
Yinxiang Ma
Articles
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Oct 31, 2024 |
pubs.aip.org | R. Pramanik |A-Man Zhang |Yinxiang Ma
When a shock wave crosses a density interface, the Richtmyer–Meshkov instability causes perturbations to grow. Richtmyer–Meshkov instabilities arise from the deposition of vorticity from the misaligned density and pressure gradients at the shock front. In many engineering applications, microscopic surface roughness will grow into multi-mode perturbations, inducing mixing between the fluid on either side of an initial interface.
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Oct 30, 2024 |
pubs.aip.org | R. Pramanik |A-Man Zhang |Yinxiang Ma
Oil-in-water (O/W) emulsions are widely used in industrial production, food science, petrochemicals, and other fields. Quantitative measurement of the interaction between droplets is essential for the in-depth understanding of the stability mechanism of O/W emulsions. Optical tweezers are able to accurately and quantitatively measure the interaction forces between droplets in oil-in-water emulsion systems at the microscopic scale and offer numerous advantages.
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Oct 28, 2024 |
pubs.aip.org | Shanghai Jiao Tong |Yinxiang Ma |A-Man Zhang |R. Pramanik
Acceleration of objects in fluids widely exists in biological propulsions and contains rich unsteady fluid mechanisms. In this paper, the instantaneous drag force on accelerating normal flat plates (circular, elliptical, square, and rectangular plates) in a wide range of dimensionless acceleration ( ) is measured, and the underlying mechanism for force generation is investigated.
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Oct 25, 2024 |
pubs.aip.org | Aerospace Engineering |Yinxiang Ma |A-Man Zhang |R. Pramanik
This experimental study investigates the fluid dynamic function of butterfly scales to reduce friction drag below that experienced in a laminar boundary layer. A previous study on flight-testing live monarch butterflies showed that the removal of the scales from the wings had a significant effect on reducing flying efficiency.
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Oct 18, 2024 |
pubs.aip.org | Yinxiang Ma |Zengshun Chen |A-Man Zhang |S. J. Kim
In a theoretical point of view, a stagnation flow is characterized by its viscous flow-like behavior due to its very low inertial contribution.53,54 The flow stagnation can be quantified by comparing the inertial term, ρa(u·∇u), and the viscous term, μa∇2u, in the Navier–Stokes equation, yielding the inertial-viscous ratio as where ρa is the air density, u is the flow velocity, and μa is the air viscosity.
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