{"id":{"repo_id":"uiuc","oai_identifier":"oai:www.ideals.illinois.edu:2142/109348"},"canonical_url":"https://search.dev.ndltd.org/etd/uiuc/oai:www.ideals.illinois.edu:2142/109348","repository":{"repo_id":"uiuc","name":"University of Illinois - Urbana-Champaign","base_url":"https://www.ideals.illinois.edu/oai-pmh"},"display":{"title":"Rheological properties, stochastic characteristics, and second law violations of atomic fluids in Couette flow","abstract":"Fluids treated as a discrete collection of particles rather than as a continuum, exhibit exotic properties under shear at sub-continuum scales. For instance, at a critical strain-rate, the fluid becomes non-Newtonian owing to an ordering transition and the thermodynamic entropy production can be negative on small length and time scales due to the probabilistic nature of the system observables. Therefore, a complete characterization and study of fluid behavior is accomplished through the interplay between statistical and continuum mechanics. Molecular dynamics (MD) is naturally suited to provide insight into the behavior of such systems. It has been widely used to probe the behavior of a wide variety of systems on very small length and time scales. This research focuses on understanding the rheological nature, in particular, shear-thinning of atomic fluids to obtain a general constitutive relationship between shear-stress and strain-rate. We studied the statistical characteristics of the fluid properties to gain insight into the structural features that result in non-Newtonian behavior, the system’s tendency to violate the second law of thermodynamics, and the latter’s consequences for continuum theories. Using non-equilibrium molecular dynamics (NEMD) simulations, we study the shear-stress under steady-state conditions and its dependency on fluid properties (temperature and density) and applied shear-strain rate. The term strain-rate, more common in the physics literature, is used here in place of deformation rate. We propose a rheological equation of state that fits observed system responses exceptionally well and captures the extreme shear-thinning effect. This model arises naturally from the Boltzmann equation and kinetic theory and gives rise to a viscosity model similar to the well-established Cross model, but absent empirical parameters. The model possesses an inherent scaling parameter that unifies the rheological properties of the Lennard-Jones (LJ) fluid. Additionally, the probabilistic nature of the shear stress and the system’s tendency to violate the second law of thermodynamics is investigated by observing negative shear-stress increments. We draw conclusions on the implications these phenomena have on continuum theories adapted to atomic fluids such as flow stability. Building on these models, we aim to understand the transitions to turbulence and flow instability in atomic fluids. Via the Poincaré inequality, we generalize a classical continuum methodology to atomic fluids and obtain a fluid dependent lower bound on the critical Reynolds number.","abstract_html":"Fluids treated as a discrete collection of particles rather than as a continuum, exhibit exotic properties under shear at sub-continuum scales. For instance, at a critical strain-rate, the fluid becomes non-Newtonian owing to an ordering transition and the thermodynamic entropy production can be negative on small length and time scales due to the probabilistic nature of the system observables. Therefore, a complete characterization and study of fluid behavior is accomplished through the interplay between statistical and continuum mechanics. Molecular dynamics (MD) is naturally suited to provide insight into the behavior of such systems. It has been widely used to probe the behavior of a wide variety of systems on very small length and time scales. This research focuses on understanding the rheological nature, in particular, shear-thinning of atomic fluids to obtain a general constitutive relationship between shear-stress and strain-rate. We studied the statistical characteristics of the fluid properties to gain insight into the structural features that result in non-Newtonian behavior, the system’s tendency to violate the second law of thermodynamics, and the latter’s consequences for continuum theories. Using non-equilibrium molecular dynamics (NEMD) simulations, we study the shear-stress under steady-state conditions and its dependency on fluid properties (temperature and density) and applied shear-strain rate. The term strain-rate, more common in the physics literature, is used here in place of deformation rate. We propose a rheological equation of state that fits observed system responses