Department of Biomedical Engineering, ‡Department of Surgery, School of Medicine, §Department of Chemical Engineering and Materials Science, ∥Chao Family Comprehensive Cancer Center, ⊥Beckman Laser Institute, and #Edwards Lifesciences Center for Advanced Cardiovascular Technology, University of California-Irvine , Irvine, California 92697, United States.
Langmuir. 2016 Dec 13;32(49):13124-13136. doi: 10.1021/acs.langmuir.6b03014. Epub 2016 Dec 5.
The targeted delivery of nanoparticle carriers holds tremendous potential to transform the detection and treatment of diseases. A major attribute of nanoparticles is the ability to form multiple bonds with target cells, which greatly improves the adhesion strength. However, the multivalent binding of nanoparticles is still poorly understood, particularly from a dynamic perspective. In previous experimental work, we studied the kinetics of nanoparticle adhesion and found that the rate of detachment decreased over time. Here, we have applied the adhesive dynamics simulation framework to investigate binding dynamics between an antibody-conjugated, 200-nm-diameter sphere and an ICAM-1-coated surface on the scale of individual bonds. We found that nano adhesive dynamics (NAD) simulations could replicate the time-varying nanoparticle detachment behavior that we observed in experiments. As expected, this behavior correlated with a steady increase in mean bond number with time, but this was attributed to bond accumulation only during the first second that nanoparticles were bound. Longer-term increases in bond number instead were manifested from nanoparticle detachment serving as a selection mechanism to eliminate nanoparticles that had randomly been confined to lower bond valencies. Thus, time-dependent nanoparticle detachment reflects an evolution of the remaining nanoparticle population toward higher overall bond valency. We also found that NAD simulations precisely matched experiments whenever mechanical force loads on bonds were high enough to directly induce rupture. These mechanical forces were in excess of 300 pN and primarily arose from the Brownian motion of the nanoparticle, but we also identified a valency-dependent contribution from bonds pulling on each other. In summary, we have achieved excellent kinetic consistency between NAD simulations and experiments, which has revealed new insights into the dynamics and biophysics of multivalent nanoparticle adhesion. In future work, we will leverage the simulation as a design tool for optimizing targeted nanoparticle agents.
纳米载体的靶向递送具有极大的潜力,可以改变疾病的检测和治疗方式。纳米粒子的一个主要特性是能够与靶细胞形成多个键,从而大大提高了附着力。然而,纳米粒子的多价结合仍然知之甚少,特别是从动态的角度来看。在以前的实验工作中,我们研究了纳米粒子附着的动力学,发现脱落的速度随时间的推移而降低。在这里,我们应用粘性动力学模拟框架来研究抗体偶联的 200nm 直径球体与 ICAM-1 涂覆表面之间的结合动力学,规模为单个键。我们发现纳米粘性动力学(NAD)模拟可以复制我们在实验中观察到的随时间变化的纳米粒子脱落行为。正如预期的那样,这种行为与平均键数随时间的稳定增加相关,但这归因于仅在纳米粒子结合的第一秒内键的积累。而长期增加的键数则是由于纳米粒子的脱落作为一种选择机制,消除了随机限制在较低键价的纳米粒子。因此,随时间推移的纳米粒子脱落反映了剩余纳米粒子群体向更高总体键价的演变。我们还发现,只要键上的机械力载荷足够高,足以直接导致断裂,NAD 模拟就能精确匹配实验。这些机械力超过 300pN,主要源于纳米粒子的布朗运动,但我们还确定了键之间相互拉拽的价依赖性贡献。总之,我们在 NAD 模拟和实验之间实现了出色的动力学一致性,这揭示了多价纳米粒子附着的动力学和生物物理学的新见解。在未来的工作中,我们将利用该模拟作为优化靶向纳米粒子试剂的设计工具。