{"id":{"repo_id":"siu-theses","oai_identifier":"oai:opensiuc.lib.siu.edu:dissertations-2399"},"canonical_url":"https://search.dev.ndltd.org/etd/siu-theses/oai:opensiuc.lib.siu.edu:dissertations-2399","repository":{"repo_id":"siu-theses","name":"Southern Illinois University","base_url":"https://opensiuc.lib.siu.edu/do/oai/"},"display":{"title":"Intruder Dynamic Response in Particulate Media","abstract":"Many everyday materials, broadly classified as ``particulate media'', are at the heart of many industries and natural phenomena. Examples range from the storage and transport of bulk foods and aggregates such as grains and coal; the processing of pharmaceutical pills and the grinding coffee beans; to the mitigation and cost control of life-threatening events like landslides, earthquakes, and silo failures. The common theme connecting all these phenomena is the mechanical stability of the granular material that arises from interactions at the microscopic level of the grain scale, and how this influences collective properties at the bulk, macroscopic scale. In this dissertation, we present an extensive study of the mechanical properties of a physics-based model of granular particle systems in two dimensions using computer simulations. Specifically, we study the dynamics of an intruder particle that is driven through a dense, disordered packing of particles. This practical technique has the benefit of being amenable to experimental application which we expect will motivate future studies in the area. We find the `microrheology' of the intruder can be traced back to the properties of underlying, original, unperturbed packing, thereby providing a method to characterize the mechanical properties of the material that may otherwise be unavailable. To perform this study, we initially created mechanically stable granular packings of bidisperse discs, for several orders of magnitude of particle friction coefficient $\\mu$, over a range in packing densities, or packing fractions $\\phi$, in the vicinity of the critical packing fraction $\\phi_c$, the density below which the packing is no longer stable. This range in $\\phi$ translates to a range in packing pressures $P$, spanning several orders of magnitude down to the $P\\rightarrow 0$ limit. For each packing, we apply a driving force to the intruder probe particle and find the critical force $F_{c}$, the minimum force required to induce motion of the probe as it is dragged through the system. We find that $F_{c}(\\mu)$ for the different friction packings, scales with the packing pressure $P$ as a power-law according to: $F_{c}(\\mu) - F_{c}^{o}(\\mu) \\sim P^{\\beta(\\mu)}$. The power-law exponent, $\\beta(\\mu)$ becomes friction dependent, but approaches the value, $\\beta(\\mu\\to0) = 1.0 \\pm 0.1$ in the zero-friction limit. $F_{c}^{o}(\\mu)$ is the value of $F_{c}$ in the limit $P \\to 0$, that similarly depends on the friction coefficient as, $F_{c}^{o}(\\mu) \\to 0$, when $\\mu \\to \\infty$. We use this property of $F_{c}^{o}(\\mu)$ to characterize the mechanical properties of different frictional packings. Another focus of this study is the `microrheology' of the intruder through force-velocity dependencies in $\\mu=0$ systems at different $P$. For this case, the intruder is driven through the packing at a steady-state velocity $<V>$, for driving forces above the critical force $F_D > F_c$. We introduce a scaling function that collapses the force-velocity curves onto a single master curve. This power law scaling of the collapsed curve as $P\\rightarrow 0$ is reminiscent of a continuous phase transition, reinforcing the notion that the mechanical state of the system exhibits critical-like features. Furthermore, we also find an alternative scaling collapse of the form: $<V>-<V_0> \\sim (F_{D} - F_{c})^{\\alpha}$, where $<V_{0}>$ represents a constant velocity term in the limit of small excess forcing, and the critical force $F_{c}$ now appears as fitting parameter that matches our explicit calculations. Thence, we are able to extract $F_{c}$ from a driven probe without a-priori having any knowledge about the state of the system. To further investigate the transition of the system through the different intruder force perturbations, we implemented a coarse graining (CG) technique that transforms our discrete particle interaction force information into continuous stress fields. Through this