Muzammil
Kuddushi
a,
Chiranjeevi
Kanike
a,
Ben Bin
Xu
*b and
Xuehua
Zhang
*a
aDepartment of Chemical and Materials Engineering, University of Alberta, Alberta T6G 1H9, Canada. E-mail: xuehua.zhang@ualberta.ca
bMechanical and Construction Engineering, Faculty of Engineering and Environment, Northumbria University, Newcastle Upon Tyne NE1 8ST, UK. E-mail: ben.xu@northumbria.ac.uk
First published on 10th March 2025
Nanoprecipitation is a versatile, low-energy technique for synthesizing nanomaterials through controlled precipitation, enabling precise tuning of material properties. This review offers a comprehensive and up-to-date perspective on nanoprecipitation, focusing on its role in nanoparticle synthesis and its adaptability in designing diverse nanostructures. The review begins with the foundational principles of nanoprecipitation, emphasizing the impact of key parameters such as flow rate, mixing approach, injection rate, and Reynolds number on nanomaterial characteristics. It also discusses the influence of physicochemical factors, including solvent choice, polymer type, and drug properties. Various nanoprecipitation configurations—batch, flash, and microfluidic are examined for their specific advantages in controlling particle size, morphology, and internal structure. The review further explores the potential of nanoprecipitation to create complex nanostructures, such as core–shell particles, Janus nanoparticles, and porous and semiconducting polymer nanoparticles. Applications in biomedicine and other fields highlight nanoprecipitation's promise as a sustainable and tunable method for fabricating advanced nanomaterials. Finally, the review identifies future directions, including scaling microfluidic techniques, expanding compatibility with hydrophilic compounds, and integrating machine learning to further enhance the development of nanoprecipitation.
A typical nanoprecipitation process involves mixing a polymer solution dissolved in an organic solvent with an aqueous solution. When the organic solution containing polymers rapidly and uniformly mixes with the aqueous non-solvent, it crosses the solubility barrier, resulting in the precipitation or phase separation of the solute into nanoparticles within the continuous phase. The resulting oversaturation and chain collapse lead to the formation of polymer nanoparticles (PNPs), which can range in size from a few nanometers to several micrometers. The formation of these nanomaterials involves three key processes: (1) mixing of the organic solution (containing solute molecules) with an anti-solvent (aqueous phase), (2) nucleation of solute molecules, and (3) aggregation and growth into nanomaterials.7,15–17 This same process can also nucleate liquid droplets through spontaneous emulsification, a phenomenon known as the “ouzo effect” or solvent exchange in flow systems.18–21 Alternatively, similar effects can occur in evaporating ternary liquid mixtures.22,23
Several review articles have summarized specific aspects of preparing polymer nanoparticles (PNPs).24–27 In this review, we aim to provide an updated and holistic perspective on the physicochemical aspects and hydrodynamics that significantly influence nanoprecipitation. We place particular emphasis on the solution and flow conditions in various mixing configurations used during synthesis and their impact on controlling nanomaterial formation. Additionally, we discuss the fundamental principles of different mixing configurations for nanoprecipitation. Special attention is given to key parameters, such as mixing methods and conditions, including flow rate, stream velocity, injection rate, and the properties of fluids and their compositions – such as solvent, non-solvent, polymer, and the physicochemical conditions of the liquid mixtures.28 The general principles discussed in this review provide a framework for understanding how the final size, structure, and properties of nanomaterials are determined. While the field of nanoprecipitation is rapidly evolving, and it is beyond the scope of this review to cover all recent articles, we aim to present representative examples in each section. These examples are intended to inspire further exploration and advancements in future studies.
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Fig. 1 Nanoprecipitation in ternary systems. (a) Ternary phase diagram for a polymer in a binary solvent and the SEM images of the synthesized polymer nanoparticle.15,32 (b) Solubility diagram and (c) photos of the ternary mixtures of ethanol, water, and anise oil.22 |
Many ternary mixtures consist of both miscible pairs and immiscible pairs. The solutes in such systems can include polymers, oils,33–36 or even gases.37,38 When the solute is oil, the nanoprecipitation process is equivalent to what is commonly referred to as the Ouzo effect.22,23,29 The most common solvent and anti-solvent combinations for nanoprecipitation are polar organic solvents with water (or an aqueous solution). However, other combinations are also feasible, including organic solvent–organic solvent systems,34–36 ionic liquid–ionic liquid systems,39,40 and deep eutectic solvents.41
The nucleation and growth of supersaturated solute molecules lead to the formation of polymer nanoparticles. Once nucleation is initiated, the growth of nanoparticles proceeds via the diffusion of solute molecules from the surrounding medium. Fick's laws of diffusion describe the transport of solute molecules, where the flux is proportional to the concentration gradient. Fast diffusion ensures uniform particle growth, while variations in local concentrations can lead to particle size heterogeneity. Both kinetic and thermodynamic factors play a role in the particle structure and size distribution.6,42–44 Both mixing and diffusion processes occur simultaneously, depleting the solute molecules in the mixture. Additionally, the anti-solvent dilutes the solute, reducing its concentration. As the solute concentration falls below the critical nucleation threshold, nucleation and growth cease. The formed nanoparticles remain dispersed in the mixture, trapped in a thermodynamically metastable state. The rate of oversaturation plays a critical role in determining nanoparticle size. A high nucleation rate leads to the formation of smaller particles with a narrow size distribution. A key complexity in this process is that nanoparticle formation arises from local and temporal oversaturation of the solute during mixing. Oversaturation evolves over time and may also vary spatially. Both the physicochemical properties of the compounds in the mixture and the mixing dynamics between the solution and the antisolvent are critical in creating the out-of-equilibrium oversaturation, which determines the size, structure, and properties of the nanoparticles. Interfacial tension plays a crucial role in the stabilization of nanoparticles. The presence of stabilizers or surfactants reduces interfacial energy, preventing coalescence.
There are three primary nanoprecipitation techniques: batch, flash, and microfluidic methods, as illustrated in Fig. 2. In batch nanoprecipitation (BNP), the polymer solution and solvent are mixed rapidly, either through dropwise addition47 or by injecting the entire polymer solution directly into the aqueous medium, as shown in Fig. 2(a).48 In batch processes, the degree of mixing significantly influences the oversaturation dynamics. Rapid mixing reduces local concentration gradients, promoting uniform nucleation and growth. The shear forces generated during mixing also play a pivotal role, as they impact the particle size distribution and morphology. Controlled addition can also be achieved using a syringe pump or slow diffusion across a dialysis membrane. Several factors—such as the mixing method,49 the polymer's molecular weight,50 and the choice of organic solvent45—influence the size and morphology of polymer nanoparticles (PNPs) synthesized via BNP. Perevyazko et al. demonstrated the fabrication of nanoparticles from solutions of poly(methyl methacrylate) and its copolymers. The particle characteristics strongly depended on the polymer's chemical structure and preparation method. In the studied cases, particle sizes ranged from 6–680 nm, with polydispersity indices (dw/dn) varying between 1.02 and 1.40. Their findings showed that nanoparticles of a desirable size range could be synthesized using solvent–nonsolvent methods. Fig. 3(a)–(f) shows the formation of nanoparticles by the batch process, achieved by varying the acetone-to-water solvent ratio.
