Eric Plaza
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Eric Plaza has a total of 36 co-authors. Here are the top co-authors by number of shared publications:
- Leonardo Di. G. Sigalotti
Departamento de Ciencias Básicas, Universidad Autónoma Metropolitana, Unidad Azcapotzalco (UAM-A), Av. San Pablo 420, Colonia Nueva el Rosario, Alcaldía Azcapotzalco, Ciudad de México 02128, Mexico
3 shared publications - Claudia Trejo-Soto
Instituto de Física, Pontificia Universidad Católica de Valparaíso, Casilla 4059, Chile
2 shared publications - Bernardo Guerrero-Rodríguez
Facultad de Ciencias Naturales y Matemáticas, Escuela Superior Politécnica del Litoral (ESPOL), ESPOL Polytechnic University, Guayaquil, Ecuador
1 shared publication - Carlos Enrique Alvarado Rodríguez
Departamento de Ingenieria Quimica, División de Ciencias Naturales y Exactas (DCNyE), Universidad de Guanajuato, Guanajuato 03605, Mexico
1 shared publication D. Aguila
ESPOL
1 shared publicationE. Santacruz
ESPOL
1 shared publication
Latest Publications
- Open Access
- 8 October 2026
- Published by IOP Publishing in Classical and Quantum Gravity
- Vol. 43 (19) , 195009
Causal gravitational memory in the galactic testbed: a no-go theorem for consistent minimal historical gravity
We present a revised assessment of Consistent Minimal Historical Gravity, a framework in which apparent galactic-scale gravitational anomalies are interpreted as a causal, historical response to local entropy production. The conceptual point of this paper is not that a massive scalar mediator produces a Yukawa falloff, which is standard in scalar–tensor effective theories, but rather that a causal, local, ghost-free historical-gravity embedding with entropy-production source Q ( x ) does not evade this generic Yukawa limitation. The covariant parent theory contains two scalar degrees of freedom, ϕ and χ , but in the static weak-field regime relevant for galactic phenomenology, it reduces to an effective single-mediator Yukawa closure generated by ϕ – χ mixing. The resulting extra acceleration therefore decays either exponentially for m χ > 0 or as r − 2 for m χ = 0 , and thus never reproduces the MOND-like asymptotic scaling Δ a ∝ 1 / r . We confront this minimal realization with an exploratory Bayesian Markov Chain Monte Carlo fit to a 153-galaxy working subset of the Spitzer Photometry and Accurate Rotation Curves (SPARC) catalogue, and we compare the inferred coupling scale with Solar System constraints. Within the universal-coupling closure adopted here, the SPARC-preferred region around α ≈ 5 × 10 − 3 lies entirely inside the Cassini-excluded region ( α < 1.15 × 10 − 5 ), which corresponds to a separation of approximately 2.6 decades in coupling strength. We therefore interpret this result as a no-go theorem for the minimal universal-coupling realization of entropy-sourced historical gravity, rather than as a blanket exclusion of environmentally screened or otherwise non-minimal historical-gravity scenarios.
- 8 October 2026
- Published by IOP Publishing in Classical and Quantum Gravity
- Vol. 43 (19) , 195009
Open AccessCausal gravitational memory in the galactic testbed: a no-go theorem for consistent minimal historical gravity
We present a revised assessment of Consistent Minimal Historical Gravity, a framework in which apparent galactic-scale gravitational anomalies are interpreted as a causal, historical response to local entropy production. The conceptual point of this paper is not that a massive scalar mediator produces a Yukawa falloff, which is standard in scalar–tensor effective theories, but rather that a causal, local, ghost-free historical-gravity embedding with entropy-production source Q ( x ) does not evade this generic Yukawa limitation. The covariant parent theory contains two scalar degrees of freedom, ϕ and χ , but in the static weak-field regime relevant for galactic phenomenology, it reduces to an effective single-mediator Yukawa closure generated by ϕ – χ mixing. The resulting extra acceleration therefore decays either exponentially for m χ > 0 or as r − 2 for m χ = 0 , and thus never reproduces the MOND-like asymptotic scaling Δ a ∝ 1 / r . We confront this minimal realization with an exploratory Bayesian Markov Chain Monte Carlo fit to a 153-galaxy working subset of the Spitzer Photometry and Accurate Rotation Curves (SPARC) catalogue, and we compare the inferred coupling scale with Solar System constraints. Within the universal-coupling closure adopted here, the SPARC-preferred region around α ≈ 5 × 10 − 3 lies entirely inside the Cassini-excluded region ( α < 1.15 × 10 − 5 ), which corresponds to a separation of approximately 2.6 decades in coupling strength. We therefore interpret this result as a no-go theorem for the minimal universal-coupling realization of entropy-sourced historical gravity, rather than as a blanket exclusion of environmentally screened or otherwise non-minimal historical-gravity scenarios.
