Muthupandian Ashokkumar

Prof. Muthupandian Ashokkumar

University of Melbourne
orcid

Research Focus & Metrics

Academic Career Length

39Years (1988-Present)

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

Representative Publications

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1 July 2011 in Ultrasonics Sonochemistry
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Journal Article
Open access
Muthupandian AshokkumarMuthupandian Ashokkumar
Muthupandian Ashokkumar
Acoustic cavitation, in simple terms, is the growth and collapse of preexisting microbubbles under the influence of an ultrasonic field in liquids. The cavitation bubbles can be characterized by the dynamics of oscillations and the maximum temperatures and pressures reached when they collapse. These aspects can be studied both experimentally and theoretically for a single bubble system. However, in a multibubble system, the formation of bubble streamers and clusters makes it difficult to characterize the cumulative properties of these bubbles. In this overview, some recently developed experimental procedures for the characterization of acoustic cavitation bubbles have been discussed.

1 April 2018 in Applied Catalysis A: General
Verified
Journal Article
Closed access
Malathi ArumugamMalathi Arumugam
Malathi Arumugam
MJMadhavan J.
Madhavan J.
Muthupandian AshokkumarMuthupandian Ashokkumar
Muthupandian Ashokkumar
Prabhakarn ArunachalamPrabhakarn Arunachalam
Prabhakarn Arunachalam

1 April 2008 in Innovative Food Science & Emerging Technologies
Verified
Journal Article
Closed access
SKSandra Kentish
Sandra Kentish
TWT.J. Wooster
T.J. Wooster
Muthupandian AshokkumarMuthupandian Ashokkumar
Muthupandian Ashokkumar
SBS. Balachandran
S. Balachandran
RMR. Mawson
R. Mawson
LSL. Simons
L. Simons

1 September 2011 in Ultrasonics Sonochemistry
Verified
Journal Article
Closed access
JCJayani Chandrapala
Jayani Chandrapala
BZBogdan Zisu
Bogdan Zisu
MPMartin Palmer
Martin Palmer
SKSandra Kentish
Sandra Kentish
Muthupandian AshokkumarMuthupandian Ashokkumar
Muthupandian Ashokkumar

1 August 2009 in Ultrasonics Sonochemistry
Verified
Journal Article
Open access
TLT.S.H. Leong
T.S.H. Leong
TWT.J. Wooster
T.J. Wooster
SKSandra Kentish
Sandra Kentish
Muthupandian AshokkumarMuthupandian Ashokkumar
Muthupandian Ashokkumar
The efficient production of nanoemulsions, with oil droplet sizes of less than 100nm would facilitate the inclusion of oil soluble bio-active agents into a range of water based foods. Small droplet sizes lead to transparent emulsions so that product appearance is not altered by the addition of an oil phase. In this paper, we demonstrate that it is possible to create remarkably small transparent O/W nanoemulsions with average diameters as low as 40nm from sunflower oil. This is achieved using ultrasound or high shear homogenization and a surfactant/co-surfactant/oil system that is well optimised. The minimum droplet size of 40nm, was only obtained when both droplet deformability (surfactant design) and the applied shear (equipment geometry) were optimal. The time required to achieve the minimum droplet size was also clearly affected by the equipment configuration. Results at atmospheric pressure fitted an expected exponential relationship with the total energy density. However, we found that this relationship changes when an overpressure of up to 400kPa is applied to the sonication vessel, leading to more efficient emulsion production. Oil stability is unaffected by the sonication process.

27 February 2009 in Physical Review Letters
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Journal Article
Closed access
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ABAdam Brotchie
Adam Brotchie
FGFranz Grieser
Franz Grieser
Muthupandian AshokkumarMuthupandian Ashokkumar
Muthupandian Ashokkumar
Acoustic bubble-size distributions have been determined using a pulsed ultrasound method at different ultrasound powers and frequencies. It was observed that the mean bubble size increased with increasing acoustic power and decreased with increasing ultrasound frequency. It was also recognized that the mean size of bubbles emitting sonoluminescence was greater than those producing sonochemiluminescence indicating that the two processes take place in different populations of cavitation bubbles in the system.