{"title":"Allotropic α→β transformation in diffusion-graded commercial-purity Ti–Zr multilayers: DSC overlapping peak deconvolution and kissinger kinetic analysis","authors":"Anas Jawabreh, Péter Barkóczy","doi":"10.1016/j.jalmes.2026.100238","DOIUrl":null,"url":null,"abstract":"<div><div>Multilayered Ti–Zr mesostructures were produced from commercially pure Ti and Zr by subsequent hot compression and heat treatment then annealed at 740 °C and 770 °C for 120 h to generate a near-continuous Ti-rich to Zr-rich concentration gradient. Differential scanning calorimetry (DSC) was used to examine the α→β transformation at heating rates of 10–25 K/min, supported by optical microscopy and SEM–EDS to assess the extent of diffusion. The first endothermic reaction starts near the ∼50–50 at% Ti-Zr region where the transformation temperature is lowest according to the published and Thermo-calc calculated phase diagrams, while subsequent reactions occur in adjacent Ti- and Zr-rich compositions, producing strongly overlapping peaks in a small temperature range. The low-temperature peak ranges occur at 549.9 °C −562.1 °C and 570.4 °C −576.6 °C after 740 °C annealing, and at 543.5 °C −589.3 °C and 584.6 °C −645.3 °C after 770 °C annealing, followed by a high-temperature β-completion peak at 838 °C −867.6 °C (740 °C) or 915 °C −926.8 °C (770 °C). A Savitzky–Golay filtering, derivative-based segmentation, and Avrami-type deconvolution were used to isolate the overlapping reactions, and Kissinger analysis of the deconvoluted peaks provided apparent activation energies for each step. For the 740 °C samples, the first two low-temperature (onset) steps show higher apparent activation energies (225.7 and 474.7 kJ·mol⁻¹) than the β-completion step (163.145 kJ·mol⁻¹), while for the 770 °C samples the trend reverses (74.5 and 60.1 kJ·mol⁻¹ vs. 676.3 kJ·mol⁻¹). This change in trend indicates that diffusion heat treatment changes the gradient geometry, which controls peak overlap and shifts the apparent kinetics from deconvolution.</div></div>","PeriodicalId":100753,"journal":{"name":"Journal of Alloys and Metallurgical Systems","volume":"13 ","pages":"Article 100238"},"PeriodicalIF":0.0000,"publicationDate":"2026-03-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Alloys and Metallurgical Systems","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S2949917826000076","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"2026/2/17 0:00:00","PubModel":"Epub","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
Multilayered Ti–Zr mesostructures were produced from commercially pure Ti and Zr by subsequent hot compression and heat treatment then annealed at 740 °C and 770 °C for 120 h to generate a near-continuous Ti-rich to Zr-rich concentration gradient. Differential scanning calorimetry (DSC) was used to examine the α→β transformation at heating rates of 10–25 K/min, supported by optical microscopy and SEM–EDS to assess the extent of diffusion. The first endothermic reaction starts near the ∼50–50 at% Ti-Zr region where the transformation temperature is lowest according to the published and Thermo-calc calculated phase diagrams, while subsequent reactions occur in adjacent Ti- and Zr-rich compositions, producing strongly overlapping peaks in a small temperature range. The low-temperature peak ranges occur at 549.9 °C −562.1 °C and 570.4 °C −576.6 °C after 740 °C annealing, and at 543.5 °C −589.3 °C and 584.6 °C −645.3 °C after 770 °C annealing, followed by a high-temperature β-completion peak at 838 °C −867.6 °C (740 °C) or 915 °C −926.8 °C (770 °C). A Savitzky–Golay filtering, derivative-based segmentation, and Avrami-type deconvolution were used to isolate the overlapping reactions, and Kissinger analysis of the deconvoluted peaks provided apparent activation energies for each step. For the 740 °C samples, the first two low-temperature (onset) steps show higher apparent activation energies (225.7 and 474.7 kJ·mol⁻¹) than the β-completion step (163.145 kJ·mol⁻¹), while for the 770 °C samples the trend reverses (74.5 and 60.1 kJ·mol⁻¹ vs. 676.3 kJ·mol⁻¹). This change in trend indicates that diffusion heat treatment changes the gradient geometry, which controls peak overlap and shifts the apparent kinetics from deconvolution.