methodology, we are able to calculate the kinetic and contact stresses as the intruder is driven through the system. We are able to qualify and quantify the directional and distance dependencies of the stress response of the packing due to the driven probe via radial and azimuthal stress calculations. In particular, we find how the stress response not only captures the wake region behind the driven intruder, but also how the stress decays in the forward direction of the intruder, which follows universal behavior.","abstract_html":"Many everyday materials, broadly classified as ``particulate media&#x27;&#x27;, are at the heart of many industries and natural phenomena. Examples range from the storage and transport of bulk foods and aggregates such as grains and coal; the processing of pharmaceutical pills and the grinding coffee beans; to the mitigation and cost control of life-threatening events like landslides, earthquakes, and silo failures. The common theme connecting all these phenomena is the mechanical stability of the granular material that arises from interactions at the microscopic level of the grain scale, and how this influences collective properties at the bulk, macroscopic scale. In this dissertation, we present an extensive study of the mechanical properties of a physics-based model of granular particle systems in two dimensions using computer simulations. Specifically, we study the dynamics of an intruder particle that is driven through a dense, disordered packing of particles. This practical technique has the benefit of being amenable to experimental application which we expect will motivate future studies in the area. We find the `microrheology&#x27; of the intruder can be traced back to the properties of underlying, original, unperturbed packing, thereby providing a method to characterize the mechanical properties of the material that may otherwise be unavailable. To perform this study, we initially created mechanically stable granular packings of bidisperse discs, for several orders of magnitude of particle friction coefficient <span class=\"etd-inline-math\">&mu;</span>, over a range in packing densities, or packing fractions $\\phi$, in the vicinity of the critical packing fraction <span class=\"etd-inline-math\">\\phi<sub>c</sub></span>, the density below which the packing is no longer stable. This range in $\\phi$ translates to a range in packing pressures $P$, spanning several orders of magnitude down to the $P\\rightarrow 0$ limit. For each packing, we apply a driving force to the intruder probe particle and find the critical force <span class=\"etd-inline-math\">F<sub>c</sub></span>, the minimum force required to induce motion of the probe as it is dragged through the system. We find that <span class=\"etd-inline-math\">F<sub>c</sub>(&mu;)</span> for the different friction packings, scales with the packing pressure $P$ as a power-law according to: <span class=\"etd-inline-math\">F<sub>c</sub>(&mu;) - F<sub>c</sub><sup>o</sup>(&mu;) \\sim P<sup>&beta;(&mu;)</sup></span>. The power-law exponent, <span class=\"etd-inline-math\">&beta;(&mu;)</span> becomes friction dependent, but approaches the value, <span class=\"etd-inline-math\">&beta;(&mu;\\to0) = 1.0 \\pm 0.1</span> in the zero-friction limit. <span class=\"etd-inline-math\">F<sub>c</sub><sup>o</sup>(&mu;)</span> is the value of <span class=\"etd-inline-math\">F<sub>c</sub></span> in the limit $P \\to 0$, that similarly depends on the friction coefficient as, <span class=\"etd-inline-math\">F<sub>c</sub><sup>o</sup>(&mu;) \\to 0</span>, when <span class=\"etd-inline-math\">&mu; \\to \\infty</span>. We use this property of <span class=\"etd-inline-math\">F<sub>c</sub><sup>o</sup>(&mu;)</span> to characterize the mechanical properties of different frictional packings. Another focus of this study is the `microrheology&#x27; of the intruder through force-velocity dependencies in <span class=\"etd-inline-math\">&mu;=0</span> systems at different $P$. For this case, the intruder is driven through the packing at a steady-state velocity $&lt;V&gt;$, for driving forces above the critical force <span class=\"etd-inline-math\">F<sub>D</sub> &gt; F<sub>c</sub></span>. We introduce a scaling function that collapses the force-velocity curves onto a single master curve. This power law scaling of the collapsed curve as $P\\rightarrow 0$ is reminiscent of a continuous phase transition, reinforcing