Ral Bielawski’s research while affiliated with University of Michigan and other places

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Publications (16)


FIG. 1: Schematic of initial and boundary conditions.
FIG. 2: Time sequence of liquid volume fraction contours (α l > 0.1) colored by temperature in the M s = 2 case.
FIG. 3: Time sequence of liquid volume fraction contours (α l > 0.1) colored by temperature in the M s = 3 case.
FIG. 5: Time sequence of z-midplane temperature contours in the M s = 3 case. α l = 1 isoline marked in white.
FIG. 6: (Left axis; solid lines) Droplet spreading over time. (Right axis; dashed lines) Droplet displacement over time.

+3

Timescales and Statistics of Shock-induced Droplet Breakup
  • Preprint
  • File available

April 2025

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26 Reads

Michael Ullman

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Ral Bielawski

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Detonation-based propulsion devices, such as rotating detonation engines (RDEs), must be able to leverage the higher energy densities of liquid fuels in order for them to be utilized in practical contexts. This necessitates a comprehensive understanding of the physical processes and timescales that dictate the shock-induced breakup of liquid droplets. These processes are difficult to probe and quantify experimentally, often limiting measurements to macroscopic properties. Here, fundamental mechanisms in such interactions are elucidated through detailed numerical simulation of Mach 2 and 3 shock waves interacting with 100 μ\mum water droplets. Using a thermodynamically consistent two-phase formulation with adaptive mesh refinement, the simulations capture droplet surface instabilities and atomization into secondary droplets in great detail. The results show that droplet breakup occurs through a coupled multi-stage process, including droplet flattening, formation of surface instabilities and piercing, and the shedding of secondary droplets from the ligaments of the deformed primary droplet. When considering the dimensionless timescale of Ranger and Nicholls (τ\tau), these processes occur at similar rates for the different shock strengths. The PDFs for the Sauter mean diameters of secondary droplets are bimodal log-normal distributions at τ=2\tau=2. Modest differences in the degree and rate of liquid mass transfer into droplets less than 5 μ\mum in diameter are hypothesized to partially derive from differences in droplet surface piercing modes. These results are illustrative of the complex multi-scale processes driving droplet breakup and have implications for the ability of shocks to effectively process liquid fuels.

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Thermochemical Equilibrium Analysis and Detailed Simulation of Conical Detonation Waves

January 2025

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12 Reads

Conical oblique detonation waves (ODWs) are studied with high-fidelity numerical simulations, including complex chemical kinetics for an ethylene-air mixture at standard temperature and pressure at a stoichiometric equivalence ratio and 14.6 μm spatial resolution resulting in 42 cells per induction length at a minimum. Control volume analysis is proposed through an equilibrium-based detonation polar algorithm to identify ODW regimes and perform thermodynamic analysis. This analysis enables the correct conditions for the three-dimensional simulation of conical ODWs that further informs their practical use in engine design. Detonation instabilities are shown to behave differently in three dimensions as multiple detonation instabilities collide, forming Mach stems with increased strength compared to two-dimensional detonations. The weak overdriven conical ODW allows cellular detonation structure that is highly irregular with instabilities moving axially along the detonation front. Large subsonic regions also provide opportunities for pressure waves to impact the detonation surface, potentially influencing the formation of detonation instability. The detonation structure observed in conical systems resembles that of two-dimensional oblique detonations formed by wedges and of planar cellular detonations.


