Lucia
Massi‡
a,
Adrian
Najer‡
a,
Robert
Chapman
b,
Christopher D.
Spicer§
a,
Valeria
Nele
a,
Junyi
Che
a,
Marsilea A.
Booth
a,
James J.
Doutch
c and
Molly M.
Stevens
*a
aDepartment of Materials, Department of Bioengineering, and Institute of Biomedical Engineering, Imperial College London, London SW7 2AZ, UK. E-mail: m.stevens@imperial.ac.uk
bCentre for Advanced Macromolecular Design (CAMD) and the Australian Centre for Nanomedicine (ACN), School of Chemistry, UNSW Sydney, Australia
cISIS Neutron and Muon Source, STFC, Rutherford Appleton Laboratory, Didcot OX11 ODE, UK
First published on 3rd September 2020
Many diseases are associated with the dysregulated activity of enzymes, such as matrix metalloproteinases (MMPs). This dysregulation can be leveraged in drug delivery to achieve disease- or site-specific cargo release. Self-assembled polymeric nanoparticles are versatile drug carrier materials due to the accessible diversity of polymer chemistry. However, efficient loading of sensitive cargo, such as proteins, and introducing functional enzyme-responsive behaviour remain challenging. Herein, peptide-crosslinked, temperature-sensitive nanogels for protein delivery were designed to respond to MMP-7, which is overexpressed in many pathologies including cancer and inflammatory diseases. The incorporation of N-cyclopropylacrylamide (NCPAM) into N-isopropylacrylamide (NIPAM)-based copolymers enabled us to tune the polymer lower critical solution temperature from 33 to 44 °C, allowing the encapsulation of protein cargo and nanogel-crosslinking at slightly elevated temperatures. This approach resulted in nanogels that were held together by MMP-sensitive peptides for enzyme-specific protein delivery. We employed a combination of cryogenic transmission electron microscopy (cryo-TEM), dynamic light scattering (DLS), small angle neutron scattering (SANS), and fluorescence correlation spectroscopy (FCS) to precisely decipher the morphology, self-assembly mechanism, enzyme-responsiveness, and model protein loading/release properties of our nanogel platform. Simple variation of the peptide linker sequence and combining multiple different crosslinkers will enable us to adjust our platform to target specific diseases in the future.
To yield high level of control of drug loading and triggered release, temperature and/or enzyme-responsive motifs can be incorporated in polymer-based drug delivery.9 With respect to temperature-triggered systems, poly(N-isopropylacrylamide) (PNIPAM) remains one of the most studied polymers incorporated in the design of temperature-responsive materials for biomedical applications due to its fast temperature-induced phase transition at a lower critical solution temperature (LCST) of ∼32 °C.10,11 Copolymers of PNIPAM with a temperature-independent hydrophilic block allow rapid assembly of nanostructures upon heating either after or during the polymerisation because of the thermally induced collapse of the PNIPAM block at temperatures above the LCST.12 However, PNIPAM-based nanoassemblies are limited to transition around 32 °C; the LCST cannot be changed easily. Copolymerisation of NIPAM with other co-monomers is one option to modulate the LCST.13,14 However, temperature is not an ideal trigger for cargo release given our fixed body temperature. Hence, modulation of the self-assembly temperatures (LCST) using a range of different copolymers, combined with a suitable stimuli-responsive cross-linking strategy, represents an interesting alternative platform that could be employed both above and below the LCST.
Our strategy uses temperature changes as a simple and fast organic solvent-free nanogel formation method to encapsulate biomolecules. Poly(N-cyclopropylacrylamide) (PNCPAM), closely related to PNIPAM, consists of pendant cyclopropylamine groups instead of the isopropylamine groups in PNIPAM and possesses a LCST of ∼49 °C.10 We propose herein that the copolymerisation of NCPAM and NIPAM to form block copolymers together with a hydrophilic block—consisting of a short block with functional reactive handles and polyethylene glycol (PEG)—provides an efficient method to precisely control the LCST, and hence the self-assembly temperature, from 32 up to 49 °C. Fine-tuning of the transition temperature using a library of copolymers, with precise control of the LCST around body temperature, enables application-dependent selection of a certain copolymer from the library to create customised vehicles for loading and release of sensitive therapeutic protein cargoes.
