Shaped stimuli-responsive hydrogel particles: syntheses, properties and biological responses

Bing Xue a, Veronika Kozlovskaya a and Eugenia Kharlampieva *ab
aChemistry Department, University of Alabama at Birmingham, AL 35294, USA
bCenter for Nanomaterials and Biointegration, University of Alabama at Birmingham, AL 35294, USA

Received 20th October 2016 , Accepted 17th November 2016

First published on 17th November 2016


Abstract

The ability to create nano- and micro-sized hydrogel matrices of well-defined shapes can provide a powerful means not only to mimic the key properties of biological systems, but also to regulate shape-dependent particle biodistribution and cellular association, and to correspondingly optimize drug delivery carriers. This review focuses on stimuli-responsive hydrogel particles of non-spherical shapes ranging from filled porous networks to hollow capsules. We summarize a pool of current experimental approaches and discuss perspectives in the development of the synergistic combination of shape and stimuli-response in particulate hydrogels. Recent advances in the design and synthesis of the pH-, redox-, temperature-sensitive, mechanical force-, magnetic- and enzyme-responsive hydrogel particles of non-spherical shapes are presented. Examples of existing and emerging technologies for creating a variety of shapes with controlled hydrogel composition and size are highlighted. We also discuss the effects of shape on the physiochemical properties of these particles as well as their shape-regulated biological interactions including particle circulation time and biodistribution.


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Bing Xue

Bing Xue received her BS in Pharmaceutical Engineering from Nanchang University in 2008 and earned her MS in Microbial and Biochemical Pharmacy from China Pharmaceutical University in 2011, Nanjing, China. She is currently a PhD graduate student under the guidance of Prof. Eugenia Kharlampieva at the University of Alabama at Birmingham. Her research focuses on the rational design and development of novel polymeric hydrogel particles of controlled shapes for drug delivery.

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Veronika Kozlovskaya

Veronika Kozlovskaya received her PhD in Polymer Chemistry in 2008 at the Stevens Institute of Technology with Prof. Svetlana Sukhishvili. She continued her work as a Postdoctoral Fellow in the group of Prof. Vladimir Tsukruk at Georgia Institute of Technology from 2008 to 2010. Since 2010 she has worked at the University of Alabama at Birmingham in the Kharlampieva research group. Her current research interests include the design and synthesis of responsive hydrogels and biomaterials, macromolecular self-assembly, surface modifications, and characterization of nanomaterials.

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Eugenia Kharlampieva

Eugenia Kharlampieva is an Associate Professor of polymer chemistry at the Department of Chemistry at the University of Alabama at Birmingham (UAB). She received her PhD in Polymer Science from the Stevens Institute of Technology and postdoctoral training in Materials Science and Engineering at the Georgia Institute of Technology. Her research is centered at the intersection of polymer chemistry, nanotechnology, and biomedical science. Dr Kharlampieva has received the NSF CAREER, the UAB Dean's Award for Excellence in Mentorship, the UAB College of Arts and Sciences Interdisciplinary Innovation Award, and was named as an Emerging Investigator by the Royal Society of Chemistry, Journal of Materials Chemistry B, in 2014. She serves on an Executive SHUG Committee at Oak Ridge National Lab (ORNL) and on an Advisory Committee Board in Neutron Scattering at UT/ORNL DOE EPSCoR.


1. Introduction

Hydrogels are three-dimensional polymeric networks with permanent (covalent) or temporary (physical) cross-links that are able to swell upon uptake of large amounts of water and which have demonstrated great utility for drug delivery and tissue engineering applications.1–3 Hydrogels with non-spherical shapes have been receiving increasing attention in biomedical applications due to their ability to mimic the shape of natural biological objects and their shape-regulated biological interactions.4,5 Depending on the distribution of material density in the network, shaped hydrogel particles can be either filled or hollow (capsular) where, in the former case, polymer is distributed throughout the hydrogel volume or, as in the latter, exists only in the particle shell with a hollow interior volume. Filled hydrogel particles can provide expanded surface area for cargo loading, while their environmentally triggered volume transition can provide on-demand delivery of molecular therapeutics.6 In this case, the bulk mechanical modulus is tuned by the chemical composition and cross-linking density and allows imitation of the elasticity ranges of living cell tissues which is useful for advanced tissue engineering.7 Conversely, hollow hydrogels may exhibit a distinguishable hierarchical/heterogeneous architecture, resembling the structure of a cell, which can facilitate the development of versatile artificial cells and help in fundamental understanding of cell behavior in flow.8,9

Shaped hydrogel particulates can be produced in macro-, micro- and nano-sizes. Macrogels can be useful as shape memory materials which alter their shape in response to environmental stimuli including pH, ionic strength, and temperature.10–12 For instance, macrogel scaffolds with a well-defined structure have been designed for localized drug delivery and are important for observing and modulating biological activities of cells, e.g., stem cells or bone cells, under various conditions.13,14 In the case of microgels and nanogels, their colloidal nature renders them exceptionally beneficial in solving biomedical challenges. Thus, for example, the small dimensions of micro- or nano-gels constrain their biological interaction to a cellular or subcellular level by which negative side effects to the surrounding tissues are minimized.15

The integration of a well-defined shape into micro/nanoscale soft materials can provide a powerful means not only to mimic the key properties of biological systems but also to regulate shape-dependent particle biodistributions and cellular association, and to correspondingly optimize drug delivery carriers.16–18 For example, bovine serum albumin (BSA) hydrogels of biconcave discoidal shape mimicking that of red blood cells (RBCs) could carry oxygen and reversibly deform to pass through capillaries smaller than the diameter of the hydrogels.16 Microgel particles with low modulus and the size and shape of RBCs showed prolonged circulation time in vivo.17,18 In another example, the discoid shape of polyethylene glycol (PEG) hydrogels promoted better internalization by mammalian epithelial and immune cells in contrast to hydrogel nanorods.19 Moreover, the threshold pressure differential indicating the critical pressure differential at which 50% of particles pass through the capillary tube was demonstrated to vary by four orders of magnitude for hydrogel particles upon changing the shape and cross-link density, where a discoid shape was the least deformable and the S-shape demonstrated the highest flexibility when passing through a constricted channel, which affected the particle circulation time and bio-distribution.20

Recently, engineering of shaped particles has been demonstrated successfully by using methods of Particle Replication In Non-wetting Template (PRINT), Step and Flash Imprint Lithography (S-FIL) and Microfluid Continuous Lithography which provide hydrogel particulates of a precisely controlled size and shape.21–24 However, these methods lack a finer control over hydrogel cross-link densities which may render the generation of stimuli-responsive hydrogels with distinctive reversible changes in dimension or shape challenging. Hydrogel particles obtained by these technologies either may be highly cross-linked and therefore incapable of a stimuli-triggered shape reconfiguration, or their shape is irreversibly dissociated upon environmental triggering. Very recently, layer-by-layer (LBL) assembly of polymers onto/into sacrificial particulate templates has been demonstrated to be useful for yielding shaped hydrogels with pre-programmed stimuli-responsiveness and mechanical robustness allowing precise control over the interior structures and mechanical properties of hydrogel particles of micrometer and sub-micrometer sizes.25,26

The objective of this review is to focus the attention on stimuli-responsive hydrogel particles of non-spherical shapes, the existing and novel emerging methods for their fabrication, and effects of their shape on the physiochemical properties of the particles as well as the biological responses. We highlight recent developments of the pH-, redox-, temperature-sensitive mechanical force-, magnetic- and enzyme-responsive hydrogel particles of non-spherical shapes for drug delivery and biomedical applications. This review illustrates some noteworthy examples and discusses perspectives in the development of the synergistic combination of shape and stimuli-response in particulate hydrogels for the design of novel ‘smart’ drug delivery systems.

2. Synthesis of microgel particles of non-spherical shape

2.1. Particle replication in non-wetting template

Particle Replication In Non-wetting Template (PRINT) is among the most advanced top-down technologies for fabricating hydrogel particles, and it has been utilized frequently for the design and synthesis of monodisperse micro- and nano-particles in large scalable quantities.21–23 As a unique soft lithography technique, PRINT can be used to generate hydrogel particles with precisely defined size, shape, chemical composition, and surface functionalities.27 A classic PRINT particle nano-molding process is illustrated in Fig. 1.28 A silicon substrate template is generated by standard photolithography with a pre-designed pattern on a 2-dimensional (2D) array. The PRINT mold can be obtained by pouring liquid photocurable perfluoropolyethers (PFPEs) onto the template and curing it in specific patterns. The elastomeric PFPE mold can preserve all micro- and nano-featured negative patterns on the template after curing and solidification because of the positive spreading coefficient of the liquid PFPE on all surfaces. Desired materials, including monomers, initiators and cross-linkers can then be filled into the cavities without wetting the surrounding areas. However, photo-sensitive initiators such as diphenyl (2,4,6-trimethylbenzoyl) phosphine oxide (TPO),24 2-hydroxyl-1-[4-(hydroxyl)phenyl]-2-methyl-1-propanone (I2959),29 and 2,2-diethoxyacetophenone (DEAP)30 are necessary to trigger polymerization reactions which are initiated by UV light and yield shaped hydrogel particle arrays on the PFPE templates. Because of the higher surface energy with the counter-sheet film of polyethylene terephthalate (PET), the produced hydrogel particles can then be transferred from PFPE films and harvested upon dissolving the sacrificial films by the roll-to-roll process.21
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Fig. 1 Illustration of the PRINT process in comparison to traditional imprint lithography in which the affinity of the liquid precursor for the surface results in a scum layer. In the PRINT process, the non-wetting nature of fluorinated materials and surfaces (shown in green) confines the liquid precursor inside the features of the mold, allowing for the generation of isolated particles. Reproduced with permission from ref. 28. Copyright © 2005 American Chemical Society.