exceptionally well and captures the extreme shear-thinning effect. This model arises naturally from the Boltzmann equation and kinetic theory and gives rise to a viscosity model similar to the well-established Cross model, but absent empirical parameters. The model possesses an inherent scaling parameter that unifies the rheological properties of the Lennard-Jones (LJ) fluid. Additionally, the probabilistic nature of the shear stress and the system’s tendency to violate the second law of thermodynamics is investigated by observing negative shear-stress increments. We draw conclusions on the implications these phenomena have on continuum theories adapted to atomic fluids such as flow stability. Building on these models, we aim to understand the transitions to turbulence and flow instability in atomic fluids. Via the Poincaré inequality, we generalize a classical continuum methodology to atomic fluids and obtain a fluid dependent lower bound on the critical Reynolds number.","abstract_has_math":false,"creators":["Raghavan, Bharath Venkatesh"],"institution":"University of Illinois at Urbana-Champaign","degree_name":"Ph.D.","degree_level":"Dissertation","degree_discipline":"Theoretical & Applied Mechanics","degree_department":null,"school":null,"contributors":["Ostoja-Starzewski, Martin","Schleife, Andre","Patricio Chamorro Chavez, Leonardo","Liebenberg, Leon"],"advisors":[],"committee_chairs":[],"committee_members":[],"year":2021,"date_issued":"2021-03-05T21:36:53Z","date_published":"2021-03-05T21:36:53Z","updated_at":"2026-07-22T22:24:50Z","subjects":["rheology","molecular dynamics","stochastic","shear-thinning","second law of thermodynamics","fluid dynamics","fluid mechanics"],"languages":["en"],"rights":["Copyright 2020 Bharath Venkatesh Raghavan"],"rights_urls":[],"identifier_entries":[]},"links":{"outbound_url":"http://hdl.handle.net/2142/109348","outbound_label":"Handle","outbound_source":"dc:identifier"},"metadata_groups":[{"id":"people","label":"People","entries":[{"key":"dc:contributor","label":"Contributor","values":["Ostoja-Starzewski, Martin","Schleife, Andre","Patricio Chamorro Chavez, Leonardo","Liebenberg, Leon"]},{"key":"dc:creator","label":"Author","values":["Raghavan, Bharath Venkatesh"]}]},{"id":"academic_context","label":"Academic Context","entries":[{"key":"dc:date","label":"Dc Date","values":["2021-03-05T21:36:53Z","2020-11-04","2020-12"]},{"key":"dc:type","label":"Dc Type","values":["text","Thesis"]},{"key":"thesis:degree_discipline","label":"Discipline","values":["Theoretical & Applied Mechanics"]},{"key":"thesis:degree_level","label":"Degree Level","values":["Dissertation"]},{"key":"thesis:degree_name","label":"Degree Name","values":["Ph.D."]},{"key":"thesis:institution_name","label":"Thesis Institution Name","values":["University of Illinois at Urbana-Champaign"]}]},{"id":"subjects_keywords","label":"Subjects and Keywords","entries":[{"key":"dc:subject","label":"Dc Subject","values":["rheology","molecular dynamics","stochastic","shear-thinning","second law of thermodynamics","fluid dynamics","fluid mechanics"]}]},{"id":"language_rights","label":"Language and Rights","entries":[{"key":"dc:language","label":"Dc Language","values":["en"]},{"key":"dc:rights","label":"Dc Rights","values":["Copyright 2020 Bharath Venkatesh Raghavan"]}]},{"id":"identifiers","label":"Identifiers","entries":[{"key":"dc:identifier","label":"Identifier","values":["http://hdl.handle.net/2142/109348"]}]},{"id":"additional","label":"Additional Metadata","entries":[{"key":"dc:description","label":"Description","values":["Fluids treated as a discrete collection of particles rather than as a continuum, exhibit exotic properties under shear at sub-continuum scales. For instance, at a critical strain-rate, the fluid becomes non-Newtonian owing to an ordering transition and the thermodynamic entropy production can be negative on small length and time scales due to the probabilistic nature of the system observables. Therefore, a complete characterization and study of fluid behavior is accomplished through the interplay between statistical and continuum mechanics. Molecular dynamics (MD) is naturally suited to provide insight into the behavior of such systems. It has been widely used to probe the behavior of a wide variety of systems on very small length and time scales. This research focuses on understanding the rheological nature, in particular, shear-thinning of atomic fluids to obtain a general constitutive relationship between shear-stress and strain-rate. We studied the statistical characteristics of the fluid properties to gain insight into the structural features that result in non-Newtonian behavior, the system’s