17 research outputs found

    Representing non-weakly compact operators

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    For each SL(E)S \in L(E) (with EE a Banach space) the operator R(S)L(E/E)R(S) \in L(E^{**}/E) is defined by R(S)(x+E)=Sx+ER(S)(x^{**}+E) = S^{**}x^{**}+E \quad (xEx^{**}\in E^{**}). We study mapping properties of the correspondence SR(S),S\to R(S), which provides a representation RR of the weak Calkin algebra L(E)/W(E)L(E)/W(E) (here W(E)W(E) denotes the weakly compact operators on EE). Our results display strongly varying behaviour of R.R. For instance, there are no non--zero compact operators in Im(R)(R) in the case of L1L^1 and C(0,1),C(0,1), but R(L(E)/W(E))R(L(E)/W(E)) identifies isometrically with the class of lattice regular operators on 2\ell^2 for E=2(J)E=\ell^2(J) (here JJ is the James' space). Accordingly, there is an operator TL(2(J))T \in L(\ell^2(J)) such that R(T)R(T) is invertible but TT fails to be invertible modulo $W(\ell^2(J)).

    Buoyancy-assisted mixed convective flow over backward-facing step in a vertical duct using nanofluids

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    Laminar mixed convective buoyancy assisting flow through a two-dimensional vertical duct with a backward-facing step using nanofluids as a medium is numerically simulated using finite volume technique. Different types of nanoparticles such as Au, Ag, Al2O3, Cu, CuO, diamond, SiO2 and TiO2 with 5 % volume fraction are used. The wall downstream of the step was maintained at a uniform wall temperature, while the straight wall that forms the other side of the duct was maintained at constant temperature equivalent to the inlet fluid temperature. The walls upstream of the step and the backward-facing step were considered as adiabatic surfaces. The duct has a step height of 4.9 mm and an expansion ratio of 1.942, while the total length in the downstream of the step is 0.5 m. The downstream wall was fixed at uniform wall temperature 0 = ?T= 30 °C, which was higher than the inlet flow temperature. The Reynolds number in the range of 75 = Re = 225 was considered. It is found that a recirculation region was developed straight behind the backward-facing step which appeared between the edge of the step and few millimeters before the corner which connect the step and the downstream wall. In the few millimeters gap between the recirculation region and the downstream wall, a U-turn flow was developed opposite to the recirculation flow which mixed with the unrecirculated flow and traveled along the channel. Two maximum and one minimum peaks in Nusselt number were developed along the heated downstream wall. It is inferred that Au nanofluid has the highest maximum peaks while diamond nanofluid has the highest minimum peak. Nanofluids with a higher Prandtl number have a higher peak of Nusselt numbers after the separation and the recirculation flow disappeared

    Surface-initiated self-healing of polymers in aqueous media

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    Polymeric materials that intrinsically heal at damage sites under wet or moist conditions are urgently needed for biomedical and environmental applications(1-6). Although hydrogels with self-mending properties have been engineered by means of mussel-inspired metal-chelating catechol-functionalized polymer networks(7-10), biological self-healing in wet conditions, as occurs in self-assembled holdfast proteins in mussels and other marine organisms(11,12), is generally thought to involve more than reversible metal chelates. Here we demonstrate self-mending in metal-free water of synthetic polyacrylate and polymethacrylate materials that are surface-functionalized with mussel-inspired catechols. Wet self-mending of scission in these polymers is initiated and accelerated by hydrogen bonding between interfacial catechol moieties, and consolidated by the recruitment of other non-covalent interactions contributed by subsurface moieties. The repaired and pristine samples show similar mechanical properties, suggesting that the triggering of complete self-healing is enabled underwater by the formation of extensive catechol-mediated interfacial hydrogen bonds.close303
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