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It is shown that reasonable simplifications according to the specific design and the typical operating conditions of compact plate heat exchangers together with a semi-discretization of the spatial domain by means of the finite volume method provides a compact finite-dimensional approximation of the underlying partial differential equations (pdes).
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In cylindrical domains, Lemma 3.3 and Lemma 3.4 in [4] have provided the method checking the conditions of asymptotic compact in (L^{p}(mathcal {O})) ((p>2)), and following a similar idea, we establish the lemma in non-cylindrical domains.
We give sufficient conditions for the sets of compact and completely compact multipliers to coincide and characterise the cases where an operator multiplier in the minimal tensor product of two C∗-algebras is automatically compact.
Under the most critical conditions for the deposition of compact zinc, i.e. low zincate concentrations of 0.2 M and low electrolyte flow velocities of 3 cm s−1, pulse interrupt current produced compact zinc deposits up to the limiting current.
The operating conditions of the processor require compact and lightweight pieces of equipment and efficient operation at different conditions.
We also find conditions to obtain the corresponding subclasses of compact matrix operators by using the Hausdorff measure of noncompactness.
We also obtain estimates for the norms of the bounded linear operators (L_{A}) defined by these matrix transformations and find conditions to obtain the corresponding subclasses of compact matrix operators by using the Hausdorff measure of noncompactness.
An ESD simulation flow contains the process simulation of the devices under investigation, their electrical operation under ESD conditions by a device simulation, extraction of compact models for the calculation of complete circuits such as I/O cells, and chip-level simulation for a final verification of the ESD concept of the IC.
We report measurements of attenuation of the T 0,1) and L 0,2) guided wave modes over a range of sand conditions, including loose, compacted, mechanically compacted, water saturated and drained.
Under the conditions of Theorem 1.1, (Phi') is compact, i.e., (Phi' u_{n})rightarrowPhi' u)) if (u_{n}rightharpoonup u) in (X^{alpha}), where (Phi X^{alpha}rightarrow mathbb {R}) is defined by Phi u)=int_{mathbb {R}}W t,u),dt.
High performance of compact heat exchangers is conditioned by correct fluid distribution.
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