{"id":579,"date":"2020-01-31T07:46:25","date_gmt":"2020-01-31T12:46:25","guid":{"rendered":"https:\/\/websitedemos.net\/alex26\/?page_id=8"},"modified":"2025-10-31T11:22:13","modified_gmt":"2025-10-31T15:22:13","slug":"research","status":"publish","type":"page","link":"https:\/\/me.jhu.edu\/fluidtransportlab\/research\/","title":{"rendered":"Research"},"content":{"rendered":"\t\t
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Our Research<\/h1>\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t
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High-temperature particle-laden turbulence and deposition <\/h2>\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t
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Through advancements in surface and interior cooling and use of robust materials for components, jet engines have experienced significant performance and efficiency boosts. In daily operation, volcanic ash, sand particles, and other air pollutants are ingested by jet engines, broken down to micron-scale sizes as they pass through the compressor, and heated to high temperature in the combustion chambers and turbine. It is important to understand the effects of these heated particles and their deposition on hot section surfaces that could compromise sensitive operating conditions, leading to performance downgrades and engine failures in extreme cases.\u00a0<\/span>\u00a0<\/span><\/p>

In this study, a novel high temperature turbulent flow channel has been developed, to replicate these outlined high temperature, multiphase turbulent flow conditions. Air flow is initially heated to 1100\u00b0C by a 60kW inline heater. Additional heating for the facility and reductions in heat loss from radiation are provided through encasing insulating sections surrounding the channel. Particles such as soda lime glass bead spheres and Arizona Road Dust are injected into the flow with compressed air jets in the mixing section. The channel height is then decreased in the contraction section to bring the facility to an aspect ratio of 10:1. Turbulent flow is then fully developed, and particle deposition is observed within the facility\u2019s test section.<\/span>\u00a0<\/span><\/p>

In-test observations include Lagrangian particle tracking and Digital Image Projection (DIP), using an overdriven LED to project a grid image into the channel and capture surface deposition through the image\u2019s displacement. Post-test analysis includes scanning of the test section\u2019s deposition substrates using Micro-CT.\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0<\/span>\u00a0<\/span><\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t

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Electrical discharges initiated by particle-laden turbulence<\/span><\/h2>\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t
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Turbulent flows laden with charged inertial particles are ubiquitous in both natural phenomena and industrial processes, such as sandstorms, thunderclouds, industrial sprays, and pharmaceutical powder manufacturing. Particles inevitably acquire charge through triboelectrification, diffusion, or field charging, introducing electrostatic interactions that can strongly influence their dynamics. Understanding how these interactions affect particle transport, electric field structures, and even discharge events is therefore of great scientific and practical interest.<\/span>\u00a0<\/span><\/p>

In this project, we construct an enclosed homogeneous isotropic turbulence (HIT) chamber, where turbulence with well-controlled properties is generated by symmetrically arranged propellers. Charged particles are introduced via compressed-air jets and acquire charge through triboelectric interactions with the injection tubes before entering the chamber. Using high-speed imaging and Lagrangian particle tracking, we capture and analyze the dynamics of charged particles in turbulence. In addition, the particle charge and the resulting electric field structures are measured using Faraday cups and electric field sensors. Finally, by applying a strong external electric field, we induce electric breakdowns. By correlating discharge events with the underlying electric field structures and particle distributions, we aim to uncover the intrinsic coupling between turbulence and electrical discharges, thereby advancing our understanding of the rich electrostatic phenomena occurring in both nature and industry.<\/span> \u00a0<\/span><\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t

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Vortex pair dynamics in stratified fluid<\/span><\/h2>\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t
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Vortex pairs play a crucial role in stratified flows, such as aircraft wake turbulence in the atmosphere and submarine-induced vortices in the ocean. In these flows, the presence of a density gradient fundamentally alters vortex evolution through baroclinic effects and stratification-induced instabilities. While numerical and theoretical studies have extensively explored these dynamics, experimental investigations remain limited due to the challenges of simultaneously measuring three-dimensional velocity and density fields.\u00a0<\/span><\/p>

