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The effects of mixed convection on the classical Falkner–Skan similarity solutions are considered, now involving a mixed convection parameter λ as well as the exponent m associated with the outer flow. The forced convection solutions indicate a singularity in the temperature field as m → 0.070722 . Numerical solutions for $$m>0$$ show the existence of a critical value λ c with λ c<0 and solutions only for λ ≥ λ c . The nature of the solution for λ 1 is investigated. For $$m=0$$ , there are solutions for all λ <0 , opposing flow, and only for a finite range of λ in aiding flow with the asymptotic solution as λ → -∞ also being considered. Solutions for $$m<0$$ are obtained in the cases when there is a solution to the Falkner–Skan system and for a value of m when no solution to this system exists. In the former case, two completely separate parts to the solution are seen, whereas in the latter case, a solution exists only in aiding flow for a limited range of λ . The variation of solution with the exponent m is also treated for both aiding and opposing flows. In both cases, a solution is seen to exist for all $$m>0$$ , which, however, is limited to a relatively small range of m when $$m<0$$ .
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J. H. Merkin (2016) studied this question.
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