56 research outputs found

    Structure and diffusion processes in laminated composites of a Cu-Ti system

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    Characteristics of diffusion transformations in a multi-layer composite of a Cu-Ti system, which was produced by high-temperature diffusion welding followed by rolling at room temperature, are reportedye

    Взаимная диффузия Π² систСмах Π½Π° основС Ρ‚ΡƒΠ³ΠΎΠΏΠ»Π°Π²ΠΊΠΈΡ… ΠΌΠ΅Ρ‚Π°Π»Π»ΠΎΠ² с ОЦК-Ρ€Π΅ΡˆΠ΅Ρ‚ΠΊΠΎΠΉ: титан–тантал ΠΈ Ρ‚ΠΈΡ‚Π°Π½ – ΠΌΠ½ΠΎΠ³ΠΎΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½Ρ‚Π½Ρ‹ΠΉ (высокоэнтропийный) сплав

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    In this work, the interdiffusion features in multicomponent (high-entropy) alloys of refractory metals were studied. The following pairs were chosen as the diffusion study objects: titanium–equiatomic alloy (Hf–Nb–Ta–Ti–Zr–Mo) and titanium–tantalum for the sake of comparison. The article covers the issues of sample preparation, microstructure study, sample preparation methodology for diffusion research, and experimental results. Diffusion annealing was carried out for 12 h in a vacuum at a residual argon pressure of 6.65Β·10–3 Pa and a temperature of 1200 Β°Π‘. Particular attention was paid to the method of combining diffusion pairs (titanium with tantalum, titanium with alloy) by thermal cycling near the polymorphic transformation temperature in titanium (882 Β°C) within Β± 50 Β°C. The behaviour of the most characteristic elements (Ta, Zr, Ti) in the weld area after the titanium and alloy diffusion pair joining was demonstrated. This is the first time that data on the dependence of the intensity of the corresponding spectral line for titanium and elements of a multicomponent alloy on the penetration depth were obtained. A change in the signal intensity for system elements was observed at a depth of 150–200 ΞΌm, whereas a sharp drop in the signal intensity was seen to occur at depths of about 50 ΞΌm. The effective value of the coefficient of diffusion of elements into titanium averaged over all elements of the alloying system (except for titanium) at a temperature of 1200 Β°C was calculated. The obtained value was compared to reference data: the self-diffusion coefficient in Ξ²-titanium and diffusion coefficients in titanium pairs with alloy doping elements.