Hrehuš, Rudolf

Jurík, R.

Jurčiová, Jana

Koštial, Pavol

Vretenár, V.

English

DSpace at VSB Technical University of Ostrava

LI. IN L 11Sborník vědeckých prací Vysoké školy báňské - Technické univerzity Ostrava číslo 1, rok 2009, ročník LIi, řada hutnická článek č. 1433 ALTERNATIVE CURRENT RESISTMTY OF RUBBER BLENDS WITH SINGLE W ALL CARBON NANOTUBES Š 1• Šl ' I Č '2 ' 3 P. KO TIAL ,R. HREHU , R. JURIK ,J. J U R  IOVA, V. V RETENAR 1 Faculty of lndustrial Technologies, Department of Physica/ Engineering of Materials, Alexander Dub&k University of Trenl{n; Púchov, Slovak RepubUc, contact author: kostial@fpt.tnuni.sk 1 Faculty of lndustrial Technologies, Department of Chemistry and Technology of Polymers, AlexanderDub&k University of Trenl{n; Púchov, Slovak Republic,jurcwva@fpt.tnuni.sk 1 -Danubia NanoTech, Ltd.; Bratislava, S/ovak Republic, vretenar@danubiananotech.comABSTRACT: In this paper we present the study of alternating current resistivity ACR, a dielectric constant and the loss factor tg<p of rub ber blends filled by single wall carbon nanotubes (SWCNI). The presence of SWCNT in the blend rises both parts of the complex dielectric constant, as we}l as the loss &ctor. On the other hand A CR decreases. KEY WORDS: electrical properties, rubber 1. INTRODUCTIONMaterial basis of fillers was being created for a long time by carbon black and later silica with silanes. We are standing before a new challenge in rubber industry created by the application of carbon nanotubes to a rubber blend. The process of a carbon black mixing is assumed in the following steps. After the addition of the filler, the agglomerates of the size up to 10-100 µm are created. The rubber shells are created around tbc filler particles in the blend, followed by filling up the voids within the filler agglomerates. Under stretching deformation caused by shearing forces, the aggregates of JOO nm till 0.5 µm appear a fter brcakage of agglomerates. Primary particles as a final product of mixing have dimension of approximately 20 nm. Smaller aggregates and primary particles appear on the expense of larger aggregates and agglomerates [1,2]. There is incomparably worse situation in the field of knowledge about dispersion process of CNT.The problem in the case of CNT application to the rubber blend lies in a destruction of agglomerates before mixing and the following incorporation of CNT in the period of mastication_ and plasticization in order to obtain good electrical, mechanical and thermal properties of the final blend. Information ISSembled on these processes are relatively poor. Authors of the European patent [3] described the realization of cables comprising polyethylene, Polypropylene, or mixture thereof, CNT, conductiv� carbon, copolymer of acrylonitrile and butadiene. In this paper, we present the resúlts of nieasurements of ACR, a dielectric constant and the loss tictor tg<p as functions of frequency for sample twins. Two mother samples of a rubber blend were Ptepared as twins. One with and the second one without SWCNT (marked as standard S).2. EXPERIMENTAL PROCEDURETwo mother samples of a rubber blend were prepared as twins. One was with and the second one Without SWCNT. Rubber blends were mixed in two steps. In the first step, we started with mixing of Datural rubber, then we successively added ZnO, carbon black (N660 Cabot) and finally we sonicated 39 

Alternative current resistivity of rubber blends with single wall carbon nanotubes

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Alternative current resistivity of rubber blends with single wall carbon nanotubes

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