Abstract
The stable levitation of an analyte sample in an acoustic levitator is a primary requirement for accurate x-ray characterization of its scientific structure. A rigid particle oscillates in an under-damped manner when introduced into the node of established standing acoustic waves. This investigation has employed the lattice Boltzmann method (LBM), a computational fluid dynamics technique, for the analysis of such rigid particle dynamics in acoustic levitation. The simulation uses the two dimensional and nine velocity (D2Q9) Bhatnagar–Gross–Krook formulation to levitate a rigid 1.6 mm diameter nylon (ρ = 1150 kg/m3) particle in the air at standard pressure and temperature conditions. The presented work is the first reported simulation of realistic acoustic levitator boundary conditions using the LBM. The simulation can capture the particle–fluid interactions that produce dynamic levitation at less than one-period timescale in the ultrasonic frequency regime. An experiment was conducted by levitating a 1.6 mm-diameter nylon sphere to estimate the oscillations, and the oscillating frequency was found to be 50 Hz. The dynamic simulation results are consistent with experimental results for particle oscillations within the same order of magnitude, indicating that LBM formulation can be successfully used to study acoustic levitation to understand and mitigate particle jitter. The distortion of the acoustic field due to a levitating particle’s presence was also analyzed to demonstrate how the presence of the particle can disrupt adjacent levitating nodes.
Highlights
Acoustic levitators are used as containerless positioning tools in x-ray experimentation in the study of material science,1 biomolecules,2 and the development of amorphous pharmaceuticals.3 These devices operate when a vibrating transducer harmonically excites a fluid field
While the Gor’kov potential offers an estimate of the forces experienced by a particle, it does not allow for the inclusion of perturbation from multiple objects, nor does it account for dynamical effects such as viscous damping
Since the estimated frequency was produced from the two-dimensional Gor’kov potential field, the results suggest that the simulation accurately predicts the standing wave dynamics near the simulation plane
Summary
Acoustic levitators are used as containerless positioning tools in x-ray experimentation in the study of material science, biomolecules, and the development of amorphous pharmaceuticals. These devices operate when a vibrating transducer harmonically excites a fluid field. Acoustic levitators are used as containerless positioning tools in x-ray experimentation in the study of material science, biomolecules, and the development of amorphous pharmaceuticals.. Acoustic levitators are used as containerless positioning tools in x-ray experimentation in the study of material science, biomolecules, and the development of amorphous pharmaceuticals.3 These devices operate when a vibrating transducer harmonically excites a fluid field. If a barrier is positioned opposite the transducer, sound waves reflect into the fluid field, and a standing wave develops. There are various configurations that researchers have developed to create levitation conditions. The most common configuration is a single-axis levitator with one transducer and one reflector or with two transducers (see, for example, the devices in Ref. 4–9). The authors have developed two-axis and three-axis levitators, while other researchers have explored levitators with arrays of transducers A review article by Andrade et al. discusses the current state of the art for acoustic levitator technology
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