Dylan Luke
Atkins
*abc,
José Augusto
Berrocal
cd,
Alexander Francesco
Mason
ce and
Ilja Karina
Voets
*ac
aLaboratory of Self-Organizing Soft Matter, Department of Chemical Engineering and Chemistry, Eindhoven University of Technology, 5600 MB Eindhoven, The Netherlands. E-mail: d.atkins@tue.nl; i.voets@tue.nl
bLaboratory of Physical Chemistry, Department of Chemical Engineering and Chemistry, Eindhoven University of Technology, 5600 MB Eindhoven, The Netherlands
cInstitute for Complex Molecular Systems, Department of Chemical Engineering and Chemistry, Eindhoven University of Technology, 5600 MB Eindhoven, The Netherlands
dLaboratory of Macromolecular and Organic Chemistry, Department of Chemical Engineering and Chemistry, Eindhoven University of Technology, 5600 MB Eindhoven, The Netherlands
eLaboratory of Bio-Organic Chemistry, Department of Chemical Engineering and Chemistry, Eindhoven University of Technology, 5600 MB Eindhoven, The Netherlands
First published on 11th October 2019
Enzymes are widely employed to reduce the environmental impact of chemical industries as biocatalysts improve productivity and offer high selectively under mild reaction conditions in a diverse range of chemical transformations. The poor stability of biomacromolecules under reaction conditions is often a critical bottleneck to their application. Protein engineering or immobilization onto solid substrates may remedy this limitation but, unfortunately, this is often at the expense of catalytic potency or substrate specificity. In this work, we show that the combinatorial approach of chemical modification and supramolecular nanoencapsulation can endow mechanistically diverse enzymes with apparent extremophilic behavior. A protein–polymer surfactant core–shell architecture facilitates construction of increasingly complex biofluids from individual biosynthetic components, each of which retain biological activity at hydration levels almost two orders of magnitude below solvation. The herein constructed multifunctional biofluids operate in tandem up to 150 °C and in the total absence of solvent under apparent diffusional mass-transport limitation. The biosynthetic promotion of extremophilic traits for enzymes with diverse catalytic motions and chemical functions highlights the extraordinary capacity for a viscous surfactant milieu to replace both hydration and bulk waters.
Extremozymes (enzymes derived from extremophiles) showcase an evolutionary honed tolerance to conditions which are considered hostile to life.6,7 Consequently, extremozymes have been touted as ideal candidates for use as industrial biocatalysts.8,9 This motivated considerable interest in extremophile discovery, especially for the isolation and characterization of extremophilic enzyme variants for potential industrial application.10,11 Further, cultivation methodologies for the large-scale expression of extremozymes have been developed.9,11 To date however, these are still less developed than conventional expression systems, and typically require conditions which mimic the natural environment of the extremophile. An alternative approach aims to understand in detail the specific structure–function adaptations of extremozymes to rationally re-design selected enzymes to enhance their tolerance to harsh environments.12–14 The use of homology modelling between TLP-ste and thermolysin to engineer an enzyme resistant to boiling14 is a prominent example showcasing the translational success of this route, which has also served to advance our understanding of the stabilizing mechanisms of extremozymes. Disadvantageously however, this strategy is protein-specific, suffers significant lag-time and consequently is expensive.