tendency to violate the second law of thermodynamics, and the latter’s consequences for continuum theories. Using non-equilibrium molecular dynamics (NEMD) simulations, we study the shear-stress under steady-state conditions and its dependency on fluid properties (temperature and density) and applied shear-strain rate. The term strain-rate, more common in the physics literature, is used here in place of deformation rate. We propose a rheological equation of state that fits observed system responses exceptionally well and captures the extreme shear-thinning effect. This model arises naturally from the Boltzmann equation and kinetic theory and gives rise to a viscosity model similar to the well-established Cross model, but absent empirical parameters. The model possesses an inherent scaling parameter that unifies the rheological properties of the Lennard-Jones (LJ) fluid. Additionally, the probabilistic nature of the shear stress and the system’s tendency to violate the second law of thermodynamics is investigated by observing negative shear-stress increments. We draw conclusions on the implications these phenomena have on continuum theories adapted to atomic fluids such as flow stability. Building on these models, we aim to understand the transitions to turbulence and flow instability in atomic fluids. Via the Poincaré inequality, we generalize a classical continuum methodology to atomic fluids and obtain a fluid dependent lower bound on the critical Reynolds number.","Submission original under an indefinite embargo labeled 'Open Access'. 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For instance, at a critical strain-rate, the fluid becomes non-Newtonian owing to an ordering transition and the thermodynamic entropy production can be negative on small length and time scales due to the probabilistic nature of the system observables. Therefore, a complete characterization and study of fluid behavior is accomplished through the interplay between statistical and continuum mechanics. Molecular dynamics (MD) is naturally suited to provide insight into the behavior of such systems. It has been widely used to probe the behavior of a wide variety of systems on very small length and time scales. This research focuses on understanding the rheological nature, in particular, shear-thinning of atomic fluids to obtain a general constitutive relationship between shear-stress and strain-rate. We studied the statistical characteristics of the fluid properties to gain insight into the structural features that result in non-Newtonian behavior, the system’s tendency to violate the second law of thermodynamics, and the latter’s consequences for continuum theories. Using non-equilibrium molecular dynamics (NEMD) simulations, we study the shear-stress under steady-state conditions and its dependency on fluid properties (temperature and density) and applied shear-strain rate. The term strain-rate, more common in the physics literature, is used here in place of deformation rate. We propose a rheological equation of state that fits observed system responses exceptionally well and captures the extreme shear-thinning effect. This model arises naturally from the Boltzmann equation and kinetic theory and gives rise to a viscosity model similar to the well-established Cross model, but absent empirical parameters. The model possesses an inherent scaling parameter that unifies the rheological properties of the Lennard-Jones (LJ) fluid. Additionally, the probabilistic nature of the shear stress and the system’s tendency to violate the second law of thermodynamics is investigated by observing negative shear-stress increments. We draw conclusions on the implications these phenomena have on continuum theories adapted to atomic fluids such as flow stability. Building on these models, we aim to understand the transitions to turbulence and flow instability in atomic fluids. Via the Poincaré inequality, we generalize a classical continuum methodology to atomic fluids and obtain a fluid dependent lower bound on the critical Reynolds number.","Submission original under an indefinite embargo labeled 'Open Access'. The submission was exported from vireo on 2021-03-04 without embargo terms","The student, Bharath Raghavan, accepted the attached license on 2020-10-23 at 11:58.","The student, Bharath Raghavan, submitted this Dissertation for approval on 2020-10-23 at 12:29.","This Dissertation was approved for publication on 2020-11-04 at 10:38.","DSpace SAF Submission Ingestion Package generated from Vireo submission #15848 on 2021-03-04 at 15:34:13","Made available in DSpace on 2021-03-05T21:36:53Z (GMT). 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