By Peter Vadasz
The first actual significant reference textual content in this subject, this booklet offers a special selection of articles reviewing the state-of-the-art within the box. It supplies specific emphasis to rising applied sciences, from bioengineering and bio-tissues to nanotechnology. the mixing of the several themes is gifted through a mixture of theoretical and utilized technique to supply a self-contained significant reference that's beautiful to either the scientist and the engineer.
Read or Download Emerging Topics in Heat and Mass Transfer in Porous Media: From Bioengineering and Microelectronics to Nanotechnology (Theory and Applications of Transport ... Applications of Transport in Porous Media) PDF
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Extra resources for Emerging Topics in Heat and Mass Transfer in Porous Media: From Bioengineering and Microelectronics to Nanotechnology (Theory and Applications of Transport ... Applications of Transport in Porous Media)
These theorems inter-relate contributions (to the temperature field) of the initial temperature distribution, the source term and the initial time-rate change of the temperature, uncover the structure of temperature field and considerably simplify the development of solutions. The thermal oscillation and resonance in the dualphase-lagging heat conduction have been examined in details. Conditions and features of underdamped, critically-damped and overdamped oscillations have been obtained and compared with those in the classical parabolic heat conduction and the hyperbolic heat conduction.
31) and rt = t /a , Eq. (35a) becomes dimensionless, θs (ξ, η) = θ f (ξ, η) + rt Ѩθ f (ξ, η) Ѩη (35b) since θ f = (T f − Ti )/(To − Ti ) and θs = (Ts − Ti )/(To − Ti ). The Laplace transform of Eq. (35b) yields a simple relation between relation θ¯ f and θ¯s ; that is θ¯s (ξ, s) = θ¯ f (ξ, s) + rt s θ¯ f (ξ, s) = (1 + rt s) θ¯ f (ξ, s) (35c) At the ξ = 0 surface, Eq. (35c) provides the surface condition, (1 + r s)θ¯ f (0, s) = θ¯s (0, s) 1 = s (35d) Using this surface condition in Eq. (34) makes D = θ¯ f (0, s) = 1/[s(1 + rt s)] and then Eq.
Whitaker S (1999) The method of volume averaging. Kluwer, Dordrecht. Xu MT, Wang LQ (2002) Int. J. Heat Mass Tran. 45: 1055–1061. Xu MT, Wang LQ (2005) Int. J. Heat Mass Tran. 48: 5616–5624. Heat Transfer Analysis Under Local Thermal Non-equilibrium Conditions A. J. Minkowycz 1 Introduction The Local Thermal Non-Equilibrium (LTNE) hypothesis emerges when studying a rapid transport of heat in porous media. The non-equilibrium phenomenon is an interesting issue during a rapid heating or a cooling process.
Emerging Topics in Heat and Mass Transfer in Porous Media: From Bioengineering and Microelectronics to Nanotechnology (Theory and Applications of Transport ... Applications of Transport in Porous Media) by Peter Vadasz
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