Stagnation point flow past a stretching/shrinking sheet driven by Arrhenius kinetics

The effect that a stagnation-point flow on a stretching/shrinking surface can have on an exothermic surface reaction is considered. The velocity of the surface relative to the outer flow is measured by the parameter λ with there being a critical value of λ. The surface reaction is described by the dimensionless reaction parameters α, β and ϵ, representing the heat of reaction, the reaction rate constant and the activation energy. The problem to determine how the dimensionless surface temperature θ0 and concentration ϕ0 varied can be simplified enabling θ0 and ϕ0 to be readily calculated in terms of reaction parameters. A hysteresis bifurcation is seen to arise distinguishing between cases where there are two critical points, and hence three solution branches, and where there is only a unique solution, the calculation of which placed an upper bound on the activation energy parameter ϵ for multiple solutions. The effect of the moving surface is seen to have a direct result on the surface temperature θ0 and concentration ϕ0 as well as on the locations of the critical values and the hysteresis bifurcation.

[1]  B. F. Gray,et al.  Thermal explosion: Escape times in the uniform temperature approximation. Part 2. Perturbations of critical initial conditions , 1993 .

[2]  F. Homann Der Einfluß großer Zähigkeit bei der Strömung um den Zylinder und um die Kugel , 1936 .

[3]  J. Merkin,et al.  Combustion in a porous material with reactant consumption: The role of the ambient temperature , 1994 .

[4]  B. F. Gray,et al.  Thermal explosion: escape times in the uniform temperature approximation. Part 1.—Effects of parameter perturbations , 1990 .

[5]  C. Wang Review of similarity stretching exact solutions of the Navier–Stokes equations , 2011 .

[6]  Yu Tian,et al.  Measurement of lubricant viscosity and detection of boundary slip at high shear rates , 2016 .

[7]  John H. Merkin,et al.  Disjoint bifurcation diagrams in combustion systems , 1991 .

[8]  Forman A. Williams,et al.  Catalytic combustion of hydrogen-air mixtures in stagnation flows , 1993 .

[9]  C. Wang,et al.  Viscous flow due to a shrinking sheet , 2006 .

[10]  Tiegang Fang,et al.  Boundary layer flow over a shrinking sheet with power-law velocity , 2008 .

[11]  L. Crane,et al.  Heat Transfer on a Continuous Stretching Sheet , 1982 .

[12]  I. Puri Extinction Criteria for Buoyant Nonpremixed Flames , 1992 .

[13]  Karl Hiemenz,et al.  Die Grenzschicht an einem in den gleichförmigen Flüssigkeitsstrom eingetauchten geraden Kreiszylinder , 1911 .

[14]  J. Merkin,et al.  Free convection stagnation point boundary layers driven by catalytic surface reactions: II times to ignition , 1996 .

[15]  J. Merkin,et al.  Free-convection stagnation-point boundary layers driven by catalytic surface reactions: I the steady states , 1994 .

[16]  W. H. H. Banks,et al.  Similarity solutions of the boundary-layer equations for a stretching wall , 1983 .

[17]  J. Merkin,et al.  Free convection boundary layers driven by exothermic surface reactions: critical ambient temperatures , 1995 .

[18]  L. Crane Flow past a stretching plate , 1970 .

[19]  J. Merkin,et al.  Free-convection boundary layers on vertical surfaces driven by an exothermic surface reaction , 1994 .

[20]  B. F. Gray,et al.  On the determination of critical ambient temperatures and critical initial temperatures for thermal ignition , 1988 .

[21]  E. G. Fisher,et al.  Extrusion of plastics , 1976 .

[22]  S. Goldstein On backward boundary layers and flow in converging passages , 1965, Journal of Fluid Mechanics.

[23]  Z. Ji,et al.  Viscous Flow over an Unsteady Shrinking Sheet with Mass Transfer , 2009 .