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<title>Engineering Mechanics Unit (EMU)</title>
<link>https://libjncir.jncasr.ac.in/xmlui/handle/10572/2</link>
<description/>
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<rdf:li rdf:resource="https://libjncir.jncasr.ac.in/xmlui/handle/123456789/3510"/>
<rdf:li rdf:resource="https://libjncir.jncasr.ac.in/xmlui/handle/123456789/3509"/>
<rdf:li rdf:resource="https://libjncir.jncasr.ac.in/xmlui/handle/123456789/3508"/>
<rdf:li rdf:resource="https://libjncir.jncasr.ac.in/xmlui/handle/123456789/3507"/>
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<dc:date>2026-04-04T05:27:46Z</dc:date>
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<item rdf:about="https://libjncir.jncasr.ac.in/xmlui/handle/123456789/3510">
<title>Analysis of vortex ring collisions using Lattice Boltzmann Method</title>
<link>https://libjncir.jncasr.ac.in/xmlui/handle/123456789/3510</link>
<description>Analysis of vortex ring collisions using Lattice Boltzmann Method
Kumar B., Ganesh
Vortical structures appear in a wide range of flow scenarios, including wall-bounded turbulence,&#13;
boundary layer separation behind bluff bodies, and large-scale phenomena such as hurricanes.&#13;
Understanding these structures is crucial for gaining insights into the overall flow behaviour.&#13;
Among them, vortex rings are unique flow features characterized by vorticity concentrated&#13;
around a closed circular loop. Due to the mutually induced velocity along the ring, they self propagate in a straight line. Coaxial vortex ring collisions, a topic widely studied in the literature,&#13;
exhibit different mechanisms of vortex stretching and dissipation across varying Reynolds&#13;
numbers. However, these cases represent idealized configurations that differ significantly from&#13;
realistic flow scenarios, where vortex collisions often occur under arbitrary orientations. In the&#13;
present work, we numerically investigate non-coaxial vortex ring interactions using the Lattice&#13;
Boltzmann method, wherein the axes of the colliding rings are offset by a finite distance. We&#13;
examine the influence of varying this offset for different Reynolds numbers. For small axial&#13;
offsets, the collision plane of the rings tilts proportionally to the offset distance. In contrast,&#13;
for larger offsets (of the order of ring radius), vortex stretching occurs predominantly on one&#13;
side of the ring while the other side undergoes reconnection, forming secondary vortex rings.&#13;
This behaviour reveals a novel breakup mechanism. Furthermore, we extend our numerical&#13;
study to explore vortex ring interactions with V-shaped walls. Due to the acute angle of&#13;
these walls, the rings exhibit enhanced curling, maintaining sufficient vorticity to generate&#13;
secondary and even tertiary vortex rings. These complex dynamics are successfully captured in&#13;
our simulations, demonstrating the capability of the numerical model to reproduce intricate&#13;
reconnection processes and multiple ring formations.
Open access
</description>
<dc:date>2025-01-01T00:00:00Z</dc:date>
</item>
<item rdf:about="https://libjncir.jncasr.ac.in/xmlui/handle/123456789/3509">
<title>Combined immersed volume-phase field approach for predicting multiphase fluid structure interactions</title>
<link>https://libjncir.jncasr.ac.in/xmlui/handle/123456789/3509</link>
<description>Combined immersed volume-phase field approach for predicting multiphase fluid structure interactions
S., Guruprasad
The application of numerical methods and the development of solution algorithms to solve&#13;
various multi-physics scenarios are of prime importance in our modern industrialised world.&#13;
This thesis deals with numerical methods to compute Fluid-Structure Interactions (FSI) oc curring with more than one fluid phase. The underlying discretisation technique used is the&#13;
versatile finite volume method. The work essentially develops two different components ca pable of accurately handling the multiphase part and the FSI part. It amalgamates them to&#13;
develop a formulation capable of handling complex multiphase + FSI problems. The problem’s&#13;
multiphase aspect is taken care of here by developing a binary and a ternary flow phase field&#13;
formulations based on the modified Cahn-Hilliard equation. The FSI part of the problem is&#13;
tackled by using the immersed volume approach, which works by employing a permeability&#13;
penalty term to the momentum equations. The final step is to combine both these techniques,&#13;
taking the ternary phase field components to compute the interfacial dynamics and using one of&#13;
the extra phases as the designated solid phase. The permeability penalty term is applied to the&#13;
solid phase, thus giving us a new numerical algorithm to compute multiphase + FSI problems.&#13;
A series of validations have been deployed for both the individual models and the combined&#13;
approach.