Protein–polymer surfactant biohybrids in the form of self-contained solvent-free biofluids have been evidenced to greatly enhance the stability and activity of mesophile-derived biocatalysts.15,16 Pioneering work by Perriman et al. (2010) revealed that solvent-free myoglobin biohybrids exhibited activity at extremely low hydration levels up to unusually high temperatures.16 Elastic incoherent neutron scattering experiments evidenced that this is because a polymer surfactant corona can act as a substitute for hydration waters, mediating motions which closely resemble those observed in the hydrated state.17 Similarly, substrate solubility, mass transport and catalytic activity were reported for solvent-free biofluids in a broad temperature range from the onset of melting at approximately Tm ∼ 30 °C up to 150 °C.18
Herein we report on the construction of a quasi-ternary biofluid, composed of three mechanistically diverse and mesophile-derived enzymes, which displays tandem catalytic behavior under solvent-free conditions (Fig. 1). We created the mixed self-contained biofluids from horseradish peroxidase (HRP), glucose oxidase (GOx), and Thermomyces lanuginosus lipase (TLL), each of which independently retained biological activity at hydration levels roughly two orders of magnitude below protein solvation. Significantly, the protein–polymer surfactant core–shell architecture promotes biohybrid miscibility and extremophilic behavior enabling the cascade to operate at temperatures far above room temperature. Surprisingly, we find an apparent thermal activation temperature of 80 °C and achieve tandem catalysis up to 150 °C under seemingly diffusional mass transport limitations within the viscous biofluid. The retention of biological activity for enzymes with distinctly different catalytic motions and chemical functions highlights the extraordinary capacity for a viscous surfactant milieu to replace both hydration and bulk waters.
Thermogravimetric analysis (TGA) revealed half-decomposition temperatures ranging from 385 °C to 395 °C for the biohybrids. Further, mass losses upon thermal annealing at 110 °C for 60 min corresponded to 2–10 specifically bound waters per nanoconjugate (Fig. S4† and Table 1). For comparison, we computed the number of waters required for complete coverage of the solvent accessible surface area using the HyPred20 online tool, and associated PDB files (1hch, 1cf3, and 1ein21–23 (ESI† and Table 1). Our estimated water contents by TGA are at least two orders of magnitude less than those computed using HyPred (1400 for HRP, 5200 for the GOx dimer, and 1200 for TLL), thus confirming the preparation of solvent-free biohybrids. In the context of enzyme activity, these values correspond to extremely small hydration levels (h < 0.002), which are also roughly two orders of magnitude less than the apparent hydration limit for activity of h ∼ 0.2. Differential scanning calorimetry (DSC) showed reversible endothermic melting transitions at 24 °C, 29 °C and 22 °C for cHRP-S1, cGOx-S1, and cTLL-S1 respectively (Fig. S5† and Table 1). Taken together, TGA and DSC analysis confirmed the preparation of solvent-free biohybrids with liquid-like behaviors which persisted in the absence of hydration. These characteristics are highly consistent with previous reports in the literature.16,18,19
Species | n bw | h | n theo | T m/°C |
---|---|---|---|---|
Neat S1 | 3.2 | — | — | 10 |
cHRP-S1 | 9.4 | 0.0019 | 1398 | 24 |
cGOx-S1 | 6.2 | 0.0015 | 5183 | 29 |
cTLL-S1 | 2.2 | 0.0007 | 1194 | 22 |
Given the successful preparation of solvent-free melts, circular dichroism (CD) spectroscopy was performed in solution on re-suspended hybrids to elucidate the impact of supercharging and subsequent electrostatic coupling of a polymer surfactant on the respective protein secondary structures (Fig. 2a–c). Due to high absorbance of the nonylphenyl moiety in S1, complementary CD experiments were performed using biohybrids prepared with a carboxylated24 Brij-L23 (S6) surfactant (ESI†). Despite the increased surface charge due to extensive covalent modification of the solvent accessible acidic sidechains, we observed near-native folding of each protein, corresponding to approximately 93.7% (cHRP), 94.4% (cGOx), and 100% (cTLL) retained secondary structures (Table 2). These were reduced to 84.0%, 83.7%, and 77.0% upon polymer surfactant conjugation for cHRP-S6, cGOx-S6, and cTLL-S6, respectively. Since S1 and S6 are structurally similar, we expect similarly modest misfolding for the S1-containing hybrids.
