Goutham
Kodali‡
a,
Joshua A.
Mancini‡
a,
Lee A.
Solomon
a,
Tatiana V.
Episova
a,
Nicholas
Roach
b,
Christopher J.
Hobbs
b,
Pawel
Wagner
b,
Olga A.
Mass
c,
Kunche
Aravindu
c,
Jonathan E.
Barnsley
d,
Keith C.
Gordon
d,
David L.
Officer
b,
P. Leslie
Dutton
a and
Christopher C.
Moser
*a
aThe Johnson Research Foundation and Department of Biochemistry and Biophysics, University of Pennsylvania, Philadelphia, PA 10104, USA. E-mail: moserc@mail.med.upenn.edu
bThe ARC Centre of Excellence for Electromaterials Science and the Intelligent Polymer Research Institute, University of Wollongong, NSW 2522, Australia
cN Carolina State University, Department of Chemistry, Raleigh, NC 27695, USA
dUniversity of Otago, Department of Chemistry, Dunedin 9016, New Zealand
First published on 17th August 2016
Natural selection in photosynthesis has engineered tetrapyrrole based, nanometer scale, light harvesting and energy capture in light-induced charge separation. By designing and creating nanometer scale artificial light harvesting and charge separating proteins, we have the opportunity to reengineer and overcome the limitations of natural selection to extend energy capture to new wavelengths and to tailor efficient systems that better meet human as opposed to cellular energetic needs. While tetrapyrrole cofactor incorporation in natural proteins is complex and often assisted by accessory proteins for cofactor transport and insertion, artificial protein functionalization relies on a practical understanding of the basic physical chemistry of protein and cofactors that drive nanometer scale self-assembly. Patterning and balancing of hydrophobic and hydrophilic tetrapyrrole substituents is critical to avoid natural or synthetic porphyrin and chlorin aggregation in aqueous media and speed cofactor partitioning into the non-polar core of a man-made water soluble protein designed according to elementary first principles of protein folding. This partitioning is followed by site-specific anchoring of tetrapyrroles to histidine ligands strategically placed for design control of rates and efficiencies of light energy and electron transfer while orienting at least one polar group towards the aqueous phase.
There is an active effort to understand how to construct efficient artificial systems that can replicate and enhance the light harvesting capabilities of natural photosynthetic systems in order to form high-energy products for a sustainable future.2 To this end, researchers have modified the cofactor environment in natural proteins through mutation,3 replaced natural cofactors with alternative cofactors in natural proteins,4,5 and constructed novel artificial proteins with both natural and synthetic cofactors.6–9 There is also growing interest in developing water-soluble light-harvesting proteins, as an alternative to the predominantly membrane bound forms found in nature, for novel applications both in vitro and in vivo to capture solar energy. Potential applications range from development of light-harvesting materials at the nano to meso scale (such as dye sensitized solar cells), to engineered coupling of solar energy to specific metabolic pathways for in vivo production of fuels and reagents, to therapeutic treatments such as photodynamic therapy.
This work exploits novel tetrapyrrole binding four-helix proteins with no sequence similarity to natural proteins; these robust and adaptable proteins are called maquettes10 (Fig. 1). As completely artificial proteins, they have not been naturally selected to interact with the pigment transport and insertion proteins naturally evolved to manage cofactor insertion in the living cell. Instead they are engineered for appropriate control of the physical chemical properties of cofactor and protein to support efficient self-assembly. Experience has shown that maquettes self-assemble a wide range of tetrapyrrole cofactors both on the bench top and during expression within the cell.8,9,11–13 While planning the synthesis of an extended range of cofactors for novel spectroscopic properties and light-harvesting application, we need to avoid compromising the speed and affinity of self-assembly, aiming to maintain nM affinities and seconds timescale binding. This means we need to avoid a common issue of tetrapyrrole cofactor aggregation in aqueous environments,14 but still facilitate entry and anchoring of cofactors in the hydrophobic protein interior.
