Ashish Karn

Prof. Ashish Karn

University of Petroleum and Energy Studies
orcid

Research Focus & Metrics

Academic Career Length

15Years (2012-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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19 January 2016 in Journal of Fluid Mechanics
Verified
Journal Article
Closed access
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Ashish KarnAshish Karn
Ashish Karn
RARoger E. A. Arndt
Roger E. A. Arndt
JHJiarong Hong
Jiarong Hong
Substantial discrepancy in the conditions for attainment of different closure modes of a ventilated supercavity has existed widely in the published literature. In this study, supercavity closure is investigated with an objective to understand the physical mechanisms determining closure formation and transition between different closure modes and to reconcile the observations from prior studies under various flow settings. The experiments are conducted in a closed-wall recirculating water tunnel to image ventilated supercavity closure using high speed and high-resolution photography and simultaneously measure pressure inside the cavity. The flow conditions are varied systematically to cover a broad range of water velocity, ventilation flow rate and cavitator size, which correspond to different Froude numbers, air entrainment coefficients and blockage ratios, respectively. In addition to the classical closure modes reported in the literature (e.g. re-entrant jet, twin vortex, quad vortex, etc.), the study has revealed a number of new closure modes that occur during the transition between classical modes, or under very specific flow conditions. Closure maps are constructed to depict the flow regimes, i.e. the range of Froude number and air entrainment coefficient, for various closure modes at different blockage ratios. From the closure map at each blockage ratio, a critical ventilation flow rate, below which the supercavity collapses into foamy cavity upon reduction of Froude number, is identified. The air entrainment coefficients corresponding to such critical ventilation rate are found to be independent of blockage ratio. It has been observed that in the process of generating a supercavity by increasing ventilation flow rate, the cavitation number gradually reduces to a minimum value and stays fixed upon further increments in the ventilation rate. Once a supercavity is formed, the ventilation rate can be decreased to a much lower value with no change in cavitation number while still maintaining a supercavity. This process is accompanied by a change in closure modes, which generally goes from twin vortex, to quad vortex, and then to re-entrant jet. In addition, the blockage effect is shown to play an important role in promoting the occurrence of twin-vortex closure modes. Subsequently, a physical framework governing the variation of different closure modes is proposed, and is used to explain mode transition upon the change of flow conditions, including the blockage effect. This framework is further extended to shed light on the occurrence of closure modes for ventilated supercavitation experiments across different types of flow facilities, the natural supercavity closure and the pulsating supercavity reported in the literature. Finally, in combination with a recent numerical study, our research discusses the role of the internal flow physics on the observed features during supercavity formation and closure-mode transition, paving the way for future investigations in this direction.

1 January 2015 in Chemical Engineering Science
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Journal Article
Closed access
Ashish KarnAshish Karn
Ashish Karn
CEChristopher Ellis
Christopher Ellis
RARoger Arndt
Roger Arndt
JHJiarong Hong
Jiarong Hong

26 September 2022 in Sustainability
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VARUN PRATAP SINGHVARUN PRATAP SINGH
VARUN PRATAP SINGH
Siddharth JainSiddharth Jain
Siddharth Jain
Ashish KarnAshish Karn
Ashish Karn
Ashwani KumarAshwani Kumar
Ashwani Kumar
gaurav dwivedigaurav dwivedi
gaurav dwivedi
Aritra GhoshAritra Ghosh
Aritra Ghosh
The scientific literature extensively mentions the use of a solar air heater (SAH) by utilizing solar energy for heating purposes. The poor heat-transfer rate of an SAH with a flat plate is caused by developing a laminar sub-layer near the heated base plate. The plate temperatures improve significantly, resulting in losses and a decrease in performance. The passive approach entails the placement of fins/turbulators/pouring material/ribs to the surface where the boundary layer forms to disrupt it. Artificially roughened SAH for gathering and efficiently using solar radiations for thermal purposes is extensively described in the literature. This paper includes a thorough literature overview of the history, basics, roughness evolution, forms of SAH, and recent breakthroughs in thermal performance improvement techniques for SAH compiled by several researchers. This paper uses a comparative evaluation of several roughness geometries and kinds of SAH to uncover thermohydraulic performance factors that may be considered in future research to pick the optimal configuration.

1 November 2015 in Experimental Thermal and Fluid Science
Verified
Journal Article
Closed access
Ashish KarnAshish Karn
Ashish Karn
RARoger E.A. Arndt
Roger E.A. Arndt
JHJiarong Hong
Jiarong Hong

1 November 2017 in Experimental Thermal and Fluid Science
Verified
Journal Article
Closed access
SSSiyao Shao
Siyao Shao
Ashish KarnAshish Karn
Ashish Karn
BAByoung-Kwon Ahn
Byoung-Kwon Ahn
RARoger E.A. Arndt
Roger E.A. Arndt
JHJiarong Hong
Jiarong Hong

1 December 2016 in Experimental Thermal and Fluid Science
Verified
Journal Article
Closed access
Ashish KarnAshish Karn
Ashish Karn
RARoger E.A. Arndt
Roger E.A. Arndt
JHJiarong Hong
Jiarong Hong