Abstract

Modern requirements to the quality of materials entail the necessity of refining methods for their control and developing various procedures for analysis of the state of the surface with the goal of having defect-free structures for high-precision instruments and devices. Gas-discharge visualization of the defects at atmospheric pressure consists in obtaining bright plasma formations in the vicinity of the surface with a defect against the background of a weak glow of the air plasma in electromagnetic fields of high strength. The potentialities of plasma technologies regarding testing the surfaces of solid materials for various kinds of defects using a self-sustained dielectric barrier discharge (DBD) at atmospheric pressure are considered. The developed rapid technique provides quick rejection of defective materials or samples prior to their technological use. A set of diagnostic tools and auxiliary equipment has been developed to visualize the mechanical defects of different origin and evaluate the quality of raw materials. A number of important issues are considered when controlling the quality of high-grade surfaces, transparent and opaque materials, including metal surfaces. The special attention is paid to the search for defects in the structural elements of industrial equipment and determination of the degree of moisture of fibrous structures, for example, woven materials.

Highlights

  • Ñîâðåìåííûå òðåáîâàíèÿ ê êà÷åñòâó ìàòåðèàëîâ òðåáóþò ñîâåðøåíñòâîâàíèÿ ñïîñîáîâ êîíòðîëÿ è ðàçðàáîòêè ìåòîäîâ àíàëèçà ñîñòîÿíèÿ èõ ïîâåðõíîñòåé

  • Ãàçîðàçðÿäíàÿ âèçóàëèçàöèÿ äåôåêòîâ ïðè àòìîñôåðíîì äàâëåíèè çàêëþ÷àåòñÿ â ïîëó÷åíèè ÿðêèõ ïëàçìåííûõ îáðàçîâàíèé â íåïîñðåäñòâåííîé áëèçîñòè îò ïîâåðõíîñòè îáúåêòà ñ äåôåêòîì íà ôîíå ñëàáîãî ñâå÷åíèÿ ïëàçìû âîçäóõà â ýëåêòðîìàãíèòíûõ ïîëÿõ âûñîêîé íàïðÿæåííîñòè

  • Gas-discharge visualization of the defects at atmospheric pressure consists in obtaining bright plasma formations in the vicinity of the surface with a defect against the background of a weak glow of the air plasma in electromagnetic fields of high strength

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Summary

Introduction

Ñîâðåìåííûå òðåáîâàíèÿ ê êà÷åñòâó ìàòåðèàëîâ òðåáóþò ñîâåðøåíñòâîâàíèÿ ñïîñîáîâ êîíòðîëÿ è ðàçðàáîòêè ìåòîäîâ àíàëèçà ñîñòîÿíèÿ èõ ïîâåðõíîñòåé. Öåëü ðàáîòû — îïòèìèçàöèÿ ðåæèìîâ âîçáóæäåíèÿ ñàìîñòîÿòåëüíîãî äèýëåêòðè÷åñêîãî áàðüåðíîãî ðàçðÿäà (ÄÁÐ) ïðè àòìîñôåðíîì äàâëåíèè äëÿ àíàëèçà ñîñòîÿíèÿ ïîâåðõíîñòè òâåðäûõ ìàòåðèàëîâ, âêëþ÷àÿ èññëåäîâàíèå îñîáåííîñòåé ïëàçìåííîé âèçóàëèçàöèè äåôåêòîâ íà ïîâåðõíîñòÿõ ìåòàëëè÷åñêèõ èçäåëèé, êîíñòðóêöèîííûõ ýëåìåíòîâ ïðîìûøëåííûõ óñòàíîâîê è îöåíêó ñòåïåíè óâëàæíåííîñòè âîëîêíèñòûõ ñòðóêòóð (íà ïðèìåðå òêàíûõ ìàòåðèàëîâ).

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