Abstract
The use of quantitative X-ray texture analysis (QXRTA) (construction of the orientation distribution function (ODF) proceeding from the measurement of direct pole figures) and simulation of the texture formation in the framework of thermoactivation model (TA) are considered to study the features of texture formation in MA2-1pch magnesium alloy subjected to rotary swaging (RS) at 400 – 350°C. A diffuse texture consisting of basic and inclined to the pressing direction basic poles is formed in the alloy when temperature decreases and the total true deformations increase up to ε = 2.77. Model textures match experimental textures rather well when RS is provided by the action of basic ({0001} á1120), prismatic ({1010} á1120ñ) slip and twinning by the systems {1012} á1011ñ, {1011} á1012ñ, {1121} á1126ñ. Mathematical modeling of the textures also shows that the activity of the twinning systems under consideration increases in the sequence {1012} á1011ñ, {1011} á1012ñ, {1121} á1126ñ as the total deformations grow and RS temperature decreases. Those results are consistent with the previously obtained microstructural data. However, the differences in the orientation factors calculated for the initial state of the alloy and state after RS indicated to the activation of the basal slip and twinning systems under consideration, as well as to the difficulty of prismatic sliding. The obtained data are also consistent with the results of mathematical modeling of textures. At a temperature of 350°C at a total true deformation of 2.77 the basic deformation mechanisms (the basic slip and twinning by the systems {1012} á1011ñ, {1011} á1012ñ, {1121} á1126ñ) which ensure texture changes upon RS stimulate an enhance in the mechanical properties of magnesium alloy MA2-1pch bars.
Highlights
ÈÑÑËÅÄÎÂÀÍÈÅ ÒÅÊÑÒÓÐÛ È ÌÅÕÀÍÈÇÌÎÂ ÄÅÔÎÐÌÀÖÈÈ Â ÌÀÃÍÈÅÂÎÌ ÑÏËÀÂÅ ÌÀ2-1ï÷ Â ÏÐÎÖÅÑÑÅ ÐÎÒÀÖÈÎÍÍÎÉ ÊÎÂÊÈ
Ðåçóëüòàòû ìîäåëèðîâàíèÿ òåêñòóð â ðàìêàõ òåðìîàêòèâàöèîííîé ìîäåëè è àíàëèç îðèåíòàöèîííûõ ôàêòîðîâ äåéñòâóþùèõ ñèñòåì äåôîðìàöèè ñâèäåòåëüñòâóþò, ÷òî òàêîå èçìåíåíèå òåêñòóðû âûçâàíî àêòèâèçàöèåé áàçèñíîãî ñêîëüæåíèÿ è ðÿäà ñèñòåì äâîéíèêîâàíèÿ è çàòðóäíåííîñòüþ äåéñòâèÿ ïðèçìàòè÷åñêîãî ñêîëüæåíèÿ
Summary
ÈÑÑËÅÄÎÂÀÍÈÅ ÒÅÊÑÒÓÐÛ È ÌÅÕÀÍÈÇÌΠÄÅÔÎÐÌÀÖÈÈ Â ÌÀÃÍÈÅÂÎÌ ÑÏËÀÂÅ ÌÀ2-1ï÷  ÏÐÎÖÅÑÑÅ ÐÎÒÀÖÈÎÍÍÎÉ ÊÎÂÊÈ. Ìîäåëüíûå òåêñòóðû õîðîøî ñîãëàñóþòñÿ ñ ýêñïåðèìåíòàëüíûìè ïðè óñëîâèè, ÷òî ÐÊ îáåñïå÷èâàåòñÿ äåéñòâèåì áàçèñíîãî ({0001}á1120ñ), ïðèçìàòè÷åñêîãî ({1010} á1120ñ) ñêîëüæåíèé è äâîéíèêîâàíèÿ ïî ñèñòåìàì {1012} á1011ñ, {1011} á1012ñ, {1121} á1126. Âìåñòå ñ òåì â ïðîöåññå ÐÊ â ñïëàâàõ ïðîèñõîäèò çàìåòíîå èçìåíåíèå òåêñòóðû, õàðàêòåðèçóþùååñÿ ðàâíîìåðíûì ñïåêòðîì îðèåíòèðîâîê îò áàçèñíûõ äî ïðèçìàòè÷åñêèõ, à òàêæå ðàññåÿíèåì îñíîâíûõ îðèåíòèðîâîê âñëåäñòâèå ôðàãìåíòàöèè çåðåí èç-çà äâîéíèêîâàíèÿ [4 – 7], ÷òî ïðè îïðåäåëåííûõ ðåæèìàõ òåìïåðàòóðû è ñòåïåíè äåôîðìàöèè ñïîñîáñòâóåò ïîâûøåíèþ èõ ïëàñòè÷íîñòè [5]. Ïðåäïîëàãàëè, ÷òî ïëàñòè÷åñêàÿ äåôîðìàöèÿ ñïëàâà â èññëåäóåìûõ èíòåðâàëàõ òåìïåðàòóð è äåôîðìàöèé îáåñïå÷èâàåòñÿ äåéñòâèåì áàçèñíîãî ({0001} á1120ñ), ïðèçìàòè÷åñêîãî ({1010} á1120ñ) ñêîëüæåíèé è äâîéíèêîâàíèÿ ïî ñèñòåìàì {1012} á1011ñ, {1011} á1012ñ, {1121} á1126ñ [5, 6] ñ ñîîòíîøåíèåì êðèòè÷åñêèõ íàïðÿæåíèé ñäâèãà (ÊÍÑ), îïðåäåëÿåìûõ èç ñîïîñòàâëåíèÿ ýêñïåðèìåíòàëüíûõ è ðàñ÷åòíûõ ïîëþñíûõ ôèãóð è ÔÐÎ. Ãäå äåéñòâóþò ñèñòåìû äâîéíèêîâàíèÿ âìåñòå ñ ñèñòåìàìè ñêîëüæåíèÿ (çåðíà, ñîäåðæàùèå äâîéíèêè), îöåíèâàëè èç àíàëèçà ìèêðî-
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