| Literature DB >> 32583981 |
Mai N Vu1,2,3,4, Hannah G Kelly1,3, Adam K Wheatley1,3, Scott Peng1,2, Emily H Pilkington1,2,3, Nicholas A Veldhuis1,2, Thomas P Davis1,2,5, Stephen J Kent1,3,6, Nghia P Truong1,2.
Abstract
A key concept in nanomedicine is encapsulating therapeutic or diagnostic agents inside nanoparticles to prolong blood circulation time and to enhance interactions with targeted cells. During circulation and depending on the selected application (e.g., cancer drug delivery or immune modulators), nanoparticles are required to possess low or high interactions with cells in human blood and blood vessels to minimize side effects or maximize delivery efficiency. However, analysis of cellular interactions in blood vessels is challenging and is not yet realized due to the diverse components of human blood and hemodynamic flow in blood vessels. Here, the first comprehensive method to analyze cellular interactions of both synthetic and commercially available nanoparticles under human blood flow conditions in a microvascular network is developed. Importantly, this method allows to unravel the complex interplay of size, charge, and type of nanoparticles on their cellular associations under the dynamic flow of human blood. This method offers a unique platform to study complex interactions of any type of nanoparticles in human blood flow conditions and serves as a useful guideline for the rational design of liposomes and polymer nanoparticles for diverse applications in nanomedicine.Entities:
Keywords: PISA nanoparticles; blood flow; cellular interactions; fresh human blood; liposomes; polymerization-induced self-assembly; reversible addition-fragmentation chain transfer (RAFT)
Mesh:
Substances:
Year: 2020 PMID: 32583981 PMCID: PMC7361276 DOI: 10.1002/smll.202002861
Source DB: PubMed Journal: Small ISSN: 1613-6810 Impact factor: 15.153
Figure 1Nanoparticle design and characterization. A) Top: Schematic illustration of negatively charged PISA nanoparticles with three different sizes of ≈40 nm (small particle—SP), ≈75 nm (medium particle—MP), and ≈150 nm (large particle—LP); Middle: Chemical structure of diblock copolymers of the PISA nanoparticles; Bottom: TEM images of the PISA nanoparticles. B) Top: Schematic illustration of liposomes with three different charges: anionic liposomes (AL), cationic liposomes (CL), and neutral liposomes (NL); Middle: Schematic illustration of lipids used to make liposomes with distinct charges; Bottom: Cryo‐TEM images of the liposomes. Scale bars = 200 nm.
Nanoparticle characterization
| Nanoparticle code | SEC | DLS | TEM | NTA | ||||
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| d [nm] | PdI | ζ [mV] | d [nm] | d [nm] | ||
| PISA | SP | 47300 | 1.36 | 42 ± 2 | 0.11 | −15 ± 1 | 39 ± 5 | 55 ± 1 |
| MP | 102500 | 1.41 | 76 ± 1 | 0.03 | −12 ± 1 | 73 ± 6 | 82 ± 1 | |
| LP | 149500 | 1.40 | 154 ± 4 | 0.08 | −14 ± 1 | 142 ± 16 | 158 ± 2 | |
| Liposomes | AL | – | – | 115 ± 4 | 0.12 | −17 ± 2 | 103 ± 19 | 135 ± 1 |
| CL | – | – | 115 ± 4 | 0.16 | 4 ± 1 | 104 ± 19 | 127 ± 11 | |
| NL | – | – | 128 ± 3 | 0.15 | −3 ± 1 | 115 ± 19 | 143 ± 2 | |
SEC measurements were carried out in DMAC + 0.03 wt% of LiBr solution and using polystyrene standards for calibration
DLS measurements were performed at 25 °C with reported values averaged over three measurements
Diameter of the particles by TEM were calculated by FIJI.
Figure 2Blood flow characterization method. A) Top: A photo of the experimental setup. Middle: A synthetic microvascular network; Bottom: Schematic illustration of interactions between nanoparticles and different types of blood cells under flow conditions. B) Images of HUVECs growing in the microchips captured by a Nikon confocal microscopy, cells were stained with Calcein AM (cytoplasm) and Hoechst 33342 (cell nucleus). C) Nuclei of HUVECs were stained with Hoechst 33342 and focal points for imaging selected at the bottom, middle, and top views of the microchannels. Scale bars = 100 µm.
Figure 3Analysis of cellular interactions. A) Gating strategies to identity HUVECs and different WBC subtypes. B) Percentage of white blood cells associated with large PISA nanoparticles (LP) with (w) or without (w/o) the presence of HUVECs under static and flow conditions. C) Percentage of white blood cells associated with anionic liposomes (AL) with or without HUVEC presence under static and flow conditions. Data are presented as mean ± SD, n = 3–4 individual experiments.
Figure 4Effect of particle size of PISA nanoparticles. A) Percentage of white blood cells associated with PISA nanoparticles of three different sizes (40 nm—SP, 75 nm—MP, 150 nm—LP). Data are presented as mean ± SD, n = 3–4 individual experiments. Statistical significance of data between static and flow conditions was determined by a paired two‐tailed t‐test; * p < 0.05, ** p < 0.01. One‐way ANOVA with Tukey's pairwise comparisons post‐hoc test was used to assess statistical significance between three‐sized PISA nanoparticles; # p < 0.05, ## p < 0.01, ### p < 0.001, #### p < 0.0001. B) Images of B cells (lymphocytic cells) associated with medium (MP) and large (LP) PISA nanoparticles. C) Images of monocytes (phagocytic cells) associated with large PISA nanoparticles (LP). Orthogonal views of with expression of indicated markers are shown in the right and bottom images. Scale bars = 2 µm.
Figure 5Effects of particle charge of liposomes. A) Percentage of white blood cells associated with liposomes of three different charges (anionic liposomes—AL, cationic liposomes—CL, neutral liposomes—NL). Data are presented as mean ± SD, n = 3–4 individual experiments. Statistical significance of data between static and flow conditions was determined by a paired two‐tailed t‐test; * p < 0.05. One‐way ANOVA with Tukey's pairwise comparisons post‐hoc test was used to assess statistical significance between three‐charged liposomes; # p < 0.05, ## p < 0.01. B) Images of B cells (lymphocytic cells) associated with three‐charged liposomes. Orthogonal views of these cells with expression of indicated markers are shown in the right and bottom images. Scale bars = 2 µm.