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All results from a given calculation for C2H4O2 (1,3-dioxetane)

using model chemistry: HF/6-31G(2df,p)

19 10 17 12 22

States and conformations

State Conformation minimum conformation conformer description state description
1 1 yes D2H 1Ag
Energy calculated at HF/6-31G(2df,p)
 hartrees
Energy at 0K-227.754919
Energy at 298.15K-227.760827
Nuclear repulsion energy132.910924
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 HF/6-31G(2df,p)
Mode Number Symmetry Frequency
(cm-1)
Scaled Frequency
(cm-1)
IR Intensities
(km mol-1)
Raman Act
4/u)
Dep P Dep U
1 Ag 3182 2882 0.00      
2 Ag 1720 1557 0.00      
3 Ag 1239 1122 0.00      
4 Ag 987 893 0.00      
5 Au 1238 1121 0.00      
6 B1g 1477 1337 0.00      
7 B1g 1109 1004 0.00      
8 B1u 3226 2921 153.88      
9 B1u 1291 1169 29.42      
10 B1u 210 190 17.53      
11 B2g 3220 2916 0.00      
12 B2g 1224 1108 0.00      
13 B2u 1593 1443 35.00      
14 B2u 1080 978 128.62      
15 B3g 1210 1096 0.00      
16 B3u 3166 2866 212.10      
17 B3u 1681 1522 22.88      
18 B3u 1212 1097 308.02      

Unscaled Zero Point Vibrational Energy (zpe) 15032.0 cm-1
Scaled (by 0.9055) Zero Point Vibrational Energy (zpe) 13611.5 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.
Rotational Constants (cm-1) from geometry optimized at HF/6-31G(2df,p)
ABC
0.46971 0.46802 0.25744

See section I.F.4 to change rotational constant units
Geometric Data calculated at HF/6-31G(2df,p)

Point Group is D2h

Cartesians (Å)
Atom x (Å) y (Å) z (Å)
C1 -0.969 0.000 0.000
C2 0.969 0.000 0.000
O3 0.000 1.013 0.000
O4 0.000 -1.013 0.000
H5 -1.587 0.000 0.893
H6 1.587 0.000 0.893
H7 -1.587 0.000 -0.893
H8 1.587 0.000 -0.893

Atom - Atom Distances (Å)
  C1 C2 O3 O4 H5 H6 H7 H8
C11.93731.40141.40141.08622.70741.08622.7074
C21.93731.40141.40142.70741.08622.70741.0862
O31.40141.40142.02532.08372.08372.08372.0837
O41.40141.40142.02532.08372.08372.08372.0837
H51.08622.70742.08372.08373.17451.78573.6422
H62.70741.08622.08372.08373.17453.64221.7857
H71.08622.70742.08372.08371.78573.64223.1745
H82.70741.08622.08372.08373.64221.78573.1745

picture of 1,3-dioxetane state 1 conformation 1
More geometry information
Calculated Bond Angles
atom1 atom2 atom3 angle atom1 atom2 atom3 angle
C1 O3 C2 87.456 C1 O4 C2 87.456
O3 C1 O4 92.544 O3 C1 H5 113.182
O3 C1 H7 113.182 O3 C2 O4 92.544
O3 C2 H6 113.182 O3 C2 H8 113.182
O4 C1 H5 113.182 O4 C1 H7 113.182
O4 C2 H6 113.182 O4 C2 H8 113.182
H5 C1 H7 110.572 H6 C2 H8 110.572
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31G(2df,p) Charges (e)
Number Element Mulliken CHELPG AIM ESP
1 C 0.198      
2 C 0.198      
3 O -0.459      
4 O -0.459      
5 H 0.131      
6 H 0.131      
7 H 0.131      
8 H 0.131      


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 0.000 0.000
CHELPG        
AIM        
ESP        


Electric Quadrupole moment
Quadrupole components in D Å
Primitive
 xyz
x -18.462 0.000 0.000
y 0.000 -28.448 0.000
z 0.000 0.000 -22.527
Traceless
 xyz
x 7.025 0.000 0.000
y 0.000 -7.953 0.000
z 0.000 0.000 0.928
Polar
3z2-r21.856
x2-y29.986
xy0.000
xz0.000
yz0.000


Polarizabilities
Components of the polarizability tensor.
Units are Å3 (Angstrom cubed)
Change units.
  x y z
x 4.776 0.000 0.000
y 0.000 3.007 0.000
z 0.000 0.000 3.596


<r2> (average value of r2) Å2
<r2> 55.390
(<r2>)1/2 7.442