Structure of three-dimensional conical oblique detonation waves

January 2025

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42 Reads

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1 Citation

Combustion and Flame

This study investigates the structure of conical detonations in premixed ethylene–air mixtures through two complementary approaches. First, a control volume-based model identifies the weakly overdriven region for stable wave formation, showing dependence on the inflow Mach number and highlighting the impact of incomplete heat release. Second, high-fidelity simulations with multistep chemical kinetics capture the formation of surface instabilities and the nature of the detonation waves. The thermodynamic analysis tool, validated against experimental data, computes detonation polars using a multi-species gas description and provides crucial insights into post-detonation properties and deflection angles for various cone half-angles. The results indicate that the regime of weakly overdriven detonations is confined by flow conditions and turning angles, with net heat release diminishing as these parameters increase. For the highest Mach number and turning angle considered, the heat release is observed to be less than 25% of the reaction enthalpy for the mixture. High-fidelity simulations corroborate the thermodynamic analysis and further demonstrate the formation of cellular instabilities on the detonation surface. For a conical system characterized by significant isentropic expansion and weaker initial shock compared to two-dimensional wedges, transverse waves reflecting off the cone surface lead to the formation of triple points, which catalyze instabilities. The overall detonation structure in conical systems is similar to that of two-dimensional wedge-based oblique detonations and planar cellular detonations.




An AMReX-based Compressible Reacting Flow Solver for High-speed Reacting Flows relevant to Hypersonic Propulsion

December 2024

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258 Reads

Shivank Sharma

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Ral Bielawski

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Oliver Gibson

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[...]

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This work presents a comprehensive framework for the efficient implementation of finite-volume-based reacting flow solvers, specifically tailored for high speed propulsion applications. Using the exascale computing project (ECP) based AMReX framework, a compressible flow solver for handling high-speed reacting flows is developed. This work is complementary to the existing PeleC solver, emphasizing specific applications that include confined shock-containing flows, stationary and moving shocks and detonations. The framework begins with a detailed exposition of the numerical methods employed, emphasizing their application to complex geometries and their effectiveness in ensuring accurate and stable numerical simulations. Subsequently, an in-depth analysis evaluates the solver's performance across canonical and practical geometries, with particular focus on computational cost and efficiency. The solver's scalability and robustness are demonstrated through practical test cases, including flow path simulations of scramjet engines and detailed analysis of various detonation phenomena.



Chemical Timescale Effects on Detonation Convergence

June 2024

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90 Reads

Numerical simulations of detonation-containing flows have emerged as crucial tools for designing next-generation power and propulsion devices. As these tools mature, it is important for the combustion community to properly understand and isolate grid resolution effects when simulating detonations. To this end, this work provides a comprehensive analysis of the numerical convergence of unsteady detonation simulations, with focus on isolating the impacts of chemical timescale modifications on convergence characteristics in the context of operator splitting. With the aid of an adaptive mesh refinement based flow solver, the convergence analysis is conducted using two kinetics configurations: (1) a simplified three-step model mechanism, in which chemical timescales in the detonation are modified by adjusting activation energies, and (2) a detailed hydrogen mechanism, in which chemical timescales are adjusted through ambient pressure modifications. The convergence of unsteady self-sustained detonations in one-dimensional channels is then analyzed with reference to steady-state theoretical baseline solutions using these mechanisms. The goal of the analysis is to provide a detailed comparison of the effects of grid resolution on both macroscopic (peak pressures and detonation wave speeds) and microscopic (detonation wave structure) quantities of interest, drawing connections between the deviations from steady-state baselines and minimum chemical timescales. This work uncovers resolution-dependent unsteady detonation regimes, and highlights the important role played by not only the chemical timescales, but also the ratio between chemical and induction timescales in the detonation wave structure on simulation convergence properties.



Citations (9)


... Our priority is on high-speed and reacting flow applications, for which this new solver provides the basis. In accompanying publications, we have extended the capability to multiphase methods [29,30], neural network-enabled chemistry for rapid GPU execution [6,31], and for in situ learning of models [32,33], and reduced order models for shock-containing flows [34]. ...

Reference:

An AMReX-based Compressible Reacting Flow Solver for High-speed Reacting Flows relevant to Hypersonic Propulsion
The Structure of Liquid and Gas Jets in a Supersonic Crossflow
  • Citing Conference Paper
  • January 2025

... Over the last decade, significant research efforts have focused on the development of detonation-based propulsion and power generation technologies, including rotating detonation engines (RDEs) [1,2], pulse detonation engines (PDEs) [3,4], linear or reflective detonation engines [5,6], and oblique detonation wave engines (ODWEs) [7][8][9]. While most studies have focused on gaseous fueling, practical detonation engines must be able to leverage the higher energy densities of liquid fuels. ...