To date, the majority of hydrogel particles generated by PRINT are cross-linked by poly(ethylene glycol) diacrylate (PEGDA) and poly(silyl ether). The functionality and cargo encapsulation of the hydrogel particle matrix can be tuned by varying the ratio of cross-linkers to monomers as well as particle sizes and the shapes. Thus, for example, DeSimone and colleagues demonstrated the use of the PRINT method for the synthesis of PEG-based rectangular hydrogel nanoparticles from a tetraethylene glycol monoacrylate monomer and a PEGDA cross-linker.28 The size of the hydrogel rectangles was shown to be precisely controlled with the particles having a 80 nm width but a varied length ranging from 180 to 5000 nm.31 The deformability of synthesized hydrogels could be accurately controlled by changing the cross-linker concentration. For instance, the 80 nm wide and 180 nm long particles with 96 wt% PEGDA retained their shape when dried unlike the particles produced with 2 wt% PEGDA which flattened and lost their shape demonstrating enhanced deformability. Atomic force microscopy (AFM) analysis revealed that the particle width decreased while its height increased upon increasing the hydrogel cross-link density.31

The PRINT particles can be imparted with biologically active functionalities by attachment of functional moieties or by introducing functional cross-linkers. For instance, the PEG hydrogels obtained from succinimidyl succinate monomethoxy-modified PEG were used to incorporate siRNA into the hydrogel matrix.32 The siRNA molecules were demonstrated to successfully attach to cylindrical PEG hydrogels having 200 nm length and diameter via free amine groups.32 PRINT hydrogels for tumor targeting therapy were produced from dimethylaminoethyl acrylate (DMAEA) using poly(silyl ether) as a cross-linker.30 In this case, the C–O–Si(R)2–O–C linkage in the bifunctional poly(silyl ether) can be hydrolyzed in acidic environments and therefore can render the particles biodegradable ensuring sustained therapeutic release from the cross-linked hydrogels.

2.2 Step and flash imprint lithography

Step and Flash Imprint Lithography (S-FIL) is a traditional lithography technique that specifically utilizes a quartz imprinting template to generate hydrogel nanoparticles with controlled dimensions.33 In a typical S-FIL process, a sacrificial layer of poly(vinyl alcohol) (PVA) is applied to bottom anti-reflective coating silicon wafers followed by the mixture containing monomers, photo-initiators and cross-linkers. The quartz template is then pressed onto PEGDA followed by exposure to UV light for polymerization. Unreacted PEGDA is removed by rinsing with DMSO after oxygen plasma etching. The polymerized particles are collected by dissolving the PVA sacrificial layer in water. Unlike the PRINT process that mostly relies on shear forces and a high surface energy with the counter sheet, S-FIL technology provides an exceptional convenience by utilizing a water-soluble sacrificial layer to release and harvest the hydrogel particles.34,35

A key feature of this method is the ability to vary the cross-link density and composition of the particle matrix using different macromers and macromer concentrations. Varying the concentration or molecular weight of the macromer solution does not significantly affect the size or shape of the particles but affects the dispensing efficiency of the solution. The S-FIL method can produce particles of various shapes with the minimal size down to 50 nm. For example, Roy et al. generated scalable amounts of cubical, discoid and rod-like PEG hydrogel particles with various swelling ratios by adjusting the concentration of PEGDA and using I2959 as an initiator.19,29,33 Apart from functionalizing the hydrogel particles by direct molecule attachment as mentioned for the PRINT particles, the S-FIL approach also provides another modification site, a sacrificial water-soluble polymer layer. Besides the PVA layer, poly(acrylic acid) (PAA) recently has been introduced as a sacrificial layer due to its ion sensitivity in aqueous solutions. For instance, switching from the PAA soluble to insoluble state in sodium and calcium ion solutions, respectively, enables a better release of the produced hydrogel particles from the template and therefore greatly improves the process's scalability with the benefit of being a one-step imprinting technology with high efficiency.34

By combining PRINT and S-FIL approaches, a novel method of sequential patterning with responsive micromolds has been recently developed.36 Temperature-responsive poly(N-isopropylacrylamide) (PNIPAM) microgels were first synthesized through PRINT technology, and then used as dynamic templates for the fabrication of agarose microgels via the imprint method. Using the PRINT technique, a PNIPAM template was molded to different shapes, including micro-grooves, circular and square micro-wells.36 Unlike the static templates used in traditional PRINT and S-FIL methods, the PNIPAM template also exhibited a dimensional change in response to temperature which enabled agarose microgels to achieve multi-compartmental structures (Fig. 2). The core–shell microgels with separate spatial distribution of red or green microbeads were obtained by sequentially adding agarose precursor containing microbeads into PNIPAM templates at a different temperature followed by agarose gelation (Fig. 2). In addition, prepared agarose microgels replicated the shapes of PNIPAM templates leading to differently shaped microstructures, e.g., cylindrical or cubical. This combined approach allows the microgels to acquire more complicated structures without sacrificing their shape.36


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Fig. 2 Top: Schematic diagram of sequential patterning of hydrogel microstructures with responsive micromolds. Fluorescent microbeads or cells (3T3 fibroblasts, HepG2 cells, and HUVECs) were encapsulated within agarose microgels during the fabrication process. (a) A gel precursor with encapsulated cells or microbeads is placed on a responsive micromold and molded with a PDMS slab at 24 °C. (b) Gel cross-linking at 4 °C for 15 min. (c) Shrinkage of responsive micromolds at 37 °C for 30 min. (d) A second gel precursor with encapsulated cells or microbeads is placed on a responsive micromold and molded with a PDMS slab at 37 °C. (e) Cross-linking of the second gel at 37 °C for 30 min. (f) Side and top views of obtained hydrogel microstructures. Bottom: (g) Phase contrast and fluorescence images for stripe, cylindrical, and cubic microgels recovered from responsive micromolds. Reproduced with permission from ref. 36. Copyright © American Chemical Society.

2.3 Flow lithography

Microfluidics-based methods have been developed for continuous hydrogel particle synthesis and can be multiplexed for a higher throughput with less effort in collecting samples. The microfluidic continuous flow lithography (CFL) technique provides a single-step route to synthesize monodisperse hydrogel particulates. Instead of exclusively relying on UV light to initiate polymerization used in the PRINT method, CFL provides flexibility by allowing other cross-linking methods.37 In a typical procedure, poly(dimethylsiloxane) (PDMS) is used to form a phase mask with a defined shape to facilitate a 3-dimensional (3D) light intensity and a microfluidic channel for the flow of a pre-polymer solution. The photo-polymerization is initiated by UV light passing through the shaped phase mask which leads to monodisperse hydrogels with a defined 3D structure.38,39

Doyle and colleagues demonstrated a wide variety of shaped PEG cross-linked particles obtained from PEGDA mixed with a photosensitive initiator.40 Particle arrays of mask-defined shapes were generated by exposing the flowing oligomer to controlled pulses of UV light. Due to the rapid polymerization kinetics, the hydrogel particles could be formed within 0.1 s, and an oxygen-aided inhibition near the PDMS surfaces favored the particle flow within a non-polymerized oligomer stream. Using this approach, the particle shape can be controlled in two directions. In the xy plane, a transparency mask with designed features determines the flat particle shape, while the height of the channel can be adjusted in the z-axis to control the particle height dimension.40

Highly curved bullet-shaped PEG hydrogel particles with magnetic functionalities were obtained by Hwang and colleagues using a variation of the microfluidic stop flow lithography (SFL) method.41 The magnetic polymeric hydrogel particles were synthesized from a mixture of PEGDA, the 2-hydroxy-2-methylpropiophenone initiator and a water-based ferrofluid.41 In addition, temperature-sensitive microgels composed of PNIPAM and alginate were achieved by using modified capillary microfluidic devices in which monodisperse spherical PNIPAM/alginate droplets were synthesized in a microfluidic channel and later changed their initial shape during cross-linking in a hot collection solution (45 °C, barium/glycerol). The final shape of the microgels could be tailored to a Janus particulate structure when the initial size of droplets was 150 μm, and to mushroom-like in the case of 300 μm droplets. The Janus particles exhibited distinct surface areas, while mushroom-like particles were shown to possess anisotropic architectures along with variable curvatures. These uniquely structured hydrogels can potentially be used in the design of stimuli-responsive drug delivery carriers for biomedical applications.42

Despite its many achievements, the continuous flow lithography method still has limitations including high costs of microscopy equipment, a decreased resolution of output particles at high flow rates, and a relatively low number of produced particles per light exposure. To address these issues, the Doyle group has advanced this technique further into contact flow lithography to fabricate shaped hydrogel particles efficiently and with lower costs.43 In the improved system, the photomask was tightened to a UV source and the distance between the mask and a microfluidic device was minimized enabling focusing of the UV light on a defined area to yield hydrogel particles of better resolved dimensions (20–50 μm).43 Using contact flow lithography, shaped particles deposited on surfaces or free-floating in the microfluidic channel can be obtained. Remarkably, after finely tuning the microfluidic multi-channel in the contact flow lithography system, in which the long sinuous channel was substituted with grouped short multi-channels while a splitting design was applied to equally split a monomer solution from a single inlet to the parallel channels, the particle synthesis rate increased by 100-fold compared to the standard continuous flow lithography approach without compromising the shape resolution of the prepared hydrogel particles. The triangular, cubical and rectangular particles maintained their sharp edges and straight side walls.43 Overall, this method provides new opportunities for the industrial scale-up of shaped hydrogels of high quality and should be able to further promote their applications.