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Fig. 2 Major types of mixing processes for nanoprecipitation. (a) Batch nanoprecipitation (BNP),48 (b) flash nanoprecipitation (FNP),51 and (c) microfluidic nanoprecipitation (MNP),52 (d) principles of batch, flash, and microfluidic nanoprecipitation techniques. |
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Fig. 3 Polymer nanoparticles (PNPs) prepared by nanoprecipitation. (a)–(f) SEM image of the PNPs prepared using two polymer poly(MMA-stat-pyMAA) (PMMA) and copolymer poly(MMA-stat-EA). (a)–(c) PMMA; (d)–(f) PMMA and copolymer. The mixing conditions are by dripping acetone to water (a) and (d), by dialysis of N,N-dimethylacetamide (c) and (f), or by dripping water to acetone (b) and (e).49 Variation of the PNP size as a function of (a) solvents under constant mixing kinetics (Re = 749), and (b) Reynolds number (Re = 400–1000).45 (i)–(l) Field emission scanning electron microscopic image representing the variation of PNP size on the final polymer concentrations (i) 0 mg mL−1, (j) 1 mg mL−1, (k) 2 mg mL−1, and (l) 5 mg mL−1 from an initial polymer concentration of 5 mg mL−1.53 |
Flash nanoprecipitation (FNP) utilizes a high-pressure injection pump to rapidly mix streams of organic solution and nonsolvent within a confined chamber, typically for milliseconds. The high shear forces generated during FNP facilitate rapid diffusion and mixing at the molecular level. The confinement within a narrow chamber ensures consistent mixing, minimizing spatial concentration gradients. The interplay between shear rates and mixing efficiency directly impacts particle size and uniformity, with higher shear rates promoting smaller, more homogeneous particles. This promotes the rapid formation of polymer colloids with specific morphologies and compositions.17,51,54,55 Wang et al. fabricated lutein-loaded nanoparticles (NPs) using FNP. In their process (Fig. 2(b)), SPI was dissolved in water at a fixed concentration of 0.8 mg mL−1, which represents the maximum solubility of SPI under the designed conditions. The properties of the kinetically controlled SPI NPs, including particle size, size distribution, drug loading efficiency, stability, and bioavailability, were investigated as well.51
Microfluidic nanoprecipitation (MNP) has been described as a simple method for drug nanosizing.56,57 Microfluidic systems rely on precise control of flow dynamics, which are dictated by the dimensions and geometry of the channels. The mixing efficiency in microfluidics is enhanced by chaotic advection and rapid diffusion-driven processes. By adjusting flow rates and channel configurations, it is possible to achieve highly controlled nanoprecipitation, with particle sizes being inversely proportional to the flow rate due to enhanced nucleation at higher mixing velocities.58 The results show that stable aqueous hydrocortisone NPs can be obtained using a bottom-up approach with microfluidic reactors. Particle size can be controlled by modifying the processing conditions and the design of the microfluidic reactors, such as internal diameters and inlet angles. Changes in flow rates were found to have a dominant effect on the size of the generated particles.44,59 The setup typically includes a central channel squeezed by two vertical channels, which allows for rapid diffusion-driven mixing (Fig. 2(c)).52 The dimensions of the channel, such as length, height, and structure, are key determinants of the properties of the particles in the microfluidic process.56,60,61 Slater et al. reported the preparation of hydrophobic branched NPs via rapid nanoprecipitation. The resulting aqueous nanoparticle dispersions were robust and stable to dilution, solvent addition, sonication, and temperature changes. The addition of small amounts of NaCl led to nanoparticle destabilization, suggesting that electrostatic repulsion is a key factor in maintaining stability. The presence of NaCl likely screens surface charges, reducing repulsive interactions and promoting aggregation, thereby emphasizing the role of charge stabilization.62 Variation in particle size and fluorescent intensity at different H2O/THF ratios (Fig. 4(i) and (j)) for EDP NPs ranged from 28 nm to 55 nm, while BDP NPs ranged from 20 nm to 80 nm (Fig. 4(k) and (l)). In the following sections, we will discuss FNP and MNP in more detail.
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Fig. 4 TEM images of CuS-NPs-FNP with different AA/Cu ratios and corresponding hydrodynamic diameters of PAA-CuS-DOX NPs: (a) 1 (173 nm) and 2.5 (117 nm), (b) 5 (85 nm) and 20 (50 nm). Variation of hydrodynamic size distributions of CuS-NPs prepared via FNP and thermal method (TM) method (c) UV-vis spectra of NPs with and without drug (DOX) molecules prepared via FNP and TM. (d) XRD patterns of the NPs prepared via different FNP and TM methods with and without DOX molecules.63 (e) The ratio of the radius of gyration to the hydrodynamic radius (Rg/Rh) of the PNPs at stream velocities. (f) Stability of the prepared PNPs as a function of time.8 (g) and (h) Variation of PNP sizes at different solution pH.64 RFNP: reactive nanoprecipitation. Run 3-1: without chitosan; run 3-2: with chitosan. DS: drip and stir method, in contrast to nanoprecipitation. (i)–(k) Variation of particle size and fluorescent intensity at different H2O/THF ratio (i) and (j) for EDP NPs (k) and (l) BDP NPs.65 (m) and (n) TEM images and the corresponding nanopesticide dispersion prepared using sophorolipids of mass concentrations (m) 100% acidic sophorolipids, and (n) 50% acidic sophorolipids and 50% lactonic sophorolipids.66 (o)–(q) TEM images of the PNPs obtained using block copolymers of different molecular weights.67 |
Flow dynamics and mixing conditions, such as stream velocity, Reynolds number, and injection rate, are crucial in achieving desired particle characteristics. Wang et al. showed that increasing the Reynolds number over 1400 reduced the hydrodynamic size of PNPs from 122 nm to 80 nm, with minimal size change beyond this threshold.51 Conversely, Zhao et al. observed that higher flow rates in a buffer solution gradually increased particle size, with a significant size jump at very high flow rates, demonstrating the need for careful control over flow to maintain size uniformity.71 Bhutto et al. investigated the internal structure of β-carotene-loaded protein PNPs, showing that increasing stream velocity resulted in densely packed core–shell structures, transitioning from laminar to turbulent flow. As stream velocity further increased, particle size stabilized, highlighting how flow dynamics affect internal particle organization and density, as shown in Fig. 4(e) and (f).8
Material properties, such as surfactant composition and polymer characteristics, also influence particle formation in FNP. Ma et al. examined the effect of surfactant ratio on lambda-cyhalothrin-loaded nanopesticides, finding that acidic sophorolipids alone produced spindle-like particles while adding lactonic sophorolipids led to spherical particles due to altered hydrophobic interactions. This demonstrates how specific surfactant compositions can direct particle shape and stability (Fig. 4(m) and (n)66). Jia et al. used FNP to create stable, low-toxicity copper sulfate nanoparticles for chemotherapy. They observed that as stream velocity increased from 6 to 30 mL min−1, particle size decreased from 64 nm to 50 nm, stabilizing beyond that point. Additionally, Jia et al.63 demonstrated the effect of varying the AA/CuS ratio, as shown in Fig. 4(a) and (b), where increasing the ratio from 1 (173 nm) and 2.5 (117 nm) in Fig. 4(a) to 5 (85 nm) and 20 (50 nm) in Fig. 4(b) led to a significant reduction in particle size. This is due to PAA acting as a capping agent, inhibiting growth through steric hindrance and electrostatic stabilization. At lower ratios, limited PAA results in larger nanoparticles, while higher concentrations restrict growth, leading to smaller sizes. Beyond an AA/CuS ratio of 10, the particle size remains unchanged, indicating surface saturation with PAA. In Fig. 4(c) and (d), Jia et al.63 demonstrated the successful loading of DOX into the PAA-CuS-DOX NPs, as confirmed by the absorbance peak at 500 nm in the UV-vis spectra, corresponding to the characteristic peak of DOX. XRD analysis was also performed to characterize the crystal structure of the PAA-CuS-DOX NPs. Despite the large background signal from the amorphous PAA polymer, intense characteristic crystalline CuS peaks were clearly observed, confirming the presence of the CuS crystal structure.
