y2 | 3.808 |
| xy | 0.267 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.342 |
0.158 |
0.000 |
| y |
0.158 |
6.593 |
0.000 |
| z |
0.000 |
0.000 |
8.796 |
<r2> (average value of r
2) Å
2
| <r2> |
128.687 |
| (<r2>)1/2 |
11.344 |