Search results

International Education is worth billions of dollars to the world economy, and many countries such as the United States, United Kingdom, Canada and Australia have government initiatives that look to stimulate and guide international student mobility, research and technology transfer. The involvement of the state into student mobility does not come without risk. Government foreign policy and international relations between sending countries and English-speaking study destinations threatens to upset the historical norms of international mobility. What is more, world events such as the global pandemic of 2020, will have a profound impact on the future of international education, and may change the international landscape altogether. This chapter will frame the challenges facing institutions who benefit from international mobility in the context of geopolitics and world events. It will explore how institutions can leverage strategic enrolment management tactics to help mitigate enrolment risks posed by global disruption.

Through the energetic initiative of “The Globe” newspaper a Middle Classes Union has been formed for the purpose of organising that great body of people into an Alliance that shall be capable of making its power felt. A preliminary meeting was held recently under the presidency of Major J. R. Pretyman Newman, M.P., of gentlemen interested in the scheme recently outlined in “The Globe” for combining the Middle Classes in a Union for their own protection. All present were unanimous as to the necessity for the formation of such an organisation, and after discussion it was provisionally agreed that its title should be—

This paper aims to provide a limited, but selective bibliography on modelling heat and mass transfer in composite fluid‐porous domains.

Since the pioneer study by Beavers and Joseph, the problem of interface continuity and/or jump conditions at a fluid‐porous interface has been of interest to the fluid mechanics and heat and mass transfer community. The paper is concerned both with numerical simulations of heat and fluid flow in such systems, and with the linear stability problems.

The one‐ and two‐domain formulations are equivalent. Using the Darcy‐Brinkman extension instead of the Darcy model reduces the number of ad hoc parameters in this configuration.

The problem of double diffusive convection has still to be solved and analyzed.

The discussion on the interface conditions is of great relevance to many industrial and practical situations.

The important question of the macroscopic formulation of the problem is tackled in the paper.

Aarhus Kommunes Biblioteker (Teknisk Bibliotek), Ingerslevs Plads 7, Aarhus, Denmark. Representative: V. NEDERGAARD PEDERSEN (Librarian).

In the present paper, the squeeze film lubrication between anisotropic porous rectangular plates with lubricants containing polar additives has been studied. The lubricants containing additives has been modelled as a Stokes couple stress fluid. The more realistic Beavers‐Joseph slip boundary conditions are used to derive the most general form of Reynolds equation, which account for the effects due to the lubricant additives and the anisotropic nature of porous material. The eigen type of expressions are obtained for the fluid film pressure, load carrying capacity and squeeze film time. It is observed that the effect of the lubricant additives is to increase the load carrying capacity and the squeeze film time as compared to the Newtonian lubricants. Further for anisotropic porous surface, the maximum load carrying capacity is attained for the rectangular (non‐square) plates.

In this study, the stationary flow of a polymeric fluid governed by the upper convected Maxwell law is computed in a 2‐D convergent geometry. A finite element method is used to obtain non‐linear discretized equations, solved by an iterative Picard (fixed point) algorithm. At each step, two sub‐systems are successively solved. The first one represents a Newtonian fluid flow (Stokes equations) perturbed by known pseudo‐body forces expressing fluid elasticity. It is solved by minimization of a functional of the velocity field, while the pressure is eliminated by penalization. The second sub‐system reduces to the tensorial differential evolution equation of the extra‐stress tensor for a given velocity field. It is solved by the so‐called ‘non‐consistent Petrov‐Galerkin streamline upwind’ method. As with other decoupled techniques applied to this problem, our simulation fails for relatively low values of the Weissenberg viscoelastic number. The value of the numerical limit point depends on the mesh refinement. When convergence is reached, the numerical solutions for velocity, pressure and stress fields are similar to those obtained by other authors with very costly mixed methods.