Vivek V. Buwa’s research while affiliated with Indian Institute of Technology Ropar and other places

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Publications (84)


(i) Experimental setup, (ii) image processing methodology: (a) raw image, (b) monochromatic image, (c) outlines of oil layer extracted using multiple images, and (d) averaged distribution of oil layer obtained using MATLAB.
(a) Solution domain (all dimensions are in mm), (b) computational mesh over a vertical plane, and (c) grid refinement near the inlet.
Comparison of measured and modeled oil layer distribution for ṁG of (a) 2.33×10−5  kg/s, and (b) 4.66  ×10−5 kg/s, ( h=15 mm).
Comparison of measured and modeled octane layer distribution for ṁG of (a) 2.33×10−5 kg/s and (b) 4.66  ×10−5 kg/s, ( h=15 mm).
Schematic of (a) undeformed and (b) deformed liquid–liquid interface, (c) schematic showing different forces acting on the deformed interface [blue: inertial force ( FI) exerted by water, black: gravitational force ( FG) exerted by the oil phase, yellow: viscous force ( FV) exerted by oil phase, and white: interfacial tension force ( Fσ) acting on the oil–water interface].

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Discrete particle-volume of fluid simulations of a bubble plume rising through two immiscible liquids
  • Article
  • Publisher preview available

March 2025

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20 Reads

Sujata Sen

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Sayantan Biswas

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Vivek V. Buwa

Bubbles rising through immiscible liquids are commonly encountered in various applications, e.g., in the steel-making and refining process. In the present work, we have modeled a bubble plume rising through an oil–water interface using the combined discrete particle method and volume of fluid method. The relative contributions of different forces (inertial, gravitational, viscous, and interfacial tension), which govern the oil phase distribution and oil–water interface topology, are investigated by varying the liquid properties (density, viscosity, and interfacial tension) and operating conditions (thickness of oil layer, gas flow rate, and bubble size). We show that the interplay among gravitational, inertial, and interfacial tension forces governs the oil–water interface topology, while the viscous force exerted by an oil layer has a negligible influence. We identified four different interface topology regimes: (i) mildly deformed, (ii) partially deformed, (iii) fully exposed, and (iv) dispersed regime, and a corresponding regime map is proposed using modified Froude ( Fr*) and capillary numbers ( Ca). For Fr*<1, the oil–water interface topology is predominantly governed by the gravitational force exerted by an oil phase, whereas for Fr*>3.2 the interface topology is governed by the inertial force exerted by water. The interfacial tension force dominates for Ca<0.08 and 1>Fr*>1.6, Ca<0.04 and 1.6>Fr*>2.2.

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Experimental characterization of dynamics of bed‐scale liquid spreading in a trickle bed

August 2024

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35 Reads

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1 Citation

We report measurements performed to understand the effects of gas (QG) and liquid (QL) flow rates, surface tension (σGL), liquid viscosity (μL), and particle diameter (dp) on dynamics of local liquid spreading, pressure drop, and overall liquid holdup in a pseudo‐2D trickle bed. We show that an increase in the gas‐phase inertia leads to a decrease in the lateral liquid spreading, whereas an increase in the liquid‐phase inertia leads to an increase in the lateral liquid spreading. We also show that an increase in dp causes a reduction in the lateral liquid spreading. Using dimensionless numbers (AB and We), we propose a regime map showing contributions of different forces to the local liquid spreading. We show that the interplay between the inertia and capillary forces governs the liquid distribution near the inlet, whereas the relative contribution of gravitational force increases toward the outlet. Finally, we propose a relation between AB and We for “bed‐scale” liquid spreading.



Effect of Bubbling/Spouting Behavior on Dynamics of Segregation of Particles with Different Size and Density Ratios

February 2024

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12 Reads

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4 Citations

Industrial & Engineering Chemistry Research

Local bubbling/spouting behavior significantly influences the segregation/mixing of particles in several chemical and energy generation processes. In the present work, we performed Eulerian simulations of binary gas–solids flows of particles (Geldart Group A, B, and D) with different size or/and density ratios for varied bed compositions, superficial gas velocity (UG), and using different modes of gas-injection: uniform, two-jet, and single-jet. We quantified the roles of gas–solid and particle–particle momentum exchange in segregation/mixing behavior under different operating conditions. For the binary mixtures differing in size or density operated at similar ratios of UG to final fluidization velocity (Uff) (i.e., UG/Uff = ∼1), we show that the differences in the minimum fluidization velocities (Umf) of the individual solid phases played a key role in significant differences in gas–solid drag forces that resulted in segregation. For binary mixtures fluidized using two-jet and single-jet distributors, we found that the solids recirculation increased in comparison to that of the uniform distributor. This enhanced the interaction of low-density solids having higher velocity with high-density solids having lower velocity and resulted in a higher particle–particle momentum exchange. Such an increase enhanced the mixing of the solid phases in the case of two-jet/single-jet distributors. An increase in the composition of higher-density solids reduced the size of jets. This reduced the recirculatory cells, decreased the velocity of the higher-density solids and resulted in segregation. The predicted spouting behavior and time-evolution of the mixing index agreed well with the measurements.