Zhu et al. reported the production of lead(II) sulfate (PbSO4) nanosuspension, with an average particle diameter of ∼50 nm, via in situ reactive flash nanoprecipitation. Fig. 4(h) shows chitosan as a pH-sensitive surface stabilizer whose hydrophobicity can be tuned by varying its pH (Fig. 4(g) and (h)). By increasing the pH of the suspension, the chitosan/PbSO4 nanoparticles rapidly aggregated and settled down. After filtration and drying, the particles were easily separated from water, with significantly reduced size enlargement due to Ostwald ripening and recrystallization.64 Pustulka et al.67 present TEM images in Fig. 4, depicting (o) 5k–5k PEG-b-PLA, (p) 5k–10k PEG-b-PLGA, and (q) 10k–10k PEG-b-PLGA nanoparticles, which demonstrated stability in suspension for at least 10 days.
The influence of drug loading on particle properties has been explored in several studies. Zhao et al. used an FNP setup with a multi-inlet vortex mixer to prepare curcumin-loaded zein nanoparticles, finding that higher drug concentrations initially increased particle size and yield, with particles exhibiting narrow size distribution at higher drug levels.71 Wang et al. similarly found that at low drug-to-polymer ratios, particle size initially decreased before increasing at higher ratios, indicating an optimal ratio range for controlling particle dimensions in drug-loaded systems.51
Flow dynamics and mixing conditions are critical in MNP. The physics of surface and interface interactions plays a pivotal role in MNP. At the nanoscale, the high surface-to-volume ratio amplifies interfacial forces, significantly impacting particle formation and stabilization. Surface tension (γ) governs the interfacial energy, while the interfacial curvature determines the Laplace pressure, influencing nanoparticle size and shape. The balance between cohesive forces (within the liquid) and adhesive forces (between liquid and solute) drives nucleation and growth processes.73
In the confined microchannels of MNP, the interplay of diffusion and interfacial tension creates a uniform solute distribution, enhancing the nucleation rate. Additionally, wetting properties, characterized by the contact angle (θ), influence solvent and anti-solvent interactions, affecting particle morphology. Hydrophilic channel walls promote spreading and mixing, while hydrophobic surfaces may induce localized aggregation due to poor wetting. The wettability of microfluidic channel walls significantly influences nanoprecipitation by affecting fluid mixing, solute diffusion, and particle formation. Hydrophilic surfaces (θ < 90°) enhance solvent spreading, promote uniform solute distribution, and improve mixing efficiency, resulting in smaller and more homogeneous nanoparticles.74 Conversely, hydrophobic surfaces (θ > 90°) can lead to poor wetting, localized aggregation, and increased particle polydispersity due to inefficient mixing.58 Furthermore, excessive hydrophobicity may cause nanoparticle adhesion to channel walls, leading to fouling and flow disturbances.75 Optimizing wettability through surface modifications, such as plasma treatment or chemical coatings, can enhance process stability and ensure consistent nanoparticle synthesis.76 Optimizing surface energy and flow conditions is crucial to ensuring uniform particle formation. Increasing the flow rate ratio between the solvent and anti-solvent promotes diffusion, generating more nucleation sites and resulting in smaller, more uniform PNPs.61 Studies by Heshmatnezhad et al. and Chiesa et al. confirmed that higher total flow rates reduce particle size due to intensified shear forces, causing oversaturation and greater nucleation.77–80 However, excessive flow rates can induce particle aggregation, leading to an increase in particle size at channel junctions, as demonstrated in the TEM images and DLS plot (Fig. 5(a)–(f)).81 The Reynolds number (Re) also influences particle size; Liu et al. found that increasing Re enhanced turbulence, improving mixing until particle size stabilized. At lower drug-to-polymer ratios, thinner polymer shells formed around drug cores, while higher Re led to smaller core–shell particles across different charged polymers (Fig. 5(g)–(m)).82
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Fig. 5 (a)–(e) TEM images of PNPs prepared at flow rate ratios. The PNPs of mPEG-PLGA from the flow ratios of (a) 0.03, (b) 0.05, (c) 0.1, (d) 0.2, (e) 0.3. (f) Corresponding dynamic light scattering plots of PNPs.81 (g)–(l) TEM images of the core–shell PNP synthesized by varying drug–polymer weight ratio and Reynolds number. (g) and (h) Drug–polymer weight ratio of 1![]() ![]() ![]() ![]() ![]() ![]() ![]() ![]() ![]() ![]() |
The material properties of microfluidic channels play a pivotal role in determining the outcomes of MNP by influencing fluid dynamics, mixing efficiency, and nanoparticle characteristics. Key material attributes such as wettability, surface charge, and mechanical properties directly impact the nucleation and growth processes of nanoparticles. The wettability of channel materials, defined by their surface energy, affects fluid flow patterns and mixing behavior within microchannels. Hydrophilic materials, characterized by high surface energy, promote effective solvent spreading and facilitate uniform solute distribution. This leads to enhanced mixing efficiency and results in the formation of smaller, more homogeneous nanoparticles. In contrast, hydrophobic materials with low surface energy can cause inadequate wetting, leading to poor mixing and localized solute concentration gradients. These conditions may result in the formation of larger, polydisperse nanoparticles due to uneven nucleation rates. For instance, the use of PDMS in microfluidic devices has been shown to influence nanoparticle synthesis outcomes due to its inherent hydrophobicity.83
The surface charge of channel materials influences electrostatic interactions between the channel walls and the solute particles. Materials with surface charges that are compatible with the solute can prevent unwanted adsorption of nanoparticles onto the channel walls, thereby reducing fouling and ensuring a stable nanoprecipitation process. Conversely, incompatible surface charges can lead to particle adhesion, affecting the yield and quality of the nanoparticles produced. The chemical compatibility between the channel material and the solvents used is also crucial, as interactions at the interface can alter the physicochemical properties of the forming nanoparticles. Additionally, the mechanical strength and thermal conductivity of channel materials determine their ability to withstand operational conditions without deforming or degrading. Materials with high mechanical strength maintain structural integrity under various flow rates and pressures, ensuring consistent nanoparticle synthesis. Thermal properties influence heat dissipation within the microchannels, affecting solvent evaporation rates and, consequently, the supersaturation levels critical for controlled nanoprecipitation. Materials like PDMS, commonly used in microfluidic devices, offer flexibility and ease of fabrication but may have limitations in mechanical and thermal stability under certain conditions.58 To optimize MNP outcomes, surface modification techniques are employed to tailor the material properties of microfluidic channels. Methods such as plasma treatment, chemical grafting, or coating with hydrophilic polymers can enhance surface wettability, improving fluid mixing and nanoparticle uniformity. These modifications can also introduce desired surface charges or functional groups, reducing particle adhesion and fouling. For example, treating PDMS surfaces to increase hydrophilicity has been shown to improve nanoparticle synthesis by promoting better mixing and reducing aggregation.83
