Self-limiting turbulent drag reduction via a viscoelastic lubricating layer
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Emanuele Milocco, Alessio Roccon, Alfredo Soldati
A thin slippery layer can make turbulent flow move more easily, but making that layer more elastic eventually makes almost no further difference. The surprising reason is that the layer starts suppressing the motion it needs to work.
We investigate drag reduction (DR) in a turbulent channel flow lubricated by a thin viscoelastic layer using direct numerical simulations at a shear Reynolds number Reτ = 300, coupling a phase-field description of the interfacial dynamics with a FENECR model for the polymeric stresses. Different elasticity levels are considered by varying the shear Weissenberg number from Wiτ = 0 (Newtonian) to Wiτ = 25 (weakly elastic) and up to Wiτ = 100 (highly elastic). The Newtonian case yields a DR of about 12 %, which increases to roughly 24 % at Wiτ = 100, with progressively smaller increments that reveal a saturation effect. To explain this behaviour, we employ the energy-box framework, which graphically represents the fluxes of mean kinetic energy, turbulent kinetic energy and elastic potential energy in each layer, together with the corresponding inter-layer exchanges. Polymer stretching and relaxation introduce an additional energy-transfer pathway in the lubricating layer, redirecting kinetic energy from viscous dissipation towards elastic storage and irreversible relaxation. As Wiτ increases, elastic stresses progressively suppress wall-normal fluctuations, thereby reducing both the capillary work and the production of turbulent kinetic energy. The resulting decrease in turbulent kinetic energy supplied to the lubricating layer reduces the kinetic-to-elastic energy transfer, leading the system to a self-limiting regime in which further increases in elasticity produce negligible additional DR. Key words: viscoelasticity, stratified turbulence, drag reduction
Transcript
A thin slippery layer can make turbulent flow move more easily—but making that layer more elastic eventually makes almost no further difference. The surprising reason is that the layer starts suppressing the motion it needs to work.
Drag reduction is a long-standing goal in fluid mechanics and engineering. One approach puts a thin, less viscous lubricating film near the wall, where it carries most of the shear and shields the bulk fluid from direct contact with the solid boundary.
Another approach adds small amounts of polymers to a liquid, changing the turbulence near the wall and reducing frictional losses. This study combines the two ideas and asks whether making the lubricating layer more elastic eventually reaches an upper limit. Earlier comparisons found that surface tension makes a substantial contribution to drag reduction, while elasticity is equally important.
Lubricating layers with elastic polymers doubled the performance of a Newtonian lubricating layer, while changes that only made the liquid thinner under stress gave marginal gains. So the next question was how drag reduction changes as the elasticity of the lubricating layer increases.
The simulations focused on a turbulent channel with a purely viscoelastic lubricating layer. As the lubricating layer becomes more elastic, its stored elastic energy spreads more evenly, while the boundary between the two liquids develops gentler waves.
That smoother boundary can help explain how elasticity changes turbulent flow and potentially reduces uneven motion. The boundary between the two liquids is not treated as a sharp line. Instead, the model lets the change from the main liquid to the viscoelastic lubricating layer happen smoothly across a thin region.
That smooth boundary can move and deform as the flow changes, allowing the calculation to follow how the two layers interact. Even before it contains elastic polymers, introducing a Newtonian lubricating layer already increases the total flow rate by twelve point two percent.
The increase reaches 24.1 percent at the highest elasticity examined, while the improvement between the two most elastic cases is less than 0.5 percent. The overall result is clear: more elasticity brings progressively smaller gains.
To understand that slowdown, the study follows where the flow's energy goes. The analysis represents energy as sources, losses, and exchanges between the layers, making the transfers visible as a connected picture.
The total kinetic energy is split into two contributions: mean kinetic energy, or MKE, and turbulent kinetic energy, or TKE. The framework then makes kinetic-energy fluxes visible as sources, sinks, and exchanges, making transfers through the system clearly visible in graphical form.
Here, polymers progressively suppress the turbulent motions that stretch them, limiting their effectiveness and producing smaller incremental gains in drag reduction as elasticity increases. At first, modest elasticity strengthens the polymer action and increases drag reduction.
Beyond a certain point, elastic stresses reduce the turbulent energy available inside the lubricating layer, so stretching becomes less efficient and the stored elastic energy approaches a limit. The measured pattern follows that explanation. A Newtonian lubricating layer gives 12.2 percent drag reduction, rising to 18.9 percent with weak elasticity and only marginally further to 24.1 percent at high elasticity.
As elasticity increases, less turbulent energy is absorbed by the lubricating layer, and the polymer action becomes less effective. The layer's elastic stresses also suppress turbulent motion across the flow, reducing both energy transfer at the moving boundary and turbulence production within the layer.
The reduced turbulence limits further polymer stretching and stored elastic energy, so the system enters a self-limiting regime in which more elasticity no longer produces additional drag reduction. This means lubrication and elasticity can be combined, but their benefits do not simply add together.
Their interaction restricts the achievable gain, because the elastic layer changes the boundary motion and the turbulence that feeds it. As elasticity increases, wall-normal fluctuations and the turbulent kinetic energy available within the lubricating layer are progressively suppressed by viscoelastic stresses.
Specifically, mean and turbulent kinetic energy move from the lubricating layer to the channel core and back as Newtonian and non-Newtonian turbulence interact across a deformable interface. Increasing elasticity can initially enhance drag reduction, but beyond a certain point it suppresses turbulent kinetic energy and polymer stretching, so the gains become progressively smaller.
Elasticity can improve flow by storing energy in stretched polymers, but the effect limits itself: stronger elastic stresses reduce the turbulence that stretches those polymers. That balance could guide more efficient ways to move fluids through pipes and channels.
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