A cross-linking strategy was further included to (i) stabilise the nanocarrier, (ii) avoiding premature release of cargo, and (iii) incorporating stimuli-responsiveness. This additional cross-linking strategy serves as an additional trigger besides temperature for cargo release, through degradation of the responsive cross-links. These are important considerations when taking into account the immensely complex environment faced by nanocarriers upon in vivo administration. We employed a copper-catalysed azide–alkyne cycloaddition (CuAAC) cross-linking strategy, which remains one of the most popular “click” reactions for cross-linking and functionalisation in the biomaterial and biomedical fields due to high efficiency, specificity, and simplicity, to incorporate the necessary functional handles.15–17 Our covalent cross-linking strategy provided the fundamental advantage of keeping our nanogels intact above and below the LCST, which in turn allows fast and simple loading of cargo and subsequent purification.
With respect to cross-linker backbone chemistry, peptides are particularly attractive due to their simple solid phase synthesis, incorporation of non-canonical functional groups for the introduction of “clickable” handles,18,19 and the possibility of using enzyme-specific cleavable peptide sequences.19,20 Due to their intrinsic involvement in biological and metabolic processes, enzymes have emerged as suitable triggers for drug delivery.21 Different classes of enzymes (e.g. proteases, phospholipases, oxidoreductases) have been leveraged for the purpose of triggered drug release from nanocarriers.22 A specific class of proteolytic enzymes, matrix metalloproteinases (MMPs), are associated with several disease conditions, including infections, inflammation, cardiovascular diseases and cancer.23 Overexpression of MMPs at disease sites can be exploited to release drugs at the target site by selective rupture of engineered MMP-responsive delivery platforms.22,24
Herein, we successfully synthesised libraries of PNIPAM-, PNCPAM- and P(NIPAM-co-NCPAM)-based triblock copolymers with tuneable compositions via reversible addition–fragmentation chain-transfer (RAFT) polymerisation. The structure of the final block copolymers was carefully designed to include these temperature-responsive blocks, a functional block for nanogel cross-linking and a hydrophilic outer block. The thermo-responsive block is hydrophilic below its LCST and turns hydrophobic above the LCST, thus switching the block copolymer from hydrophilic to amphiphilic, which promotes the formation of self-assembled nanostructures. The choice over amphiphilicity or hydrophilicity of degradation products at body temperature, through selecting a copolymer with a transition temperature below or above 37 °C, offers means of potentially modulating elimination pathways upon in vivo administration in the future. Choosing a suitable NIPAM–NCPAM ratio in the thermo-responsive block will further allow one to adjust the LCST to only slightly below body temperature, which could be a means of speeding up cargo release at the disease site, when close to the surface, through locally applied cold patches. To increase nanoparticle stability and incorporate responsiveness to a model MMP enzyme (MMP-7), azido-bi-functionalised peptides were synthesised and used to cross-link the nanoparticles via the alkyne groups present in the functional middle block using CuAAC.
A considerable challenge when deciphering the exact morphology of copolymer assemblies is the structural ambiguity that is provided by certain routine characterisation techniques such as conventional dynamic light scattering (DLS) and negative stain transmission electron microscopy (TEM). However, accurate information on morphology is of great importance since it directly affects choice of suitable disease targets, drug cargo, delivery route, stability and release mechanism. Thus, the use of additional complementary characterisation techniques is needed to characterise the morphology of soft self-assembled nanostructures. TEM at cryogenic temperatures (cryo-TEM)25,26 and small-angle neutron scattering (SANS)27 are two complementary methods to study these types of nanostructures in their native hydrated state.28–30 A third technique, fluorescence correlation spectroscopy (FCS) is a diffusion-based single-molecule analysis technique.31,32 FCS allows accurate characterisation of nanoparticle assembly/disassembly—including in the presence of enzymatic triggers—surface functionalisation, cargo loading, and release.33–35 Our thoroughly characterised nanogel system is shown to serve as a versatile protein delivery platform with a simple and gentle temperature induced formation and loading protocol, and triggered release through stimuli-responsiveness provided by enzymatically cleavable cross-links. This modular platform can be adjusted for disease-specific applications by choosing the appropriate copolymer, peptide cross-linker sequence, and therapeutic protein cargo.
We used RAFT polymerisation for the synthesis of these polymers, due to the ease of preparing well-defined multi-block copolymers and PNIPAM via this route.11,36–40 The detailed synthetic procedure is shown in Scheme 2.
