Variable-Order Fractional Models for Wall-Bounded Turbulent Flows

Modeling of wall-bounded turbulent flows is still an open problem in classical physics, with relatively slow progress in the last few decades beyond the log law, which only describes the intermediate region in wall-bounded turbulence, i.e., 30–50 y+ to 0.1–0.2 R+ in a pipe of radius R. Here, we prop...

Full description

Bibliographic Details
Main Authors: Fangying Song, George Em Karniadakis
Format: Article
Language:English
Published: MDPI AG 2021-06-01
Series:Entropy
Subjects:
Online Access:https://www.mdpi.com/1099-4300/23/6/782
_version_ 1797529484932415488
author Fangying Song
George Em Karniadakis
author_facet Fangying Song
George Em Karniadakis
author_sort Fangying Song
collection DOAJ
description Modeling of wall-bounded turbulent flows is still an open problem in classical physics, with relatively slow progress in the last few decades beyond the log law, which only describes the intermediate region in wall-bounded turbulence, i.e., 30–50 y+ to 0.1–0.2 R+ in a pipe of radius R. Here, we propose a fundamentally new approach based on fractional calculus to model the entire mean velocity profile from the wall to the centerline of the pipe. Specifically, we represent the Reynolds stresses with a non-local fractional derivative of variable-order that decays with the distance from the wall. Surprisingly, we find that this variable fractional order has a universal form for all Reynolds numbers and for three different flow types, i.e., channel flow, Couette flow, and pipe flow. We first use existing databases from direct numerical simulations (DNSs) to lean the variable-order function and subsequently we test it against other DNS data and experimental measurements, including the Princeton superpipe experiments. Taken together, our findings reveal the continuous change in rate of turbulent diffusion from the wall as well as the strong nonlocality of turbulent interactions that intensify away from the wall. Moreover, we propose alternative formulations, including a divergence variable fractional (two-sided) model for turbulent flows. The total shear stress is represented by a two-sided symmetric variable fractional derivative. The numerical results show that this formulation can lead to smooth fractional-order profiles in the whole domain. This new model improves the one-sided model, which is considered in the half domain (wall to centerline) only. We use a finite difference method for solving the inverse problem, but we also introduce the fractional physics-informed neural network (fPINN) for solving the inverse and forward problems much more efficiently. In addition to the aforementioned fully-developed flows, we model turbulent boundary layers and discuss how the streamwise variation affects the universal curve.
first_indexed 2024-03-10T10:14:33Z
format Article
id doaj.art-4dceed1b38a8487fa96aca1db6f003de
institution Directory Open Access Journal
issn 1099-4300
language English
last_indexed 2024-03-10T10:14:33Z
publishDate 2021-06-01
publisher MDPI AG
record_format Article
series Entropy
spelling doaj.art-4dceed1b38a8487fa96aca1db6f003de2023-11-22T00:54:21ZengMDPI AGEntropy1099-43002021-06-0123678210.3390/e23060782Variable-Order Fractional Models for Wall-Bounded Turbulent FlowsFangying Song0George Em Karniadakis1College of Mathematics and Computer Science, Fuzhou University, Fuzhou 350108, ChinaDivision of Applied Mathematics, School of Engineering, Brown University, Providence, RI 02912, USAModeling of wall-bounded turbulent flows is still an open problem in classical physics, with relatively slow progress in the last few decades beyond the log law, which only describes the intermediate region in wall-bounded turbulence, i.e., 30–50 y+ to 0.1–0.2 R+ in a pipe of radius R. Here, we propose a fundamentally new approach based on fractional calculus to model the entire mean velocity profile from the wall to the centerline of the pipe. Specifically, we represent the Reynolds stresses with a non-local fractional derivative of variable-order that decays with the distance from the wall. Surprisingly, we find that this variable fractional order has a universal form for all Reynolds numbers and for three different flow types, i.e., channel flow, Couette flow, and pipe flow. We first use existing databases from direct numerical simulations (DNSs) to lean the variable-order function and subsequently we test it against other DNS data and experimental measurements, including the Princeton superpipe experiments. Taken together, our findings reveal the continuous change in rate of turbulent diffusion from the wall as well as the strong nonlocality of turbulent interactions that intensify away from the wall. Moreover, we propose alternative formulations, including a divergence variable fractional (two-sided) model for turbulent flows. The total shear stress is represented by a two-sided symmetric variable fractional derivative. The numerical results show that this formulation can lead to smooth fractional-order profiles in the whole domain. This new model improves the one-sided model, which is considered in the half domain (wall to centerline) only. We use a finite difference method for solving the inverse problem, but we also introduce the fractional physics-informed neural network (fPINN) for solving the inverse and forward problems much more efficiently. In addition to the aforementioned fully-developed flows, we model turbulent boundary layers and discuss how the streamwise variation affects the universal curve.https://www.mdpi.com/1099-4300/23/6/782fractional conservations lawsvariable fractional modelturbulent flowsfractional PINNphysics-informed learning
spellingShingle Fangying Song
George Em Karniadakis
Variable-Order Fractional Models for Wall-Bounded Turbulent Flows
Entropy
fractional conservations laws
variable fractional model
turbulent flows
fractional PINN
physics-informed learning
title Variable-Order Fractional Models for Wall-Bounded Turbulent Flows
title_full Variable-Order Fractional Models for Wall-Bounded Turbulent Flows
title_fullStr Variable-Order Fractional Models for Wall-Bounded Turbulent Flows
title_full_unstemmed Variable-Order Fractional Models for Wall-Bounded Turbulent Flows
title_short Variable-Order Fractional Models for Wall-Bounded Turbulent Flows
title_sort variable order fractional models for wall bounded turbulent flows
topic fractional conservations laws
variable fractional model
turbulent flows
fractional PINN
physics-informed learning
url https://www.mdpi.com/1099-4300/23/6/782
work_keys_str_mv AT fangyingsong variableorderfractionalmodelsforwallboundedturbulentflows
AT georgeemkarniadakis variableorderfractionalmodelsforwallboundedturbulentflows