Variant | Secondary structure retained/% |
---|---|
cHRP | 93.7 |
cHRP-S6 | 84.0 |
cGOx | 94.4 |
cGOx-S6 | 83.7 |
cTLL | 100 |
cTLL-S6 | 77.0 |
We performed small-angle X-ray scattering (SAXS) experiments in the solution-state to characterize morphological changes of the globular protein structure, and to validate the encapsulation of the proteins to produce biosynthetic nanoconjugates (Fig. 2d–f). The SAXS profiles of native HRP and cHRP were fitted with an ellipsoid form factor25 of comparable dimensions (HRP: rmin = 18.2 Å, rmax = 32.9 Å; cHRP: rmin = 18.6 Å, rmax = 33.1 Å), which were roughly consistent with the crystallographic dimensions determined from the associated PDB file 1hch. The slightly larger radii used to fit the cHRP SAXS curves (Table S1†) are in line with the small loss of native globular fold observed by CD. Significantly, the construction of nanoencapsulated biosynthetic enzymes was confirmed for cHRP-S1 by fitting the SAXS profile with fixed cHRP protein dimensions while accounting for a thin polymeric corona using a core–shell ellipsoid26,27 form factor. This revealed a compressed polymeric corona of approximately 3.1 nm primarily located along the minor axis of cHRP, with a very minimal contribution (∼0.5 nm) at the ellipsoidal extremities (Table S2†). For comparison we show a scattering profile using a homogenous shell thickness (3.1 nm) encapsulating cHRP which resulted in a significantly poorer fit (Fig. S10†).
The compacted and patchy coverage of a supercharged enzyme in aqueous solution is in line with previous reports on polymer-tethered lysozyme and myoglobin studied by a combination of small-angle neutron scattering and molecular dynamics simulations.28 We further confirmed its correspondence with the cationized protein's surface charge distribution by performing continuum electrostatics calculations via the PDB2PQR web server29,30 to map the electrostatic potential of the supercharged protein surface (Fig. S3†). Convincingly, this revealed considerably high positive charge densities on the cHRP minor axis, with a relatively neutral charge remaining at the major axis extremities.
Scattering profiles were also computed using Crysol31 and respective crystal structures for GOx (symmetrical dimer) and TLL. These results first confirmed that the associated homodimeric state of GOx was largely lost upon modification of solvent accessible acidic residues. This is evidenced by the loss of subtle undulations associated with the quaternary structure of dimeric assembly at values of q > 0.1 Å. Further, the globular state of TLL is distinctly well-preserved upon covalent modification to produce cTLL, as demonstrated by the excellent correspondence between the respective scattering profiles. Finally, the subsequent charge-driven self-assembly of supercharged protein and polymer surfactant is signalled by distinct transformations in scattering profiles of cGOx-S1 and cTLL-S1 compared to their respective supercharged variants. Convincingly, these transformations closely match that of cHRP-S1, and are qualitatively similar to previously published scattering profiles of core–shell biohybrid enzymes.32 Given these insights, we reasonably conclude the successful construction of core–shell structured biosynthetic enzymes.
We were now confident that the amphiphilic environment afforded by the surfactant should effectively mediate small molecule transport. Aiming to interrogate the chemical and thermal limits of enzymatic catalysis in solvent-free liquids, and to supply H2O2 in a well-controlled manner, we devised a 2-step catalytic pathway producing H2O2in situ via the cGOx-S1 catalyzed conversion of glucose into glucono-1,5-lactone and H2O2. We anticipated that this would be followed by the cHRP-S1 catalyzed and H2O2 mediated conversion of ODP into DAP given that H2O2 diffusion appeared to be possible despite a bulk surfactant milieu.35,36 Preliminary microscopy experiments confirmed efficient solubilization of glucose at the solid–liquid interface, and independent liquid–liquid miscibility of the substrate OPD above 100 °C (Fig. S7 and S8†).
