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Special Focus Issue – Review Xyloglucan and its Interactions with Other Components of the Growing Cell Wall Yong Bum Park and Daniel J. Cosgrove* Department of Biology, 208 Mueller Laboratory, Pennsylvania State University, University Park, PA 16802, USA *Corresponding author: E-mail, [email protected]; Fax, +1-814-865-9131. (Received November 18, 2014; Accepted December 3, 2014) The discovery of xyloglucan and its ability to bind tightly to cellulose has dominated our thinking about primary cell wall structure and its connection to the mechanism of cell enlargement for 40 years. Gene discovery has advanced our understanding of the synthesis of xyloglucan in the past decade, and at the same time new and unexpected results indicate that xyloglucan’s role in wall structure and wall extensibility is more subtle than commonly believed. Genetic deletion of xyloglucan synthesis does not greatly disable cell wall functions. Nuclear magnetic resonance studies indicate that pectins, rather than xyloglucans, make the majority of contacts with cellulose surfaces. Xyloglucan binding may be selective for specific (hydrophobic) surfaces on the cellulose microfibril, whose structure is more complex than is commonly portrayed in cell wall cartoons. Biomechanical assessments of endoglucanase actions challenge the concept of xyloglucan tethering. The mechanically important xyloglucan is restricted to a minor component that appears to be closely intertwined with cellulose at limited sites (‘biomechanical hotspots’) of direct microfibril contact; these may be the selective sites of cell wall loosening by expansins. These discoveries indicate that wall extensibility is less a matter of bulk viscoelasticity of the matrix polymers and more a matter of selective control of slippage and separation of microfibrils at specific and limited sites in the wall. Keywords: Biomechanical hot spots Cellulose microfibrils Cell wall loosening Endoglucanase Expansin Pectins. Abbreviations: AFM, atomic force microscopy; CEG, cellulose-specific endoglucanase; CSLC, cellulose synthase-like C; CXEG, cellulose and xyloglucan hydrolyzing endoglucanase; EM, electron microscopy; GPC, gel permeation chromatography; NMR, nuclear magnetic resonance; SEC-MALLS, size exclusion chromatography coupled with multiangle laser light scattering; ssNMR, solid-state NMR; XEG, xyloglucanspecific endoglucanase; XTH, xyloglucan endo-transglycosylase/hydrolase. Introduction Xyloglucans were initially identified as seed storage polysaccharides from nasturtium, tamarind and other seeds (Kooiman 1957), and later as extracellular polysaccharides in sycamore cell suspension cultures (Aspinall et al. 1969, Bauer et al. 1973) and soon thereafter as components of primary cell walls of many species (reviewed by Hayashi 1989). The concept that xyloglucans play a central role in the control of wall extensibility originated with the pioneering molecular model of the cell wall of sycamore cell suspension cultures by the Albersheim group (Keegstra et al. 1973) and the discovery that auxin-induced growth in pea epicotyls is accompanied by increased xyloglucan metabolism (Labavitch and Ray 1974). Further evidence for xyloglucan binding to cellulose (e.g. Hayashi and Maclachlan 1984), and for auxin-induced changes in xyloglucan size (e.g. Nishitani and Masuda 1983, Talbott and Ray 1992a), cemented xyloglucan as a focal element in discussions of cell wall structure and growth for decades. The view that ‘enzyme-catalyzed modification of xyloglucan crosslinks in the cellulose/xyloglucan network is required for the growth and development of the primary cell wall’ (Pauly et al. 1999) became almost axiomatic in the cell wall field for more than two decades. Hence the report of an Arabidopsis mutant that lacked xyloglucan, yet exhibited only minor growth phenotype, came as a jolt to cell wall researchers (Cavalier et al. 2008). This report, combined with a number of other results at odds with current models, has led us and some other researchers to rethink the structure of primary cell walls and the role of xyloglucan in cell wall extensibility. In the 40 years since xyloglucan came to be viewed as an indispensable component controlling wall extensibility, the concepts of how xyloglucan interacts with cellulose and other wall components have evolved considerably. The original hypothesis of a macromolecular matrix made of covalently linked domains of xyloglucan, pectins and structural proteins (Keegstra et al. 1973) was