Ramesh R, Thimonier C, Desgranges S, Faugeras V, Coulouvrat F, Laurent J, Marrelec G, Contino-Pépin C, Urbach W, Tribet C, Taulier N
CNRS, INSERM, Laboratoire d'Imagerie Biomédicale, LIB, Sorbonne Université, F-75006 Paris, France.
Laboratoire de Physique de l'École Normale Supérieure, ENS, Université PSL, CNRS, Sorbonne Université, Université de Paris Cité, F-75005 Paris, France.
Langmuir. 2023 Nov 7;39(44):15716-15729. doi: 10.1021/acs.langmuir.3c02272. Epub 2023 Oct 27.
Droplets made of liquid perfluorocarbon undergo a phase transition and transform into microbubbles when triggered by ultrasound of intensity beyond a critical threshold; this mechanism is called acoustic droplet vaporization (ADV). It has been shown that if the intensity of the signal coming from high ultrasonic harmonics are sufficiently high, superharmonic focusing is the mechanism leading to ADV for large droplets (>3 μm) and high frequencies (>1.5 MHz). In such a scenario, ADV is initiated due to a nucleus occurring at a specific location inside the droplet volume. But the question on what induces ADV in the case of nanometer-sized droplets and/or at low ultrasonic frequencies (<1.5 MHz) still remains. We investigated ADV of perfluorohexane (PFH) nano- and microdroplets at a frequency of 1.1 MHz and at conditions where there is no superharmonic focusing. Three types of droplets produced by microfluidics were studied: plain PFH droplets, PFH droplets containing many nanometer-sized water droplets, and droplets made of a PFH corona encapsulating a single micron-sized water droplet. The probability to observe a vaporization event was measured as a function of acoustic pressure. As our experiments were performed on droplet suspensions containing a population of monodisperse droplets, we developed a statistical model to extrapolate, from our experimental curves, the ADV pressure thresholds in the case where only one droplet would be insonified. We observed that the value of ADV pressure threshold decreases as the radius of a plain PFH droplet increases. This value was further reduced when a PFH droplet encapsulates a micron-sized water droplet, while the encapsulation of many nanometer-sized water droplets did not modify the threshold. These results cannot be explained by a model of homogeneous nucleation. However, we developed a heterogeneous nucleation model, where the nucleus appears at the surface in contact with PFH, that successfully predicts our experimental ADV results.
由液态全氟碳化合物制成的液滴会发生相变,并在强度超过临界阈值的超声触发下转变为微泡;这种机制被称为声滴汽化(ADV)。已经表明,如果来自高超声谐波的信号强度足够高,超谐波聚焦是导致大液滴(>3μm)和高频(>1.5MHz)发生ADV的机制。在这种情况下,ADV是由于在液滴体积内的特定位置出现一个核而引发的。但是,在纳米级液滴和/或低超声频率(<1.5MHz)的情况下,是什么引发ADV的问题仍然存在。我们研究了全氟己烷(PFH)纳米液滴和微液滴在1.1MHz频率以及不存在超谐波聚焦的条件下的ADV。研究了微流体产生的三种类型的液滴:纯PFH液滴、含有许多纳米级水滴的PFH液滴以及由包裹单个微米级水滴的PFH电晕制成的液滴。测量了观察到汽化事件的概率作为声压的函数。由于我们的实验是在含有单分散液滴群体的液滴悬浮液上进行的,我们开发了一个统计模型,以便从我们的实验曲线推断出仅一个液滴被声照射的情况下的ADV压力阈值。我们观察到,纯PFH液滴的ADV压力阈值随着半径的增加而降低。当PFH液滴包裹一个微米级水滴时,该值进一步降低,而包裹许多纳米级水滴并没有改变阈值。这些结果不能用均匀成核模型来解释。然而,我们开发了一个非均匀成核模型,其中核出现在与PFH接触的表面,该模型成功地预测了我们的实验ADV结果。