Jie-Yu Yang (Shirley)
About
My research project
Evaluating residual stress for manufacturing optimisation in advanced TiC-graphene hybrid reinforced Al matrix composites (AMCs)This project aims to design, manufacture, characterise and optimise the TiC/GNPs hybrid-reinforced AMCs. To achieve the desired outcome, the following objectives are identified:
(i) To design and manufacture the AMCs at different TiC-to-GNPs ratios.
(ii) To evaluate the residual stress distribution and establish correlative analysis with microstructures and compressive properties to reveal underpinning strengthening and deformation mechanisms.
Supervisors
This project aims to design, manufacture, characterise and optimise the TiC/GNPs hybrid-reinforced AMCs. To achieve the desired outcome, the following objectives are identified:
(i) To design and manufacture the AMCs at different TiC-to-GNPs ratios.
(ii) To evaluate the residual stress distribution and establish correlative analysis with microstructures and compressive properties to reveal underpinning strengthening and deformation mechanisms.
University roles and responsibilities
- PhD student
ResearchResearch interests
- Material Science
- Powder metallurgy
- Diffraction-based technique
Research interests
- Material Science
- Powder metallurgy
- Diffraction-based technique
Publications
Pinning phenomena were investigated in the superconducting Nb thin film with composite hexagonal arrays. The composite pinning arrays were consisting of two kinds of pinning sites with different pinning sizes. The smaller pinning defects were added to the center of every honeycomb pinning array to observe the configuration of the vortices, comparing to the periodic triangular and honeycomb arrays. The film with this kind of composite array can be regarded as a transition between the films with triangular array and honeycomb array. The critical current as a function of magnetic field for four samples were measured. Regular 150 Oe interval of the matching fields for the triangular arrays was found, while for the honeycomb arrays, the interstitial vortices were caged at the center of every honeycomb array, causing 50 Oe interval of the matching fields. For the samples with composite arrays, the 100 Oe or 50 Oe intervals of matching fields correspond to every larger or smaller pinning site capturing one more vortex, respectively. We found that the relative pinning strength of the large pinning sites is greater than that of the small ones. We conducted the simulations based on the time dependent Ginzburg-Landau theory to confirm that the interstitial vortices did exist in the honeycomb arrays which caused the various intervals between the matching fields.
The exact superconducting phase of K2−xFe4+ySe5 has so far not been conclusively decided since its discovery due to its intrinsic multiphase in early material. In an attempt to resolve this mystery, we have carried out systematic structural studies on a set of well-controlled samples with exact chemical stoichiometry K2−xFe4+xSe5 (x = 0–0.3) that are heat-treated at different temperatures. Using high-resolution synchrotron radiation X-ray diffraction, our investigations have determined the superconducting transition by focusing on the detailed temperature evolution of the crystalline phases. Our results show that superconductivity appears only in those samples that have been treated at high-enough temperature and then quenched to room temperature. The volume fraction of superconducting transition strongly depends on the annealing temperature used. The most striking result is the observation of a clear contrast in crystalline phase between the nonsuperconducting parent compound K2Fe4Se5 and the superconducting K2−xFe4+ySe5 samples. The X-ray diffraction patterned can be well indexed to the phase with I4/m symmetry in all temperatures investigated. However, we need two phases with similar I4/m symmetry but different parameters to best fit the data at a temperature below the Fe vacancy order temperature. The results strongly suggest that superconductivity in K2−xFe4+ySe5 critically depends on the occupation of Fe atoms on the originally empty 4d site.