Bounds on heat transfer for B\'enard-Marangoni convection at infinite Prandtl number

TL;DR

This paper derives improved upper bounds on heat transfer in Bénard-Marangoni convection at infinite Prandtl number, refining previous estimates and exploring the effects of background field profiles and non-monotonicity.

Contribution

The study extends background method analysis to include balance parameters and optimizes bounds over various background profiles, achieving tighter bounds and insights into the role of non-monotonicity.

Findings

Bound on Nu improved to 0.803 Ma^{2/7} with a piecewise-linear profile.

Optimal bound scales as O(Ma^{2/7} (ln Ma)^{-1/2}) with non-monotonic backgrounds.

Monotonic background fields cannot surpass the 2/7 power-law scaling.

Abstract

The vertical heat transfer in B\'enard-Marangoni convection of a fluid layer with infinite Prandtl number is studied by means of upper bounds on the Nusselt number $Nu$ as a function of the Marangoni number $Ma$. Using the background method for the temperature field, it has recently been proven by Hagstrom & Doering that $ Nu\leq 0.838\,Ma^{2/7}$. In this work we extend previous background method analysis to include balance parameters and derive a variational principle for the bound on $Nu$, expressed in terms of a scaled background field, that yields a better bound than Hagstrom & Doering's formulation at a given $Ma$. Using a piecewise-linear, monotonically decreasing profile we then show that $Nu \leq 0.803\,Ma^{2/7}$, lowering the previous prefactor by 4.2%. However, we also demonstrate that optimisation of the balance parameters does not affect the asymptotic scaling of the optimal bound achievable with Hagstrom & Doering's original formulation. We subsequently utilise convex optimisation to optimise the bound on $Nu$ over all admissible background fields, as well as over two smaller families of profiles constrained by monotonicity and convexity. The results show that $Nu \leq O(Ma^{2/7}(\ln Ma)^{-1/2})$ when the background field has a non-monotonic boundary layer near the surface, while a power-law bound with exponent 2/7 is optimal within the class of monotonic background fields. Further analysis of our upper-bounding principle reveals the role of non-monotonicity, and how it may be exploited in a rigorous mathematical argument.