Precise control over flow dynamics and channel design allows for fine-tuning of the nanoprecipitation process. The ratio of flow rates between solvent and anti-solvent governs mixing efficiency and interfacial area generation, both critical for particle nucleation. For instance, high flow rates create thinner diffusion layers, reducing interfacial resistance and promoting rapid saturation of solute molecules. At the same time, the Re dictates whether flow remains laminar or transitions to turbulent, with laminar flow providing the most reproducible conditions for nanoprecipitation.84 Channel geometry, including T-junctions, staggered herringbone micromixers, and bifurcating designs, determines shear rates and residence times. Shear rates at the interface influence interfacial stability, where excessive shear can disrupt particle formation or cause aggregation.85,86 Scaling up these designs while maintaining optimal mixing conditions remains a challenge due to the complex interplay of surface forces and flow dynamics. Fig. 5(n) and (o) illustrates the effect of flow rates on NP size, showing that increasing the flow rate reduces NP size.59 Silverman et al. demonstrated that increasing drug-to-polymer ratios in poly(caprolactone)-block-poly(ethylene glycol) NPs primarily affected polydispersity. At the same time, particle size changed only slightly due to curcumin's plasticizing effect, as shown in TEM images (Fig. 5(p) and (q)).5 Ma et al. showed that surfactant ratios affect particle morphology in nanopesticides.66 The chemical composition of surfactants and stabilizers significantly influences interfacial properties during MNP. Surfactants reduce interfacial tension, stabilizing newly formed nanoparticles by preventing coalescence or Ostwald ripening. For example, ionic surfactants provide charge stabilization, while non-ionic surfactants rely on steric hindrance to maintain particle dispersion. The choice of surfactant must balance these stabilization mechanisms to achieve desired particle properties, particularly under varying flow rates and solvent compositions. Additionally, interfacial rheology—describing the deformation and flow of the interface—determines the stability of emulsions formed during nanoprecipitation. For instance, interfacial elasticity resists deformations under shear, preventing coalescence in high-shear environments such as those in microfluidic channels.
FNP and MNP both enable controlled production of PNPs but differ significantly in their methodologies and applications. FNP is characterized by rapid mixing in a confined space, producing particles with narrow size distributions and high loading efficiency, particularly suitable for hydrophobic drugs. However, FNP has limitations in processing water-soluble biomolecules and often requires high-pressure pumps, which increase operational complexity. In contrast, MNP leverages ultra-low volumes and precise control over flow rates within microchannels, allowing for highly reproducible particle sizes and morphologies through laminar flow and diffusion-driven mixing. MNP excels in its fine-tuning capabilities, accommodating various solvent compositions and complex surfactant systems, making it ideal for applications requiring small-scale, precise formulations. While MNP offers high precision and low energy consumption, it faces challenges in scalability due to the small channel size. FNP, by contrast, can more readily accommodate larger production scales, albeit with less precise control over certain particle properties. Both methods are versatile tools in nanoparticle synthesis, with FNP favored for rapid production and MNP for applications demanding intricate control over nanoparticle characteristics. From an interfacial physics perspective, FNP operates under conditions of high interfacial tension and rapid mixing, which can lead to kinetic control over particle size but may limit precision. In contrast, MNP emphasizes interfacial control through diffusion-driven mixing, allowing finer tuning of particle characteristics.36 The lower interfacial tension achieved in MNP setups, often facilitated by surfactants or solvent composition, supports the formation of more uniform nanoparticles. For instance, in MNP, the relationship between surface energy and flow velocity can be optimized to achieve a balance between nucleation and growth, ensuring monodispersity. Meanwhile, FNP relies on intense mixing to overcome interfacial resistance, often resulting in broader size distributions.87
Microfluidic platforms, such as Y-junction mixers, have demonstrated precise control over mixing dynamics, leading to uniform NPs synthesis with high reproducibility.91 The application of staggered herringbone micromixers further enhances mass transfer efficiency, facilitating the synthesis of metal–organic frameworks (MOFs) with tunable porosity and controlled drug release.92 Beyond microfluidic devices, high-speed homogenization remains an effective approach for achieving rapid solvent-exchange-driven nanoprecipitation, yielding lipid–polymer hybrid nanoparticles with enhanced colloidal stability and encapsulation efficiency.58 Additionally, ultrasonic-assisted nanoprecipitation has been employed for the synthesis of bioactive metal–organic frameworks, enabling targeted and responsive drug delivery applications.93 Electrohydrodynamic mixing techniques, including jetting-based nanoprecipitation, have further optimized particle formation by leveraging charge-induced forces, leading to highly monodisperse NPs for biomedical applications. The potential of these techniques is evident in diverse fields, from drug delivery to energy storage, where precise NPs control is critical.94 These advancements in nanoprecipitation mixing techniques highlight the growing role of controlled microenvironment engineering in NPs synthesis, offering new opportunities for enhanced functionality and efficiency.