2.4 Layer-by-layer assembly of polymers

The layer-by-layer (LbL) assembly of polymers at surfaces is a method of creating multilayer coatings at solid/solvent interfaces where one type of polymer chain can interact with another type via ionic-pairing, hydrogen-bonding, host–guest, and covalent and/or hydrophobic interactions when deposited on surfaces in a stepwise manner.44 When this polymer assembly method is applied to surfaces of colloidal organic, inorganic or biological (cells, bacteria) particles which can be later dissolved, polymeric particles replicating the size and shape of a sacrificial template can be obtained (Table 1).45–47 A high degree of control over composition, nanoscale thickness, mechanical and stimuli-responsive properties of the resultant polymeric particles is among the main advantages of this method.48–54 Conventionally, this method of polymer assembly onto particulates relies on centrifugation of the particles to separate excess polymer in solution from coated particulates followed by several rinsing steps with polymer-free solvent. When a desired number of polymer pairs (bilayers) is assembled on particle surfaces, the particulate template is dissolved or decomposed leading to a polymeric replica of the template. Because of the multistep process, this method can be time-consuming in the case when a large number of polymer bilayers is required, and may also suffer from partial colloid coagulation/aggregation resulting in partial loss of the colloids. To circumvent the issues of the time required for the polymer multilayer deposition and for an industrial scale-up, various approaches to automate the polymer deposition and increase the coated particle throughput have been developed by the Caruso group including electrophoretic polymer assembly,55 immersive polymer assembly on immobilized particles,56 a fluidized-bed assembly (Fig. 3),57 and the flow-based assembly using tangential flow filtration (Fig. 4),58 as well as a continuous ionic LbL assembly method using a tubular flow type reactor.59
Table 1 Sacrificial particulate templates of various non-spherical shapes used for the preparation of shaped multilayer capsules via LbL assembly of polymers
Shape Template Template decomposition Ref.
Cubical CdCO3; MnCO3; CaCO3 0.1 M HCl 73–77
Tetrahedral SnS 0.5 M HCl 78
Rod SiO2 HF 79
Polystyrene particles THF 80
Ellipsoid Bacteria E. coli NaCl + NaOCl 45
CaCO3 HCl 77
Discoid Si particles HF + HNO3 75 and 81
Echinocyte Red blood cells NaCl + NaOCl 45
Dodecahedral Metal organic frameworks EDTA 82



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Fig. 3 Top: Comparison of the steps required for conventional LbL assembly versus fluidized bed assembly to deposit a polymer bilayer. Bottom: Illustration of the flow stream, fluidized bed and microcapsule formation. The fluidized bed is formed in the column when the force of gravity on the template particles is balanced by the drag force of the flow. Polymer solution can be injected into the flow and is distributed upon entering the column so that the template particles can be uniformly layered. After a sufficiently thick film is generated, the template particles can be removed to yield microcapsules. Reproduced with permission from ref. 57. Copyright © 2014 American Chemical Society.

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Fig. 4 Hollow fiber tangential flow filtration (TFF) LbL assembly of capsules. Particulate templates are mixed with polymer A and, after incubation, purified using TFF. The layered and purified particles can then be mixed with the complementary polymer B to create a second layer. This process of TFF purification and LbL film deposition can then be repeated, yielding core–shell particles or capsules after core dissolution. Reproduced with permission from ref. 58. Copyright © 2015 American Chemical Society.

The polymer LbL assemblies might not fully represent the hydrogel-like structures unless one or both polymer components of the multilayer are covalently linked. In this case, the multilayer can resemble a hydrogel structure when exposed to conditions causing high swelling of polymeric networks. The polyelectrolyte capsule wall in which the polymer chains are held together via temporary physical links can exhibit stimuli-triggered polymer chain rearrangements which can lead to capsule volume alterations, and changes in capsule properties.60 For example, in ionically-paired poly(styrene sulfonate)/poly(allylamine hydrochloride) (PSS/PAH) capsules, electrostatic repulsions between accumulated excess charges lead to wall swelling, softening, increased permeability, and changes in capsule dimensions followed by capsule dissolution.61,62 Hydrogen-bonded systems, such as poly(methacrylic acid)/poly(N-vinyl pyrrolidone) (PMAA/PVPON), are stable at low pH but dissolve at elevated pH due to PMAA ionization. Therefore, in the case of multilayer hydrogel capsules, hydrogen-bonded or ionically paired LbL films as initial platforms are exposed to thermal-, photo-, or chemical cross-linking at the post-assembly step.63,64 Depending on the cross-linking method, single- or multi-polymer component hydrogels can be obtained.65–67 The covalent links stabilize the hydrogel wall upon environmentally-triggered core dissolution, while functional groups which are not involved in binding provide stimuli-responsive behavior.68–70 The resulting multilayer hydrogel capsules represent a unique example of fluid encapsulated by a stimuli-responsive nanothin hydrogel wall.71,72

2.4.1 Multilayer hydrogel capsules. When the hydrogel capsule wall is unconstrained after core removal, it is subject to the thermodynamic force of mixing which favors swelling due to the increased osmotic pressure and the elastic retractive force of the network that opposes swelling.83 The critical pressure difference and the corresponding hydrogel stiffness which control capsule deformation are directly proportional to the hydrogel thickness and inversely proportional to the capsule size.48,84 Remarkably, despite the inherent softness and swelling of a hydrogel capsule wall, both the size and shape of hollow multilayer hydrogel capsules have been demonstrated to follow those of the sacrificial template particles after the template dissolution.74,85 For example, single-component (PMAA)20 capsules retained the cubical shape of the MnCO3 cubical microparticle sacrificial template of 2 μm when the MnCO3 cores were dissolved in hydrochloric acid at pH = 3. This result demonstrated that ultrathin hollow hydrogels are capable of maintaining the anisotropic shape.85 The number of PMAA layers was shown to play a crucial role in the retention of the cubical capsule shape after core dissolution, and (PMAA)n hydrogels with n < 15 would result in capsules with buckled walls.85 Those shape instabilities of thinner PMAA capsules were attributed to low stiffness of the thin hydrogel wall resulting from a relatively high flexibility of PMAA chains and a relatively low number of cross-links. Hollow hydrogel capsules have been shown to be utilized as flexible micro-containers for encapsulation and delivery of therapeutics and/or imaging functional molecules.86
2.4.2 Multilayer hydrogel particles. Unlike other techniques described above, the LbL polymer assembly can offer the fine-tuning of a hollow hydrogel interior structure. In the case of solid non-porous particles, polymer infiltration is prohibited during LBL deposition and therefore leads to hydrogel capsules with an open cavity and nanothin walls. Conversely, when polyelectrolyte multilayers are deposited inside porous sacrificial templates, nano-porous particles of interconnected macromolecular networks are obtained (Fig. 5a).25,26,87,88 Porous silica and calcium carbonate particles are widely used as sacrificial inorganic cores with benefits of controllable size, large surface area, and pore size. For instance, nano-porous particles of thiolated PMAA were prepared by mesoporous silica templating and showed rapid internalization by HeLa cells.89 Our group has recently demonstrated the synthesis of stimuli-responsive nano-porous hydrogel microparticles of cubic shape and showed that these cubic hydrogels maintained their three-dimensional shapes in the dry state (Fig. 5d–f).25 These cubic PMAA hydrogels were produced by sequential infiltration of PMAA and PVPON inside 2 μm porous cubic templates by their exposure to the polymer solutions at pH = 3.6.25 After the sequential infiltration of seven (PMAA/PVPON) bilayers, the on-template assembly was cross-linked with ethylenediamine using carbodiimide-assisted coupling followed by exposure to pH = 8.5. This procedure resulted in PVPON release due to the disruption of hydrogen bonds between PVPON and deprotonated PMAA leading to cross-linked PMAA networks inside the pores.
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Fig. 5 (a) Non-porous MnCO3 cubic particles (1) transformed into porous Mn2O3 cubic particles (2) upon heating at 700 °C in air. Hydrogen-bonded PMAA/PVPON complexes formed inside pores of PEI-coated templates (3) were cross-linked with ethylenediamine to form an interconnected PMAA hydrogel network (4). After core dissolution, responsive hydrogel cubes of interconnected PMAA networks are formed (5). SEM images of MnCO3 (b) and porous Mn2O3 (c) cubic inorganic templates. Three-dimensional reconstructions of consecutive focal plane confocal microscopy images of 2 μm cubic hydrogels of PMAA (d) with their corresponding orthogonal (side panel) view (e) imaged in 0.01 M phosphate buffer solutions at pH = 7.4. SEM images of cubic (PMAA)5 multilayer hydrogel particles (f) and capsules (g). Adopted with permission from ref. 25, Copyright © 2014 Royal Society of Chemistry and from ref. 26, Copyright © 2015 American Chemical Society.

In contrast to multilayer hydrogel capsules which collapse upon drying and lose their non-spherical solution shape, the PMAA network of a multilayer-derived hydrogel particle is ‘packed’ throughout the volume of the particle, therefore providing an enormous area of interaction for various species in contrast to that in a capsule which has only a thin hydrogel shell. Moreover, these hydrogel particles preserve their three-dimensional structure when dried because of their enhanced rigidity (Fig. 5f and g).25,26 It is worth noting that when multilayer hydrogel capsules and particles are done through LBL, cross-linkers are not limited to photo-sensitive molecules like in the PRINT method which may broaden their future applications in biomedicine and biotechnology.

3. Stimuli-sensitive properties of non-spherical hydrogel particles

3.1. pH Sensitivity

Acidity in biological environments can vary significantly which is widely exploited for designing pH-sensitive particulate hydrogels for the delivery of therapeutics. For example, the extracellular pH decreases in the tumor space due to the high rate of aerobic glycolysis down to pH ∼ 6.1–5.6.90,91 In addition, the acidic pH can render tumors resistant to some anticancer drugs because of increased drug polarity which may prevent their crossing of biological barriers92 and therefore may warrant their encapsulation into delivery vehicles.49,93 Also, intracellular release of therapeutics from pH-sensitive hydrogel drug carriers can be designed based on acidification of cellular organelles when they progress along the endocytic pathway from early to late endosomes, and further to late lysosomes with the corresponding acidity values decreasing from pH = 6.5 to pH < 6.0, and to pH < 5.5, respectively.94 These pH variations are used to design pH-responsive hydrogel particles for site-specific drug delivery.

The typical structure of a pH-sensitive hydrogel contains ionizable pendant groups which undergo reversible ionization at different pH values leading to pH-dependent particle size changes.95 In general, synthetic polymer-based anionic hydrogels are synthesized from acidic polyacids including poly(acrylic acid) (PAA), PMAA, and poly(ethacrylic acid) (PEAA) or their copolymers, which swell at pH greater than their pKa values due to the osmotic pressure of ions.96 Cationic hydrogels derived from poly(N,N-dimethylaminoethyl methacrylate) or other primary amine-containing polymers become polar and swell at pH < pKa.97,98 The hydrogel volume changes induced by the environmental pH shifts can be used for drug loading and release under hydrogel swelling and collapse, respectively.