the notion that the mechanical state of the system exhibits critical-like features. Furthermore, we also find an alternative scaling collapse of the form: <span class=\"etd-inline-math\">&lt;V&gt;-&lt;V<sub>0</sub>&gt; \\sim (F<sub>D</sub> - F<sub>c</sub>)<sup>&alpha;</sup></span>, where <span class=\"etd-inline-math\">&lt;V<sub>0</sub>&gt;</span> represents a constant velocity term in the limit of small excess forcing, and the critical force <span class=\"etd-inline-math\">F<sub>c</sub></span> now appears as fitting parameter that matches our explicit calculations. Thence, we are able to extract <span class=\"etd-inline-math\">F<sub>c</sub></span> from a driven probe without a-priori having any knowledge about the state of the system. To further investigate the transition of the system through the different intruder force perturbations, we implemented a coarse graining (CG) technique that transforms our discrete particle interaction force information into continuous stress fields. Through this methodology, we are able to calculate the kinetic and contact stresses as the intruder is driven through the system. We are able to qualify and quantify the directional and distance dependencies of the stress response of the packing due to the driven probe via radial and azimuthal stress calculations. In particular, we find how the stress response not only captures the wake region behind the driven intruder, but also how the stress decays in the forward direction of the intruder, which follows universal behavior.","abstract_has_math":true,"creators":["Warnakulasooriya, Niranjan Mahaguruge"],"institution":null,"degree_name":"Doctor of Philosophy","degree_level":"Campus Only Dissertation","degree_discipline":"Physics","degree_department":null,"school":null,"contributors":["Silbert, Leonardo"],"advisors":[],"committee_chairs":[],"committee_members":[],"year":2017,"date_issued":"2017-05-01T07:00:00Z","date_published":"2017-05-01T07:00:00Z","updated_at":"2026-07-24T04:35:23Z","subjects":["coarse graining","contact stress","Granular materials","intruder","kinetic stress","Mechanical stability"],"languages":[],"rights":[],"rights_urls":[],"identifier_entries":[]},"links":{"outbound_url":"https://opensiuc.lib.siu.edu/dissertations/1395","outbound_label":"Repository record","outbound_source":"dc:identifier"},"metadata_groups":[{"id":"people","label":"People","entries":[{"key":"dc:contributor","label":"Contributor","values":["Silbert, Leonardo"]},{"key":"dc:creator","label":"Author","values":["Warnakulasooriya, Niranjan Mahaguruge"]}]},{"id":"academic_context","label":"Academic Context","entries":[{"key":"dc:date.available","label":"Dc Date Available","values":["2018-08-03T07:00:00Z"]},{"key":"thesis:degree_discipline","label":"Discipline","values":["Physics"]},{"key":"thesis:degree_level","label":"Degree Level","values":["Campus Only Dissertation"]},{"key":"thesis:degree_name","label":"Degree Name","values":["Doctor of Philosophy"]}]},{"id":"subjects_keywords","label":"Subjects and Keywords","entries":[{"key":"dc:subject","label":"Dc Subject","values":["coarse graining","contact stress","Granular materials","intruder","kinetic stress","Mechanical stability"]}]},{"id":"identifiers","label":"Identifiers","entries":[{"key":"dc:identifier","label":"Identifier","values":["https://opensiuc.lib.siu.edu/dissertations/1395"]}]},{"id":"additional","label":"Additional Metadata","entries":[{"key":"dc:description.abstract","label":"Abstract","values":["Many everyday materials, broadly classified as ``particulate media'', are at the heart of many industries and natural phenomena. Examples range from the storage and transport of bulk foods and aggregates such as grains and coal; the processing of pharmaceutical pills and the grinding coffee beans; to the mitigation and cost control of life-threatening events like landslides, earthquakes, and silo failures. The common theme connecting all these phenomena is the mechanical stability of the granular material that arises from interactions at the microscopic level of the grain scale, and how this influences collective properties at the bulk, macroscopic scale. In this dissertation, we present an extensive study of the mechanical properties of a physics-based model of granular particle systems in two dimensions using computer simulations. Specifically, we study the dynamics of an intruder particle that is driven through