Here we systematically explore the binding of Zn tetrapyrroles with different patterns of polar and non-polar substituents to four-alpha-helix maquettes engineered with either two widely spaced histidines for independent Zn metal ligation or lacking ligating histidines altogether. We use phenyl rings with and without sulphonato or carboxy functional groups to vary tetrapyrrole polarity, obtaining dissociation constants (Kd values) through singular value decomposition (SVD) analysis of visible spectra during binding titrations. We find that a balance of polar and non-polar substituents on porphyrins is key to fast and efficient binding for both porphyrins and chlorins. Amphiphilic tetrapyrroles, with one non-polar end and one polar end, allow for efficient hydrophobic partitioning into the interior of the protein while the hydrophilic part remains exposed to the aqueous portion of the protein stabilizing the complex by polar interactions. Partitioning facilitates histidine ligation to central Zn, which in turn thermally stabilizes the protein–tetrapyrrole complex by ∼3.5 kcal mol−1.
To determine the acceptable range and pattern of hydrophobic vs. hydrophilic perimeters for Zn porphyrins, we synthesized all permutations of phenyl and carboxyphenyl tetra meso substituents (Fig. 3 and 4). The visible spectral changes that occurred as these porphyrins were titrated into a His maquette solution were fitted to a simple binding model with a single dissociation constant (Kd) for each His site using singular value decomposition.16 Porphyrins with either all-hydrophobic substituents, Zn(II) 5,10,15,20-tetraphenylporphyrin (3), or all-hydrophilic substituents, Zn(II) 5,10,15,20-tetra(4-carboxyphenyl)porphyrin (8), showed no detectable spectral shift, signifying that binding was weaker than 100 μM. Clear spectral shifts were observed for the mono-phenylcarboxylic acid (4), the syn-diphenylcarboxylic acid (5), the anti-diphenylcarboxylic acid (6) and the tri-phenylcarboxylic acid (7) with fitted Kd values of 0.14 ± 2 nM, 18 ± 3.0 nM, 14 ± 4 nM and 8 ± 3 nM, respectively. At least one hydrophobic and one hydrophilic group substitution is necessary for porphyrin ligating to the maquettes with nanomolar affinities. Mono-carboxyphenylporphyrin (4) affinity is estimated at about two orders of magnitude tighter than both di-carboxyphenyl porphyrins (5) and (6) and the tricarboxyphenol porphyrin (7).
Fig. 4 Comparative binding affinity of amphiphilic Zn porphyrins to maquettes. Polar groups are highlighted in red. Binding of (3) and (8) are too weak to measure accurately. |
Resonance Raman changes of the bound tetrapyrroles show changes in “core size” vibrations17 upon addition of maquette (Fig. S2–S5†) consistent with binding and histidine ligation. The most drastic spectroscopic change occurred for data collected at 448 nm. In the region of band ν4 and ν29 (1340–1360 cm−1), the lowest energy ν4 decreases in intensity (over 40%) relative to ν29. Frequency changes with regards to ν4 are well documented as a way to detect environmental changes close to the porphyrin core. At 1421 cm−1, there is a considerable decrease in intensity of the ν3 band, whilst ν12 at 1296 cm−1 completely disappears. At the lower energy region, there is also a red shift of the 1016 cm−1 band (ν15) to 1003 cm−1. Metalloporphyrin vibrational modes such as these are generally sensitive to planarity, metal oxidation state/spin or the presence of an axillary moiety, and are expected to be affected by Zn porphyrin binding to a maquette histidine.
To determine if the pattern of enhanced binding affinity with amphiphilic character of 5,10,15,20-tetrasubstituted porphyrins also applies to simpler 5,15-disubstituted porphyrins, we characterized the binding of the relatively simple carboxyphenyl construct (9) (Fig. 5). Although this amphiphilic Zn porphyrin apparently displays desirable <100 nM affinity, stopped flow mixing shows that binding equilibrium occurs slowly and reaches completion in 20 minutes (Fig. S1†). Fig. 5 also shows that the unbound species has a red shifted Soret typical of multimerized tetrapyrrole, which complicates accurate determination of the binding affinity. Strengthening the polar character of the 15 substituent by replacing the single carboxylic group with a first generation Newkome dendrimer made up of three carboxylic acid groups (10), substantially increased the water solubility of the porphyrin, eliminated pigment multimerization and permitted binding on a few ms timescale (Fig. S1†).
