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

using model chemistry: B1B95/6-31+G**

19 10 17 12 22

States and conformations

State Conformation minimum conformation conformer description state description
1 1 yes D2H 1Ag
Energy calculated at B1B95/6-31+G**
 hartrees
Energy at 0K-228.930865
Energy at 298.15K-228.936529
Nuclear repulsion energy131.347104
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 B1B95/6-31+G**
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 3045 2913 0.00      
2 Ag 1587 1519 0.00      
3 Ag 1151 1101 0.00      
4 Ag 882 844 0.00      
5 Au 1137 1088 0.00      
6 B1g 1354 1296 0.00      
7 B1g 1049 1003 0.00      
8 B1u 3092 2958 124.95      
9 B1u 1181 1130 18.05      
10 B1u 135 129 16.41      
11 B2g 3089 2955 0.00      
12 B2g 1130 1081 0.00      
13 B2u 1450 1387 25.20      
14 B2u 988 945 118.47      
15 B3g 1073 1027 0.00      
16 B3u 3031 2899 209.87      
17 B3u 1553 1485 15.92      
18 B3u 1124 1075 265.70      

Unscaled Zero Point Vibrational Energy (zpe) 14025.2 cm-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 13416.5 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 B1B95/6-31+G**
ABC
0.46294 0.45259 0.25132

See section I.F.4 to change rotational constant units
Geometric Data calculated at B1B95/6-31+G**

Point Group is D2h

Cartesians (Å)
Atom x (Å) y (Å) z (Å)
C1 -0.976 0.000 0.000
C2 0.976 0.000 0.000
O3 0.000 1.030 0.000
O4 0.000 -1.030 0.000
H5 -1.596 0.000 0.904
H6 1.596 0.000 0.904
H7 -1.596 0.000 -0.904
H8 1.596 0.000 -0.904

Atom - Atom Distances (Å)
  C1 C2 O3 O4 H5 H6 H7 H8
C11.95141.41901.41901.09632.72631.09632.7263
C21.95141.41901.41902.72631.09632.72631.0963
O31.41901.41902.06052.10402.10402.10402.1040
O41.41901.41902.06052.10402.10402.10402.1040
H51.09632.72632.10402.10403.19291.80733.6689
H62.72631.09632.10402.10403.19293.66891.8073
H71.09632.72632.10402.10401.80733.66893.1929
H82.72631.09632.10402.10403.66891.80733.1929

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 86.884 C1 O4 C2 86.884
O3 C1 O4 93.116 O3 C1 H5 112.912
O3 C1 H7 112.912 O3 C2 O4 93.116
O3 C2 H6 112.912 O3 C2 H8 112.912
O4 C1 H5 112.912 O4 C1 H7 112.912
O4 C2 H6 112.912 O4 C2 H8 112.912
H5 C1 H7 111.030 H6 C2 H8 111.030
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31+G** Charges (e)
Number Element Mulliken CHELPG AIM ESP
1 C 0.140      
2 C 0.140      
3 O -0.424      
4 O -0.424      
5 H 0.142      
6 H 0.142      
7 H 0.142      
8 H 0.142      


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 -18.708 0.000 0.000
y 0.000 -29.343 0.000
z 0.000 0.000 -22.937
Traceless
 xyz
x 7.432 0.000 0.000
y 0.000 -8.520 0.000
z 0.000 0.000 1.088
Polar
3z2-r22.177
x2-y210.635
xy0.000
xz0.000
yz0.000


Polarizabilities
Components of the polarizability tensor.
Units are Å3 (Angstrom cubed)
Change units.
  x y z
x 5.277 0.000 0.000
y 0.000 3.655 0.000
z 0.000 0.000 4.033


<r2> (average value of r2) Å2
<r2> 56.647
(<r2>)1/2 7.526