- 1 August 2025
- Published by AIP Publishing in Physics of Fluids
- Vol. 37 (8)
Smoothed particle hydrodynamics modeling and experimental validation of pressure-driven microchannel filling
The filling of microchannels represents a challenge from both the physical-mathematical and computational perspectives due to the inherent complexity of the phenomena involved, such as the solid–fluid interaction and inertial forces. In this paper, we propose a novel numerical approach to study the filling phenomenon and the dynamic of a fluid-air interface (front) advancement based on the smoothed particle hydrodynamics (SPH) method. We implemented a modified hydrostatic pressure within SPH simulations intended to generate an artificial fluid column that drives the fluid through the microchannels, thereby mimicking and controlling the microchannel filling process. The simulation results are successfully compared with an analytical model and experimental measurements, demonstrating that both experiments and simulations closely match the analytical solution. These findings highlight the robustness of the model and the experimental methodology employed while also demonstrating the ability of the SPH method to represent the pressure-driven filling phenomenon in microchannels realistically.
- 1 August 2025
- Published by AIP Publishing in Physics of Fluids
- Vol. 37 (8)
Smoothed particle hydrodynamics modeling and experimental validation of pressure-driven microchannel filling
The filling of microchannels represents a challenge from both the physical-mathematical and computational perspectives due to the inherent complexity of the phenomena involved, such as the solid–fluid interaction and inertial forces. In this paper, we propose a novel numerical approach to study the filling phenomenon and the dynamic of a fluid-air interface (front) advancement based on the smoothed particle hydrodynamics (SPH) method. We implemented a modified hydrostatic pressure within SPH simulations intended to generate an artificial fluid column that drives the fluid through the microchannels, thereby mimicking and controlling the microchannel filling process. The simulation results are successfully compared with an analytical model and experimental measurements, demonstrating that both experiments and simulations closely match the analytical solution. These findings highlight the robustness of the model and the experimental methodology employed while also demonstrating the ability of the SPH method to represent the pressure-driven filling phenomenon in microchannels realistically.
- Open Access
- 29 March 2025
- Published by Elsevier in Computational Particle Mechanics
- Vol. 12 (5) , 2729-2744
A pair potential force model for surface tension calculations with smoothed particle hydrodynamics
- 29 March 2025
- Published by Elsevier in Computational Particle Mechanics
- Vol. 12 (5) , 2729-2744
Open AccessA pair potential force model for surface tension calculations with smoothed particle hydrodynamics
- Open Access
- 1 March 2025
- Published by Sociedad Mexicana de Fisica A C in Revista Mexicana de Física
- Vol. 71 (2 Mar-Apr)
Consistency and errors in Smoothed Particle Hydrodynamics using several approaches in a 2D pipe
Smoothed Particle Hydrodynamics (SPH) has become a promising tool for the simulation of fluids. Although too much research has been addressed to improve the method over the years, a comparison of the errors and consistency evolution when trying different approaches are still necessary to define the best scheme for practical applications. Here, a two-dimensional Poiseuille flow test benchmark is employed to enforce comparisons when varying the kernel, the definition of the sound speed inthe pressure term, the viscosity and the Reynolds number.