Effect of Local Hydrodynamics on the Performance of a Fluidized-Bed Gasifier

July 2023

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25 Reads

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8 Citations

Industrial & Engineering Chemistry Research

Fluidized beds are widely used for chemical processing and power generation processes. It is important to understand how the local hydrodynamics and bubbling characteristics influence the spatial distributions of gas and solid phases, heat and mass transfer, reaction rates, and ultimately the performance of the fluidized-bed reactors. In the present work, we simulated the coal gasification process in a fluidized-bed gasifier and analyzed the differences in local bubbling behaviors caused by the use of different models for gas-inert solid phase (i.e., sand) momentum exchange (βgas-inert). We investigated the effect of the local bubbling behavior on the spatial distributions of coal and inert solid phases, heterogeneous reaction rates, temperatures, species distributions of coal and gas phases, and eventually on the syngas quality. In a case with higher/variable reactor temperature, we show that the segregation of the less dense coal phase in the top (due to low βgas-inert) led to a high char combustion rate locally and low CO2 and H2O gasification rates. However, the cases with a higher magnitude for βgas-inert resulted in a well-mixed state of inert and coal phases and led to homogeneity in the heterogeneous reaction rates, temperature, and species distributions of coal and gas phases. Overall, a well-mixed bed resulted in higher gasification efficiency, gas yield, and carbon conversion rate than the segregated bed. Further, the gasification efficiency and gas yield are found to be higher for the variable temperature reactor than the constant temperature reactor due to low steam and CO2 gasification rates in the latter case. The predictions agreed well with the corresponding measurements reported in the literature for different coal mass flow rates.



Citations (64)


... Significant research efforts are also being made to simulate the local liquid distribution in the trickle bed using the continuum (Eulerian) method. 30 While it is known that the Eulerian CFD models can predict the overall liquid holdup and pressure drop reasonably well, the ability of such CFD models to predict the local liquid holdup is not established and is limited by the availability of the measurements on the local liquid distribution. Therefore, it is important to have simultaneous measurements of overall as well as local liquid distribution for a wide range of operating conditions for the development and rigorous validation of the CFD models. ...

Reference:

Experimental characterization of dynamics of bed‐scale liquid spreading in a trickle bed
Eulerian Simulations of Local Liquid Distribution in a Trickle Bed: Effects of Flow Rates and Liquid Properties
  • Citing Article
  • August 2023

Chemical Engineering Science

... Another study focused on the effect of the local bubble behaviors (β gas-inlert , gasinert solid phase momentum exchange using different drag models) on heterogeneous reaction rate, gas phase temperature, and gas compositions. With a high β gas-inlert , the mixing content of coal and inert solid phase increases, resulting in a high content of H 2 and CO (Parvathaneni et al. 2023). Bubble containing various combustible gas (H 2 , CO, and CH 4 ) were mainly found in the lower part of the gasifier . ...

Effect of Local Hydrodynamics on the Performance of a Fluidized-Bed Gasifier
  • Citing Article
  • July 2023

Industrial & Engineering Chemistry Research

... Thus far, various numerical and experimental approaches have been employed to investigate the two-phase hydrodynamics inside a trickle bed. Particle-resolved Computational Fluid Dynamics (CFD) methods, such as the Volume of Fluid (VOF) method [5][6][7][8][9][10] and Euler-Euler methods, [11][12][13] are a couple of popular numerical approaches to model and investigate trickle beds. 14 An appropriate experimental technique that can provide local information on the two-phase flow texture and hydrodynamics inside a trickle bed can greatly help validate and develop such computational models. ...

Forces governing the dynamics of liquid spreading in packed beds

Journal of Fluid Mechanics

... A tapered FB with an increase in the cross section from bottom to top is considered unlike the cylindrical FB in FIOR and FINMET processes. For a similar operating flow rate, due to less injection area in a tapered FB than in a cylindrical FB, the gas velocity is high in the tapered FB. 45,46 Due to this, in the tapered FB, iron ore with a wide size distribution can be homogenously fluidized with a lower elutriation rate than in the cylindrical FB. 47 Cyclones with a dip-leg are present in the FB, and the transport disengagement height is optimized to minimize elutriation and heat loss. 44 The hematite fine ore typically in the mean size range of 1− 2 mm (maximum size up to 8 mm) is pneumatically charged into the Stage-I FB (i.e., R4) reactor and conveyed to the next stages 48,49 (see Figure 8). ...