A series of high temperature assays from 40–140 °C were subsequently performed for cGOx-S1/cHRP-S1 by first annealing neat desiccated OPD with the two-component biofluid, followed by the addition of solid glucose substrate (Fig. 4a and b). We found no appreciable DAP production below 80 °C (Fig. S12†) despite temperatures far exceeding the melting point of the mixed fluid (Fig. S6†). By contrast, DAP was efficiently produced above 80 °C. An impressive initial rate of 3.46 ± 1.81 μM s−1 was measured at 80 °C, which was followed by an apparent exponential enhancement in enzymatic turnover with respect to temperature (Table 3). For example, at 140 °C we found an almost 22-fold enhancement in turnover up to 74.50 ± 1.58 μM s−1. The enhanced solvent-free turnovers clearly demonstrate that glucose can access the deep internalized binding pocket of cGOx-S1 despite the absence of solvent (Fig. 3b). The unhindered access of the deep pocket is striking considering the hybrid undergoes structural reordering upon polymer conjugation. This reordering does not appear to have greatly perturbed the deep pocket opening or collapsed the internal cavity. Further, glucose binding necessitates a degree of flexibility of the oxygen activation site (His516) in order to accommodate hydrogen bonding with neighboring residues within the rigid, tight cavity.22,37 Catalysis confirms a polymer surfactant corona effectively replaced hydration water in order to mediate the small-scale motion required for residue-specific flexibility. However, we cannot rule out that the 6 waters per cGOx-S1 nanoconjugate observed by TGA are located at the entrance, or within the deep pocket itself. Residual waters may assist in small molecule transport or aid in stabilization of the deep pocket.
T/°C | |||||||
---|---|---|---|---|---|---|---|
80 | 90 | 100 | 110 | 120 | 130 | 140 | |
DAP production/μM s−1 | 3.46 | 5.30 | 10.04 | 18.03 | 28.41 | 41.09 | 74.50 |
St. Dev./μM s−1 | 1.81 | 1.37 | 1.52 | 1.31 | 1.29 | 1.88 | 1.58 |
The rapid conversion of glucose in the solvent-free cGOx-S1/cHRPS1 biofluid confirms reactant solubilization, conversion, mass transport, and active site access despite the absence of hydration waters and bulk solvent at h < 0.002. Furthermore, the observed catalytic behavior of biosynthetic enzymes was strongly temperature-dependent above 80 °C. However, protection of the glucose substrate via acetylation36 (AcGl, ESI†) resulted in total loss of enzymatic recognition of the substrate at 110 °C (Fig. 4d). Control over substrate turnover and specificity further suggest a remarkably well-preserved active-site environment, with small-scale catalytic motions which should closely resemble aqueous GOx. Finally, we were able to reinitiate the cascade by introduction of a third biosynthetic enzyme component to yield the cTLL-S1/cGOx-S1/cHRP-S1 mixed biofluid.
A new series of high-temperature kinetic assays were performed by first annealing OPD with the three-enzyme complex biofluid, followed by addition of the protected AcGl. Initially, we confirmed that the absorbance profile for the multicomponent biofluid indeed plateaued over extensive time periods up to 2600 s (Fig. S13†). We then observed efficient production of DAP at elevated temperatures up to 150 °C (Fig. 4d and e) despite the requirement of a water molecule for the hydrolysis of the acetyl moiety. Further, pronounced thermophilic behavior was observed, corresponding to an almost 7-fold enhancement in turnover from 3.92 ± 0.63 μM s−1 at 100 °C up to 26.45 ± 0.58 μM s−1 at 150 °C (Table 4). The estimated turnover per mass of the solvent-free biofluid is roughly 5.3 μM s−1 mg−1 at 150 °C, which is similar to the catalytic performance of a reported three-component (HRP, GOx, and β-glucosidase) self-standing film operating in solution and at 37 °C for which we estimate a performance of 5.8 μM s−1 mg−1.38 Crucially, herein biocatalysis is achieved in the total absence of a solvent, whereby polymer surfactant replaces both hydration and bulk waters to stabilize enzymes and permits bioactivity up to at least 150 °C.
T/°C | ||||||
---|---|---|---|---|---|---|
100 | 110 | 120 | 130 | 140 | 150 | |
DAP Production/μM s−1 | 3.92 | 6.07 | 10.60 | 16.92 | 18.83 | 26.45 |
St. Dev./μM s−1 | 0.63 | 0.63 | 0.64 | 0.71 | 0.69 | 0.58 |
Evidently, the small loss of the native fold upon polymer surfactant conjugation for cTLL-S1 does not disrupt the catalytic-triad constructed by the Ser146-His258-Asp201 residues. This is in line with a previous study reporting on the hydrolysis of short- and long-chain fatty acid esters in cTLL-S1 melts at temperatures as low as 30 °C, corresponding roughly to the onset of melting.18 We anticipate that this remarkably low-temperature activation of the TLL helical lid-motif (Fig. 3c) is a result of the amphiphilic environment afforded by the polymer surfactant corona, which may facilitate the conformational transition from the closed-state (hydrophilic) to the open-state (hydrophobic).23 An alternative explanation that we cannot yet rule out is that the helical loop may be unstructured, which would provide a permanently exposed active-site.
