Abstract:The chemical effects of acoustic cavitation are obtained in sono-reactors built-up from a vessel and an ultrasonic source. In this paper, simulations of an existing sono-reactor are carried out, using a linear acoustics model, accounting for the vibrations of the solid walls. The available frequency range of the generator (19 kHz-21 kHz) is systematically scanned. Global quantities are plotted as a function of frequency in order to obtain response curves, exhibiting several resonance peaks. The attenuation coe… Show more
“…Further, the zero flux boundary condition at the surfaces of the heaters and the sonoreactor include some basic assumptions. A comprehensive way to account for more realistic boundary conditions is the coupling of elastic deformation and the wave propagation as implemented succesfully in [48,49,50]. Finally, other numerical methods, such as, the finite element method (FEM), the boundary element method (BEM) or the finite volume method (FVM), may be employed to solve the Helmholtz equation in order to compare their convergence rates with the current numerical approach.…”
Please cite this article as: H. Dogan, V. Popov, Numerical simulation of the nonlinear ultrasonic pressure wave propagation in a cavitating bubbly liquid inside a sonochemical reactor, Ultrasonics Sonochemistry (2015), doi: http://dx
“…Further, the zero flux boundary condition at the surfaces of the heaters and the sonoreactor include some basic assumptions. A comprehensive way to account for more realistic boundary conditions is the coupling of elastic deformation and the wave propagation as implemented succesfully in [48,49,50]. Finally, other numerical methods, such as, the finite element method (FEM), the boundary element method (BEM) or the finite volume method (FVM), may be employed to solve the Helmholtz equation in order to compare their convergence rates with the current numerical approach.…”
Please cite this article as: H. Dogan, V. Popov, Numerical simulation of the nonlinear ultrasonic pressure wave propagation in a cavitating bubbly liquid inside a sonochemical reactor, Ultrasonics Sonochemistry (2015), doi: http://dx
“…The acoustic field within the liquid microchannel and the deformation of the stacked microreactor have been calculated by following simulation strategies found in the literature [27,28].…”
Possible drawbacks of microreactors are inefficient reactant mixing and the clogging of microchannels when solid-forming reactions are carried out or solid (catalysts) suspensions are used. Ultrasonic irradiation has been successfully implemented for solving these problems in microreactor configurations ranging from capillaries immersed in ultrasonic baths to devices with miniaturized piezoelectric transducers. Moving forward in process intensification and sustainable development, the acoustic energy implementation requires a strategy to optimize the microreactor from an ultrasound viewpoint during its design. In this work, we present a simple analytical model that can be used as a guide to achieving a proper acoustic design of stacked microreactors. An example of this methodology was demonstrated through finite element analysis and it was compared with an experimental study found in the literature.
“…A non-optimized flow sonoelectrochemical system was used for process scale-up ( Figure 4.2). In this work, the polypropylene sonoelectrochemical reactor was designed to be used in divided and undivided configurations, whereby the acoustic field in the reactor was calculated according to the finite-element simulation method [24,25].…”
Section: Sonoelectrochemical Degradation Of Chlorinated Pollutantsmentioning
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