The role of primary and secondary delays in the effective resonance frequency of acoustically interacting microbubbles

• Published in: Ultrasonics sonochemistry Vol. 86; p. 106033
• Main Authors: Haghi, Hossein, Kolios, Michael C.
• Format: Journal Article
• Language: English
• Published: Netherlands Elsevier B.V 01.05.2022; Elsevier
• Subjects: Acoustic cavitation; Bubble dynamics; Bubble-bubble interaction; Cavitation; Microbubbles; Short Communication; Bubble-bubble interaction; Microbubbles; Bubble dynamics; Acoustic cavitation; Cavitation
• ISSN: 1350-4177; 1873-2828
• DOI: 10.1016/j.ultsonch.2022.106033

•Primary and secondary delays of within microbubble (MB) clusters is introduced.•Primary delays spread the resonance frequency of identical MBs within a range.•The closest MB to the ultrasound source resonates at the lowest frequency.•The furthest MB from the ultrasound source resonates at the highest frequency.•Secondary delays cause the resonance frequency of MBs to increase with concentration. Acoustically excited microbubbles (MBs) are known to be nonlinear oscillators with complex dynamics. This has enabled their use in a wide range of applications from medicine to industry and underwater acoustics. To better utilize their potential in applications and possibly invent new ones a comprehensive understanding of their dynamics is required. In this work, we explore the effect of bubble-bubble interactions on the resonance frequency of MB suspensions. MBs oscillate in response to an external acoustic wave and since bubbles in a cluster are at different locations compared to the excitation source, they are excited at different times. In this work we refer to these delays as primary delays. Interactions between the scattered pressure fields from adjacent bubbles have also been shown to alter the dynamics of MBs that exist within clusters. These secondary waves generated by MBs reach MBs in their proximity at different times that depend on their spatial location in the cluster. Here we refer to these delays as secondary delays. Inclusion of the secondary delays modifies the class of the differential equations governing the oscillations of interacting MBs in a cluster from ordinary differential equations to neutral delay differential equations. Previous work has not considered the all the delays associated with the bubble distances when modeling the interactions between bubbles. In this work we investigate the effect of both the primary and secondary delays on the effective resonance frequency of MB clusters. It is shown that primary delays cause spreading the resonance frequency of identical MBs within a range where the closest MB to the acoustic source exhibits the lowest resonance frequency and the furthest MB resonates at the highest frequency. This range has been shown to be up to 0.12 MHz for the examples investigated in this work. The effect of secondary delays is shown to be very significant. In the absence of secondary delays, the ordinary differential equation model predicts a decrease of up to 26% in the resonance frequency of 4 identical interacting MBs as the inter-bubble distances are decreased. However, we show that inclusion of the secondary delays result in the increase of the resonance frequency of MBs if they are situated close to each other. This increase is shown to be significant and for the case of 4 identical interacting MBs we show an increase of 58% in the resonance frequency.