2017
DOI: 10.1007/s11242-017-0832-1
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Linear and Nonlinear Stability Analysis of a Horton–Rogers–Lapwood Problem with an Internal Heat Source and Brinkman Effects

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Cited by 16 publications
(5 citation statements)
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“…The author considered four different types of heat supply functions, and discussed the results by obtaining the values of the critical Rayleigh number of energy theory Ra E and the critical Rayleigh number of linear instability theory Ra L . Most recently, Nandal and Mahajan [23] studied the effect of internal heat source on the onset of convection in a fluid layer saturated porous medium. The authors considered four different types of internal heat supply functions, and discussed the results for stress-free and isothermal boundary conditions.…”
Section: Introductionmentioning
confidence: 99%
“…The author considered four different types of heat supply functions, and discussed the results by obtaining the values of the critical Rayleigh number of energy theory Ra E and the critical Rayleigh number of linear instability theory Ra L . Most recently, Nandal and Mahajan [23] studied the effect of internal heat source on the onset of convection in a fluid layer saturated porous medium. The authors considered four different types of internal heat supply functions, and discussed the results for stress-free and isothermal boundary conditions.…”
Section: Introductionmentioning
confidence: 99%
“…These papers represent quite a wide range of different types of boundary condition such as a free upper surface in [4] or the presence of an insulated bounding surface [8,10]. The case where both surfaces are impermeable and are at identical constant temperatures has a critical Darcy-Rayleigh number of 471.38 and a critical wavenumber of 4.6752, values which have been obtained by various authors such as Barletta et al [11], Nandal and Mahajan [12] and Nouri-Borujerdi et al [13,14]. This ten-fold rise in the critical Darcy-Rayleigh number may be explained at least qualitatively by the facts that (i) the internally-heated case admits a destabilising temperature gradient only in the upper half of the layer and (ii) the maximum temperature difference is only 1 8 of that of that of the classical Darcy-Bénard layer.…”
Section: Introductionmentioning
confidence: 93%
“…Results of asymptotic stability in this vein have been the subject of several recent articles using a judicious choice of an energy functional, cf. Amendola & Fabrizio [2], Amendola et al [3], Amendola et al [4], Deepika & Narayana [6], Deseri et al [8], Fabrizio & Lazzari [9], Fabrizio et al [10], Fabrizio et al [11], Franchi & Morro [12], Nandal & Mahajan [15], Straughan [20][21][22].…”
Section: Nonlinear Stabilitymentioning
confidence: 99%