- 1 March 2025
- Published by Sociedad Mexicana de Fisica A C in Revista Mexicana de Física
- Vol. 71 (2 Mar-Apr)
Open AccessConsistency and errors in Smoothed Particle Hydrodynamics using several approaches in a 2D pipe
Smoothed Particle Hydrodynamics (SPH) has become a promising tool for the simulation of fluids. Although too much research has been addressed to improve the method over the years, a comparison of the errors and consistency evolution when trying different approaches are still necessary to define the best scheme for practical applications. Here, a two-dimensional Poiseuille flow test benchmark is employed to enforce comparisons when varying the kernel, the definition of the sound speed inthe pressure term, the viscosity and the Reynolds number.
- Open Access
Smoothed Particle Hydrodynamics Simulations of Porous Medium Flow Using Ergun’s Fixed-Bed Equation
A popular equation that is often employed to represent the relationship between the pressure loss and the fluid flow in fluidized or packed granular beds is the Ergun equation, which is an extension of Darcy’s law. In this paper, the method of Smoothed Particle Hydrodynamics (SPH) is used to numerically study the flow field across a rectangular channel partially filled with a porous layer both at the Representative Elementary Volume (REV) scale using the Ergun equation and at the pore scale. Since the flow field can be estimated at the REV scale with a much lower cost compared to the pore scale, it is important to evaluate how accurately the pore-scale results can be reproduced at the REV scale. The comparison between both scales is made in terms of the velocity profiles at the outlet of the rectangular channel and the pressure losses across the clear and porous zones for three different arrays of solid grains at the pore scale. The results show that minimum differences in the flow structure and velocity profiles between the REV and the pore scale always occur at intermediate values of the porosity ( and 0.55). As the porosity increases, the differences between the REV and the pore scale also increase. The details of the pressure losses are affected by the geometry of the porous medium. In particular, we find that the pressure profiles at the REV scale match those at the pore scale almost independently of the porosity only when the grains are uniformly distributed in a non-staggered square array.Open AccessSmoothed Particle Hydrodynamics Simulations of Porous Medium Flow Using Ergun’s Fixed-Bed Equation
A popular equation that is often employed to represent the relationship between the pressure loss and the fluid flow in fluidized or packed granular beds is the Ergun equation, which is an extension of Darcy’s law. In this paper, the method of Smoothed Particle Hydrodynamics (SPH) is used to numerically study the flow field across a rectangular channel partially filled with a porous layer both at the Representative Elementary Volume (REV) scale using the Ergun equation and at the pore scale. Since the flow field can be estimated at the REV scale with a much lower cost compared to the pore scale, it is important to evaluate how accurately the pore-scale results can be reproduced at the REV scale. The comparison between both scales is made in terms of the velocity profiles at the outlet of the rectangular channel and the pressure losses across the clear and porous zones for three different arrays of solid grains at the pore scale. The results show that minimum differences in the flow structure and velocity profiles between the REV and the pore scale always occur at intermediate values of the porosity ( and 0.55). As the porosity increases, the differences between the REV and the pore scale also increase. The details of the pressure losses are affected by the geometry of the porous medium. In particular, we find that the pressure profiles at the REV scale match those at the pore scale almost independently of the porosity only when the grains are uniformly distributed in a non-staggered square array. - 3 June 2015
- Published by Springer Nature in Journal of Nanoparticle Research
- Vol. 17 (6) , 1-11
Electric field effect in the growth of carbon nanotubes
- 3 June 2015
- Published by Springer Nature in Journal of Nanoparticle Research
- Vol. 17 (6) , 1-11
Electric field effect in the growth of carbon nanotubes
- 12 January 2014
- Published by Springer Nature
- p. 345-356
Brownian Dynamics Simulation by Reticular Mapping Matrix Method
- 12 January 2014
- Published by Springer Nature
- p. 345-356
Brownian Dynamics Simulation by Reticular Mapping Matrix Method
- 1 September 2012
- Published by Elsevier in Journal of Magnetism and Magnetic Materials
- Vol. 324 (18) , 2926-2931
Effects of synthesis variables on the magnetic properties of CoFe2O4 nanoparticles
- 1 September 2012
- Published by Elsevier in Journal of Magnetism and Magnetic Materials
- Vol. 324 (18) , 2926-2931
Effects of synthesis variables on the magnetic properties of CoFe2O4 nanoparticles