Fig. 5 Maquette binding of amphiphilic 5,15-substituted Zn porphyrins with relatively short (9) and extended (10) polar groups. |
Chlorin (11) binding also stabilizes the helical structure of the maquette as seen by circular dichroism spectroscopy (Fig. 7). Thermal mid point transition of α-helical structure (Tm) increases from 46 to 61 °C upon chlorin binding with a sigmoidal behavior suggesting cooperative melting. This Tm shift corresponds to 6.8 kcal mol−1 of structure stabilization. Stopped-flow mixing shows that the chlorin (11) binds much faster than the similarly substituted porphyrin (9).
We exploited the ability to manipulate tetrapyrrole substituents to shift light harvesting Qy absorption bands to the red, while maintaining a hydrophobic/hydrophilic balance, by replacing the 5-p-tolyl group of (11) with a 3-phenylethynyl group (12). SVD analysis clarified binding induced bandshifts, shown together with a graphic representation of the bound pigment titration at the 423 minus 313 nm isosbestic for unbound pigment in Fig. 6 (middle). While changing the phenyl group at 5-position to the bulkier phenylethynyl group at the 3-position lowers the affinity 4.5 fold (Kd of 360 ± 18 nM), binding is still strong enough to drive the self-assembly of the protein tetrapyrrole complex.
Pheophorbide a is a popular, comparatively soluble chlorin derivative of chlorophyll in which the hydrophobic phytol tail is cleaved to leave a propionic acid. The extra oxophorbine ring (compared to the synthetic chlorins) introduces an asymmetry that makes them less prone to aggregation. We replaced the central Mg with Zn to make Zn pheophorbide a (13). Like the synthetic chlorins (11) and (12), (13) has a charged group on one edge of the tetrapyrrole, but also includes some uncharged but polar groups on this same edge. SVD binding analysis and 435 minus 368 nm difference absorption to track binding is shown in Fig. 6 (bottom), with a tight Kd of 4 ± 3 nM.
Just how natural Mg and Zn20 chlorophyll (Chl) and bacteriochlorophyll (BChl) cofactors are loaded in vivo into specific sites in the natural light harvesting systems has not been resolved.21 It is clear that a molecular chaperone is needed to enable light harvesting complex (LHC) proteins to insert properly into thylakoid membranes22 and that the protein folding requires the presence of the Chl cofactors. It is not clear how the Chl cofactor is managed before protein binding and how the potential threat of free Chl photo-oxidative reactions is avoided. Chl can be reconstituted into natural LHC proteins outside the cell, but this requires the assistance of detergent. In these systems, long tailed esterifying alcohols on the BChls and the carboxyl group on the mesoporphyrin ring are important structural requirements for binding.4 Many studies with artificial proteins also rely on detergent to solubilize light active tetrapyrrole cofactors and/or the proteins themselves.23–26 These systems are clarifying what factors determine the binding specificity and different protein-metal coordination preferences of detergent solubilized Chl a, b and c.27
Artificial light-harvesting proteins offer a wider engineering freedom of design compared to natural proteins. Furthermore, the protein maquettes described here, which have no significant sequence similarity to natural proteins, have relatively simple sequences and structures that allow the roles of individual amino acids and cofactor substituents to be more easily isolated to resolve general engineering principles. The conformationally rigid protein scaffolds of maquettes have interior binding sites that are sufficiently malleable to accommodate structurally diverse tetrapyrroles through variety of protein–cofactor interactions both inside and outside the cell.5,8,9,11–13 Multi-cofactor binding maquettes demonstrate light absorption, energy transfer and light-induced charge separation.7,28,29 Furthermore, because these proteins are designed from first principles of protein folding, they can be extremely stable, tolerating boiling temperatures in some cases; as seen in Fig. 7, cofactor binding generally increases the thermal stability of maquettes. These properties make the maquette platform attractive for engineering light activated energy converting systems outside of the cell as a biomaterial, and inside the cell, when integrated into natural bioenergetic pathways. Indeed, our ability to create water-soluble light-harvesting and charge-separating maquettes should allow us to design energy harvesting systems that work directly in the cytoplasm, free of cell membranes.