a dense, disordered packing of particles. This practical technique has the benefit of being amenable to experimental application which we expect will motivate future studies in the area. We find the `microrheology' of the intruder can be traced back to the properties of underlying, original, unperturbed packing, thereby providing a method to characterize the mechanical properties of the material that may otherwise be unavailable. To perform this study, we initially created mechanically stable granular packings of bidisperse discs, for several orders of magnitude of particle friction coefficient $\\mu$, over a range in packing densities, or packing fractions $\\phi$, in the vicinity of the critical packing fraction $\\phi_c$, the density below which the packing is no longer stable. This range in $\\phi$ translates to a range in packing pressures $P$, spanning several orders of magnitude down to the $P\\rightarrow 0$ limit. For each packing, we apply a driving force to the intruder probe particle and find the critical force $F_{c}$, the minimum force required to induce motion of the probe as it is dragged through the system. We find that $F_{c}(\\mu)$ for the different friction packings, scales with the packing pressure $P$ as a power-law according to: $F_{c}(\\mu) - F_{c}^{o}(\\mu) \\sim P^{\\beta(\\mu)}$. The power-law exponent, $\\beta(\\mu)$ becomes friction dependent, but approaches the value, $\\beta(\\mu\\to0) = 1.0 \\pm 0.1$ in the zero-friction limit. $F_{c}^{o}(\\mu)$ is the value of $F_{c}$ in the limit $P \\to 0$, that similarly depends on the friction coefficient as, $F_{c}^{o}(\\mu) \\to 0$, when $\\mu \\to \\infty$. We use this property of $F_{c}^{o}(\\mu)$ to characterize the mechanical properties of different frictional packings. Another focus of this study is the `microrheology' of the intruder through force-velocity dependencies in $\\mu=0$ systems at different $P$. For this case, the intruder is driven through the packing at a steady-state velocity $<V>$, for driving forces above the critical force $F_D > F_c$. We introduce a scaling function that collapses the force-velocity curves onto a single master curve. This power law scaling of the collapsed curve as $P\\rightarrow 0$ is reminiscent of a continuous phase transition, reinforcing the notion that the mechanical state of the system exhibits critical-like features. Furthermore, we also find an alternative scaling collapse of the form: $<V>-<V_0> \\sim (F_{D} - F_{c})^{\\alpha}$, where $<V_{0}>$ represents a constant velocity term in the limit of small excess forcing, and the critical force $F_{c}$ now appears as fitting parameter that matches our explicit calculations. Thence, we are able to extract $F_{c}$ from a driven probe without a-priori having any knowledge about the state of the system. To further investigate the transition of the system through the different intruder force perturbations, we implemented a coarse graining (CG) technique that transforms our discrete particle interaction force information into continuous stress fields. Through this methodology, we are able to calculate the kinetic and contact stresses as the intruder is driven through the system. We are able to qualify and quantify the directional and distance dependencies of the stress response of the packing due to the driven probe via radial and azimuthal stress calculations. In particular, we find how the stress response not only captures the wake region behind the driven intruder, but also how the stress decays in the forward direction of the intruder, which follows universal behavior."]},{"key":"dc:title","label":"Title","values":["Intruder Dynamic Response in Particulate Media"]}]}],"canonical_facts":{"dc:contributor":["Silbert, Leonardo"],"dc:creator":["Warnakulasooriya, Niranjan Mahaguruge"],"dc:date.available":["2018-08-03T07:00:00Z"],"dc:description.abstract":["Many everyday materials, broadly classified as ``particulate media'', are at the heart of many industries and natural phenomena. Examples range from the storage and transport of bulk foods and aggregates such as grains and coal; the processing of pharmaceutical pills and the grinding coffee beans; to the mitigation and cost control of life-threatening events like landslides, earthquakes, and silo failures. The common theme connecting all these phenomena is the mechanical stability of the granular material that arises from