The first step consisted of the synthesis of the RAFT agent 1, following a procedure previously reported in the literature,41 which was then conjugated to a PEG block (113 units) via esterification to form a macroRAFT agent. Chain extension of this macroRAFT agent with a random copolymer of MAA and TMSPMA enabled the introduction of carboxylic groups and terminal alkyne functionalities (in their protected form) as functional handles. Good control over the polymerisation of PEG-b-P(MAA-co-TMSPMA) 3 was evidenced by low dispersity Đ = 1.07, and a clean shift in the gel permeation chromatography traces (GPC, Fig. S1a, ESI†). The same polymer (with 113 PEG units, 5 MAA units and 19 TMSPMA units) was used throughout the remainder of the study and chain extended to produce three different libraries of triblock copolymers: (i) a library of PNIPAM-based block copolymers (5a1–5a5) with increasing number of NIPAM units; (ii) a library of PNCPAM-based block copolymers (5b1–5b5) with increasing number of NCPAM units; (iii) a library of P(NIPAM-co-NCPAM)-based block copolymers (5c1–5c3) with different NIPAM/NCPAM (NI/NC) ratios. We hypothesised that the incorporation of cyclopropyl moieties (NCPAM) would lead to an increase in the LCST providing a Tcp (cloud point temperature as measured by DLS) for nanogel self-assembly/disassembly at temperatures just above body temperature.
Successful synthesis of the three block copolymer libraries was confirmed by 1H NMR and GPC yielding degree of polymerisation (DP), number average molecular weight (Mn), and dispersity (Đ) (Table 1). Full composition and characterisation details of selected 5a4/5c1–3 block copolymers are reported in Table 1, whilst data for the remaining block copolymers can be found in Table S6 of the ESI.†
# | NI/NC ratioa | DP (NMR) | M n (Da) (NMR) | M n (Da) (GPC) | Đ (Mw/Mn) (GPC) | D H (nm) (DLS) | T cp (°C) |
---|---|---|---|---|---|---|---|
a NI/NC ratio is NIPAM to NCPAM ratio; DP is degree of polymerisation calculated by 1H NMR; Mn is the number average molecular weight calculated by GPC and NMR; Mw/Mn represents the dispersity obtained by GPC; DH in nm represent the hydrodynamic diameters of the resulting self-assembled nanostructures (T above Tcp: 5a4 = 34 °C, 5c1 = 60 °C, 5c2 = 55 °C, 5c3 = 55 °C) reported by DLS (number/%) and Tcp is the cloud point temperature as measured by DLS. | |||||||
5a4 | NI1.0NC0.0 | 421 | 55![]() |
66![]() |
1.41 | 74 ± 7 | 33 |
5c1 | NI0.8NC0.2 | 421 | 55![]() |
61![]() |
1.31 | 80 ± 2 | 37 |
5c2 | NI0.5NC0.5 | 395 | 52![]() |
77![]() |
1.34 | 179 ± 20 | 44 |
5c3 | NI0.4NC0.6 | 357 | 48![]() |
58![]() |
1.29 | 295 ± 74 | — |
For the P(NIPAM-co-NCPAM)-based copolymers (5c1–3), full chain extension was observed for all the copolymers with a minimal amount of macro-RAFT agent left behind and minimal shouldering in the GPC traces (Fig. S1a, ESI†). Due to the structural similarity and similar degree of reactivity between NIPAM and NCPAM, the formation of a random block stemming from their simultaneous polymerisation rather than two distinct blocks was assumed. In general, the dispersity was Đ < 1.5. The length of the thermo-responsive block was successfully modulated in the separate NIPAM and NCPAM libraries (Table S6, ESI†), whilst the copolymers shown in Table 1 were of similar length, as shown by NMR and GPC. The evolution of Mn and Đ versus DP is shown in Fig. S1b (ESI†). We also determined the block copolymer cloud point temperatures Tcpvia temperature sweeps and monitoring by dynamic light scattering (DLS). The corresponding sizes of the self-assembled nanostructures resulting from heating the block copolymer solutions above the Tcp are included in Table 1 and Table S6 (ESI†). The small difference in the number mean size between 5a4 (69.0 ± 2.7 nm, n = 3, N = 3) and 5c1 (98.1 ± 9.6 nm, n = 3, N = 3) above the LCST is significant (*p = 0.043, Student's t-test, n = 3, N = 3) when comparing three independent samples.
