On the large-Weissenberg-number scaling laws in viscoelastic pipe flows
arXiv:2205.09525 · doi:10.1017/jfm.2022.489
Abstract
This work explains a scaling law of the first Landau coefficient of the derived Ginzburg-Landau equation (GLE) in the weakly nonlinear analysis of axisymmetric viscoelastic pipe flows in the large-Weissenberg-number () limit, recently reported in Wan et al. J. Fluid Mech. (2021), vol. 929, A16. Using an asymptotic method, we derive a reduced system, which captures the characteristics of the linear centre-mode instability near the critical condition in the large- limit. Based on the reduced system we then conduct a weakly nonlinear analysis using a multiple-scale expansion method, which readily explains the aforementioned scaling law of the Landau coefficient and some other scaling laws. Particularly, the equilibrium amplitude of disturbance near linear critical conditions is found to scale as , which may be of interest to experimentalists. The current analysis reduces the numbers of parameters and unknowns and exemplifies an approach to studying the viscoelastic flow at large , which could shed new light on the understanding of its nonlinear dynamics.
18 pages, 4 figures, submitted to JFM
References in corpus (10)
- An Introduction to Adjoint Problems
- Understanding viscoelastic flow instabilities: Oldroyd-B and beyond
- The center-mode instability of viscoelastic plane Poiseuille flow
- A continuous pathway between the elasto-inertial and elastic turbulent states in viscoelastic channel flow
- Weakly nonlinear analysis of the viscoelastic instability in channel flow for finite and vanishing Reynolds numbers
- Coherent structures in plane channel flow of dilute polymer solutions with vanishing inertia
- Tollmien-Schlichting route to elastoinertial turbulence in channel flow
- Subcritical and supercritical bifurcations in axisymmetric viscoelastic pipe flows
- Finite-amplitude elastic waves in viscoelastic channel flow from large to zero Reynolds number
- The mean conformation tensor in viscoelastic turbulence