Biomedical Engineering, Thorax Center, Erasmus MC, Rotterdam, The Netherlands.
Ultrasound Med Biol. 2013 Mar;39(3):490-506. doi: 10.1016/j.ultrasmedbio.2012.09.025. Epub 2013 Jan 21.
In this study, we investigated the effect of secondary Bjerknes forces on targeted microbubbles using high-speed optical imaging. We observed that targeted microbubbles attached to an underlying surface and subject to secondary Bjerknes forces deform in the direction of their neighboring bubble, thereby tending toward a prolate shape. The deformation induces an elastic restoring force, causing the bubbles to recoil back to their equilibrium position; typically within 100 μs after low-intensity ultrasound application. The temporal dynamics of the recoil was modeled as a simple mass-spring system, from which a value for the effective spring constant k of the order 10(-3) Nm(-1) was obtained. Moreover, the translational dynamics of interacting targeted microbubbles was predicted by a hydrodynamic point particle model, including a value of the spring stiffness k of the very same order as derived experimentally from the recoiling curves. For higher acoustic pressures, secondary Bjerknes forces rupture the molecular adhesion of the bubbles to the surface. We used this mutual attraction to quantify the binding force between a single biotinylated microbubble and an avidin-coated surface, which was found to be between 0.9 and 2 nanonewtons (nN). The observation of patches of lipids left at the initial binding site suggests that lipid anchors are pulled out of the microbubble shell, rather than biotin molecules unbinding from avidin. Understanding the effect of ultrasound application on targeted microbubbles is crucial for further advances in the realm of molecular imaging.
在这项研究中,我们使用高速光学成像研究了次级 Bjerknes 力对靶向微泡的影响。我们观察到,附着在基底表面并受到次级 Bjerknes 力作用的靶向微泡会朝着相邻微泡的方向变形,从而趋向于拉长的形状。这种变形会产生弹性恢复力,导致微泡返回到平衡位置;通常在低强度超声应用后 100 μs 内。回弹的时间动态被建模为一个简单的质量-弹簧系统,从中获得了有效弹簧常数 k 的约 10(-3) Nm(-1)的数值。此外,相互作用的靶向微泡的平移动力学通过一个包含弹簧刚度 k 的水动力点粒子模型来预测,该刚度值与从回弹曲线实验得出的非常相同的顺序。对于更高的声压,次级 Bjerknes 力会破坏微泡与表面的分子附着力。我们利用这种相互吸引力来量化单个生物素化微泡与亲和素涂层表面之间的结合力,发现其在 0.9 到 2 纳牛顿(nN)之间。在初始结合位点留下的脂质斑块的观察表明,脂质锚从微泡壳中被拉出,而不是生物素分子从亲和素上解吸。了解超声应用对靶向微泡的影响对于分子成像领域的进一步发展至关重要。