Open access
</description>
<dc:date>2025-01-01T00:00:00Z</dc:date>
</item>
<item rdf:about="https://libjncir.jncasr.ac.in/xmlui/handle/123456789/3508">
<title>Thermal analysis of a modular plant growth chamber: Experiments and numerical simulation</title>
<link>https://libjncir.jncasr.ac.in/xmlui/handle/123456789/3508</link>
<description>Thermal analysis of a modular plant growth chamber: Experiments and numerical simulation
Tanagawade, Manoj Tanaji
India, an agriculture-based economy, is the second-largest producer of vegetable crops globally.&#13;
However, the seasonal and weather-dependent nature of these crops poses significant challenges,&#13;
prompting a growing adoption of technologies like protected farming. Introduced to India in&#13;
1998 through the Indo-Israel Greenhouse Project, greenhouse farming has expanded rapidly&#13;
but brought unique challenges, especially the issue of overheating during the summer months.&#13;
India’s abundant sunlight, particularly in summer, often results in temperatures inside&#13;
greenhouses exceeding optimal levels for plant growth. To address this, evaporative cooling&#13;
systems, such as pad-and-fan setups, are commonly employed. However, these systems signifi cantly increase water consumption, contradicting one of the primary objectives of protected&#13;
farming—efficient resource usage, particularly water.&#13;
The focus of this work is to quantify the extent of overheating in a lab-scale greenhouse&#13;
model and explore the potential of Infrared (IR) filtering to mitigate this issue. Experimental&#13;
results demonstrate the effectiveness of IR filters in reducing overheating, offering a promising&#13;
solution to this challenge. Additionally, this study presents a comprehensive approach to&#13;
predicting bulk air temperature inside greenhouses through two methodologies: Computational&#13;
Fluid Dynamics (CFD) simulations and a simplified lumped mass reduced-order model. Both&#13;
models exhibit good accuracy in temperature prediction, providing valuable tools for optimizing&#13;
greenhouse designs and ensuring favorable growing conditions with efficient resource usage.
Restricted access up to (20-08-2026)
</description>
<dc:date>2025-01-01T00:00:00Z</dc:date>
</item>
<item rdf:about="https://libjncir.jncasr.ac.in/xmlui/handle/123456789/3507">
<title>Experimental and numerical investigation of continuous dip-coating for wire with immiscible two-fluid system</title>
<link>https://libjncir.jncasr.ac.in/xmlui/handle/123456789/3507</link>
<description>Experimental and numerical investigation of continuous dip-coating for wire with immiscible two-fluid system
Goswami, Jishnu
Dip-coating is one of the extensively used industrial coating processes. The popularity of this&#13;
technique coating process is due to its ease of application, versatility in using a wide variety&#13;
of substrates and coating liquids, low wastage, etc. Understanding this coating process holds&#13;
economic and industrial importance in having better control of the final film thicknesses. The&#13;
pioneering work in dip-coating is because of Landau-Levich [19] and subsequent improvements&#13;
by Derjaguin [8]. The entrainment law given by Landau-Levich stressed the importance of&#13;
the interaction of capillary and viscous forces. Several modifications and improvements were&#13;
made to this theoretical work and David Quéré and his group did a voluminous amount of&#13;
work in understanding the fibre/wire coating process [30]. They incorporated the effect of&#13;
inertia into the film formation process and showed the possibility of various regimes within the&#13;
flow. In recent years, the multiphase dip-coating processes become increasingly popular and&#13;
this present work aims to extend our understanding of fibre/wire coating using a single liquid,&#13;
involving a liquid-air interface to a two-fluid flow configuration, which contains an evolving&#13;
fluid-fluid interface. Experimental and numerical work has been performed to study this problem. Experiments&#13;
are performed by direct visualization of the coating film with varying control parameters. A&#13;
numerical model is then established by solving fluid flow equations and capturing the fluid fluid interface with the help of a level-set method. The data generated upon this exercise in&#13;
JNCASR and performed experiments at Universite de Lille, France, we set to discover and&#13;
understand various flow regimes present in this flow problem. The results show the presence of&#13;
a visco-capillary regime where the role of inertia and gravity can be assumed to have minimal&#13;
importance. In this regime, the entrainment is shown to have a close resemblance with the&#13;
classical LLD theory, which is being followed at higher Ca numbers. The role of inertia is&#13;
manifested in providing a sharp deviation to the film thickness from the LLD thickness values&#13;
and the sharpness becomes gentler as viscous, capillary, gravity and inertia all start to play&#13;
important roles simultaneously. At higher inertia, the film formation is limited by the growth&#13;
of the boundary layer and this gives rise to a regime solely dominated by boundary layer&#13;
effects. An alternate visco-gravitational regime is also present suggesting the formation of the&#13;
film primarily because of the interaction of viscous and gravity forces with negligible inertia&#13;
and capillary suction. Moreover, film formation over a thin fibre/wire is often susceptible to&#13;
instabilities and our numerical exercise shows the presence of them for an extensive range of control parameters and non-dimensional numbers.
Open access
</description>
<dc:date>2025-01-01T00:00:00Z</dc:date>
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