replaced by the simpler tethered network model (Hayashi 1989, Carpita and Gibeaut 1993, Nishitani 1998, Cosgrove 2001) which highlighted direct coating and tethering of cellulose by xyloglucan as the key structural determinant of wall extensibility. Despite widespread acceptance of this model, numerous points in the model have not been critically tested and it is probably too tight-knit a structure to be compatible with the high mechanical extensibility and flexibility of many primary cell walls (Hepworth and Bruce 2004). Some alternative models lacking direct cellulose–cellulose linkages have been suggested; for instance, Talbott and Ray (1992b) proposed a ‘multicoat’ structure in which cellulose was coated with tightly bound xyloglucan, which was coated with more loosely held arabinans/galactans, Plant Cell Physiol. 56(2): 180–194 (2015) doi:10.1093/pcp/pcu204, Advance Access publication on 21 January 2015, available online at www.pcp.oxfordjournals.org ! The Author 2015. Published by Oxford University Press on behalf of Japanese Society of Plant Physiologists. All rights reserved. For permissions, please email: [email protected] Plant Cell Physiol. 56(2): 180–194 (2015) doi:10.1093/pcp/pcu204 which were intermingled with a gelled interface of acidic polysaccharides and structural protein; Thompson (2005) suggested that wall extensibility is controlled by spatial constraints in the movement of microfibrils rather than by direct interfibril linkages. These authors noted important shortcomings in the popular model, but their alternative concepts have garnered little support or follow-up. Recent results based on solid-state nuclear magnetic resonance (ssNMR) and biomechanical approaches have raised fresh doubts about the correctness of the tethered network model and, more generally, about the significance of xyloglucan’s role in wall structure and mechanics. Concomitantly, pectin has seen a resurgence as an important element in discussions of cell wall mechanics (Zykwinska et al. 2008, Palin and Geitmann 2012, Braybrook and Peaucelle 2013). Thus, this seems to be a good juncture to review recent developments in the field of xyloglucan and to assess their implications for cell wall structure and extensibility as well as to point out areas in need of more in-depth inquiry. This review considers xyloglucan function in the context of common models (or, more correctly, depictions) of growing cell walls: cellulose microfibrils are represented as well-spaced and non-contacting rods; xyloglucan covers most cellulose surfaces, preventing direct contact between microfibrils and simultaneously acting as the major (or sole) load-bearing tether between cellulose microfibrils; wall strength stems from xyloglucan tethers between adjacent microfibrils and wall loosening depends on breaking or shifting the xyloglucan tethers. These concepts of xyloglucan function emerged from a large body of work, cogently summarized in various reviews (Fry 1989, Hayashi 1989, Carpita and Gibeaut 1993, Cosgrove 2001) and extended by later results, including transgenic expression of xyloglucanase and cellulase in plant tissues (Park et al. 2003, Hayashi and Kaida 2011). The tethered network is the most common depiction in overviews of plant cell walls (e.g. Somerville et al. 2004, Cosgrove 2005, Burton et al. 2010, Scheller and Ulvskov 2010), but many of its features and implications are untested. In this article, we emphasize some of the more physical aspects of xyloglucan–cellulose interaction that are not often discussed in the biological literature, we review recent results that appear to run counter to these wellentrenched concepts of primary walls, and we suggest possible ways to resolve some apparent contradictions. We begin with a brief update on xyloglucan structure and synthesis, then summarize studies on the physical binding of xyloglucan to cellulose, followed by recent physical, genetic and biomechanical tests of the tethered network model. We do not discuss the potential role of xyloglucans in secondary cell walls (but see Mellerowicz et al. 2008, Baba et al. 2009, Hayashi and Kaida 2011, Nishikubo et al. 2011). Structure, Size, Diversity and Conformation of Xyloglucans Xyloglucans comprise a heterogeneous collection of polysaccharides of variable length and side chain pattern. They are widespread if not universal in the primary cell walls of land plants, but their amounts vary considerably. In many dicots, xyloglucans constitute the major hemicellulose of growing cell walls, comprising approximately 20% of the