The cyclopropyl-dependent size increase might be caused by the higher rigidity and lower rotational freedom of the cyclopropyl group when compared to the isopropyl group, which might affect the packing parameters to yield larger structures. The self-assembly temperature of the resulting triblock copolymers was successfully tuned from 33 °C, corresponding to the Tcp of the 5a4 copolymer with 0% NCPAM content, to a Tcp of about 47 °C for the 5c3 copolymer with 60% NCPAM content. It can be concluded that by increasing the number of cyclopropyl units in the copolymers, the self-assembly temperature increases proportionally. However, when the NCPAM content exceeds 50%, the stability of the resulting self-assembled structures is compromised. Formation of large particles/aggregates, which led to sedimentation was observed (Fig. 1b). The self-assembly process of PNIPAM- and P(NIPAM-co-NCPAM)-based copolymers can be reversed by cooling the solution below the transition temperature (down to 25 °C) causing complete nanogel dissolution yielding free polymer chains in solution (Fig. 1b and Fig. S1c, ESI†). The slight hysteretic behaviours in Fig. 1b could be explained by a slightly slower globule-to-coil transition compared to the coil-to-globule transition. According to this initial DLS analysis, the selected block copolymers (5a4/5c1–3) revealed an LCST-type, reversible thermo-responsive behaviour that yielded nanogels at temperatures above their LCST. We also tested all the other copolymers from the separate PNIPAM (5a1 to 5a5) and PNCPAM (5b1 to 5b5) series for the formation of nanogels at temperatures above the LCST (Table S6, ESI†). All copolymers except 5b1 assembled into nanogels, however, no clear trends regarding polymer lengths and corresponding nanostructure sizes could be found.
Cryo-TEM of self-assembled nanostructures made from copolymers 5a4 and 5c1 revealed a spherical morphology with homogenous contrast across whole particles (Fig. 2a and d). This indicates formation of dense, polymer-filled, non-vesicular spherical nanogels. The sizes of the nanogels (Fig. 2b and e) made from both copolymers were measured via image analysis and were in good agreement with the hydrodynamic diameters obtained by DLS. The increase in size of the self-assembled structures when NCPAM is present, as measured by DLS (Fig. 1c and d), was confirmed by cryo-TEM. We additionally studied the zeta potential of self-assembled nanostructures above the LCST (45 °C), which yielded slightly negative values (5a4 = −5.5 ± 0.2 mV; 5c1 = −16.0 ± 0.5 mV).
SANS enabled us to capture the morphology change from coil-to-globule (Fig. 2c and f), which is induced by the temperature-triggered transition in agreement with literature on other PEG-b-PNIPAM-based block copolymer systems.45–47 Neutron scattering data of the two selected block copolymers below and above the LCST (25 and 45 °C, respectively) are shown (Fig. 2c and f). Both copolymers, either without cyclopropyl units (5a4) or including cyclopropyl units (20%, 5c1) in the thermo-responsive block, revealed a drastic change in the scattering profiles at the two different temperatures. Below the LCST (at 25 °C), SANS confirmed that the block copolymers are present as chains in solution. Two shape-independent models, Guinier–Porod (5a4; Porod exponent of 1.77 ± 0.04; radius of gyration Rg of 4.6 ± 0.7 nm; dimension variable s is 0.86 ± 0.07) and power law (5c1; power law exponent of 1.96 ± 0.01) were used to fit the scattering profiles at 25 °C. Scattering data of copolymer 5a4 revealed a clear Guinier region, therefore we could fit the data with the Guinier–Porod model to obtain accurate Rg values. The data obtained for 5a4 suggests that this block copolymer has fully swollen chains in good solvent conditions at 25 °C (below the LCST) in agreement with literature on similar copolymers.46 A power law exponent of 1.96 ± 0.01 for block copolymer 5c1 is explained by the presence of polymer chains in theta conditions with equally favoured polymer–polymer and polymer–solvent interactions. This might also explain the bimodal distribution in the DLS data below the LCST (Fig. 1c), which was not observed in case of 5a4 (monomodal DLS) and is supported by the SANS data (see discussion above).