Previous work with water-soluble artificial proteins6,11,13,30,31 recognized that the water insolubility of natural Chls and BChls and other light active tetrapyrroles impedes binding. Often, water-soluble derivatives of Chl and BChl removing the hydrophobic tail were used instead.13,30,31 While increasing cofactor water solubility reduces aggregation in water, cofactor hydrophobicity is nevertheless useful for tight cofactor binding. The hydrophobic effect for binding in the non-polar protein interior is estimated at 2.4 kcal nm−2.6,32 Experimentally, we distinguish the energetic effect of hydrophobic portioning of a cofactor into a maquette interior from the effect of axial tetrapyrrole metal ligation by comparing maquette designs that are histidine-free from those with independent histidines orientated towards the bundle core ((1) vs. (2) vs. (3) in Fig. 2). Maquette tetrapyrrole binding occurs via a step-wise partitioning of the cofactor into the hydrophobic bundle interior, followed by histidine ligation.33 Clearly, for successful incorporation of light active tetrapyrrole cofactors into an artificial water-soluble protein frame, a balance must be struck between the hydrophobic and hydrophilic character of tetrapyrrole ring substituents. The work reported here was initiated to systematically define what makes a successful balance in order to provide a guide for cofactor construction and customization for a range of artificial light-harvesting protein functions.
meso-Substitutions that are either all charged/polar (8) or all non-polar (3) represent extremes of the hydrophobic/hydrophilic spectrum that fall prey to far too weak partitioning into the hydrophobic protein interior or aggregation in aqueous solution (Fig. 4). Iron tetrapyrrole self-assembly to bis-histidine sites displays a similar pattern.33 A charged/polar meso-substituent on one edge of the tetrapyrrole appears to offer the best compromise (4); this may be because hydrophobic burial of the other three edges may maximize hydrophobic effect forces. Adding charged groups to other faces ((5), (6), (7)) may well be forcing energetically unfavorable protein adjustments to expose these charges to the aqueous phase, or the energetic penalty of protonation/deprotonation of the charged group to neutrality.
Porphyrins with a single charged and non-polar substituent on opposite side of the tetrapyrrole perimeter without any other peripheral groups recapitulate the balance seen in the best tetra-substituted porphyrins, although binding may be slowed because of porphyrin stacking issues that can be present in aqueous solution (e.g. (9)). Increasing the number of charge groups on one edge (e.g. (10)) can clearly speed binding (Fig. S1†). Note that Zn protoporphyrin IX, an early successful cofactor choice for light activated water-soluble maquettes,11 falls into this category, with two charged propionates on one edge and non-polar methyl and vinyl groups on the other edges. A similar, even balance between a charged group and non-polar groups on opposite tetrapyrrole edges applies to successful chlorin self-assembly as well (Fig. 6). The pattern that emerges for rapid and tight self association of light active Zn tetrapyrroles to buried histidines in water soluble helical bundle proteins is to place one or more charge groups on one edge of the tetrapyrrole perimeter, hydrophobic groups up to ∼8 Å long on the opposite edge, with other non polar groups tolerated on the other two edges. Groups that disrupt pi stacking of tetrapyrroles in aqueous solution are also helpful. This pattern for single His ligated Zn tetrapyrrole binding is consistent with and extends the pattern previously described for a range of bis-His ligated Fe tetrapyrroles.33 Furthermore, this pattern appears generalizable not just to Fe vs. Zn tetrapyrrole cofactors, but to a range of different 4 helix bundle maquettes with different helical threading, loop length, helical charge and His positions (additional sequences and binding affinities in ESI†).
Maquette modularity, self-assembly and robust adaptability to changes in the pattern of exterior amino acids is now being explored in the construction of nano and meso scale architectures for solar light capture.35 Preliminary results also show that with certain designs, not only hemes8 but natural chlorophyll and bilin tetrapyrroles self-assemble into maquettes inside the cell. However, further work is needed to resolve which protein binding site properties interact most favorably with natural or modified tetrapyrroles to optimize in vivo self-assembly, so that we can begin to tap into and divert energy flow of cellular bioenergetic systems towards a new class of light driven fuel production.
Footnotes |
† Electronic supplementary information (ESI) available: Experimental methods and supplementary Fig. S1–10. See DOI: 10.1039/c6sc02417c |
‡ These authors contributed equally to the work. |
This journal is © The Royal Society of Chemistry 2017 |