interactions at the microscopic level of the grain scale, and how this influences collective properties at the bulk, macroscopic scale. In this dissertation, we present an extensive study of the mechanical properties of a physics-based model of granular particle systems in two dimensions using computer simulations. Specifically, we study the dynamics of an intruder particle that is driven through a dense, disordered packing of particles. This practical technique has the benefit of being amenable to experimental application which we expect will motivate future studies in the area. We find the `microrheology' of the intruder can be traced back to the properties of underlying, original, unperturbed packing, thereby providing a method to characterize the mechanical properties of the material that may otherwise be unavailable. To perform this study, we initially created mechanically stable granular packings of bidisperse discs, for several orders of magnitude of particle friction coefficient $\\mu$, over a range in packing densities, or packing fractions $\\phi$, in the vicinity of the critical packing fraction $\\phi_c$, the density below which the packing is no longer stable. This range in $\\phi$ translates to a range in packing pressures $P$, spanning several orders of magnitude down to the $P\\rightarrow 0$ limit. For each packing, we apply a driving force to the intruder probe particle and find the critical force $F_{c}$, the minimum force required to induce motion of the probe as it is dragged through the system. We find that $F_{c}(\\mu)$ for the different friction packings, scales with the packing pressure $P$ as a power-law according to: $F_{c}(\\mu) - F_{c}^{o}(\\mu) \\sim P^{\\beta(\\mu)}$. The power-law exponent, $\\beta(\\mu)$ becomes friction dependent, but approaches the value, $\\beta(\\mu\\to0) = 1.0 \\pm 0.1$ in the zero-friction limit. $F_{c}^{o}(\\mu)$ is the value of $F_{c}$ in the limit $P \\to 0$, that similarly depends on the friction coefficient as, $F_{c}^{o}(\\mu) \\to 0$, when $\\mu \\to \\infty$. We use this property of $F_{c}^{o}(\\mu)$ to characterize the mechanical properties of different frictional packings. Another focus of this study is the `microrheology' of the intruder through force-velocity dependencies in $\\mu=0$ systems at different $P$. For this case, the intruder is driven through the packing at a steady-state velocity $<V>$, for driving forces above the critical force $F_D > F_c$. We introduce a scaling function that collapses the force-velocity curves onto a single master curve. This power law scaling of the collapsed curve as $P\\rightarrow 0$ is reminiscent of a continuous phase transition, reinforcing the notion that the mechanical state of the system exhibits critical-like features. Furthermore, we also find an alternative scaling collapse of the form: $<V>-<V_0> \\sim (F_{D} - F_{c})^{\\alpha}$, where $<V_{0}>$ represents a constant velocity term in the limit of small excess forcing, and the critical force $F_{c}$ now appears as fitting parameter that matches our explicit calculations. Thence, we are able to extract $F_{c}$ from a driven probe without a-priori having any knowledge about the state of the system. To further investigate the transition of the system through the different intruder force perturbations, we implemented a coarse graining (CG) technique that transforms our discrete particle interaction force information into continuous stress fields. Through this methodology, we are able to calculate the kinetic and contact stresses as the intruder is driven through the system. We are able to qualify and quantify the directional and distance dependencies of the stress response of the packing due to the driven probe via radial and azimuthal stress calculations. In particular, we find how the stress response not only captures the wake region behind the driven intruder, but also how the stress decays in the forward direction of the intruder, which follows universal behavior."],"dc:identifier":["https://opensiuc.lib.siu.edu/dissertations/1395"],"dc:subject":["coarse graining","contact stress","Granular materials","intruder","kinetic stress","Mechanical stability"],"dc:title":["Intruder Dynamic Response in Particulate Media"],"thesis:degree_discipline":["Physics"],"thesis:degree_level":["Campus Only Dissertation"],"thesis:degree_name":["Doctor of Philosophy"]},"updated_at":"2026-07-24T04:35:23Z"}