Π˜Π·ΡƒΡ‡Π΅Π½Ρ‹ особСнности Π²Π·Π°ΠΈΠΌΠ½ΠΎΠΉ Π΄ΠΈΡ„Ρ„ΡƒΠ·ΠΈΠΈ Π² ΠΌΠ½ΠΎΠ³ΠΎΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½Ρ‚Π½Ρ‹Ρ… (высокоэнтропийных) сплавах Π½Π° основС Ρ‚ΡƒΠ³ΠΎΠΏΠ»Π°Π²ΠΊΠΈΡ… ΠΌΠ΅Ρ‚Π°Π»Π»ΠΎΠ². Π’ качСствС ΠΎΠ±ΡŠΠ΅ΠΊΡ‚ΠΎΠ² Π΄ΠΈΡ„Ρ„ΡƒΠ·ΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ исслСдования Π±Ρ‹Π»ΠΈ Π²Ρ‹Π±Ρ€Π°Π½Ρ‹ ΡΠ»Π΅Π΄ΡƒΡŽΡ‰ΠΈΠ΅ ΠΏΠ°Ρ€Ρ‹: Ρ‚ΠΈΡ‚Π°Π½ – эквиатомный сплав (Hf–Nb–Ta–Ti–Zr–Mo) ΠΈ, для сравнСния, титан–тантал. РассмотрСны вопросы приготовлСния ΠΎΠ±Ρ€Π°Π·Ρ†ΠΎΠ², исслСдования микроструктуры, ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΈΠΊΠ° ΠΏΠΎΠ΄Π³ΠΎΡ‚ΠΎΠ²ΠΊΠΈ ΠΎΠ±Ρ€Π°Π·Ρ†ΠΎΠ² для изучСния Π΄ΠΈΡ„Ρ„ΡƒΠ·ΠΈΠΈ ΠΈ ΡΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Ρ‹Π΅ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹. Π”ΠΈΡ„Ρ„ΡƒΠ·ΠΈΠΎΠ½Π½Ρ‹ΠΉ ΠΎΡ‚ΠΆΠΈΠ³ Π±Ρ‹Π» ΠΏΡ€ΠΎΠ²Π΅Π΄Π΅Π½ Π² Ρ‚Π΅Ρ‡Π΅Π½ΠΈΠ΅ 12 Ρ‡ Π² Π²Π°ΠΊΡƒΡƒΠΌΠ΅ с остаточным Π΄Π°Π²Π»Π΅Π½ΠΈΠ΅ΠΌ Π°Ρ€Π³ΠΎΠ½Π° 6,65Β·10–3 Па ΠΏΡ€ΠΈ Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Π΅ 1200 Β°Π‘. ОсобоС Π²Π½ΠΈΠΌΠ°Π½ΠΈΠ΅ ΡƒΠ΄Π΅Π»Π΅Π½ΠΎ ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΈΠΊΠ΅ соСдинСния Π΄ΠΈΡ„Ρ„ΡƒΠ·ΠΈΠΎΠ½Π½Ρ‹Ρ… ΠΏΠ°Ρ€ (Ρ‚ΠΈΡ‚Π°Π½Π° с Ρ‚Π°Π½Ρ‚Π°Π»ΠΎΠΌ, Ρ‚ΠΈΡ‚Π°Π½Π° со сплавом) ΠΏΡƒΡ‚Π΅ΠΌ тСрмоциклирования Π²Π±Π»ΠΈΠ·ΠΈ Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Ρ‹ ΠΏΠΎΠ»ΠΈΠΌΠΎΡ€Ρ„Π½ΠΎΠ³ΠΎ прСвращСния Π² Ρ‚ΠΈΡ‚Π°Π½Π΅ (882 Β°Π‘) Π² ΠΏΡ€Π΅Π΄Π΅Π»Π°Ρ… Β±50 Β°Π‘. Показано ΠΏΠΎΠ²Π΅Π΄Π΅Π½ΠΈΠ΅ Π½Π°ΠΈΠ±ΠΎΠ»Π΅Π΅ Ρ…Π°Ρ€Π°ΠΊΡ‚Π΅Ρ€Π½Ρ‹Ρ… элСмСнтов (Ta, Zr, Ti) Π² области сварного шва послС соСдинСния Π΄ΠΈΡ„Ρ„ΡƒΠ·ΠΈΠΎΠ½Π½ΠΎΠΉ ΠΏΠ°Ρ€Ρ‹ Ρ‚ΠΈΡ‚Π°Π½Π° ΠΈ сплава. Π’ΠΏΠ΅Ρ€Π²Ρ‹Π΅ ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Ρ‹ Π΄Π°Π½Π½Ρ‹Π΅ ΠΎ зависимости интСнсивности ΡΠΎΠΎΡ‚Π²Π΅Ρ‚ΡΡ‚Π²ΡƒΡŽΡ‰Π΅ΠΉ Π»ΠΈΠ½ΠΈΠΈ спСктра для Ρ‚ΠΈΡ‚Π°Π½Π° ΠΈ элСмСнтов ΠΌΠ½ΠΎΠ³ΠΎΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½Ρ‚Π½ΠΎΠ³ΠΎ сплава ΠΎΡ‚ Π³Π»ΡƒΠ±ΠΈΠ½Ρ‹ проникновСния. ИзмСнСниС интСнсивности сигнала для элСмСнтов систСм Π½Π°Π±Π»ΡŽΠ΄Π°Π΅Ρ‚ΡΡ Π½Π° Π³Π»ΡƒΠ±ΠΈΠ½Π΅ 150–200 ΠΌΠΊΠΌ, Π° Ρ€Π΅Π·ΠΊΠΎΠ΅ ΠΏΠ°Π΄Π΅Π½ΠΈΠ΅ интСнсивности сигнала происходит Π½Π° Π³Π»ΡƒΠ±ΠΈΠ½Π°Ρ… порядка 50 ΠΌΠΊΠΌ. Рассчитано усрСднСнноС ΠΏΠΎ всСм элСмСнтам систСмы лСгирования сплава (Π·Π° ΠΈΡΠΊΠ»ΡŽΡ‡Π΅Π½ΠΈΠ΅ΠΌ Ρ‚ΠΈΡ‚Π°Π½Π°) эффСктивноС Π·Π½Π°Ρ‡Π΅Π½ΠΈΠ΅ коэффициСнта Π΄ΠΈΡ„Ρ„ΡƒΠ·ΠΈΠΈ элСмСнтов Π² Ρ‚ΠΈΡ‚Π°Π½ ΠΏΡ€ΠΈ Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Π΅ 1200 Β°Π‘. ΠŸΡ€ΠΎΠ²Π΅Π΄Π΅Π½ΠΎ сравнСниС ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Π½ΠΎΠ³ΠΎ значСния со справочными Π΄Π°Π½Π½Ρ‹ΠΌΠΈ: коэффициСнтом самодиффузии Π² Ξ²-Ρ‚ΠΈΡ‚Π°Π½Π΅, коэффициСнтами Π΄ΠΈΡ„Ρ„ΡƒΠ·ΠΈΠΈ Π² ΠΏΠ°Ρ€Π°Ρ… Ρ‚ΠΈΡ‚Π°Π½Π° с Π»Π΅Π³ΠΈΡ€ΡƒΡŽΡ‰ΠΈΠΌΠΈ элСмСнтами сплава

    Structure and diffusion processes in laminated composites of a Cu-Ti system

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    yesCharacteristics of diffusion transformations in a multi-layer composite of a Cu-Ti system, which was produced by high-temperature diffusion welding followed by rolling at room temperature, are reporte
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