When heated above the LCST (45 °C), the copolymers are expected to transition from hydrated and flexible coils to collapsed globules.48–50 SANS data for copolymers 5a4 and 5c1 above the LCST were successfully fitted with a Sphere model. This indicates formation of dense spherical polymer nanogels rather than vesicles (polymersomes), which confirms the conclusions from the cryo-TEM images (Fig. 2a and d). The insertion of 20% cyclopropyl repeating units (5c1) did not affect the final morphology and the scattering data could again be fitted with the simple Sphere model. The best-fit diameters were 47.6 ± 1.0 nm (5a4) and 78.0 ± 0.5 nm (5c1), respectively. Data for size obtained by SANS, cryo-TEM and DLS are similar and the formation of larger structures for the NCPAM-containing copolymer 5c1 compared to 5a4 was consistent across all the measurements. SANS typically shows the smallest diameter of all the three methods, because it does not account for the hydration shell in the measurement.
None of our synthesised block copolymers self-assembled into vesicular morphologies, which would have been observed as membranous structures in the cryo-TEM micrographs and distinct SANS curves that could be fitted with a Hollow sphere model as shown previously.28 This is in disagreement with previous studies on similar PEG-b-PAA-b-PNIPAM block copolymer assemblies,40,51 which highlights the challenge of using theoretical rules to predict the final structure and encourages the use of various complementary techniques to precisely evaluate morphology. A combination of techniques such as DLS, cryo-TEM and scattering techniques like SANS, small-angle X-ray scattering (SAXS) and combining dynamic and static light scattering (DLS/SLS) is necessary to obtain a clear picture of the size and morphology of self-assembled nanostructures, which allows identification of the type of nanostructure formed.
Three of the block copolymers (5a4/5c1/5c2) were used for the development of peptide cross-linked nanogels because these copolymers formed stable structures upon heating above their LCST (Fig. 1b and c). The peptide cross-linker was prepared by solid phase peptide synthesis inserting an azido-lysine residue at both the C- and N-termini according to literature procedures.18 An MMP-7-cleavable sequence (K(N3)PLELRAK(N3), see Fig. S2a for the structure, ESI†) was installed into the peptide backbone enabling enzyme-triggered nanogel degradation. LC-MS spectra of the functionalised MMP-7-cleavable peptide after purification is shown in Fig. S2b (ESI†). In order to prepare the cross-linked nanogels, we developed a two-step protocol. First, the formation of self-assembled nanogels was induced by heating the block copolymer solution to 45 °C (above the LCST). A solution of the cross-linker was then added, together with small amounts of CuSO4·5H2O and (+)-sodium-L-ascorbate, leading to covalent crosslinking; the mixture was subsequently purified by size exclusion chromatography. Between the different samples we expect similar cross-linking due to the availability of the same number of alkynes per chain for all the copolymers and use of same equivalents of all the reagents for cross-linking. Upon cooling below the LCST, our nanogels therefore retained their structure, despite the solubilisation of the polymer chains. Details of the cross-linking strategy are schematically shown in Fig. 3a.
![]() | ||
Fig. 3 Nanogel cross-linking via enzyme-responsive peptides using azide-bi-functionalised peptides via CuAAC. (a) Schematic representation of the cross-linking strategy showing how cross-linking enhances nanogel stability below the LCST. (b) DLS traces comparing size distribution of 5a4-based self-assembled (before cross-linking from Fig. 1c) and cross-linked nanogels below (dashed line) and above (solid line) the LCST (33 °C for 5a4). (c) DLS traces comparing size distribution of 5a4- and 5c1-based cross-linked nanogels at 25 °C (below the LCST). (d) Study of long-term stability of cross-linked 5a4- and 5c1-based nanogels in PBS incubated at 37 °C and measured by DLS at 25 °C (open symbols) and 37 °C (closed symbols) at each timepoint (N = 1, n = 3). |
After the cross-linking reaction, the resulting polymer nanogels were analysed by DLS, both above and below the LCST, which is shown in Fig. 3b and c. A small difference in the hydrodynamic diameter was observed between the cross-linked (93 ± 2 nm) and self-assembled 5a4 nanogels (74 ± 7 nm, before cross-linking) above the LCST. In contrast, DLS measurements at 25 °C (below the LCST) revealed successful cross-linking had taken place. The non-cross-linked polymer nanogels were disassembled when the temperature was lowered below the LCST, as described above (Fig. 1b and c), but nanogels remained stable when cross-linked. When comparing the DLS traces of the cross-linked 5a4 nanogels at 37 °C and 25 °C, a size increase can be observed (93 ± 2 nm compared to 133 ± 9 nm). The slight size increase with decreasing temperature can be attributed to the thermo-responsive phase transition of the PNIPAM block, which switches from hydrophobic nature above the LCST to hydrophilic below the LCST. This could cause relaxation and water-induced swelling of the polymer chains, as previously observed in the literature.40,52 These networks are expected to swell and relax up to a limit determined by constraints imposed by the crosslinking, which will be dependent on the length and chemical structure of the peptide, and the cross-linking density.