In one example, cubic PMAA multilayer hydrogel microparticles showed pH-dependent swelling ratios of 1.7, defined as the ratio of swollen to deswollen hydrogel particle size.25 Hydrogel cubes made from 21 kDa PMAA increased in size from 1.9 ± 0.2 μm to 3.2 ± 0.1 μm when the solution pH was changed from pH = 5 to pH = 7.4 (Fig. 6). Similarly, cubic hydrogels of 360 kDa PMAA changed from 1.9 ± 0.2 μm to 3.1 ± 0.2 μm, resembling the previous pH variations and indicating no effect of PMAA molecular weight on cubic hydrogel pH-responsive behavior. The pH-triggered volume changes were completely reversible. Remarkably, these hydrogels retained their cubic shape upon pH change and preserved their cubic geometry in the swollen state at pH = 7.4 indicating uniform swelling/shrinkage of the networks. Both cubic and spherical hydrogels underwent a nearly 2-fold reversible swelling/shrinkage response to pH variations and retained their shape while increasing in size, providing remarkable examples of pH-responsive shaped hydrogels. The swelling behavior of these cubic and spherical hydrogel particles is controlled by the network structure, which can be regulated by the PMAA molecular weight and the template properties.


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Fig. 6 Left: Optical microscopy images of 2 μm cubic (21 kDa PMAA) (a and b), 4 μm cubic (21 kDa PMAA) (d and e) particles imaged at pH = 7.4 (a and d) and at pH = 5 (b and e). Right: pH-Induced size variations of 2 μm cubic (c) and 4 μm cubic PMAA hydrogel particles (f) produced from 21 kDa or 360 kDa PMAA. The size measurements were performed using confocal microscopy. Reproduced with permission from ref. 25. Copyright © 2014 Royal Society of Chemistry.

Apart from using ionizable polymers, the use of pH-cleavable network linkers can confer pH-responsiveness along with pH-induced degradability. The DeSimone group has demonstrated the synthesis of silyl ether-containing monomers which were molded into cubic or hexnut microgel particles using the PRINT technique (Fig. 7).30 The particle degradation and the encapsulated drug release rate were shown to be precisely controlled by introducing various substituent groups to the Si atom. All hydrogel particles underwent pH-induced degradation showing a significant acceleration in degradation rates at pH = 5 compared to those at pH = 7 regardless of the substituent groups used for the modification. The bulkiness of the substituent groups, however, affected the microgel particle degradation at a fixed pH leading to a prolonged degradation time. For example, by using dimethyl, diethyl and diisopropyl substituent groups, the degradation of PRINT hydrogel cubes could be tuned from several hours to several weeks at pH = 5.30 Notably, the silyl ether hydrogels swelled and then degraded to lose their distinctive hexnut shape after internalization by HeLa cells while non-degradable hexnut hydrogels retained their original size and shape inside the cells. The silyl ether chemistry was used to conjugate a drug molecule to the shaped PRINT hydrogels for controlled drug delivery, and the release of the drug was also regulated by changing the solution pH and the substituents around the Si atom (Fig. 8).99 The controlled intracellular drug release was further verified through the apoptosis and proliferation assessment of LNCaP cells. The ethyl-substituted silyl ether prodrug-hydrogel exhibited comparable cytotoxicity as the free drug, indicating successful drug transport into cancer cells after 72 h incubation. In contrast, the tert-butyl substitution on the Si atom led to negligible drug release from the hydrogel, resulting in nontoxicity to LNCaP cells at the same incubation time (Fig. 8).99


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Fig. 7 (A and B) Synthesis of bifunctional silyl ether cross-linkers. Scanning electron micrographs of (C and D) 5 μm cubes and (E and F) 3 μm hexnut particles fabricated using the PRINT process (scale bars are 10 μm). Reproduced with permission from ref. 30. Copyright © 2010 American Chemical Society.

image file: c6tb02746f-f8.tif
Fig. 8 (A) (a) Asymmetric bifunctional silyl ether prodrugs of gemcitabine; (b) structure of gemcitabine; (c) percent release of gemcitabine versus time for 200 × 200 nm PRINT nanoparticles fabricated with Et-GEM (blue, Et: ethyl), iPr-GEM (red, iPr: isopropyl), and tBu-GEM (green, tBu: tert-butyl) prodrugs. Closed symbols represent particles degraded at pH 5.0 and open symbols represent particles degraded at pH 7.4. (B) Confocal microscopy images of LNCaP cells stained with the PathScan apoptosis and proliferation kit. The cells were separately dosed with (a) free gemcitabine, (b) Et-GEM particles, (c) tBu-GEM particles, and (d) blank particles. Red indicates a healthy cell containing fundamental cytosolic fibers important in meiotic/mitotic chromosome alignment. Green indicates a healthy cell undergoing microtubule assembly during mitosis. Purple indicates cytoskeleton proteins and nuclear protein experiencing an apoptotic event. Reproduced with permission from ref. 99. Copyright © 2010 American Chemical Society.

Similarly, the pH-sensitive degradation of ester bonds in a highly cross-linked diacrylate PLA-b-PEG-b-PLA water-swollen gel network that degraded through the hydrolysis of ester bonds in the PLA block was utilized in microgel particles made by stop-flow lithography from this bulk-erodable polymer with cubical and triangular shapes and tunable time-degradation properties.100

3.1.1 pH-Induced shape change. There exists an important issue for hydrogel microparticles of non-spherical shapes: whether their swelling or collapse can significantly alter the particle size and shape. The possibility of such an alteration can be regarded in opposing manners: it would either compromise the benefit of the intended original shape, or would be favorable as observed in biological microsystems including red blood cells, leucocytes, bacteria, and spores that serve as examples of shape adaptability. In this regard, although the highly cross-linked micro-sized networks obtained by microfluidics, lithography, and PRINT offer excellent control over shape and size, they lack the capabilities of stimuli-induced dynamic size/shape changes.101–103 Thus, pH-induced shape transitions due to network swelling may require spatial conditions for polymer chain rearrangement that may not be readily available in particles obtained from those processes.

Related to hydrogel size consideration, experimental and theoretical results on monodisperse hydrogel particles with various lengths but with the same cross-sectional dimensions of 800 nm by 100 nm by 100 nm, 400 nm by 100 nm by 100 nm, and 100 nm by 100 nm by 100 nm made from PEGDA of various percent polymers 10–50% (v/v) using the S-FIL technique demonstrated that geometric (size) and mechanical (surface attachment) constraints may result in anisotropic and inhomogeneous swelling for hydrogel particles.33 For example, it was reported that the swelling ratio of bulk versus surface-attached particles is comparable when the particle length is longer than 400 nm, but the surface-attached swelling ratio becomes significantly larger than the bulk value when all particle dimensions are less than or equal to 100 nm. Theoretical analysis also confirmed that the highly cross-linked PEGDA hydrogels could not swell to the point where the shape and size of these particles would be altered for particle sizes larger than 100 nm. These findings may provide important insights into dimensional parameters of hydrogel particles capable of dynamic shape changes.

Unlike bulk microscopic networks, hydrogel microcapsules have much larger free volume due to the capsule interior and the ultrathin (<100 nm) hydrogel wall which can result in much larger swelling ratios compared to those of bulk hydrogels of the same chemistry. In addition, because the swelling rate is inversely proportional to the square of network dimensions,104 nanoscale capsule hydrogel walls can exhibit an extremely fast response to external stimuli, unlike microscopic hydrogels.105,106 For instance, cubical single-component (PMAA)14 multilayer hydrogel capsules cross-linked with ethylenediamine74 and (PMAA)20 capsules obtained from multilayers of the PMAA-co-((3-aminopropyl)methacrylamide) statistical copolymer became bulged into sphere-like structures after exposure to pH = 8. The bulging was attributed to the stress in the capsule wall resulting from uncompensated electrostatic repulsion between COO groups at pH = 8 and small counter ions penetrating the hydrogel to compensate negative charges. The shape, however, was not completely reversed when the (PMAA)20 cubical capsules were exposed to acidic pH and the PMAA hydrogel collapsed.

Increasing the capsule wall thickness and/or the cross-link density should lead to reversibility in the capsule shape change or even to the ability of the non-spherical capsules to maintain their shape upon size increase when the hydrogel wall swells. Indeed, when the second component was retained within the hydrogel capsule wall by chemical cross-linking of PVPON-co-((3-aminopropyl)methacrylamide) (PVPON–NH2) to PMAA layers using a water-soluble carbodiimide, the two-component (PMAA–PVPON)5 cubical hydrogel capsules did not bulge and remained cubical, increasing in size instead when solution acidity was increased from pH = 3 to pH = 8.85 These distinctively different pH-triggered shape responses of (PMAA) and (PMAA–PVPON) multilayer hydrogel capsules were achieved by controlling the capsule shell rigidity.85

Hydrogel rigidity and capsule geometry are key factors in regulating the shape response of a hydrogel capsule. As reported in a computational study, faceted capsules can display inhomogeneous strain/stress distributions along the edges, while vertices provide mechanical reinforcement to edges restricting their expansion/contraction.107 Thus, pH-induced stress may release inhomogeneously through mechanically weak facets resulting in anisotropic swelling of non-spherical capsules. For example, our group demonstrated two types of discoid multilayer hydrogel capsules mimicking the shape of red blood cells which exhibited different shape transitions in response to pH changes.81 The (PMAA)15 and (PMAA–PVPON)5 discoidal capsules demonstrated various degrees of out-of-plane swelling of the discoidal circular faces, i.e., circular face bulging at pH = 7.4. The spherical (PMAA)15 capsules displayed a dramatic 19-fold volume increase when the solution pH was altered from 4 to 7.4. Unlike the 19-fold swelling of (PMAA)15 systems, two-component (PVPON–PMAA)5 capsules underwent only a 2.9-fold increase in their volume. This difference in pH-triggered variations in capsule size was rationalized by comparing free volume within the capsule hydrogel shell. The (PMAA)5 multilayer planar hydrogel displayed a 2-fold greater water uptake than (PMAA–PVPON)5 at pH = 3 with water content values of 41% and 19% for (PMAA)5 and (PMAA–PVPON)5, respectively.81 Apparently, the presence of the second component reduced the free volume in the dual-component network suppressing the capsule swelling.