Structure of three-dimensional conical oblique detonation waves
  • Citing Article
  • January 2025

Combustion and Flame

... Their results categorize five phases of the interaction: induction period, meridian spreading, tail formation, recurrent droplet piercing, and lagging breakup. The phases describe the interaction process observed in experiments: droplet deformation, shearing/stripping, and Rayleigh-Taylor (RT) piercing [25]. Eulerian-Eulerian simulations by Xu et al., of detonation-droplet interactions between an Argon diluted H 2 -O 2 detonation and a water droplet show that the breakup characteristics and dynamics vary due to the spatial locations of the detonation front, transverse waves, and triple point relative to the droplet location [26]. ...

Analysis of Secondary Droplet Formation by Shock Induced Break-up of Droplets
  • Citing Conference Paper
  • January 2024

... All numerical simulations in this study are based on the combustion suite PeleC 22 from AMReX, 23 and the solutions are run on a heterogeneous high performance computing (HPC) cluster consisting of NVIDIA RTX3090 graphic processing units (GPUs) and Intel i7-10700 central processing units (CPUs), with up to 10 GPUs used in parallel. This suite has been extensively validated and is widely used for simulations of compressible flow, including turbulent boundary layers, 24 shock-induced boundary layer separations, 25 combustion, 22,26 and detonation, 27,28 ensuring reliable and accurate results. ...

High-fidelity Computational Study of High-speed Reacting Jets in Crossflow
  • Citing Conference Paper
  • January 2024

... Full flowpath simulations of the University of Virginia Supersonic Combustion Facility (UVaSCF) with a cavity flameholder operating in dual ramjet/scramjet mode were carried out [67]. Simulation of the full flowpath is critical to capturing the correct fluid state and turbulence characteristics entering the combustor region. ...

High-Fidelity Numerical Simulations of a Scramjet Flowpath
  • Citing Conference Paper
  • January 2024

... To address this gap, high-fidelity simulations can be leveraged to probe the underlying microscale phenomena in greater detail. One common approach for simulating shock-and detonation-droplet interactions [23][24][25], as well as full-scale detonation engines [26][27][28], is to use Euler-Lagrangian formulations with empirical breakup and evaporation models. However, in order to examine breakup processes themselves, numerical approaches that capture or track phasic interfaces are needed. ...

Three-dimensional Numerical Simulations of a Liquid RP-2/O 2 based Rotating Detonation Engine
  • Citing Article
  • January 2024

Combustion and Flame

... To generate ground-truth detonation data to train the data-based models, the compressible reacting NS equations are solved using a flow solver developed at the University of Michigan based on the AMReX framework [77,78]. The solver is a block-structured adaptive mesh refinement (AMR) extension of the extensively verified UMReactingFlow [79] (note that although an AMR-based solver is employed here, grid refinement is not used in this study). A globally second-order finite-volume strategy is utilized, where advection terms are treated with slope-limited Harten-Lax-van Leer-Contact approximate Riemann solver [80] and diffusion terms are treated using standard central schemes. ...

Highly-scalable GPU-accelerated compressible reacting flow solver for modeling high-speed flows
  • Citing Article
  • June 2023

Computers & Fluids

... The value for volume-fraction is estimated based on the liquid fuel injection rate and is approximately 9 × 10 −5 . Even though realistic RDEs would employ liquid injectors which result in a wide distribution of droplets size and velocity [56], to fundamentally understand the effect of injected droplet size on mixing, vaporization, and detonation propagation, a monodisperse injection is considered here. The initialization procedure of the detonation wave in the periodic channel is carefully designed to minimize any numerical artifacts. ...

Detonation wave driven by aerosolized liquid RP-2 spray
  • Citing Article
  • November 2022

Proceedings of the Combustion Institute