The developed cross-linking protocol was then applied to the preparation of cross-linked polymer nanogels composed of the other P(NIPAM-co-NCPAM)-based block copolymers. Fig. 3c shows DLS characterisation of 5c1 (NI0.8NC0.2)-based nanogels after cross-linking. 5c1-based nanogels could be cross-linked successfully, yielding larger sizes compared to 5a4-based nanogels when measured below the LCST (181 ± 4 nm vs. 133 ± 9 nm). Cross-linking of 5c2-based nanogels could not be achieved due to severe aggregation and precipitation. Hence, detailed morphological analysis was restricted to the two copolymers that could also be cross-linked successfully (5a4 and 5c1). Long-term stability of cross-linked nanogels made from these two block copolymers when incubated in PBS at 37 °C was demonstrated by DLS (Fig. 3d). The hydrodynamic diameters did not decrease when observed over 9 days, both below and above the LCST, which demonstrates integrity of the structure and the absence of nanogel disassembly.
Besides obtaining morphological information at fixed temperatures above and below the LCST, as also demonstrated previously with similar PNIPAM-based block copolymers,46,47 SANS was applied herein to dynamically monitor the transition using one selected copolymer. During SANS measurements, 5c1 block copolymers and the corresponding cross-linked nanogels were subjected to a temperature ramp from 25 to 45 °C and from 32 to 42 °C, respectively (Fig. 4 and Tables S7, S8, ESI†).
SANS data of 5c1 block copolymers at temperatures between 25 and 34 °C (Fig. 4a and b) were fitted with the power law model (power law exponent of ∼1.9 obtained for all), which suggests the presence of Gaussian polymer chains in theta solvent conditions and the absence of self-assembly. Upon heating to 35 °C, the scattering data was better fitted using the Unified power Rg model. The obtained power law exponent of 2.40 ± 0.03 indicates a transition from Gaussian chains to a more entangled polymer network (Rg of 52.0 ± 0.6 nm) indicating the start of the coil-to-globule transition. At higher temperatures (36 and 45 °C) data were fitted using a triaxial ellipsoid model, which suggests the formation of non-perfect spherical nanogels, with an observable trend of ellipse transitioning to more sphere shape with increasing temperature (Table S7, ESI†). From these experiments a Tcp of 35–36 °C was obtained, which was similar to the value found by DLS (37 °C). Multiplying the scattering intensity by Q2 allowed us to obtain the Kratky plot with linear x- and y-axes (Fig. 4b and d). This plot is useful for studying nanogel degree of globularity, flexibility and compactness.29,55 The peak appearing in the Kratky plot at higher temperatures suggests the formation of globular particles above 35 °C. As the temperature further increases, the peak becomes more defined suggesting an increase in globularity.
The effect of cross-linking can be seen in the temperature-dependent SANS data of peptide cross-linked 5c1 nanogels (Fig. 4c, d and Table S8, ESI†) when compared to the purely self-assembled nanogels (Fig. 2f, 4a, b and Table S7, ESI†). We measured a narrower temperature range around the LCST, because we already knew the transition temperature from the non-cross-linked nanogels (Fig. 4a and b). The power law exponent value below 2 for the non-cross-linked copolymer compared to a value of ∼2.4 for the cross-linked nanogels, reveals the difference of the two populations at lower temperatures. As expected, by cross-linking the polymer chains a stable polymer network was formed, and the chains remained interconnected between each other also at temperatures below the LCST. When comparing the two Kratky plots (Fig. 4b and d) it can be concluded that the self-assembled and cross-linked nanogels both transition from coil to globule at 36 °C, whilst the cross-linked particles were slightly smaller after the transition as seen by the shift of the peak to the higher Q region. This trend is also confirmed by cryo-TEM (Fig. 2d and Fig. S3, ESI†). An explanation for this smaller size could be that the peptide cross-linkers restrict chain flexibility, keeping the polymer chains tightly connected.56
From the evolution of scattering intensity in Fig. 5a it is apparent that degradation has already occurred to some extent after 1 h incubation with MMP-7. The number mean size of the nanogels has already decreased (measured below the LCST), which suggests the presence of differently sized fragments and partial degradation. Within the next few hours of incubation with enzyme, a mixture of differently sized particles/fragments/polymers (large errors) was detected. After 24 h incubation, a clear size difference between the control and enzyme incubated sample became apparent (Fig. 5b) and the small error indicates that an endpoint has been reached. Indeed after 24 h incubation, the fragment size (27 ± 9 nm) is much closer to that of the corresponding free block copolymer chains (10 ± 2 nm).