Importantly, pH-triggered dimensional changes of (PMAA)15 and (PMAA–PVPON)5 discoidal capsules were demonstrated to be drastically different. The (PMAA)15 showed dramatic volume transitions of 24-fold; while a moderate 2.3-fold volume change was found for (PMAA–PVPON)5 discoidal capsules upon the pH shifts. Both radial and axial dimensions of (PMAA) capsules were 1.8-fold greater than those for (PMAA–PVPON) capsules at pH = 7.4. The larger expansion of the one-component hollow hydrogel discs was consistent with the greater swelling of the corresponding hydrogel spheres and surface-attached hydrogel films as compared to their dual-component counterparts. However, the aspect ratios of two types of discoidal capsules, i.e., length-to-height ratios, remained similar at pH = 7.4 indicating that both types of hydrogels expanded in a similar way in the ionized state. Those values were smaller than the aspect ratio for their solid templates which indicated the preferential expansion in the axial direction for both types of capsules upon core dissolution and exposure to neutral pH.81

The pH-triggered change in capsule dimensions resulted in anisotropic swelling/shrinkage leading to discoidal-to-ellipsoidal shape transformations with the degree of this shape transition depending on the wall composition. The observed variations in pH-dependent aspect ratios for the two types of the discoid hydrogel capsules were explained by a greater degree of the out-of-plane swelling of (PMAA) capsules compared to that of (PVPON–PMAA) systems at pH = 7.4. Quantifying the degree of swelling in the axial and radial directions revealed a negligible difference between the ratios for both types of the discoidal capsules which implied no preferential swelling in axial or radial directions upon pH variations.81

Apart from the shape anisotropy, anisotropic structures of a hydrogel composed of passive (non-swellable) and active (highly swellable) hydrogel layers on top of each other can also be used to induce an overall shape change using a pH trigger. For example, a dual hydrogel composed of a poly(2-hydroxyethyl methacrylate) (PHEMA) layer on top of a poly(2-hydroxyethyl methacrylate-co-acrylic acid) P(HEMA-co-AA) layer prepared in the shape of a planar circle using photolithography quickly (within a minute) formed a microcapsule with the PHEMA as an inner coating of the particle shell when exposed to a pH = 9 solution.108 The reversible shape transformation occurred due to P(HEMA-co-AA) layer swelling at pH = 9 which could swell up to 1000 v/v% while the PHEMA layer remained de-swollen leading to two-dimensional bending due to the highly flexible hydrogel matrix. This result is particularly interesting demonstrating the importance of softness and mechanical robustness of the hydrogel matrix to induce particle shape reconfiguration.

3.2. Redox sensitivity

There is a significant difference in the redox potential between intracellular and extracellular environments. Glutathione (GSH), a tripeptide enzyme in cells, can reduce disulfide bonds to the corresponding thiols as an electron donor.109 The intracellular GSH concentration of 2–10 mM is 1000 times higher than that of 2–20 μM in the extracellular environment and some tumor cells have GSH concentration several times more than normal cells.110 Furthermore, the endosomes/lysosomes contain a high content of the reducing enzyme γ-interferon-lysosomal thiol reductase (GILT) that can reduce protein disulfide bonds at low pH, and of cysteine which may also exhibit reducing properties.111 Therefore, the hydrogel particles with an engineered redox response can facilitate a rapid intracellular drug release while being stable in the extracellular media, which can inhibit drug resistance.112–116 The disulfide bond is among the most widely used to impart redox responsiveness to gel particles while other redox-sensitive linkers are still overlooked, most likely due to the challenge of their incorporation into particles in aqueous solution.117

Redox-sensitive hydrogel particulates, similar to other types of hydrogels, swell in aqueous solutions owing to the presence of hydrophilic moieties. Cross-linkers that have disulfide centers can be used to establish and stabilize the three-dimensional structure of a gel particle under physiological conditions which can rapidly disassemble upon the cleavage of disulfide bonds in the presence of increased concentrations of reducing agents present in intracellular or tumor sites, resulting in the fast and complete release of encapsulated therapeutics.26,118–121

A variety of factors including hydrogel geometry, cross-link density, and the type of reducing agents present in solution can affect the degradation profile of the redox-sensitive non-spherical hydrogels. For example, redox-labile PRINT cubes 2 μm in size reported by DeSimone and coworkers demonstrated a different anticancer effect compared to those with non-degradable linkers.122 After incubation of the PRINT cubes loaded with doxorubicin (DOX) in a 100 mM dithiothreitol solution for 48 hours, a ∼20% decrease in DOX fluorescence was observed for the reductively-labile cubes indicating DOX release in the reducing environment unlike non-degradable cubes where there was an absence of DOX in the bulk solution.122 The reduction of the disulfide bonds was believed to cause a decrease in the particle mesh density which allowed DOX to diffuse out. The viability of cancer HeLa cells also decreased for the reductively-labile PRINT cubes compared to the particles with non-cleavable linkers, confirming a redox-triggered drug release in the cells. In addition, the redox-sensitive PRINT cubes were surface-functionalized with avidin for further incorporation of biotinylated targeting ligands for targeted delivery.122

Apart from stabilizing the hydrogel network, disulfide-containing linkers can also be used not only to conjugate therapeutic agents to a non-spherical hydrogel but also to control the rate of drug release as well as to protect therapeutics from premature release or even destruction by active molecules in serum. For example, cylindrical hydrogel rods (with the aspect ratio of 4) bearing primary amines were synthesized first and thiol-modified siRNA was conjugated to the hydrogels via succinimidyl 3-(2-pyridyldithio)propionate (SPDP) chemistry with the loading ratio of 18 wt% (Fig. 9).123 The siRNA molecules attached to the hydrogel cylinders were stable after incubation in 30% fetal bovine serum (FBS) solution for 24 hours in contrast to naked unprotected siRNA molecules which were completely degraded by FBS under the same incubation conditions. This pro-drug strategy of conjugating siRNA into the shaped cylindrical hydrogel through disulfide bonds used for gene delivery also prevented siRNA leakage from the pro-siRNA hydrogel under physiological conditions and resulted in increased stability of the siRNA. The in vivo study further indicated that the coagulation factor VII (FVII) siRNA was successfully delivered to liver tissues through hydrogel particles and was able to exert its bio-function, leading to a significant reduction in FVII mRNA expression in a dose-dependent manner (Fig. 9).123


image file: c6tb02746f-f9.tif
Fig. 9 (A) Surface modification of PRINT hydrogel cylinders with post-fabricated siRNA: (a) NHS–PEG–COOH, DMF, pyridine; (b) (succinimidyl 3-(2-pyridyldithio)propionate) (SPDP), PBS/CH3CN; (c) siRNA-SH, PBS; (d) poly-L-lysine, 1-ethyl-3-(3-(dimethylamino)propyl)carbodiimide hydrochloride (EDC), sulfo-NHS, PBS. (B) Coagulation factor VII (FVII) mRNA level in the liver with qRT-PCR assay. (C) Confocal micrograph of liver tissue (24 h after intravenous administration of nanoparticles) from mice treated with DyLight 680 labeled nanoparticles (green). Cellular actin cytoskeleton was stained with phalloidin (red), macrophages with MARCO (magenta), and nuclei with DAPI (blue). Reproduced with permission from ref. 123. Copyright © 2015 American Chemical Society.

Using simultaneous copolymerization of the siRNA macromonomer with the hydrogel matrix components, a larger degree of loading of the nucleic acid into a PRINT cylindrical particle could be achieved. For instance, when a degradable disulfide siRNA pro-drug macromer (where siRNA was derivatized with a photopolymerizable acrylate) with a degradable disulfide center was covalently incorporated inside PRINT hydrogel particles during the network formation of loosely cross-linked cationic PRINT discoid cylinders, the siRNA loading ranged from 15 to 35% depending on the content of 2-aminoethylmethacrylate hydrochloride incorporated within the hydrogel during polymerization (Fig. 10).124 The siRNA inside the particles was also demonstrated to be protected from degradation by RNAses for 48 hours when incubated in serum, while a naked macro-monomer siRNA was rapidly degraded in serum under the same conditions.124


image file: c6tb02746f-f10.tif
Fig. 10 (a) Structures of degradable and nondegradable siRNA macromers as well as native siRNA, (b) illustration of pro-siRNA hydrogel behavior under physiological and intracellular conditions, and (c) SEM micrograph of pro-siRNA, 200 × 200 nm cylindrical nanoparticles (scale bar = 2 μm). Reproduced with permission from ref. 124. Copyright © 2012 American Chemical Society.

Since hydrogel degradation and subsequent release of therapeutics depend on particle surface area, size, and other dimensional characteristics, it would be highly desirable to explore the effect of shape on the degradation behavior of non-spherical hydrogel particles. This is especially interesting as hydrogels of complex shapes can produce complex multistep degradation profiles due to variations in thicknesses as well as changes in particle shape which follow the degradation process.

For example, a slightly faster degradation of nano-porous hydrogel spheres compared to cubes made of (PMAA)5 multilayer hydrogels and cross-linked with cystamine was observed in the presence of intracellular concentrations of glutathione as measured using suspension turbidity changes.26 The relative turbidity, defined as the ratio of the (PMAA)5 hydrogel particle solution scattering intensity at certain time points to the initial scattering intensity, was measured in the presence of 5 mM GSH solution in PBS (pH = 7.4, 37 °C) using fluorescence spectrophotometry. With no GSH in the hydrogel suspension, the relative turbidity of (PMAA)5 hydrogels did not change with time indicating the chemical stability of the hydrogel particles while GSH treatment provided complete hydrogel particle degradation in 3 hours. The faster degradation of the spherical multilayer hydrogels versus that of cubical shaped hydrogels was observed within the first hour with the relative turbidities of 40 ± 3 and 50 ± 2%, respectively, and was attributed to a 1.9-fold larger hydrogel cube volume compared to that of spheres of the same size. Despite the micrometer size of the hydrogels, the reduction of the disulfide groups within the cystamine-cross-linked (PMAA) multilayer hydrogel cubes or spheres to the corresponding thiols in the cytoplasm still releases only short polymer chains capable of rapid renal clearance.