Membrane nanoprecipitation is another method for producing polymer-based nanoparticles, where mixing occurs directly at the pores of a membrane.95 In this method, an organic solvent and anti-solvent are introduced on opposite sides of a membrane with defined pore structures. Mixing occurs at these pores, enabling nanoparticle formation by regulating solvent diffusion. For example, the organic solvent may occupy the shell side of the membrane, mixing with the anti-solvent in the lumen side, or vice versa, driven by a pressure gradient. Membrane properties, particularly pore size and wettability, significantly influence particle size and polydispersity. Despite its precision, membrane nanoprecipitation faces challenges in scaling up due to the limited availability of suitable membranes with defined pore characteristics.
Electrospray nanoprecipitation combines solvent-shifting techniques with electrospray to synthesize polymer nanoparticles (PNPs).96,97 In this process, the polymer solution is pumped through a nozzle connected to a high-voltage power supply, generating charged droplets that are subsequently mixed with a non-static aqueous phase under stirring. The electric field controls droplet size, facilitating rapid solvent evaporation, oversaturation, and nanoparticle formation. This technique produces monodisperse, surfactant-free nanoparticles, allowing for precise control over particle characteristics.
Techniques such as UV-vis absorption, Raman spectroscopy, and fluorescence can be employed in microfluidic channels to monitor the particle formation process in real-time. By coupling these spectroscopic methods with machine learning algorithms, we can dynamically adjust parameters like flow rates, solvent composition, and temperature to maintain consistent particle size and morphology. Additionally, dynamic light scattering (DLS) and in situ light scattering or particle tracking microscopy offer real-time monitoring of particle size distribution and growth dynamics. Temperature control and monitoring within the microfluidic system ensures consistent reaction kinetics, while solvent composition monitoring provides further precision in maintaining optimal conditions for nanoprecipitation. This integration enhances reproducibility and scalability, providing a precise and adaptable framework for controlling nanoprecipitation and producing nanoparticles with tailored properties.
For systems involving metal-based nanoparticle synthesis, electrochemical techniques such as cyclic voltammetry (CV) or electrochemical impedance spectroscopy (EIS) can be employed to monitor ion reduction and redox processes. These methods are particularly effective in controlling the nucleation and growth of metal nanoparticles, enabling real-time adjustments to ion concentrations, pH, and other critical parameters in metal nanoprecipitation processes.
Additionally, the interaction between the organic phase and the solute molecules determines the quality of the solvent for a given polymer, whether it is a good or poor solvent. In the case of a good solvent for a polymer, the resulting particle size tends to be larger due to the extended conformation of the solute molecules. Conversely, in a poor solvent, the solute molecules collapse, resulting in smaller particle sizes. Since these interactions vary for different solvents, the size and properties of the PNPs also change with variations in the organic phase.
This section will discuss the effects of polymer characteristics (such as concentration, molecular weight, and degree of hydrophobicity) and solvents on the size and properties of nanomaterials. The variation in particle properties with changes in solution parameters in nanoprecipitation techniques is summarized in Table 1.
Mixing technique | Advantages | Disadvantages | Ref. |
---|---|---|---|
Batch | – Simple setup and easy to scale up | – Longer mixing times | 101 and 102 |
– Suitable for large volumes | – Poor control over mixing conditions | ||
– Cost-effective | – Higher batch-to-batch variability | ||
Flash | – Rapid mixing | – Requires precise control of flow rates | 67 and 103 |
– Suitable for high-throughput processes | – Limited to specific reaction conditions | ||
– Reduces aggregation in nanoparticle synthesis | – Equipment may be expensive | ||
Microfluidic | – Excellent control over mixing parameters | – Low throughput | 58 and 104 |
– High reproducibility | – Complex fabrication and operation | ||
– Suitable for small volumes and lab-on-a-chip applications | – Higher initial costs |
The interactions between the organic phase, aqueous phase, and solute molecules are crucial in determining the size and characteristics of polymer nanoparticles (PNPs) in nanoprecipitation.16 The diffusivity between phases influences the distribution of solute molecules: slower diffusion typically results in larger particles, while stronger affinity between the phases tends to reduce particle size. Furthermore, the interaction between the organic phase and solute molecules determines the solvent quality for a given polymer. In the case of good solvents, which extend the polymer chains, larger particles are typically formed, whereas poor solvents cause the polymer chains to collapse, resulting in smaller particles (Tables 2 and 3).
Polymer | Organic/aqueous phase | Parameter varied | Size | Morphology |
---|---|---|---|---|
PEG-b-PLA, PEG-b-PLGA, or PEG-b-PCL | DMF, acetone, acetonitrile, THF, or DMSO/water | Organic solvents | 50–100 nm | Spherical45 |
Poly(vinyl alcohol) | Methanol, ethanol, propanol, tert-butanol/water | Polymer concentrations, interaction parameters | 50–300 nm | Spherical16 |
p(HPMA50-EGDMA) | Acetone/water | Polymer structure (linear and branched), temperature, volume of organic phase, NaCl | 50–800 nm | Spherical62 |
Poly(lactic-co-glycolic acid) | Acetonitrile, acetone and tetrahydrofuran (THF)/PVA aqueous solution | Polymer concentration, organic solvent, ionic strength of aqueous phase and temperature | 80–3500 nm | Spherical105 |
Polystyrene | Acetone, chloroform, tetrahydrofuran and acetonitrile/Tween-40, Pluronic F-68 | Polymer, surfactant, non-solvent | 100 nm–3 μm | Spherical106 |
Cellulose acetates | Acetone/water | Concentrations of cellulose acetate | 160–400 nm | Spherical and bean-shaped particles107 |
FNP: effects of nanoprecipitation conditions on the size and morphology of the PNPs. | ||||
---|---|---|---|---|
Polymer | Organic/aqueous phase | Parameter varied | Size | Morphology |
Polystyrene | Tetrahydro-furan/water | Time, molecular weight, solution concentrations, stirring rate, solvent/non-solvent ratio | 60–200 nm | Spherical15 |
Poly(ethylene glycol)-block-poly(ε-caprolactone) | Tetrahydro-furan and dimethyl sulfoxide (DMSO)/water | Solvent/non-solvent ratio, stream velocity | 20–80 nm | Spherical65 |
Poly(3-hydroxybutyrate-co-3-hydroxyvalerate) | Dichloro-methane/SDS and PVA solutions | Polymer and surfactant concentrations | 100–600 mm | Spherical53 |
PEG-b-PLGA, PS(10k)-b-PEG, PEG-b-PLA | Tetrahydro-furan/water | Nanoparticle concentrations | 60–180 nm | Spherical67 |
PEO-b-PS, PEG-b-PCL | Tetrahydro-furan/water | Reynolds number | 25–500 nm | Spherical108 |
PS-b-PI | Tetrahydro-furan/water | Polymer concentrations, chain length | 30–300 nm | Spherical particles with concentric shells or a disordered lamellar109 |