Following DLS analysis, we also monitored nanogel degradation by a single-molecule detection method called fluorescence correlation spectroscopy (FCS). We previously used FCS for a detailed study of MMP-responsive degradation using another peptide-based nanostructure for diagnostic applications.35 Herein, FCS was employed to first observe nanogel degradation and subsequently to quantitatively analyse model biomolecule loading and release. In order to study MMP-7 triggered degradation of nanogels by FCS, cross-linked nanogels were labelled with Cy5-azide and incubated with excess MMP-7 (9 μM). Successful labelling of nanogels with Cy5-azide can be seen when calculating the hydrodynamic diameters from the FCS autocorrelation analysis (Fig. 5c) that yielded nanogel size rather than free dye (Fig. 5d). Further, non-crosslinked Cy5-azide labelled copolymers in non-assembled form revealed an intermediate diffusion time between free dye and nanogels (Fig. S6, ESI†). FCS curves of control experiments to check for non-specific interactions of dyes with nanogels/copolymers yielded diffusion times similar to free dye (Fig. S6, ESI†), which confirms successful specific labelling in the case of Cy5-azide (Fig. 5c and d).
After MMP-7 incubation, the corresponding autocorrelation curves shifted to faster diffusion times indicating cleavage of the peptide bonds (Fig. 5c). In the presence of MMP-7, a two-component fit of the autocorrelation curves revealed complete disappearance of any structures with original nanogel sizes. We only detected the presence of free Cy5-polymer chains (54% of total diffusing species) and some bigger, possibly entangled degradation products (DH value of 35 ± 6 nm, 46%, shown in Fig. 5d), demonstrating MMP-7-dependent peptide cleavage and complete nanogel disassembly below the LCST. By comparing the nanogel signal intensity (counts per particle, CPP in kHz) to the dye intensity, the number of dye molecules per single nanogel could be determined. Upon enzyme-mediated nanogel degradation, the calculated number of dyes per particle changed from about 54 dyes per particle before degradation, to about 2 dyes per particle for the degradation products. This is a further indication of nanogel disassembly. Together with the DLS analysis (Fig. 5a and b), enzyme-responsiveness of our nanogel system was successfully demonstrated.
![]() | ||
Fig. 6 Study of model protein (OG-BSA) loading and MMP-7-triggered release by FCS. (a) Normalised autocorrelation curves (coloured lines) and corresponding fits (black lines) from FCS data of three nanogel batches (A–C). (b) Hydrodynamic diameter of the three different batches of OG-BSA loaded nanogels with controls (free OG and free OG-BSA) as calculated from FCS data. (c) Number of OG-BSA per nanogel for the three nanogel batches as calculated from FCS data. (d) Cumulative release (%) of OG-BSA over time. This graph shows the release from loaded nanogels A, B and C upon incubation with increasing concentration of MMP-7 (0.9 nM, 9 nM and 90 nM) as compared with diffusion-mediated release (no MMP-7). These results are calculated from the FCS autocorrelation curves displayed in Fig. S7 (ESI†). Error bars are SEM (N = 3, n = 30). |
Successful loading of OG-BSA into peptide cross-linked 5a4 nanogels was observed by FCS. Free dye, OG-BSA and OG-BSA incorporated in nanogels can already be distinguished clearly in the fitted autocorrelation curves (Fig. 6a). When calculating the corresponding diffusion times (τD) and hydrodynamic diameters (DH) the size difference between the diffusing species was obtained (Fig. 6b). In the case of the nanogel measurements, the diffusing species correspond to the nanogel hydrodynamic diameter obtained in other measurements (Fig. 3c and 5c, d), which indicates successful incorporation of OG-BSA. Comparing the signal intensity per nanogel (counts per particle, CPP in kHz) with that of free OG-BSA, the number of loaded OG-BSA per single nanogel was determined and shows that multiple protein cargos were loaded per nanogel (Fig. 6c). Release studies were performed in triplicate by incubating OG-BSA loaded nanogels (batches A–C) with various MMP-7 concentrations in a physiologically relevant nanomolar range.58,59 FCS curves recorded at different time points in the presence or absence of MMP-7 revealed the release kinetics (Fig. 6d and Fig. S7, ESI†). This allowed us to compare diffusion-driven release (non-specific release from the nanogels over time) to MMP-7 triggered release.
