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Application of PALS to Study Structure of Elastomers

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Katarzyna

Bandzierz: Applicątion

of PALS

to

Study

Structure

of

Elastomers

K.

Bandzierzt'*, J.

Kleczewskal, L.

Reuvekamp2, J.

Dryzek',

E. Dryzek3, W. Dierkes2,

D.

M.

Bieli

skil

and

A.

Blume2

1lnstitute of Polymer and Dye

kchnology,

Ł

University of Technology, Stefanowskiego 12/16, 90-924

Ł

dź,

Poland

'Elastomer

kchnology

&

Engineering, University of TWente,

Drienerlolaan

5, 7500

AE

Enschede, The Netherlands

3Institute of

Nuclear

Physics, Polish Academy of Science, Radzikowskiego 752, 31-342

Krak

w,

Poland

email : katarzyna. bandzi erz@ gmail. com

Crosslink density, defined as a number of network chains per cubic centimeter of a sample, describes a three-dimensional structure of elastomers. Due to the fact that the crosslink density influences to a high extent numerous properties of elastomers, its comprehension and

determinability is fundamental. Hereunder, the structure and packing of macromolecular chains, and the number and length of crosslinks between them, influence the size of free volumes. However, the structure of elastomers can be highly complicated, due to complexity of reactions

which

occur

during high-temperature curing process. Precise characterization of structure of crosslinked

elastomer systems

still

remains challenging.

A

powerful technique, which can serve to investigate the microstructure of polymeric materials is Positron

Annihilation Lifetime

Spectroscopy

(PALS).

The subject of the study were sets of samples on the matrix of styrene-butadiene rubber (SBR),

crosslinked with use of three types of curing systems

-

dicumyl peroxide

(DCP), zinc

dialkyldithiophosphate in combination with rhombic sulphur (ZDT/S8), and

N-cyclohexyl-1-benzothiazole sulfenamide with rhombic sulphur (CBS/SB), differing significantly in the length and structure of crosslinks, but similar according to crosslink density. The room temperature

PALS

studies were employed to provide information on the free volumes, which were correlated with crosslink density, determined with use of equilibrium swelling in toluene and calculated on the basis of Flory*Rehner equation. The lifetime of o-Ps as a function of crosslink density exhibits in general

a downward trend. For

DCP

cured samples, the shortening of o-Ps lifetime is very little, whereas for CBS/Ss and

ZDTlSs,

the rE value considerably drops with increase in crosslink density. However, the r: values are scattered and cannot be directly assigned to the formation of crosslinks and more dense packing. The intensity of the rs cofirponent, i.e., 13 decreases with increasing crosslink density, indicating on reduction of free volumes fraction. The change of Is value is very

little

for peroxide

cured samples, in contrary to CBS/Ss and ZDTlSa. It demonstrates that the obtained data are strongly dependent on the type of curing system used

-

particular types of molecules, such as

rhombic sulphur and/or accelerators, present in the elastomer matrix. They can

significantly

influence, by

inhibition

or quenching, formation of o-Ps.

These studies reveal that the obtained values from

PALS

for crosslinked elastomers, due to various possible types and amounts of curatives incorporated into the polymer matrix, cannot be always directly correlated with crosslink density, what is often overlooked in scientific publications.

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