In this study, we employ a scanning mirror system to generate multiple laser sheets, enabling multi-plane stereo Particle Image Velocimetry (stereo-PIV) to capture all three velocity components across multiple planes. By reconstructing these planes, we obtain a three-dimensional representation of the vortex structure. Simultaneously, we measure the density field using a fluorescent dye with concentration proportional to density, allowing visualization through laser-induced fluorescence. This approach provides a unique opportunity to analyze the interplay between velocity and density gradients, offering new insights into the evolution and stability of vortex pairs in stratified flows.<\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t

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Plume-Surface Interaction <\/h2>\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t
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With NASA embarking on a new journey to the moon, one of the key problems that needs to be solved is Plume-Surface Interaction (PSI). Where a jet, like one from a lunar lander, will impinge on the lunar soil and cause particles to be kicked up into the lunar atmosphere. These particles can liberate from the soil bed at such a high velocity that they can damage sensitive equipment on the lunar lander and anything in the surrounding area. It is crucial to investigate how these particles interact with the gas phase from the jet, which is expected to go at Mach 5, and how those particles will move relative to it. This project is fully funded by NASA.<\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t

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Particle Image Velocimetry <\/h2>\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t
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We are upgrading our jet facility system to use particle image velocimetry (PIV) to capture the gas phase velocity of our particle laden jet. By providing crucial information using this system on the velocity and overall dynamics of the gas phase, we can better understand how the particles interact with the surrounding flow. This is done by seeding the flow with tracer particles and using a pulsed laser system as a light source synchronized to a high-speed camera. This project is involved with our collaboration with NASA JPL and University of Michigan.<\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t

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We are working on improving the existing 3D particle tracking code to handle high tracer concentrations (up to 0.1 particle per pixel). The aim of this project is to demystify the high-concentration tracking algorithm in 3D and make it more transparent for students and non-experts to use. The other great feature of this new in-house code is the simple parallelization for computer clusters and quantification of propagation of experimental uncertainty. This will help us to better understand, evaluate, and eventually control the measurement uncertainties<\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t

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The\u00a0V-ONSET facility provides a unique flow environment for us to probe the inter-facial couplings between two phases in the Lagrangian framework. That includes bubble deformation and breakup physics, as well as simultaneous measurement of the surrounding turbulent flow.<\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t

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FATE (F<\/u>ish A<\/u>quarium with a T<\/u>urbulent E<\/u>nvironment)<\/h2>\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t
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(A)Our FATE (F<\/strong>ish A<\/strong>quarium with a T<\/strong>urbulent E<\/strong>nvironment) facility was designed to enable us to better understand how fish schools navigate through turbulent environments and how their dynamics modulates the background turbulence. This unique facility leverages a jet array to systematically control the intensity of the oncoming turbulence that the fish schools will encounter. (B) Demonstrates the range of turbulence intensities (I<\/i>) achievable in this facility as a function of the injection ratio (J<\/i>). Using high-speed cameras, the (C)-(D) dynamics of the fish school can be recorded, and (E) the school\u2019s wake can be measured using our in-house Lagrangian Particle Tracking code (OpenLPT).<\/span><\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t

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To better understand how fish react to unsteady flows, it is necessary to intercept the hydrodynamic signals sensed by their lateral line in a non-invasive manner. To do this, we utilize a physics-informed neural network (PINN) to predict an optimized solution for the velocity and pressure fields that satisfy the governing equations and the constraints from the PIV measurements. The PINN method can provide an accurate prediction of the pressure signals sensed by the fish.\u00a0<\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t

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Reference = 2D slice from DNS data, Regressed = PINN Prediction <\/figcaption>\n\t\t\t\t\t\t\t\t\t\t<\/figure>\n\t\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t
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Enhanced Visual Hull Reconstruction<\/h2>\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t
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A perfect geometrical reconstruction of a sophisticated 3D object requires infinite optical views covering all possible angles around the object. This is not always feasible or affordable for high-speed imaging, as the fast cameras are expensive. With the reduced number of cameras, the traditional Visual Hull method suffers from a problem that some virtual mass appears in the reconstructed volume, contributing to relatively large uncertainties. We have designed a novel virtual camera method to mitigate this problem. This framework is designed mostly for our bubbly flow application, but it can also be used for other applications. Please send Dr. Rui Ni an email if you want to collaborate on this idea.<\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t