FCS curves at the different time points were fitted using a two-component fit to account for both diffusing species (loaded nanogels and released OG-BSA). Further, a correction was included to account for the disproportional effect of bright slow diffusing species (loaded nanogels) compared to the less bright free OG-BSA.60 We propose herein (see Materials and methods in ESI†) to simply combine the fraction of free OG-BSA (directly from the two-component fit) with the decrease in the number of cargo for the remaining nanogels (via CPP), which is a second indicator for OG-BSA release (number of proteins per nanogel is decreasing). This correction is necessary because nanogels with several loaded proteins overlap with the free protein signal, as demonstrated in the literature for mixtures of differently sized nanoparticles of varying brightness.60 This finally yielded the percentage of free OG-BSA and allowed us to further calculate the cumulative release profile over time (Fig. 6d). A clear difference between 90 nM MMP-7-triggered release and diffusion-based profiles was detected, whilst the release profile in the presence of 9 and 0.9 nM MMP-7 gave intermediate results as expected for an enzyme-triggered release. Diffusion-based release (no MMP-7) reached 87 ± 4% after 39 h (N = 3, n = 30). This successful enzyme-triggered release profile justifies the further study of these copolymer libraries using therapeutic cargo and studying release behaviour at various temperatures, accompanied by corresponding delivery data at the cell and tissue level but this is beyond the scope of this paper. It is also clear that MMP-7 triggered release profiles will vary significantly in vivo compared to the in vitro data, due to a much higher level of environmental complexity that will cause differences in cross-linker degradation and hence release. Reasons for these differences include the presence of other substrates and specific cofactors, as well as continuous turn-over of enzymes. Release studies in more complex environments, including in the presence of cells and tissue, are needed in the future to choose an optimal copolymer system for the delivery of a specific drug for a chosen disease that involves upregulation of MMP enzymes at the disease site. Cytocompatibility of new materials is one critical aspect for moving towards biomedical applications. We have tested cytotoxicity of cross-linked nanogels (5a4) in a macrophage cell line (RAW 264.7 cells) (Fig. S8, ESI†), where we found no cytotoxic effects.
Due to the involvement of MMPs, such as MMP-7, in several disease conditions, including infections, inflammatory diseases, cardiovascular disease and cancer, our MMP-7-responsive platform could be used for local MMP-7 dependent drug delivery. Additionally, the tuneable temperature-range for nanogel disassembly would allow the formulation of nanogels with purely hydrophilic nature at body temperature (LCST above 37 °C), potentially enabling rapid clearance from the body after disassembly. Alternatively, nanogels with LCST just slightly below body temperature could be used to achieve MMP7-responsive release that could be accelerated by applying e.g. cold patches locally. Simply changing the peptide cross-linker sequence will further allow application of our nanogel platform using other enzymes as triggers, as relevant in specific diseases.
Experiments at the ISIS Neutron and Muon Source were supported by beamtime allocations from the Science and Technology Facilities Council (RB1810203). This work benefited from the use of the SasView application, originally developed under NSF award DMR-0520547. SasView contains code developed with funding from the European Union's Horizon 2020 research and innovation programme under the SINE2020 project, grant agreement 654000. The authors acknowledge the use of microscopy facilities within the Harvey Flower Electron Microscopy Suite at Imperial College London. The Light Microscopy Facilities at the Francis Crick Institute London is acknowledged for providing access to the FCS machine. The authors wish to acknowledge Dr Ulrike Kauscher Pinto and Dr Margaret N. Holme for assistance with cryo-TEM, and Dr Michael R. Thomas and Dr Hanna M. G. Barriga for assistance with SANS experiments.
Raw data are available upon reasonable request from E-mail: rdm-enquiries@imperial.ac.uk.
Footnotes |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/d0tb01546f |
‡ Contributed equally. |
§ Current address: Department of Chemistry and York Biomedical Research Institute, University of York, Heslington, YO10 5DD, UK. |
This journal is © The Royal Society of Chemistry 2020 |