dry mass of primary cell walls (reviewed in Fry 1989, Hayashi 1989, Schultink et al. 2014), but xyloglucan content may be as low as 2% (Thimm et al. 2002). Grasses—but not monocots in general—have a reduced xyloglucan content; values of approximately 5% of primary walls are typical in grasses, but values as high as 10% occur (Carpita 1996, Gibeaut et al. 2005). Xyloglucans consist of a b(1,4)-D-glucan backbone that is quasi-regularly substituted with a-D-xylosyl residues linked to glucose through the O-6 position (Fig. 1A, B). In many species, the backbone has a regular pattern of three substituted glucose units followed by an unsubstituted glucose residue. Substitution is less frequent in some taxonomic groups. For instance, only about 40% of the glucose residues are substituted in tomato and other species in the Solanaceae (Ring and Selvendran 1981, York et al. 1996) while xyloglucans from grass cell walls have 30–40% substitution (Hsieh and Harris 2009). The xylosyl residue may be b-(1,2) linked with a D-galactosyl residue which may be additionally linked a-(1,2) with an L-fucosyl residue; other side chain patterns have also been documented (Schultink et al. 2014, Tuomivaara et al. 2015). A concise nomenclature is used as shorthand for the side chain structure (Fig. 1D). Diagnostically useful endoglucanases cut the xyloglucan backbone selectively at the unsubstituted position, producing a mixture of oligosaccharides commonly made of four glucose residues in the backbone with three xylose and a smaller number of galactose and fucose substituents. These oligosaccharides are readily identified by high-performance anion exchange chromatography with pulsed amperometric detection or matrix-assisted laser-desorption/ionization time of flight mass spectrometry, which have been adapted for sensitive and rapid xyloglucan analysis (Gunl et al. 2011, Tuomivaara et al. 2015). In many dicots, the most common oligosaccharides produced by endoglucanase digestion of xyloglucan are the Glc4 oligosaccharides designated XXXG, XXFG, XXLG and XLFG, but numerous species-dependent and organ-dependent variations in the side chain pattern have been documented (Schultink et al. 2014, Tuomivaara et al. 2015). For instance, galactose is frequently replaced by arabinose in xyloglucans of tomato and other species in the Solanaceae (Ring and Selvendran 1981, Hoffman et al. 2005), whereas galacturonic acid partially replaces galactose in an unusual acidic xyloglucan recently identified in Arabidopsis root hairs (Pena et al. 2012). The xyloglucan side chains in grasses are generally not extended beyond xylose; upon endoglucanase digestion, the most common oligosaccharides are XXGG and XXGGG. Thus, the defining structure for xyloglucan is a glucan backbone with O-6-linked xylose side chains, but the extent of further substitution and sugar identity varies considerably. As discussed below, side chains may affect interactions with cellulose and possibly other components of the cell wall, but whether such interactions play a significant functional role in the biological variation of xyloglucan is not entirely clear at this point. 181 Y. B. Park and D. J. Cosgrove | Xyloglucan interactions in growing cell walls Fig. 1 Xyloglucan structure. (A) Structure of the XLLG oligosaccharide, showing the b-1,4-D-glucan backbone (gray) with side chains made of xylose (green) and galactose (blue). (B) Pattern of linkages for sugars in the XLFG oligosaccharide with the associated glycosyl transferases indicated in upper case letters. (C) Xyloglucans may have short regions in a flat-ribbon conformation, suitable for binding to the hydrophobic surface of cellulose microfibrils or may assume a twisted conformation. (D) List of naturally occurring xyloglucan side chains and their one-letter designations. Image credits: B is from Zabotina (2012), reprinted under Creative Commons Attribution Non Commercial License; C is reprinted from O’Neill and York (2003), copyright Wiley-Blackwell, used with permission. D is adapted from Tuomivaara et al. (2014), copyright by Elsevier and used with permission. 182 Plant Cell Physiol. 