Experimental–numerical investigation of solid–liquid jet erosion in AISI 304 stainless steel: effect of impingement angle and strain hardening

Solid–liquid jet erosion of AISI 304 austenitic stainless steel was investigated at impingement angles of 30° and 45° using a coupled experimental–numerical framework. One-hour slurry jet tests (2 wt% SiO₂, mean particle size 230 μm, velocity 1 m·s⁻¹) were combined with transient Eulerian–Lagrangian computational fluid dynamics (CFD) simulations employing the Oka erosion model. The novelty of this work lies in directly linking CFD-predicted erosion fields to the dynamic evolution of surface hardness and microstructure. Both experimental and numerical results confirmed that erosion severity increased with impingement angle, from 30° to 45°. However, the CFD model overestimated the measured mass-loss flux by factors of 6.2 and 6.4 at 30° and 45°, respectively. This discrepancy is primarily attributed to the constant-hardness assumption (149 HV) embedded in the Oka model, as well as to the trap-wall boundary condition and the one-way coupling approach. Post-erosion Vickers microhardness measurements and microstructural analyses revealed an inverse relationship between erosion severity and residual surface hardening. Despite exhibiting the lowest mass-loss flux (6.84 × 10⁻⁷ kg·m⁻²·s⁻¹), the 30° condition produced the highest surface hardening, with hardness increasing from 149 to 162 HV (+ 8.5%), accompanied by pronounced shear-induced deformation. In contrast, the 45° condition, which generated the highest mass-loss flux (8.76 × 10⁻⁷ kg·m⁻²·s⁻¹), exhibited the lowest hardening, with hardness increasing only from 149 to 157 HV (+ 5.4%), together with evidence of indentation-assisted material removal. This inverse trend suggests that higher erosion rates continuously remove the work-hardened surface layer before it can fully develop and stabilize. Consequently, the more severe the erosion, the lower the hardness retained at the eroded surface. These findings establish a direct relationship between erosion severity, hardness evolution, microstructural response, and impact angle, while highlighting the need for erosion models that account for strain-hardening-dependent material evolution to improve predictive accuracy under slurry-jet erosion conditions.

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Journal
Journal of Engineering and Applied Science
Published
2026-08-18
DOI
https://doi.org/10.1186/s44147-026-01175-4
Primary Topic
Erosion and Abrasive Machining
Type
article
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article

Experimental–numerical investigation of solid–liquid jet erosion in AISI 304 stainless steel: effect of impingement angle and strain hardening

B. Ouaki, K. Mesbah, M. K. El Kouifat
Journal of Engineering and Applied Science
Erosion and Abrasive Machining
article

Experimental–numerical investigation of solid–liquid jet erosion in AISI 304 stainless steel: effect of impingement angle and strain hardening

B. Ouaki, K. Mesbah, M. K. El Kouifat
article en

Abstract

Solid–liquid jet erosion of AISI 304 austenitic stainless steel was investigated at impingement angles of 30° and 45° using a coupled experimental–numerical framework. One-hour slurry jet tests (2 wt% SiO₂, mean particle size 230 μm, velocity 1 m·s⁻¹) were combined with transient Eulerian–Lagrangian computational fluid dynamics (CFD) simulations employing the Oka erosion model. The novelty of this work lies in directly linking CFD-predicted erosion fields to the dynamic evolution of surface hardness and microstructure. Both experimental and numerical results confirmed that erosion severity increased with impingement angle, from 30° to 45°. However, the CFD model overestimated the measured mass-loss flux by factors of 6.2 and 6.4 at 30° and 45°, respectively. This discrepancy is primarily attributed to the constant-hardness assumption (149 HV) embedded in the Oka model, as well as to the trap-wall boundary condition and the one-way coupling approach. Post-erosion Vickers microhardness measurements and microstructural analyses revealed an inverse relationship between erosion severity and residual surface hardening. Despite exhibiting the lowest mass-loss flux (6.84 × 10⁻⁷ kg·m⁻²·s⁻¹), the 30° condition produced the highest surface hardening, with hardness increasing from 149 to 162 HV (+ 8.5%), accompanied by pronounced shear-induced deformation. In contrast, the 45° condition, which generated the highest mass-loss flux (8.76 × 10⁻⁷ kg·m⁻²·s⁻¹), exhibited the lowest hardening, with hardness increasing only from 149 to 157 HV (+ 5.4%), together with evidence of indentation-assisted material removal. This inverse trend suggests that higher erosion rates continuously remove the work-hardened surface layer before it can fully develop and stabilize. Consequently, the more severe the erosion, the lower the hardness retained at the eroded surface. These findings establish a direct relationship between erosion severity, hardness evolution, microstructural response, and impact angle, while highlighting the need for erosion models that account for strain-hardening-dependent material evolution to improve predictive accuracy under slurry-jet erosion conditions.

Journal of Engineering and Applied ScienceVol. 73(1)
National School of Mineral Industry (MA)
Sustainable cities and communities
Openalex Percentile: Top 11%
Erosion and Abrasive Machining
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