Interestingly, while cTLL-S1 biofluids are active at low temperatures near the onset of melting,18 the temperatures required for the self-contained two- and three-enzyme cascades to function were almost 50 °C above their melting transition. Hence, we conclude that either GOx or HRP must limit the enzymatic cascade by the requirement for thermal activation. As the polymer surfactant appears to effectively replace hydration waters in the solvent-free environment,17 we anticipate that cGOx-S1 retains catalytic activity below 80 °C, given that the GOx internalized active site is extremely rigid and does not exhibit large-scale shape fluctuations.37 We speculate that the cascades are inactive at low temperatures, when the diffusive motions (a fluctuating-entry point) required for cHRP-S1 activity are impeded. Elevated temperatures are required to overcome this activation barrier affording sufficient conformational “flexibility” of the biomacromolecular machine. In future work, we plan to rigorously test this hypothesis in a systematic study involving scattering, spectroscopic and modelling tools. While the relative activities of the biohybrids are yet to be elucidated, our findings clearly reveal that whilst the capacity for substrate solubilization and mass transport is essential for enzyme activity, these alone are insufficient to ensure catalysis.
Due to the apparent high viscosity of the solvent-free biofluids we initially anticipated that the restricted diffusional mobility of substrates would play a critical role in limiting catalytic turnover. However, we find that enzyme activation is in fact the bottleneck at low temperatures. To examine the impact of substrate diffusion on catalysis, variable-temperature rheology experiments of the reaction mixtures were performed to probe the temperature-dependence of the viscosity of the solvent-free biofluids up to 150 °C (Fig. S9†). A comparison of the corresponding substrate diffusion coefficients with catalytic turnover above 80 °C reveals a linear relationship between initial reaction velocities and substrate diffusion coefficients (Fig. 4c and f), which is characteristic for diffusion-limited catalysis. These findings confirm that at sufficiently high temperatures when the expected catalytically vital conformations can be accessed efficiently, the polymer surfactant emulates both hydration and bulk solvent environments in the solvent-free biohybrids.
For solution-state investigations, small-angle X-ray scattering (SAXS) profiles were obtained for samples measured in 2.0 mm quartz capillaries (Hilgenberg), mounted with custom-built capillary holders. A known sample-to-detector distance of 713 mm gave an accessible q-range of 0.015 < q < 0.445 Å−1. The scattering profile of the protein buffer and quartz capillary were subtracted to produce a final SAXS profile. Background subtraction was performed using the SAXSutilities39 package (available for download http://www.sztucki.de/SAXSutilities), and the HRP series profiles were fitted using either ellipsoidal or core–shell ellipsoidal form factors25–27 in SASview (available for download http://www.sasview.org). For GOx and TLL, the online tool Crysol31 was used to compute scattering profiles based from crystallographic structure PDB files 1cf3 (symmetric dimer) and 1ein, respectively.22,23
The temperature-dependent initial reaction velocities were estimated by linear regression analysis over 60 s (two-enzyme biofluid) or 100 s (three-enzyme biofluid) of each recorded profile. The concentration of DAP was then calculated from the initial slope using the molar extinction coefficient of 16.7 mM−1 cm−1 and a 0.01 mm pathlength. The standard deviation of regression analysis was then converted in the same way to obtain a confidence interval for DAP concentration. The calculated rates of DAP production were plotted with respect to temperature, revealing a distinct temperature-dependent increase in DAP production. The temperature-dependent parameters of DAP production and substrate diffusion coefficient were compared, where a diffusion-limited process is defined by linearity.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c9nr06045f |
This journal is © The Royal Society of Chemistry 2019 |