56(2): 180–194 (2015) doi:10.1093/pcp/pcu204 Another notable feature of XyG is O-acetylation, which is often overlooked because the ester linkage is broken by the strong alkaline conditions commonly used to extract xyloglucan from cell walls. In Arabidopsis and many other dicots, O-acetylation of XyG is found principally on galactosyl residues at the O-3 or O-2 positions (Kiefer et al. 1989). This contrasts with xyloglucans in grasses (Poaceae) and the Solanaceae where the glucan backbone is acetylated at O-6, in effect replacing the xylose side chain with an acetyl group (Gibeaut et al. 2005, Jia et al. 2005). Acetylation was not detected in xyloglucans from apple pulp or tamarind seeds (Sims et al. 1998), indicating biological variation in this structural trait. Acetylation of galactose is not essential in Arabidopsis, as at least one ecotype lacks it, but it may contribute to pathogen resistance (Manabe et al. 2011, Gille and Pauly 2012). Acetylation of the substituted glucose residues in xyloglucans of the Poaceae and the Solanaceae improves xyloglucan solubility and prevents self-association and aggregation in these xyloglucan variants that have relatively low substitution (Sims et al. 1998). One might surmise that grass xyloglucans bind more tightly to cellulose than do the more highly substituted xyloglucans of other plant groups (see below), but this issue has evidently not been examined closely. Chain length Published size estimates of xyloglucan from primary cell walls are based mostly on gel permeation chromatography (GPC; also known as gel filtration chromatography or size exclusion chromatography). Peak values for relative molecular mass (Mr) vary enormously, ranging from 9 kDa to >900 kDa, with most estimates in the 100–300 kDa range; moreover, xyloglucan is reported to undergo rapid shifts in Mr under various conditions (Nishitani and Masuda 1983, Talbott and Ray 1992a, Talbott and Pickard 1994, Thompson and Fry 1997). Storage xyloglucans, i.e. from tamarind, nasturtium and other seeds, are exceptionally large, reported to exceed 1,000 kDa (Lima et al. 2004). The smallest values (9 kDa) (Talbott and Ray 1992a) correspond to a backbone length of 28 glucose residues (14 nm) whereas 900 kDa corresponds to 2,800 glucose residues (1,400 nm). This 100-fold range in peak values is truly remarkable for a wall component thought to play a central structural role in cell wall architecture and mechanics. Chain length estimates based on GPC must be regarded with caution because they are sensitive to the conformation, hydrodynamic radius and aggregation of the polymer, as well as to interactions with the column matrix and other potential influences. Moreover, iodine staining, which is used to quantify xyloglucan, may bias the results toward the large size because it is insensitive to xyloglucans <10–20 kDa (Hayashi 1989, O’Neill and York 2003). GPC columns are typically calibrated with dextrans [a-1,6-D-glucan backbones with 5% a-(1,3)glucose substitution] which have a different conformational behavior from xyloglucans, potentially introducing large overestimates in Mr. This issue is generally well recognized (Talbott and Ray 1992b, Gaborieau and Castignolles 2011, Kohnke et al. 2011) and such Mr data are best interpreted as relative rather than absolute size. Size exclusion chromatography coupled with multiangle laser light scattering (SEC-MALLS) can provide better estimates of polymer size (Harding 2005), but this method has rarely been employed for xyloglucan from primary cell walls. An appreciation of the problems of chain length estimates based on GPC alone can be gained from a study of wheat arabinoxylan that was partially digested with arabinosidase to remove some of the side chains but to leave the backbone intact. The hydrodynamic radius of the polymer shrank from 24 nm to 9 nm as the percentage of unsubstituted backbone residues increased from 63% to 84% (Kohnke et al. 2011). Using dextrans for calibration (Armstrong et al. 2004), one would estimate a 10-fold reduction in polymer length from these values, but in this instance the difference was primarily due to conformation because arabinose removal reduced the molecular mass by only 11%. The polymer with less substitution assumed a more compact conformation; self-aggregation of the backbone may have contributed to the smaller size. In the case of xyloglucans, conformation may vary with the degree of substitution, the length of side chains and the acetylation pattern; xyloglucans may also be modified during extraction and may undergo changes in aggregation and association with other substances that affect their elution from a GPC column. Most GPC-based estimates of xyloglucan Mr probably lead to overestimates of xyloglucan chain length. A very different approach to estimating chain length makes use of electron microscopy (EM) or atomic force microscopy (AFM) to measure the length of extracted polymers dispersed on a smooth mica surface. These