MNP: effects of nanoprecipitation conditions on the size and morphology of the PNPs. | ||||
---|---|---|---|---|
Polymer | Organic/aqueous phase | Parameter varied | Size | Morphology |
Poly(methyl methacrylate) (PMMA) | Tetrahydrofuran/water | Polymer concentrations, volume flow rate ratio between water and the polymer solution | 100–200 nm | Spherical72 |
Poly(lactic-co-glycolic acid) | Dimethylformamide/water | Micro-channel geometry, aspect ratio | 50–300 nm | Spherical59 |
Pluronic F127 | Tetrahydrofuran/water | Drug to polymer concentrations, flow rate, mixing time | 70–200 nm | Spherical110 |
PLGA | Dimethylformamide (DMF) and tetrafluoroethylene/water | Flow rate | 50–250 nm | Spherical60 |
PLGA-lipid-NPs | Tetrafluoroethylene (TFE) and 0.7 mL dimethylformamide (DMF)/water | Flow rate | 60–90 nm | Spherical111 |
Polycaprolactone | THF and DMF/PVA solution | Flow rate ratio and total flow rate | 100–300 nm | Spherical77 |
Polymer properties, such as concentration, molecular weight, and architecture, also significantly affect PNP size and stability. For instance, Slater et al. observed that increasing polymer concentration led to a reduction in PNP size and polydispersity for vinyl polymers, while polysaccharide nanoparticles exhibited the opposite trend, with particle size increasing as polymer concentration increased.62,112 Additionally, J. H. Lee and colleagues found that higher lignin concentrations resulted in larger PNPs with increased polydispersity and surface charge.50 Polymer architecture also influences nanoparticle stability. For example, Slater et al. found that branched polymers produced more stable PNPs than linear polymers, which tended to precipitate after synthesis.62 Furthermore, Pustulka et al. reported that higher polymer hydrophobicity, measured by the water–octanol partition coefficient, enhanced PNP stability. Specifically, coefficients above 7 led to more stable particles that were resistant to rapid aggregation.67
Solvent choice plays a critical role in controlling PNP properties, influencing size, stability, and morphology. Rao and Geckeler113 examined various solvent-based methods, highlighting how solvent evaporation and nanoprecipitation impact particle size through solvent diffusion rates and polymer–solvent interactions. Dwivedi et al.114 explored nanoprecipitation and emphasized that the choice of solvent and its miscibility with water dictate the final nanoparticle size, with polar solvents like acetone yielding smaller particles due to rapid diffusion into the aqueous phase. Huang and Zhang105 systematically studied factors affecting PLGA nanoparticle size and found that solvent diffusion coefficient strongly dictates size distribution, with solvents like acetonitrile producing finer nanoparticles compared to acetone or THF.
Additionally, Aubry et al. demonstrated that lower polymer concentrations in PMMA, combined with a high aqueous phase volume, resulted in PNPs with narrow size distributions. However, higher polymer concentrations led to the formation of a mixture of micro- and nanoparticles, in line with the Smoluchowski kinetic model.115 Similarly, Bovone et al. observed that solvent type influences PNP growth dynamics. Initial dynamic aggregates, formed through polymer exchange, stabilize once the solvent-specific water fraction is reached, ultimately determining the final particle size.45 Solvent effects have also been explored in microfluidic nanoprecipitation (MNP) systems; Donno et al. found that increasing polymer molecular weight and flow rate ratio in MNP reduced PNP size and increased surface charge, with larger particles forming in the presence of surfactants at higher viscosities.116
Surfactants and other additives further modulate PNP size and morphology by controlling particle interactions during formation. Luque-Alcaraz et al. studied chitosan-based PNPs and found that surfactant presence, polymer concentration, and solvent-to-non-solvent ratios significantly influenced particle characteristics. For example, the presence of Tween 80 as a surfactant reduced particle size, while the absence of surfactant led to larger, more irregular PNPs due to coalescence.117 Heshmatnezhad et al. showed that combining surfactants like PVA and Tween 80 improved particle uniformity and prevented aggregation, resulting in smoother, smaller, and more stable PNPs. In contrast, PNPs formed without surfactants were larger, with rougher morphology and non-uniform distributions.77
Deep eutectic solvents (DESs) have emerged as promising alternatives to traditional organic solvents in nanoprecipitation. Comprising a mixture of hydrogen bond donors and acceptors, DESs exhibit low volatility, biodegradability, and tunable solubility parameters. Their unique properties facilitate the efficient extraction of bioactive compounds from natural sources, which can subsequently act as reducing and stabilizing agents in nanoparticle synthesis. For instance, Vorobyova et al. demonstrated the use of a DES-based plant extract for the biosynthesis of silver nanoparticles, highlighting the solvent's role in enhancing nanoparticle stability and antibacterial efficacy.118 Similarly, ionic liquids (ILs) particularly those based on imidazolium cations, have been extensively studied for their role in stabilizing nanomaterials during synthesis. Their negligible vapor pressure, thermal stability, and ability to dissolve a wide range of compounds make them suitable candidates for green nanoprecipitation processes. ILs can act as both solvents and stabilizing agents, influencing nanoparticle size, morphology, and dispersion stability. Tshemese et al. reviewed the application of imidazolium-based ILs in nanomaterial stabilization, emphasizing their potential to replace conventional, more hazardous solvents.119
The utilization of solvents derived from renewable biological sources, such as plant extracts and natural surfactants, aligns with the principles of green chemistry. These solvents often contain bioactive compounds capable of reducing metal ions and stabilizing nanoparticles. For example, sophorolipids, which are glycolipid biosurfactants, have been employed in flash nanoprecipitation techniques to construct nanodelivery systems. Their natural origin and biodegradability make them attractive alternatives to synthetic surfactants in nanoparticle formulation.66 The incorporation of green solvents into nanoprecipitation processes offers several advantages such as (i) environmental sustainability: green solvents reduce the reliance on toxic organic solvents, thereby decreasing environmental pollution and health hazards,120 (ii) enhanced biocompatibility: nanoparticles synthesized using bio-based solvents often exhibit improved compatibility for biomedical applications due to the absence of harmful residues,121 and (iii) controlled nanoparticle characteristics: the unique properties of green solvents, such as viscosity and polarity, can be tailored to control nanoparticle size, morphology, and dispersion, which are critical parameters in various applications.122 The adoption of green solvents in nanoprecipitation processes represents a significant advancement in the sustainable synthesis of nanomaterials. Ongoing research in this area is expected to further optimize these processes, leading to environmentally friendly and efficient production of nanoparticles for diverse applications.