The thiolated PMAA obtained by modification of the polyacid carboxylic groups with pyridine dithioethylamine hydrochloride using carboddimide chemistry has been developed and widely used by the Caruso group for the fabrication of redox degradable spherical multilayer hydrogel capsules using LbL assembly. This technique was also applied to fabricate rod-like multilayer hydrogel capsules with various aspect ratios ranging from 1 to 4 (Fig. 11).79 Due to the coexistence of PMAA and disulfide bonds, the hydrogel capsules could both swell at physiological pH and degrade after cellular internalization via endocytotic pathways.


image file: c6tb02746f-f11.tif
Fig. 11 TEM images of PMAA hollow hydrogel capsules with aspect ratios of (a) AR = 1, (b) AR = 2, (c) AR = 3, and (d) AR = 4, obtained by using silica rod templates. Scale bars are 2 μm. Scale bars in the insets are 0.2 μm. Reproduced with permission from ref. 79. Copyright © 2013 American Chemical Society.

3.3. Temperature sensitivity

Temperature-sensitive hydrogels exhibit volume-phase transitions in response to temperature change in the surroundings, which can be classified into two main categories: (1) those composed of polymers which have an upper critical solution temperature and (2) those composed of polymers which have a lower critical solution temperature (LCST). Among the LCST polymers, special interest is devoted to hydrogel particles made of PNIPAM and poly(N-vinylcaprolactam) (PVCL) with their LCSTs close to the physiological temperature range. For PNIPAM- or PVCL-based hydrogels the phase transition is described by a volume phase transition temperature when the hydrophobicity of the cross-linked polymer chains increases and water molecules are expelled from the gel interior. Even though PNIPAM and PVCL have similar LCSTs in the range of 32–36 °C, the mechanism and thermodynamics of the phase transition are different and therefore require different methods for the LCST variation. While PNIPAM has an LCST independent of polymer molecular weight, with environmental conditions such as pH and composition controlling its LCST, PVCL exhibits an LCST which follows classical Flory–Huggins thermoresponsive phase diagram behavior125 with the LCST value being highly dependent on the polymer molecular weight and concentration.126,127

An amazing example of hydrogel particle shape control via reaction temperature during a micro-emulsion polymerization was demonstrated by Zhu and coworkers who synthesized temperature-sensitive PNIPAM/chitosan/Fe3O4 microgels with a spindle-shaped, cuboid, and spherical morphologies by increasing the reaction temperature from 28 to 34, and to 40 °C, respectively.128 This polymerization is based on the precipitation of polymeric chains as particles as they grow and become insoluble in a solvent. During polymerization, the growing polymer chain phase separates from the solvent and forms a nucleic aggregate by capturing newly formed polymer chains. Interestingly, the corresponding PNIPAM/chitosan microgels produced at corresponding temperatures were all of spherical shape. In this case the various degrees of stabilization provided by Fe2O3 nanoparticles affected both the polymer chain conformation during polymerization (from more extended to more collapsed) and the subsequent particle shape. The temperature sensitivity of these hydrogel particles was measured by dynamic light scattering and it was found that a sharp decrease in the hydrodynamic diameter resulting from collapsed PNIPAM chains occurred when the temperature was increased above 32 °C. The temperature-sensitivity study, however, was limited to spherical hydrogels and the effect of the temperature-induced volume changes on the shape of non-spherical hydrogels was not reported.128

The effect of temperature-triggered hydrogel volume changes on the shape of non-spherical hydrogel structures was recently explored and reported by Zhang et al.129 and Crassous et al.130 In the first case, a temperature-sensitive dendrite-shaped hybrid hydrogel particle composed of PNIPAM/dextran-allyl isocyanate (PNIPAM/Dex-AI) in which Dex-AI served as a precursor and a biodegradable cross-linker was fabricated through a precipitation polymerization.129 The swollen hydrogel particles had cotton ball-like morphology and each particle had a central mass with many spikes protruding in a dendritic fashion. An average dendrite-like particle exhibited significant geometry changes over the temperature range of 10 to 60 °C. The volume of hydrogel particles decreased by 11% from 10 to 22 °C and could reach up to 39% shrinkage at 60 °C due to the temperature sensitivity of the PNIPAM component. The freeze-dried PNIPAM/Dex-AI hydrogel particles had the appearance of coral with a heterogeneous porous microstructure. In the second case, PNIPAM-based, core–shell composite ellipsoidal, faceted, and bowl-like microgels composed of a polystyrene core and a cross-linked PNIPAM shell were reported.130 The specific particle shapes were achieved through different techniques, including uniaxial stretching for ellipsoidal shapes, phase separation in dodecane for faceted gels, and freeze-drying for bowl-shaped gel particles. These (PS core–PNIPAM hydrogel shell) particles exhibited shape-dependent temperature responsiveness. For example, the volume-phase transition of the spherical hydrogels occurred at 42 °C whereas it shifted to 38 °C for the ellipsoidal and to 45 °C for the faceted hydrogels. The bowl-shaped hydrogels had a volume-phase transition similar to that of the spherical particles at 42 °C. The shape-dependent variation of the volume-phase transition was shown to originate from various deformation processes during particle formation resulting in different stiffness of the particle shell.

Our group recently reported on cubical hollow capsules with a shell made of a PVCL multilayer hydrogel which showed distinctive and reversible temperature-responsive behavior (Fig. 12).131 These cubical PVCL hydrogel cages were produced by selective cross-linking of PVCL–NH2 copolymer layers within LbL hydrogen-bonded multilayer films of PMAA and PVCL–NH2 which were assembled on monodisperse spherical silica and cubical manganese carbonate templates, followed by the release of PMAA from the PVCL multilayer hydrogel at basic pH and dissolution of the inorganic template particle in hydrochloric acid.131 In contrast to the above-mentioned hydrogel particles where temperature changes during or after particle synthesis could affect and/or alter a hydrogel particle shape to some degree, these PVCL hydrogel cubical capsules could shrink in size when the temperature of the capsule solution was elevated from 25 to 50 °C but maintained their cubical shape. Numerically, the cubical (PVCL)7 capsules decreased in size by 21 ± 1%. The fact that the capsules retained their cubical shape at the elevated temperature indicated a uniform decrease in the capsule size upon heating. Spherical (PVCL)7 hydrogel capsules of the same size demonstrated similar shrinkage of 23 ± 1%. The temperature-triggered size changes of both types of capsules were completely reversible. The degree of the temperature-triggered shrinkage was controlled by varying the cross-link density from 9 to 23 cross-links per chain for the hydrogels derived from PVCL–NH2-n with n = 7 and n = 14, respectively, where n denotes the molar percentage of amine group-containing polymer units. The hydrogel films made from PVCL–NH2-7 exhibited a shrinkage of 1.9 ± 0.1. An increase in the cross-link density in PVCL–NH2-14 hydrogels significantly suppressed the shrinkage ratio down to 1.3 ± 0.1.


image file: c6tb02746f-f12.tif
Fig. 12 (a) SEM image of (PVCL)15 hydrogel cubical hollow capsules dried on a Si wafer from aqueous solution at pH = 3. (b and c) Hollow cubical (PVCL)7 multilayer hydrogel capsules in aqueous solution at T = 25 °C. (d) Cubical (PVCL)7 capsules imaged after 25 °C/50 °C/25 °C/50 °C temperature cycles. Scale bar is 2.7 μm. (e) The shrinkage ratios (the ratio of the capsule size at 25 °C to that at 50 °C, d25/d50) of (PVCL)7 multilayer hydrogel hollow spherical and cubical capsules. Reproduced with permission from ref. 131. Copyright © 2012 American Chemical Society.

3.4. Enzyme sensitivity

Enzyme-responsive hydrogel particles usually contain ester or peptide linkages in their network and can be cleaved by intracellular esterases and proteases. Similar to the redox-sensitive hydrogels, the enzyme-responsive hydrogels can lose their cross-linked structure in response to enzymatic degradation which can be highly advantageous for fast and site-specific drug delivery. Unlike pH- or redox-sensitive hydrogels, the enzymatically-sensitive hydrogel particles may be designed to release encapsulated therapeutics at a particular diseased tissue or inside a specific cellular compartment. This specificity provided by selective enzymes should yield a significant improvement in the delivery of highly toxic chemotherapeutics or drugs with a short half-life.

In this regard, Roy and colleagues fabricated enzymatically degradable hydrogels of square, triangular and pentagonal shapes using the S-FIL technique.29 The hydrogels were composed of hydrophilic PEGDA, acrylated peptide, Gly-Phe-Leu-Gly-Lyse, and a diacrylated GFLGK peptide cross-linker which served as a cleavable moiety. The Gly-Phe-Leu-Gly can be selectively degraded in the presence of several lysosomal thiol proteases, and it is particularly sensitive to Cathepsin B which is overexpressed in the lungs, ovarian and colorectal tumor cells and is present extracellularly in tumor tissues.132 After incubation with Cathepsin B, the shaped hydrogels obtained from the mixture of PEGDA and acrylated GFLGK with a molar ratio of 1[thin space (1/6-em)]:[thin space (1/6-em)]1 started to degrade within 30 minutes and completely disassembled after 48 hours. To confirm that the prepared hydrogels exhibited the enzyme-triggered drug behavior, an antibody and small DNA were used as model drugs which were loaded into hydrogels during S-FIL fabrication. In both cases, major drug release occurred only after exposure to the Cathepsin B enzyme indicating the highly controlled, disease-specific release of drugs.