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Interfacial Mass Transfer<\/h2>\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t
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Multiphase flow can often find its applications in boiling heat transfer and chemical and biological reactors. A common feature of these applications is the mass and heat exchange between two phases via complex interfaces. The aim of this project is to unveil the underlying physical processes and bridge the scale difference between the microscopic interfacial dynamics to macroscopic transport and mixing statistics.<\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t

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Porous Medium Flow<\/h2>\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t
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Multiphase flow is also ubiquitous in subsurface oil reservoir, where the environment is rather porous. If a porous medium flow is contaminated with fine particles, those particles can gradually deposit on the surface of grains, reducing the permeability of the reservoir and thus lowering the production efficiency of oil. Supported by the American Chemical Society PRF grant, we aim to provide new insights in this problem by visualizing the entire process in a refractive-index-matched porous flow system.<\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t

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Our Research High-temperature particle-laden turbulence and deposition Through advancements in surface and interior cooling and use of robust materials for components, jet engines have experienced significant performance and efficiency boosts. In daily operation, volcanic ash, sand particles, and other air pollutants are ingested by jet engines, broken down to micron-scale sizes as they pass through […]<\/p>\n","protected":false},"author":18,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"_monsterinsights_skip_tracking":false,"_monsterinsights_sitenote_active":false,"_monsterinsights_sitenote_note":"","_monsterinsights_sitenote_category":0,"site-sidebar-layout":"no-sidebar","site-content-layout":"page-builder","ast-site-content-layout":"default","site-content-style":"default","site-sidebar-style":"default","ast-global-header-display":"","ast-banner-title-visibility":"","ast-main-header-display":"","ast-hfb-above-header-display":"","ast-hfb-below-header-display":"","ast-hfb-mobile-header-display":"","site-post-title":"","ast-breadcrumbs-content":"","ast-featured-img":"disabled","footer-sml-layout":"","ast-disable-related-posts":"","theme-transparent-header-meta":"enabled","adv-header-id-meta":"","stick-header-meta":"","header-above-stick-meta":"","header-main-stick-meta":"","header-below-stick-meta":"","astra-migrate-meta-layouts":"default","ast-page-background-enabled":"default","ast-page-background-meta":{"desktop":{"background-color":"","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""},"tablet":{"background-color":"","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""},"mobile":{"background-color":"","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""}},"ast-content-background-meta":{"desktop":{"background-color":"var(--ast-global-color-5)","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""},"tablet":{"background-color":"var(--ast-global-color-5)","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""},"mobile":{"background-color":"var(--ast-global-color-5)","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""}},"footnotes":""},"class_list":["post-579","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/me.jhu.edu\/fluidtransportlab\/wp-json\/wp\/v2\/pages\/579","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/me.jhu.edu\/fluidtransportlab\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/me.jhu.edu\/fluidtransportlab\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/me.jhu.edu\/fluidtransportlab\/wp-json\/wp\/v2\/users\/18"}],"replies":[{"embeddable":true,"href":"https:\/\/me.jhu.edu\/fluidtransportlab\/wp-json\/wp\/v2\/comments?post=579"}],"version-history":[{"count":114,"href":"https:\/\/me.jhu.edu\/fluidtransportlab\/wp-json\/wp\/v2\/pages\/579\/revisions"}],"predecessor-version":[{"id":3155,"href":"https:\/\/me.jhu.edu\/fluidtransportlab\/wp-json\/wp\/v2\/pages\/579\/revisions\/3155"}],"wp:attachment":[{"href":"https:\/\/me.jhu.edu\/fluidtransportlab\/wp-json\/wp\/v2\/media?parent=579"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}