methods do not reveal the chemical identity of the polymers, which must be verified by other means. An EM analysis of presumptive xyloglucans (linear polymers from a 1 M KOH extract of onion scale parenchyma walls) showed chain lengths ranging from 20 to 300 nm, with a number-averaged length of approximately 150 nm (McCann et al. 1992). Assuming these were indeed single xyloglucan molecules, not aggregates or concatenated chains, they would correspond to an average xyloglucan size of approximately 90 kDa (number-average estimate; the mass-average estimate would be larger). This study also noted a stepwise distribution of xyloglucan chain lengths, with steps of approximately 30 nm. The basis for the steps is uncertain, but it suggests a mechanism of blockwise assembly or restructuring of xyloglucan in muro, i.e. by xyloglucan endo-transglucosylase (Nishitani and Tominaga 1992, Thompson and Fry 1997, Rose et al. 2002). Microscopic measurements of polymer chain lengths are labor intensive and have their own set of technical problems, but they provide detailed information not provided by other methods. This appears to be the only study of xyloglucan size distribution by this method up to now. AFM has been used to image tamarind xyloglucan dried on mica, but without detailed length analysis (Morris et al. 2004); it has also been used to quantify the distribution of pectin chain lengths (Round et al. 2010). Different biological sources undoubtedly contribute to the wide range of xyloglucan Mr values, but even with the same material (third internode of etiolated pea epicotyl) the major xyloglucan peak was estimated in one study to be approximately 300 kDa (Hayashi and Maclachlan 1984) and 30 kDa in 183 Y. B. Park and D. J. Cosgrove | Xyloglucan interactions in growing cell walls another (Talbott and Ray 1992b). The difference was attributed to rapid and reversible changes in xyloglucan size induced by a variety of biological treatments (Talbott and Ray 1992a), but the molecular basis for such reversible changes has not been established. After reviewing the xyloglucan literature, we must admit to being impressed by the striking variation in peak Mr values for xyloglucans in growing cell walls. Can they really vary dynamically by >10-fold? How do such changes influence cell wall extensibility? A common view is that smaller xyloglucans mean greater wall extensibility, e.g. as expressed by Fry (1989), but a well-controlled study of this point has not been published. The observations of Talbott and Ray (1992a) challenge a simple correlation between Mr and extensibility, as do recent results with substrate-specific endoglucanases, to be discussed below. Another issue concerns xyloglucan conformation in the wall. At short length scale (10 glucose residues) the xyloglucan backbone assumes an extended, relatively rigid conformation (Fig. 1C) whose flexibility depends on the side chains and their interaction with the backbone (Gidley et al. 1991, Levy et al. 1997), whereas at longer scale the polymer in solution forms a ‘semiflexible swollen coil’ (Muller et al. 2011). Small-angle neutron scattering measurements indicate that xyloglucan in solution has a persistence length of 8 nm (four Glc4 units or 16 glucose residues). Other techniques give similar or somewhat smaller values (Patel et al. 2008). Persistence length is a measure of polymer rigidity; roughly, it is the distance over which a chain will bend significantly (or lose orientational correlation) by thermal fluctuations. For comparison, the DNA double helix has a persistence length of 50 nm, i.e. it is a much more rigid molecule, whereas dextran has a much smaller persistence length, estimated as 0.4 nm (Rief et al. 1998). Well-solvated, self-avoiding polymers whose length is much longer than the persistence length will occupy a time-averaged spheroidal shape with a diameter much less than the chain length. In the case of tamarind xyloglucan, the hydrodynamic radius was measured as 51 nm and its weight-average molecular mass was determined by SEC-MALLS to be 470 kDa, corresponding to approximately 750 nm extended chain length (Muller et al. 2011). These results show that xyloglucan in solution assumes a coiled shape, characteristic of most polymers, but stiffer than highly flexible chains such as dextran. The shape of xyloglucans in solution thus differs from the extended conformation represented in many depictions or ‘cartoons’ of primary cell walls. It may be argued that xyloglucan–cellulose interactions would force xyloglucan into an extended