Nanoprecipitation is particularly advantageous for hydrophobic drugs, improving their solubility and bioavailability. Yang et al. utilized salt-induced precipitation to achieve high drug loading (66.5% w/w) for hydrophobic drugs. By varying salt concentrations, they controlled particle size and aggregation, resulting in uniformly dispersed nanoparticles (50 nm) with high loading efficiency in high-salt conditions (Fig. 6(d)–(g)).128 Liu et al. created stable core–shell PNPs with loading up to 58.5% by adjusting polymer precipitation timing, allowing for either single-core or multi-core formations depending on the desired release profile.129 For the antioxidant drug astaxanthin, Azaman et al. encapsulated it in PLGA nanoparticles, producing stable and homogeneous PNPs (142 nm), optimized for enhanced oral bioavailability and antioxidant efficacy.130
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Fig. 6 Nanoprecipitation for fabrication of nanocarriers of pharmaceutical active ingredients. (a) Schematic representation of the preparation of the insulin-loaded PNPs (Ins-NPs). (b) TEM images of Ins-NPs and (c) PLGA–PEG NPs without insulin.131 (d) The snapshot of the mixtures, TEM images, and schematic for the nanoparticles produced by (d) and (e) bad salt concentration and (f) and (g) good salt concentration in producing 50 wt% docetaxel-loaded PLGA10k–PEG5k nanoparticles.128 (h) Schematic representation of the formation of the polymer-stabilized peroxide antimalarial drug nanoparticle and the drug release profile of the nanoparticle and unencapsulated powder in the bio media.81 |
Batch nanoprecipitation (BNP) has proven effective for encapsulating proteins and peptides, which benefit from controlled release. Chopra et al. developed insulin-loaded PLGA–PEG PNPs using BNP, achieving a tenfold increase in insulin loading while maintaining small particle size. The encapsulated insulin retained its structure, promoting long-term stability (Fig. 6(a)–(c)).131 Zada et al. used BNP in a non-aqueous setup for nasal insulin delivery, yielding rapid release rates with nearly 50% of the drug released within the first hour, ideal for nasal administration where quick absorption is advantageous.132
Flash nanoprecipitation (FNP) has shown success in stabilizing hydrophobic drugs with complex release profiles. A “complex release profile” refers to a non-uniform or multi-phase drug release behavior over time, characterized by an initial burst followed by sustained, delayed, controlled, extended, or environment-responsive release. This behavior is influenced by factors such as drug–polymer interactions, nanoparticle composition, and external environmental conditions (e.g., pH, temperature), making it critical for optimizing therapeutic efficacy. In this context, FNP enables precise control over nanoparticle formation, facilitating tailored drug release kinetics. Li et al. numerically studied the effect of solution/water flow rate ratios and microfluidic device geometry on mixing time. Fig. 6(h)133 shows the microfluidic nanoprecipitation of curcumin nanoparticles. In the first stage, most of the polymer precipitates, forming polymeric NPs, followed by curcumin NPs. Some are stabilized by mPEG-PLGA, creating drug-loaded NPs. However, at higher curcumin concentrations, theres insufficient mPEG-PLGA to stabilize the drug NPs, leading to aggregation and microchannel blockage. To improve drug loading and stability, its ideal to precipitate the drug first, ensuring enough polymer is available to stabilize the NPs. Thus, the precipitation times for the polymer and drug should be aligned.133 Qi et al. used FNP to encapsulate celastrol, achieving tunable drug loading (11–63%) in dextran-based PNPs. The formulation exhibited controlled release and reduced cytotoxicity toward liver cells, with effective inhibition of lung cancer cells, demonstrating potential for targeted cancer therapies.134
Caggiano et al. employed FNP with confined impinging jets to co-encapsulate cannabidiol (CBD) and iron oxide. This design increased particle density, improving sedimentation for controlled release studies. Stabilized with HPMCAS or lecithin, the nanoparticles demonstrated enhanced dissolution, with HPMCAS-coated particles releasing six times faster in intestinal media compared to bulk CBD as shown in Fig. 7(a).135 Zeng et al. utilized a scalable approach to prepare lipid-coated solid drug (methotrexate) nanoparticles by combining flash nanoprecipitation and extrusion techniques (Fig. 7(b)), optimizing individual steps and providing flexibility in selecting nanoparticle surface functionalities.136 Ye et al. encapsulated the cancer drug paclitaxel within PEG-PLA/zein nanoparticles using FNP, achieving high encapsulation efficiency (up to 78.1%) and controlled, sustained release. The presence of zein promoted hydrophobic interactions, allowing slow release at acidic pH, advantageous for tumor-targeted delivery.137
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Fig. 7 (a) Schematic representation of the preparation of drug-loaded nanoparticles and the comparative in vitro release profile of drug-loaded nanoparticles with bulk crystalline and bulk amorphous CBD in fed-state simulated intestinal media,136 (b) cartoon representing the microfluidic nanoprecipitation method to synthesize the curcumin-loaded block co-polymer.135 |
Microfluidic nanoprecipitation (MNP) enables precise control over particle size, ideal for creating pH-responsive nanocarriers. Li et al. synthesized PEG-PLGA PNPs for curcumin delivery, achieving a loading capacity of 2.6% and 77.3% encapsulation efficiency. However, they observed particle aggregation at higher curcumin concentrations, highlighting the importance of concentration control for stable dispersions.81 Baby et al. developed pH-responsive shellac nanoparticles for curcumin delivery using MNP, achieving up to 50% drug loading. At neutral pH, the nanoparticles released 28% of the drug in 4 hours, increasing to 51% over 51 hours, demonstrating suitability for sustained release in response to pH changes.80 The pH-responsive capabilities of FNP were further explored by Qi et al., who used dextran-based PNPs to encapsulate celastrol, an anti-cancer drug. The PNPs achieved adjustable drug loading (11–63%) with effective release, reduced liver toxicity, and significant inhibition of lung cancer cells. This adaptable release profile shows promise for personalized cancer therapies.134
Future research could focus on enhancing nanoprecipitations versatility for hydrophilic drugs by developing novel polymer–drug conjugates or exploring stimuli-responsive polymers that adapt to various biological environments. Other promising avenues include optimizing process parameters to improve the encapsulation efficiency and stability of delicate biomolecules, such as proteins and peptides, and scaling up microfluidic-based nanoprecipitation methods. Furthermore, exploring the use of eco-friendly solvents and biodegradable polymers can make nanoprecipitation more sustainable, aligning with green chemistry goals. Addressing these areas could further enhance the applicability and impact of nanoprecipitation in drug delivery.
