ReviewSimulation of the spatial distribution of the acoustic pressure in sonochemical reactors with numerical methods: A review
Introduction
Sonochemistry [1] is the area of high-energy chemistry which studies chemical reactions and processes involving acoustic cavitation formed by the application of an ultrasonic field in a frequency range which commonly varies between 20 kHz and 10 MHz. It allows chemists to increase the conversion, improve the yield, initiate and change the reaction pathways in all sorts of biological, chemical or electrochemical processes [2], becoming a prominently used technique in a wide variety of research areas, including: (i) material science [3] (ii) synthetic chemistry [4], [5], (iii) water remediation [6], [7], (iv) biotechnological applications [8], (v) electrochemical processes [9], (vi) food technology [10], and (vii) spent nuclear fuel reprocessing [11], among others. The versatility of the use of ultrasound in chemistry permits its combination with other technologies such as photocatalysis [12] or microwaves [13], proving the enormous potential of Sonochemistry.
Despite this extensive research at laboratory scale, a limited number of applications have been industrially scaled-up due to two main reasons: (i) the lack of expertise in diverse areas such as ultrasonics or sonochemical engineering, and (ii) the lack of proper reactor designing strategies. Related to this, Sutkar and Gogate have stated that understanding the cavitational activity and its distribution would yield efficiently designed sonochemical reactors and systems [14], and for this purpose, theoretical analysis of the cavitational activity distribution with proper experimental validation could be used for the optimization of sonochemical processes taking into account building materials, geometry of the reactor and working frequency of the sonochemical system. A correct understanding of the acoustic field structure inside a sonochemical reactor is therefore needed to proceed with its optimization and scale-up in order to design efficient large scale reactors [15].
The numerical simulation of the spatial distribution of the acoustic pressure inside sonochemical reactors has widely emerged in the last 15 years to shed new light on this issue, and quite a few groups around the world have tried to model the acoustic field inside sonoreactors with the aim of predicting the cavitation events within the reactor. To our knowledge, the most recent review on this topic found in the literature was published more than 10 years ago [16], and no exhaustive literature revisions are usually found in most of the papers that deal with the simulation of the acoustic field in a sonoreactor. Therefore, the goal of the present paper is to introduce numerical methods for the development of sonochemical reactors to a wider audience of scientists by summarizing the continuous development of numerical methods employed by the scientific community from the late 1990s until now. In this paper, basic methodologies and results from many works are briefly commented, pointing out the strong and weak points in the most representative cases from a qualitative point of view. And new trends and future challenges on the problem are also discussed.
Section snippets
Basic linear-based models
The vast majority of the works dealing with the simulation of the acoustic field inside a sonochemical reactor rely on the resolution of the equations that describe the linear propagation of sound in a liquid. Such equations, which are derived from the linearization of the Euler equations [17], yield the well-known Helmholtz equation for the linear propagation of sound waves:being P the acoustic pressure and the wave number, where ω is the angular frequency and is the sound
Numerical simulations of the acoustic field inside sonochemical reactors using nonlinear-based models
Even though the acoustic pressure attenuation or damping effect (and implicit energy dissipation) due to the presence of cavitating bubbles has been accounted for in some of the previously mentioned studies, the different methodologies followed in all those works were basically linear-based approaches to actually solve a strongly nonlinear acoustic field where nonlinearity specially comes from the formation, growth and collapse of the cavitating bubbles. Nevertheless, as argued by Harvey and
Simulation of the ultrasonic transducer
In the previous section, accounting for the vibration of the solid boundaries was briefly commented, concluding that the deformation of the reactor walls effectively affects the acoustic field and, therefore, it should not be neglected. In this sense, a question rapidly comes up: why not considering the vibration of the ultrasonic transducer too? Most of the works found in the literature usually treat the emitter boundary as a acoustic field source where a uniformly distributed acoustic
New challenges and trends in coming years
Even if the simulation of the whole electromechanical transducer can be accounted for in a relatively easy way, we have to keep in mind the complexity of rigorously modeling the electromechanic transducer, the vibrations of the reactor walls, and the acoustic field inside the reactor. Regarding the electromechanic transducer, pre-stress must be accounted for in order to avoid the estimation of resonant frequencies that may significantly differ from the real one. It must be also taken into
Acknowledgments
All the authors would like to express their deepest affection and gratitude to Dr. José González-García, who passed away on 25th February 2012, for impulsing the research on Sonochemistry and Sonoelectrochemistry at the University of Alicante. The authors would also like to acknowledge the significant contribution to the discussions included in this review made by the referees.
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