Eulerian simulations of bubbling and jetting regimes in a fluidized bed
  • Citing Article
  • June 2022

Particuology

... This is being used in the measurement of scalar concentration fields in fluid flows which can be resolved both spatially and in time [1][2][3]. The technique is widely used and is being adopted in many fields including but not limited to investigation of reacting flows [4], study of heat transfer characteristics [5], fluorescent thermometry using LIF [6,7], eduction of 3D time resolved concentration field [8,9] and simultaneous momentum and concentration measurement [10][11][12] to name a few. The scalar whose concentration is to be measured is 'tagged' with a small amount of a suitable fluorescent dye (e.g. ...

PIV and PLIF measurements of interacting bubble plumes and their role in liquid‐phase mixing in a shallow vessel

... From a hydrodynamic standpoint, these simulation studies provide insightful analysis that helps to optimize, design, and run fixed-bed reactors. Besides these, for the area of multiphase flow CFD simulations, the development of PRCFD has provided an excellent modeling tool for detailed simulations of hydrodynamics in the structure of packed packing [23][24][25][26]. In addition, as a precise modeling tool for PRCFD simulations of packed bed hydrodynamics, it has been utilized for comparative analyses with other methods and measurement techniques, such as pore network modeling [27], Magnetic Resonance Imaging (MRI) [28], and Particle Image Velocimetry (PIV) regarding packed bed hydrodynamics [29]. ...

Particle-resolved simulations of local liquid spreading in packed beds: Effect of wettability at varying particle size
  • Citing Article
  • May 2022

... Ambekar et al.'s PRCFD simulations indicated that local velocity and second-order quantities, such as strain rate and vorticity, predicted by both RANS (with various eddy-viscosity models) and LES, are in reasonable agreement with DNS predictions. Specifically, ε-based RANS models, which focus on turbulent dissipation per unit mass, show good agreement with DNS, while ω-based RANS models, which focus on turbulent dissipation per unit volume, significantly under-predict turbulence quantities by several orders of magnitude due to their inadequacy in handling strongly wall-dominated flows [67]. As for ε-based RANS models, the realizable k-ε RANS model with enhanced wall treatment provides higher accuracy compared to the standard k-ε model, as it improves the turbulent viscosity coefficient and turbulent stress predictions, and can adapt to a wider range of y + value, especially for resolving viscous sub-layer region. ...

Particle‐resolved turbulent flow in a packed bed: RANS, LES, and DNS simulations

... where ðÀP si I þ s si Þ is the formation of the fluctuation energy due to shear in the solid phase and H si is the energy dissipation rate due to collision between solid particles and estimated as follows: 38,39 ...

Eulerian Multifluid Simulations of Segregation and Mixing of Binary Gas-Solids Flow of Particles with Different Densities
  • Citing Article
  • July 2021

Chemical Engineering Science

... A tapered FB with an increase in the cross section from bottom to top is considered unlike the cylindrical FB in FIOR and FINMET processes. For a similar operating flow rate, due to less injection area in a tapered FB than in a cylindrical FB, the gas velocity is high in the tapered FB. 45,46 Due to this, in the tapered FB, iron ore with a wide size distribution can be homogenously fluidized with a lower elutriation rate than in the cylindrical FB. 47 Cyclones with a dip-leg are present in the FB, and the transport disengagement height is optimized to minimize elutriation and heat loss. 44 The hematite fine ore typically in the mean size range of 1− 2 mm (maximum size up to 8 mm) is pneumatically charged into the Stage-I FB (i.e., R4) reactor and conveyed to the next stages 48,49 (see Figure 8). ...

Role of bubbling behaviour in segregation and mixing of binary gas-solids flow of particles with different density
  • Citing Article
  • May 2020

Powder Technology

... This value then decreases to 40 kg m −2 s −2 at L/D = 6.5. Jain et al. [51] conducted a study of a chimney distributor element as well as a bubbling cap distributor element. The distributor plates are the most important devices for achieving the most optimal distribution of the gas-liquid mixture over the catalytic bed. ...

Eulerian Simulations of Liquid Distribution Generated by Chimney and Bubble Cap Distributors
  • Citing Article
  • November 2020

Chemical Engineering Journal