3.5. Other stimuli

3.5.1. Mechanical force. The mechanical flexibility of hydrogel particles intended for in vivo applications is an important parameter which may allow for control over particle circulation in the blood stream and the circulation lifetime, while control over elasticity can also govern the particle's bio-distribution.18,133 For example, DeSimone and colleagues have demonstrated that increasing the deformability of hydrogel particles of 6 μm composed of 2-hydroxyethyl acrylate slightly cross-linked with PEGDA and mimicking the shape of human RBCs produced by the PRINT technique (Fig. 13) significantly increased their circulation times and altered their bio-distributions.18 The 10%- and 1%-cross-linked RBC-shaped microgels with the corresponding bulk moduli of ∼64 and ∼8 kPa demonstrated the elimination half-life of 3 and 93 hours, respectively. Moreover, when these RBC-shaped microgels were flown through a microfluidic channel of a 2-fold smaller diameter of 3 μm, only the discoidal hydrogels with a low modulus (<17 kPa) could pass through the channel pore by stretching and increasing in length and recovering their discoidal shape in the absence of flow, while the more rigid discoids rapidly clogged the pores.18
image file: c6tb02746f-f13.tif
Fig. 13 (A) The PRINT process used to fabricate RBC-shaped microgels: an elastomeric fluoropolymer mold (green) with disk-shaped wells was covered by an aliquot of the prepolymer liquid (red). The mold was passed through a pressured nip (black) covered by a high-surface energy sheet (gray), wicking away excess liquid from the mold surface while filling the wells. The filled mold was cured photochemically, yielding crosslinked particles, which were harvested from the mold by laminating a PVA film (blue) on top of the mold through a pressured nip and peeling way the mold. Dissolving the poly(vinyl alcohol) film resulted in a suspension of hydrogel particles. (B) Fluorescence micrograph of polymerized particles in the mold, and (C) fully hydrated particles free of the mold, suspended in PBS. Scale bars = 20 μm. Reprinted with permission from ref. 133. Copyright © 2012 American Chemical Society.

The use of a filamentous shape in PRINT hydrogel particles was shown to circumvent the problem of large particle stiffness for passing through pores with much smaller diameters than the particle size.134 When the hydrogel particle recovery was assessed by measuring the percentage of particles that could squeeze through a filter with 0.2 μm pores, it was found that the recovery of 80 nm particles with varied lengths was largely independent of the cross-linker concentration for lengths of up to 2 μm and was in the range of 93 to 77%.134 However, the lowest particle recovery of 29% was found for larger 80 × 5000 nm particles when the cross-linker concentration was greater than 50% which was attributed to decreased flexibility and deformability (Fig. 14).


image file: c6tb02746f-f14.tif
Fig. 14 SEM images of the PEG-based hydrogel particles 80 nm in diameter. Lengths of the particles are (A) 180 nm, (B) 320 nm, (C) 2000 nm, and (D) 5000 nm. Scale bar values are (A) 1 μm, (B) 3 μm, and (C and D) 5 μm. (E) Percent recovered fluorescence for 80 nm particles as a function of cross-linker concentration. The percentage values also refer to the percentage of particles recovered following filtration. Reproduced with permission from ref. 134. Copyright © 2012 American Chemical Society.

The mechanical flexibility necessary for a hydrogel particle to successfully navigate through size constrictions of blood vasculature under pressure differentials observed in healthy and diseased human capillaries can be regulated by varying only the shape of the hydrogel vehicle with the same nominal dimensions. For instance, squishy hydrogel disks, rings, crosses, and S-shapes of 8 μm in size and 2 μm in thickness obtained by polymerization of 700 Da PEGDA using the stop flow lithography technique demonstrated different deformabilities as a function of their microstructure.20 The threshold pressure differential for the hydrogels with a 10% cross-linker for passage of disks through 4 μm × 4 μm constrictions was 2.8 mmHg, while being only 0.05 mmHg for S-shapes. Ranking the four shapes by increasing flexibility gives disks, followed by rings, crosses, and then S-shapes as the most flexible. Interestingly, disk-, ring-, or cross-shaped hydrogel particles which were trapped within the constriction adopted a folded-over shape, while in the case of S-shapes, the two ends of the particle twisted in opposite directions resulting in only minimal bending.20

Unlike the discoidal PRINT or SFL hydrogel particles discussed above, a different deformation behavior was observed for discoidal PAH hydrogel capsules produced by LbL assembly and cross-linked with glutaraldehyde.135 Statistical analyses of the 6.7 μm hydrogel discoidal capsules squeezed through a glass capillary tip of 5 μm revealed that 90% of the discoidal capsules not only passed through the capillary constriction but also recovered their original discoidal shape. The remarkable fact is that the elasticity modulus of this discoidal capsule was in the order of hundreds of MPa, which is much larger than the passage threshold for the discoidal PRINT hydrogels, indicating that the hollow hydrogel structure can exhibit larger flexibility than that of a filled hydrogel of the same shape.18,20 This difference can be attributed to the fact that the hollow capsule interior, which resembles the RBC structure of a vesicle with fluid wrapped by a flexible cell membrane, facilitates better shape recovery by a more fluid-like deformation of the capsule membrane than an uninterrupted hydrogel of the PRINT and SFL hydrogel disks.18 The discoidal hydrogel capsule shape also allowed for better shape recovery when passing through pores with sizes smaller than those of the spherical hydrogel capsules which showed only 63% recovery ratio of the same (PAH)10 composition and size (6.7 μm).135

In another example,136 2 μm-sized multilayer cubical capsules made of hydrogen-bonded PVPON and tannic acid with a lower elasticity of 0.6 MPa were demonstrated to be able to extravasate through membrane pores of 0.8 μm under 18 psi of flow pump-controlled pressure. In contrast, filled PRINT hydrogels of a filamentous shape 80 nm in diameter with various lengths were able to cross 200 nm pores under 40 psi of manual pressure.31 Confocal microscopy analysis revealed that 80% of the cubical shells which penetrated the membrane fenestrations could maintain their initial cubical shape (Fig. 15).


image file: c6tb02746f-f15.tif
Fig. 15 (a) Rigid core–shells and soft shells are produced using LbL assembly of TA and PVPON on sacrificial inorganic manganese carbonate and silicon dioxide cores of cubic and spherical shapes, respectively. Confocal microscopy images of (b) cubical and (c) spherical hollow capsules obtained via dissolution of the cores. The scale bar is 5 μm. (d) Percentage of the particles able to traverse through the pores. The labels denote S = spherical, C = cubical, RM = rigid core–shell, EM = soft capsule. Reproduced with permission from ref. 136. Copyright © 2015 Wiley.

The cell-line dependent intracellular force exerted by cells on the particles upon their internalization can also serve as guidelines for the synthesis of mechano-responsive shaped hydrogel drug carriers for cell-specific drug delivery. For example, in a recent study, the Caruso group137 discovered that a different mechanical force could be generated by cells during internalization of soft PMAA hydrogel capsules of spherical and cylindrical shapes in a cell line-dependent way. This led to different deformations of capsules distributed within cell interiors. For both spherical and cylindrical hydrogel capsules, the highest capsule deformation occurred in HeLa cells (human epithelial cell line) when the capsules were highly deformed and lost their initial shape. In contrast, in differentiated human monocyte-derived macrophage cells, a large amount of capsules could maintain their distinguishable shape after cellular internalization.137

3.5.2. Magnetic field. The inclusion/incorporation of inorganic nanoparticles into the hydrogel network can lead to a hybrid system which may exhibit synergistic benefits unavailable to the individual hydrogel. The nanoparticles distributed in the network can improve the mechanical properties of hydrogel, and in return, the hydrogel can protect the environment from unfavorable effects of the nanoparticles.2 Non-spherical magnetic hydrogel particles also demonstrate great potential for biomedical applications like guided tumor-targeted delivery because of their magnetic sensitivity, biocompatibility and structural benefits such as porosity and large surface areas.138

In one example, magnetic hydrogel particles of spherical, dicoidal and plug-like shapes were synthesized by photopolymerization of an iron oxide-containing PEGDA solution in a microfluidic device.139 These non-spherical hydrogels assembled into long chains upon exposure to uniform external magnetic fields due to attractive interactions between the particles parallel to the field direction. Unlike the magnetic spherical hydrogels, the discoidal and plug-like particles exhibited a directional preference in the external magnetic field because of their shape anisotropy. The non-spherical hydrogels flipped up perpendicular to the plane of view and aligned along the field direction. This unique magnetic response and the ability of these anisotropic particles to form more complex patterns can be further exploited for field-induced pattern formation.

In another example, the inclusion of superparamagnetic iron oxide nanoparticles into electrosprayed cellulose-based RBC-shaped particles provided a magnetic-field response and a magnetic resonance imaging (MRI) signal contrast.140 Interestingly, the observed formation of a discoidal shape was believed to be due to the sheet-like molecular structure of the cellulose polymer. During the electrospraying process, the formed discoid was believed to become dented in its center due to electrostatic repulsions between the surface charge and the resistance between the nozzle and the collector.140 Due to the unique assembly possibilities and potential for imaging capability, magnetic field sensitivity enables shaped microparticles to be promising platforms for bio-imaging and in vivo drug delivery.

4. Effect of shape of non-spherical hydrogel particles on biological responses

Cell association with drug carriers is among the most crucial parameters for controlled drug delivery, and both the geometry and rigidity of delivery vehicles can regulate the cellular internalization efficiency in a cell type-dependent way.141 Remarkably, the upper size limit for cell internalization of hydrogel colloids by non-phagocytotic cells is much higher than that of rigid inorganic or polymeric nanoparticles which are excluded from cellular uptake at sizes greater than 150–200 nm, while softer and more flexible hydrogel particulates with sizes up to 3–5 μm can be internalized by cells.26,79,81,136,142

Apart from the conventional factors such as size, surface charge, and hydrogel rigidity that control cellular interactions of hydrogel particles, the shape of non-spherical hydrogel particles has undoubtedly been found to be critical for cell interactions including the rate and percentage of internalization. With regard to the hydrogel shape, the impact of the aspect ratio of the particle on cellular interactions has been studied on both filled, uninterrupted hydrogels made via PRINT technology142 as well as on hollow hydrogel particles, i.e., multilayer hydrogel capsules made via the LbL approach.79 In the former case, cylindrical PEG-based PRINT hydrogels with a high aspect ratio of 3 (length = 450 nm, width = 150 nm) were internalized by HeLa cells more rapidly and efficiently than those with an aspect ratio of 1 (length = width = 200 nm) (Fig. 16a). This difference in cellular uptake favoring the high-aspect ratio hydrogel cylinders was attributed to more cationic interactions with cells available with the higher-aspect-ratio particles due to the larger surface areas in contact with the cell. In contrast to those results, increasing the aspect ratio of hollow PMAA hydrogel capsules diminished the efficiency of the capsule internalization by HeLa cells (Fig. 16b). Increasing the aspect ratio in the case of cylindrical PMAA hydrogel capsules decreased their internalization by the cells from 91 to 82 and to 77% when the capsule aspect ratio increased from 1 to 3, and to 4, respectively, after 24 h of incubation.79 The differences in cell internalization between high-aspect-ratio filled and hollow hydrogel particles could also be related to their different rigidities as well as their net-surface charges. In other words, the negative surface charge of the high-aspect-ratio hydrogel capsules could play a negative role in the cell association/internalization process, and is worthy of continued studies in the future.


image file: c6tb02746f-f16.tif
Fig. 16 (a) Internalization of PRINT PEG-based hydrogels with HeLa cells over a 4 h incubation period at 37 °C. Legend depicts the particle diameter per particle volume. Reproduced with permission from ref. 142. Copyright 2008 National Academy of Sciences. (b) Internalization of PMAA hydrogel capsules in HeLa cells quantified by imaging flow cytometry. The degree of internalization is expressed as the internalization factor (IF). An overlay of the bright-field and fluorescence images of cells is shown in the insets for two areas: capsules bound with the cell membrane (negative IF) and capsules internalized within cells (positive IF). Reproduced with permission from ref. 79. Copyright 2012 American Chemical Society.