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Fig. 8 (a) Complex morphologies through mono-component PNPs obtained by varying the solution pH.140 (b)–(d) Effect of temperature on morphology of the PNPs.141 (e) Schematic illustration of the Janus colloid formed from a blend of homo and block co-polymers solutions.109 (f) and (g) SEM images of the particles of different morphologies (f) MoDo-SiO2 and (g) CTS-MoDo-SiO2.142 (h) and (i) TEM images of organosilica nanoparticles (h) collapsed hollow structure with intrinsic flexibility and deformation. (i) Ultra-thin shells with deformable hollow structure14 (j) and (k) AFM images of the polymer Janus nanoparticles obtained using (j) thiol-PLGA (k) PLA/PGA solutions.143 |
Nanocrystals are crystalline nanoparticles with a wide range of potential applications in opto-electronics, biosensing, bioimaging, and catalysis due to their enhanced dissolution rates and tunable physicochemical properties.13,144,145 Their properties can be customized by selecting appropriate stabilizing agents, and nanoprecipitation offers a simple yet effective synthesis method.146,147 For example, Xu et al.147 used nanoprecipitation to create aggregation-induced emission (AIE) activated nanocrystals for super-resolution imaging. These AIE nanocrystals exhibited enhanced brightness and photostability, making them ideal for stimulated emission depletion nanoscopy. This technique improved the resolution of lysosomal imaging and enabled dynamic tracking of lysosomal motion over extended periods, surpassing standard confocal microscopy capabilities. Thakkur et al.148 employed electrospray nanoprecipitation to produce docetaxel nanocrystals, which showed a significant increase in dissolution rates (77% vs. 30% for bulk docetaxel) due to their high surface area. In vivo studies demonstrated effective tumor load reduction in a lung cancer model, underscoring the therapeutic potential of nanocrystals in oncology.
Semiconducting polymer nanoparticles (SNPs) are emerging materials with applications in sensing, imaging, and diagnostics, owing to their fluorescence, biocompatibility, and superior optical and photothermal properties compared to traditional dyes.12,139,149 The molecular structure of the semiconducting polymers largely determines the properties of the SNPs. Holmes et al.12 synthesized Janus SNPs with electron- and hole-accepting faces using batch nanoprecipitation. These Janus SNPs were employed to fabricate organic field-effect transistors, demonstrating efficient charge transport across thin films, highlighting their potential in optoelectronic applications. He et al.54 used flash nanoprecipitation (FNP) to synthesize ultra-small polymer dots (less than 10 nm) with narrow size distribution and tunable optical properties. By selecting polymers such as MEH-PPV, PFBT, and PFPV, they achieved highly bright and stable polymer dots suitable for high-resolution imaging. The size of these polymer dots was controlled by adjusting the polymer type and precursor concentration, showcasing the flexibility of FNP for tailoring nanoparticle properties.
Pu et al.150 developed low-bandgap diketopyrrolopyrrole (DPP) SNPs for in vivo photoimaging. DPP, known for its photostability and thermal stability, was copolymerized with electron-donating monomers to fine-tune band gaps, resulting in stable SNPs (45 nm) with modifiable fluorescence and photoacoustic properties. By adjusting the donor–acceptor composition, they optimized SNPs for photothermal applications, enhancing photothermal conversion efficiency while reducing fluorescence. This tunable property makes DPP SNPs particularly promising for biomedical imaging and therapy. Wang et al.140 demonstrated that vesicles, porous spheres, and dimpled beads could be synthesized by controlling the pH of an aqueous solution of carboxyl-terminated polyimide (Fig. 8(a)). At pH 8.07, the polymers aggregated into dimpled beads (100–600 nm), while increasing the pH to 10 produced smooth, spherical particles (100–200 nm). This pH-dependent assembly highlights how solution conditions can direct nanoparticle morphology (Fig. 8(b)–(d)). Similarly, Higuchi et al. used thermal annealing to induce disorder–order and order–order phase transitions in block copolymer nanoparticles (Fig. 8(b)–(d)). The unusual thermal behaviors suggest that the nanoparticle effect lowers the glass transition temperature of the block copolymer, likely due to the increased surface-area-to-volume ratio.141
Grundy et al.109 synthesized colloids with complex internal structures by blending poly(styrene) and poly(styrene-b-isoprene) block copolymers in an FNP process. Low-molecular-weight copolymers produced concentric, onion-like shells, while higher molecular weights resulted in disordered, lamellar structures, demonstrating control over internal nanoparticle architecture through polymer selection (Fig. 8(e)). Shahnavas et al.151 developed pH-sensitive core–shell nanoparticles composed of PLGA and carboxymethyl chitosan, allowing dual drug loading. Doxorubicin was loaded in the shell, while docetaxel was encapsulated in the core, creating a system responsive to environmental pH. The core–shell structure enabled controlled drug release: doxorubicin was released rapidly from the shell, while docetaxel in the core showed slower release, allowing for layered, sequential delivery.
Ma et al.14 used a modified FNP setup to develop deformable hollow mesoporous organosilica nanoparticles (HMONs) with high surface area and tunable mechanical properties (Fig. 8(f)–(i)). By introducing disulfide bonds into the silica network, they created nanoparticles with lower Young's modulus, enabling deformation. Loaded with the model nanopesticide abamectin, these HMONs demonstrated improved insecticidal efficacy, showing their potential for applications in agriculture where controlled-release carriers are needed. In another work, Xie et al.143 designed a fluidic nanoprecipitation system capable of fabricating biocompatible Janus polymeric nanoparticles made from the FDA-approved polymer poly(lactic-co-glycolic acid) (PLGA), as shown in AFM images (Fig. 8(j) and (k)). The system features dual inlets, each for one-half of the particle, which is inserted into the precipitation stream.
The possible future scope of nanoprecipitation includes AI and ML integration for predictive control over nanoparticle synthesis, automated and scalable processes using continuous-flow and microfluidic systems, and hybrid/multi-functional nanoparticles for advanced applications in drug delivery, sensing, and catalysis. These advancements will enhance precision, reproducibility, and scalability, making nanoprecipitation more efficient and versatile.
Despite its potential, challenges persist, particularly in large volume of solvents, scaling microfluidic techniques and optimizing formulations for hydrophilic compounds. Future advancements in nanoprecipitation could address these limitations through several innovative approaches. First, the development of fast and efficient methods for concentrating and separating nanoparticles from large liquid volumes would streamline production, making the process more time-efficient. Second, extending nanoprecipitation techniques to include hydrophilic compounds could broaden its applicability across biomedical and industrial fields. Finally, the automation of nanoprecipitation through robotic systems, coupled with machine learning for optimizing formulation and flow conditions, could accelerate the discovery and development of new nanomaterial formulations.
BNP | Batch nanoprecipitation |
CBD | Cannabidiol |
DMF | Dimethylformamide |
DMSO | Dimethyl sulfoxide |
FNP | Flash nanoprecipitation |
HMONs | Hollow mesoporous organosilica nanoparticles |
HPMCAS | Hydroxypropyl methylcellulose acetate succinate |
MNP | Microfluidic nanoprecipitation |
PBS | Phosphate buffer solution |
PDI | Polydispersive index |
PEG-b-PLA | Poly(ethylene glycol)-block-poly(DL-lactide) |
PNP | Polymer nanoparticle |
PMMA | Poly(methyl methacrylate) |
PLGA | Poly(lactic-co-glycolic acid) |
PLGA | Poly(lactide-co-glycolide) |
PVA | Poly(vinyl alcohol) |
Re | Reynolds number |
THF | Tetrahydrofuran |
PbSO4 | Lead(II) sulfate |
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