323 research outputs found

    Riesz-type inequalities and maximum flux exchange flow

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    Let DD stand for the open unit disc in Rd\mathbb{R}^d (d1d\geq 1) and (D,B,m)(D,\,\mathscr{B},\,m) for the usual Lebesgue measure space on DD. Let H\mathscr{H} stand for the real Hilbert space L2(D,m)L^2(D,\,m) with standard inner product (,)(\cdot,\,\cdot). The letter GG signifies the Green operator for the (non-negative) Dirichlet Laplacian Δ-\Delta in H\mathscr{H} and ψ\psi the torsion function GχDG\,\chi_D. We pose the following problem. Determine the optimisers for the shape optimisation problem αt:=sup{(GχA,χA):ADis open and(ψ,χA)t} \alpha_t:=\sup\Big\{(G\chi_A,\chi_A):\,A\subseteq D\text{is open and}(\psi,\chi_A)\leq t\,\Big\} where the parameter tt lies in the range 0<t<(ψ,1)0<t<(\psi,1). We answer this question in the one-dimensional case d=1d=1. We apply this to a problem connected to maximum flux exchange flow in a vertical duct. We also show existence of optimisers for a relaxed version of the above variational problem and derive some symmetry properties of the solutions

    An isoperimetric inequality in the plane with a log-convex density

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    Computation of flow behind three side-by-side cylinders of unequal/equal spacing

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    This paper aims to simulate unstable gap flows of three side-by-side cylinders unequally/equally spaced at T1/d = 1.5 and T2/d = 1.6 in a uniform cross flow (Re=300). The simulation is carried out using ANSYS Flotran 7.0. A mesh-independent study is conducted on a single cylinder at Re=100. The Strouhal number and wake flow characteristics compare well with experimental results. Simulation of three side-by-side cylinders in uniform cross flow has revealed that the gap flows are unstable and constantly re-orientating, which has the effect of restructuring the wake flows behind the cylinders. The flow field for unequal spacing of the cylinders is similar to the equal spacing case for some period of time with a symmetrical near wake. However, at other times, the wake flow is asymmetrical. This agrees well with the visualisation of Wang et al. (2002), in which the gap flows and the wake flow are constantly in transition

    Cellular interactions with polystyrene nanoplastics-The role of particle size and protein corona.

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    Plastic waste is ubiquitously spread across the world and its smaller analogs-microplastics and nanoplastics-raise particular health concerns. While biological impacts of microplastics and nanoplastics have been actively studied, the chemical and biological bases for the adverse effects are sought after. This work explores contributory factors by combining results from in vitro and model mammalian membrane experimentation to assess the outcome of cell/nanoplastic interactions in molecular detail, inspecting the individual contribution of nanoplastics and different types of protein coronae. The in vitro study showed mild cytotoxicity and cellular uptake of polystyrene (PS) nanoplastics, with no clear trend based on nanoplastic size (20 and 200 nm) or surface charge. In contrast, a nanoplastic size-dependency on bilayer disruption was observed in the model system. This suggests that membrane disruption resulting from direct interaction with PS nanoplastics has little correlation with cytotoxicity. Furthermore, the level of bilayer disruption was found to be limited to the hydrophilic headgroup, indicating that transmembrane diffusion was an unlikely pathway for cellular uptake-endocytosis is the viable mechanism. In rare cases, small PS nanoplastics (20 nm) were found in the vicinity of chromosomes without a nuclear membrane surrounding them; however, this was not observed for larger PS nanoplastics (200 nm). We hypothesize that the nanoplastics can interact with chromosomes prior to nuclear membrane formation. Overall, precoating PS particles with protein coronae reduced the cytotoxicity, irrespective of the corona type. When comparing the two types, the extent of reduction was more apparent with soft than hard corona
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