Judy Lee

Dr. Judy Lee

Chemical and Process Engineering, University of Surrey, Guildford, UK
orcid

Research Focus & Metrics

Academic Career Length

22Years (2005-Present)

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

Representative Publications

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1 February 2020 in Journal of Hazardous Materials
Verified
Journal Article
Closed access
MEMarie Enfrin
Marie Enfrin
Judy LeeJudy Lee
Judy Lee
YGYann Gibert
Yann Gibert
FBFaiza Basheer
Faiza Basheer
Lingxue KongLingxue Kong
Lingxue Kong
Ludovic DumeeLudovic Dumee
Ludovic Dumee

1 September 2017 in Ultrasonics Sonochemistry
Verified
Journal Article
Open access
RWRichard James Wood
Richard James Wood
Judy LeeJudy Lee
Judy Lee
MBMadeleine J. Bussemaker
Madeleine J. Bussemaker
In this review the phenomenon of ultrasonic cavitation and associated sonochemistry is presented through system parameters. Primary parameters are defined and considered, namely; pressure amplitude, frequency and reactor design; including transducer type, signal type, vessel-transducer ratio, liquid flow, liquid height, liquid temperature and the presence of a reflective plate. Secondary parameters are similarly characterised and involve the use of gas and liquid additives to influence the chemical and physical environments. Each of the parameters are considered in terms of their effect on bubble characteristics and subsequent impact on sonochemical activity. Evidence suggests that via parametric variation, the reaction products and efficiency may be controlled. This is hypothesised to occur through manipulation of the structural stability of the bubble.

1 April 2007 in Ultrasonics Sonochemistry
Verified
Journal Article
Open access
Muthupandian AshokkumarMuthupandian Ashokkumar
Muthupandian Ashokkumar
Judy LeeJudy Lee
Judy Lee
SKSandra Kentish
Sandra Kentish
FGFranz Grieser
Franz Grieser
Acoustic cavitation is the fundamental process responsible for the initiation of most of the sonochemical reactions in liquids. Acoustic cavitation originates from the interaction between sound waves and bubbles. In an acoustic field, bubbles can undergo growth by rectified diffusion, bubble-bubble coalescence, bubble dissolution or bubble collapse leading to the generation of primary radicals and other secondary chemical reactions. Surface active solutes have been used in association with a number of experimental techniques in order to isolate and understand these activities. A strobe technique has been used for monitoring the growth of a single bubble by rectified diffusion. Multibubble sonoluminescence has been used for monitoring the growth of the bubbles as well as coalescence between bubbles. The extent of bubble coalescence has also been monitored using a newly developed capillary technique. An overview of the various experimental results has been presented in order to highlight the complexities involved in acoustic cavitation processes, which on the other hand arise from a simple, mechanical interaction between sound waves and bubbles.

1 August 2021 in Ultrasonics Sonochemistry
Verified
Journal Article
Open access
PAPello Alfonso-Muniozguren
Pello Alfonso-Muniozguren
ESEfraím A. Serna-Galvis
Efraím A. Serna-Galvis
MBMadeleine Bussemaker
Madeleine Bussemaker
RTRicardo Torres-Palma
Ricardo Torres-Palma
Judy LeeJudy Lee
Judy Lee
• Pharmaceutical removal using biological digesters, sonication and membrane filtration. • Biotransformation of pharmaceutical in biological and ultrasound treatment. • Hybrid ultrasound coupled treatment processes with biological reactor and membrane filtration.

13 May 2008 in The Journal of Chemical Physics
Verified
Journal Article
Closed access
KYKyuichi Yasui
Kyuichi Yasui
TTToru Tuziuti
Toru Tuziuti
Judy LeeJudy Lee
Judy Lee
TKTeruyuki Kozuka
Teruyuki Kozuka
ATAtsuya Towata
Atsuya Towata
YIYasuo Iida
Yasuo Iida
Numerical simulations of nonequilibrium chemical reactions inside an air bubble in liquid water irradiated by ultrasound have been performed for various ambient bubble radii. The intensity of sonoluminescence (SL) has also been calculated taking into account electron-atom bremsstrahlung, radiative attachment of electrons to neutral molecules, radiative recombination of electrons and ions, chemiluminescence of OH, molecular emission from nitrogen, etc. The lower bound of ambient radius for an active bubble in SL and sonochemical reactions nearly coincides with the Blake threshold for transient cavitation. The upper bound is in the same order of magnitude as that of the linear resonance radius. In actual experiments, however, the distribution of ambient radius for active bubbles may be narrow at around the threshold ambient radius for the shape instability. The threshold peak temperature inside an air bubble for nitrogen burning is higher than that for oxidant formation. The threshold peak temperatures depend on ultrasonic frequency and acoustic amplitude because chemical reactions inside a bubble are in nonequilibrium. The dominant emission mechanism in SL is electron-atom bremsstrahlung except at a lower bubble temperature than 2000K, for which molecular emissions may be dominant.