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- Kothapalli, Satya V.V.N. 1985-, et al.
(författare)
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Investigation of Polymer-Shelled Microbubble Motions in Acoustophoresis
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Annan publikation (övrigt vetenskapligt/konstnärligt)abstract
- The objective of this paper is to explore the trajectory motion of microsize (typically smaller than a redblood cell) encapsulated polymer-shelled gas bubbles propelled by radiation force in an acousticstanding-wave field and to compare the corresponding movements of solid polymer microbeads. Theexperimental setup consists of a microfluidic chip coupled to a piezoelectric crystal (PZT) with aresonance frequency of about 2.8 MHz. The microfluidic channel consists of a rectangular chamberwith a width, w, corresponding to one wavelength of the ultrasound standing wave. It creates one fullwave ultrasound of a standing-wave pattern with two pressure nodes at4w and43w and threeantinodes at 0,2w , and w. The peak-to-peak amplitude of the electrical potential over the PZT wasvaried between 1 and 10 volts. From Gor’kov’s potential equation, the acoustic contrast factor, Φ, forthe polymer-shelled microbubbles was calculated to about -60.7. Experimental results demonstratethat the polymer-shelled microbubbles are translated and accumulated at the pressure antinode planes.This trajectory motion of polymer-shelled microbubbles toward the pressure antinode plane is similarto what has been described for other acoustic contrast particles with a negative Φ. First, primaryradiation forces dragged the polymer-shelled microbubbles into proximity with each other at thepressure antinode planes. Then, secondary radiation forces caused them to aggregate at different spotsalong the channel. The relocation time for polymer-shelled microbubbles was 40 times shorter thanthat for polymer microbeads, and in contrast to polymer microbeads, the polymer-shelledmicrobubbles were actuated even at driving voltages (proportional to radiation forces) as low as 1 volt.In short, the polymer-shelled microbubbles demonstrate the behavior attributed to the negativeacoustic contrast factor particles and thus can be trapped at the antinode plane and thereby seperatedfrom solid particles, such as cells. This phenomenon could be utilized in exploring future applications,such as bioassay, bioaffinity, and cell interaction studies in vitro in a well-controlled environment.
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