The same study by the Caruso group showed that the cylindrical hydrogel capsule shape is less prone to interaction with HeLa cells compared to the spherical shape.79 In this work, they found that spherical 1100 nm PMAA hydrogel capsules which had greater volume than the cylindrical capsules with an aspect ratio of 4 demonstrated almost 2-fold greater cellular association over 24 h of incubation. This finding agreed with the earlier observations by Crespy and colleagues143 that cellular internalization of high-aspect-ratio colloids required extended membrane wrapping time during the process. Despite the differences in the aspect ratio, both spherical and rod-like capsules accumulated within cellular lysosomes indicating that intracellular capsule distribution was independent of capsule shape.

The discoidal shape of the hydrogel capsules was also shown to decrease the capsule association with cells compared to their spherical counterparts.81 When spherical and discoidal (PMAA–PVPON)5 hydrogel capsules were incubated with J744.A1 macrophages, human microvascular endothelial cells (HMVEC), and 4T1 breast cancer cells, the hydrogel capsules showed a negligible uptake by the J774A.1 macrophages. Also, cell association with discoidal capsules was shown to be 60% lower than that of spherical capsules. The internalization of discoidal hydrogel capsules by 4T1 breast cancer cells was found to be 5-fold smaller than that of the spherical ones. This finding correlates with the studies on rigid polymeric particles,144 which explained the decreased cellular uptake of polymeric discs by stronger cell surface binding due to their shape as compared to spheres. Indeed, the PMAA–PVPON hydrogel capsules could be regarded as discoidal plates with a high aspect ratio of 5 at pH = 4 and of 3 at pH = 7.4.81

A recent computational study by Gompper and co-workers145 analyzed the effects of shape, aspect ratio, and orientation of rigid rod and cubical nanoparticles on cellular membrane bending and wrapping and predicted the extent and kinetics of the endocytosis based on particle geometry. The study revealed that to sufficiently determine particle uptake, local geometrical properties such as the local mean curvature along with particle size and aspect ratio are extremely important factors in predicting the membrane wrapping behavior. They found that both particle adhesion to the cell and wrapping of the cell membrane around it are controlled by the competition between the adhesion energy gain for particle-cell membrane contact and the energy cost for the lipid bilayer deformation. Therefore, membrane wrapping can be a crucial mode of entry for particle uptake (Fig. 17). For example, enhanced binding but lower uptake can occur for ellipsoidal particles when oriented parallel to the membrane compared with spherical ones. However, reorientation from the parallel to perpendicular state may suppress particle uptake because wrapping the highly curved tip of an ellipsoid will cost a high bending energy per area.145 Also, it was shown that for cubical particles, the adhesion strength for a cube should be 3-fold more than that of a sphere to compensate the membrane deformation energy at the upper edges of the cube.145 Because of a higher wrapping energy barrier for cubes compared to that for spheres, rigid spheres can be internalized faster than cubes.


image file: c6tb02746f-f17.tif
Fig. 17 Modes of entry for nanoparticle uptake by membrane wrapping: (I) submarine mode with the long axis of the particles oriented parallel to the membrane, (II) rocket mode with the long axis oriented perpendicular to the membrane, and (III) competition between the submarine and rocket modes as observed for rod-like particles with high aspect ratios. The completely wrapped particle is connected by an infinitely small neck to the membrane; the particle orientation in this state is irrelevant. Reprinted with permission from ref. 145. Copyright © 2014 American Chemical Society.

Indeed, the effect of the cubical hydrogel shape on the cell internalization was observed within the first 10 hours of the incubation of redox-sensitive PMAA multilayer hydrogel cubes and spheres with HeLa cells (Fig. 18).26 The DOX-loaded hydrogel spheres exhibited 12% higher cell cytotoxicity when incubated with HeLa cells for 10 hours as compared to that of hydrogel cubes, which indicated a more rapid internalization of spherical hydrogels, indicating an important role of the hydrogel particle shape in the membrane adhesion process in the initial steps of cell internalization. However, since both DOX-loaded (PMAA)5 spheres and cubes demonstrated similar cytotoxicity to HeLa cancer cells after longer incubation times of 24 and 48 hours, and given their similar DOX payload, long-term amounts of the hydrogel cubes or spheres internalized by HeLa cancer cells seemed to be similar.


image file: c6tb02746f-f18.tif
Fig. 18 Viability of HeLa cells (% of negative control) after (a) 3, 10 and 24 and (b) 48 hours of incubation with free DOX, and DOX-loaded (PMAACS)5 cubes and spheres. Particle-free supernatants from suspensions of the DOX-loaded cubes and spheres were used as a negative control with the same volume as that of DOX-loaded particle suspensions. Each data point represents an average of four replicates ± std dev (*p < 0.05). Reproduced with permission from ref. 26. Copyright © 2016 American Chemical Society.

Conversely, the cubical geometry of soft multilayer capsules was shown to promote the interaction of the particles with breast cancer cells.136 The cellular uptake of the cubical shells was demonstrated to be five-fold more efficient by human microvascular endothelial cells and six-fold and 2.5-fold more efficient by MDA-MB-231 and by SUM159 breast cancer cells, respectively, compared to the spherical capsules.136 This difference in the uptake efficiency was attributed to a softer structure of the cubical capsules.

Besides cellular internalization, the immunological cell responses have also been demonstrated to be modulated by particle shape. Although most studies on the effect of particle shape on immune responses have been conducted with solid inorganic particles, very recently soft PMAA hydrogel capsules have been demonstrated to induce shape-dependent cytokine secretion by human monocyte-derived macrophages (dTHP-1 cells).146 Unlike previously reported interactions with HeLa cancer cells, the thiolated (PMAA) hydrogel capsules with spherical, short rod- and long rod-shapes prepared by LbL assembly were internalized slightly differently by the dTHP-1 professional phagocytes showing slightly increased internalization levels of 90.6, 96, and 96.8% with increasing capsule aspect ratios.146 However, hydrogel capsules shaped like short rods promoted a stronger, 1.7-fold in TNF-α and 2.1-fold in IL-8, synthesis of pro-inflammatory cytokines by the macrophages compared to spherical and by 2.8- and 2.0-fold in TNF-α and IL-8 cytokines, respectively, compared to the long rod-shaped hydrogel capsules (Fig. 19).146 The exact mechanism for the observed effect of the hydrogel capsule shape on the release of these cytokines by the macrophage cells remains unclear, although this phenomenon could be utilized for the rational design of the hydrogel delivery vehicles.


image file: c6tb02746f-f19.tif
Fig. 19 Transmission electron microscopy images of thiolated PMAA hydrogel capsules with spherical (A1) short rod (A2) and long rod (A3) shapes. Scale bar is 1 μm. (B) TNF-α and (C) IL-8 secretion from dTHP-1 cells treated with PMAA hydrogel capsules at capsule-to-cell ratios of 0, 25, 50, and 100 for 24 h (red: spherical capsules; green: short rod-shaped capsules; black: long rod-shaped capsules). Reproduced with permission from ref. 146. Copyright © 2016 American Chemical Society.

5. Conclusion and outlook

This review summarizes a pool of experimental approaches for the design and synthesis of non-spherical hydrogel particles with well-defined shapes. Multiple scientific reports have indicated the great potential of environmentally responsive hydrogel biomaterials which utilize specific well-defined shapes. Biomedical applications including targeted drug delivery, selective cellular interactions, and controlled bio-distributions require reliable methods of particulate synthesis of well-defined shapes with imparted on-demand stimuli responsiveness. These particles additionally need to be able to navigate in biological fluids and interact with biological tissues in a controllable programmed way. These challenges are being faced with the development of new synthetic approaches and methods using various lithography techniques as well as expanding polymer assembly protocols. Strategies for the fabrication of non-spherical hydrogel particles are being developed to mimic the shape and flexibility of innate biological species in order to mimic and incorporate the architectural peculiarities essential to their biological functions. An emerging class of hydrogel particulates with a variety of shapes based on LbL assembly can be uniquely suitable for creating either hollow or filled porous particles of multilayer hydrogel-like networks with well-defined, precisely controlled size and shape. Considering the potentially regulated mechanical properties and interior structures of the resultant hydrogel particles, the multilayer assembly approach can be utilized for systematic investigation of fundamental relationships between the particle's architectural features and their effects on the non-spherical particle's behavior in flow and biological responses.

Despite some progress in studies of non-spherical hydrogel particulates, the area of research still has many uncharted territories. For example, there is still need for the development of new strategies to scale-up the production of stimuli-responsive hydrogels and to further investigate their interaction with various tissues and cells. Also, there are only a few reports attempting to study the effect of temperature on shape changes of temperature-sensitive hydrogel particles which is especially intriguing in the case of hollow temperature-responsive particulates. The development of and studies on shape changes of soft hydrogel particulates induced by magnetic fields and other biomedically and biologically relevant triggers should be of further interest for researchers in the field of nanotechnology and nanomedicine.

Acknowledgements

This work was supported by the NSF CAREER Award #1350370. We also thank Mr Aaron Alford for technical assistance.

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Footnote

Chemistry Department, University of Alabama at Birmingham, 901 14th St South, CHEM 279, Alabama, 35294, USA. E-mail: ekharlam@uab.edu

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