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)
An error occurred on the server when processing the URL. Please contact the system administrator.
If you are the system administrator please click
here to find out more about this error.