conformation, but NMR results, discussed below, suggest that only a small fraction of xyloglucan in the wall has such a conformation. A final structural issue is the extent to which xyloglucan is covalently cross-linked to other components of the cell wall, as well as the (unknown) nature of the putative covalent linkage. There are reports that up to 30% or more of the xyloglucan in walls from cell suspension cultures is covalently linked to pectin, evidently cross-linked during synthesis within the Golgi apparatus (Thompson and Fry 2000, Popper and Fry 2008). In contrast, numerous studies of cell walls from growing 184 tissues (not cell cultures) show that little or none of the xyloglucan is covalently linked to pectins (see Talbott and Ray 1992b, and references therein). A simple method dubbed ‘epitope detection chromatography’ was recently combined with a simple sample preparation procedure to characterize polysaccharide complexes from Arabidopsis cell walls (Cornuault et al. 2014). The method passes solubilized components through an anion exchange column and uses antibodies to detect specific epitopes in the eluted fractions. The results indicated that the vast majority of xyloglucan was not linked to pectin, judged by lack of retention on the anion exchange column. In extracts from shoots, the xyloglucan–pectin component amounted to only a trace, while root extracts showed a notable but still minor peak, approximately 5% of the total, that is potentially a xyloglucan–pectin hybrid. These results are consistent with most biochemical dissections of primary cells walls. They contrast profoundly with a study of xyloglucans from Arabidopsis cell cultures where 50% of the xyloglucans appeared to be synthesized on a pectin primer, forming a chimeric polysaccharide that was stable in the cell wall for several days (Popper and Fry 2008). How can such divergent results be understood? Perhaps the ability to link xyloglucan and pectin intracellularly is adaptively expressed under special circumstances and may be particularly well developed in cell suspension cultures. Cell cultures differ from cells in the plant body and are capable of remarkable adaptations in wall structure (Shedletzky et al. 1990). Xyloglucan–pectin complexes might be an intermediate stage in the synthesis of specific wall components (Tan et al. 2013), followed by polymer rearrangements in the cell wall mediated by transglycosylases or other lytic enzymes. Cross-linking of xyloglucan with pectin also offers a potential mechanism for rigidifying cell walls as they cease growth and become insensitive to wall-loosening agents such as a-expansin (Cosgrove 1996, Zhao et al. 2008). We conclude that chimeric xyloglucan–pectin molecules are quantitatively minor components of most growing cell walls. This does not necessarily mean they are insignificant for wall integrity or wall extensibility, but this point has not been critically tested to date. A major step toward this goal would be to identify the enzyme that forms the putative linkage between the two polymers, followed by biomechanical analysis of walls from mutants with defects in the corresponding gene. Biosynthesis Identification of the genes underlying xyloglucan biosynthesis has progressed rapidly in recent years (Zabotina 2012, Zabotina et al. 2012 Pauly et al. 2013) and is only briefly recapped here (Fig. 1B). The b-(1,4)-D-glucan backbone of XyG is synthesized by Golgi-localized glycan synthases, encoded by CELLULOSE SYNTHASE-LIKE C (CSLC) genes (Cocuron et al. 2007). Side chains are added in the Golgi by multiple glycosyltransferases including a-(1,6)-xylosyltransferases (XXT1, XXT2 and XXT5), b-(1,2)-galactosyltransferases and a-(1,2)-fucosyltransferase (Perrin et al. 1999, Faik et al. 2002, Vanzin et al. 2002, Madson Plant Cell Physiol. 56(2): 180–194 (2015) doi:10.1093/pcp/pcu204 et al. 2003, Pena et al. 2004, Lerouxel et al. 2006, Zabotina et al. 2008, Zabotina et al. 2012). Moreover side chain substitution is finely tuned by different glycosyltransferases that add the same glycosyl moiety to different positions (Schultink et al. 2014). The transfer of galacturonic acid to xylose in Arabidopsis root hairs appears to be catalyzed by a family-47 glycosyltransferase (Pena et al. 2012). CSLC4 and some of the xylosyltransferases form a multiprotein synthesis complex in the Golgi (Chou et al. 2012; see also the review in Zabotina 2012). To create novel xyloglucans, Schultink et al. (2013) expressed foreign arabinosyltransferases in a mur3/xlt2 Arabidopsis mutant lacking xyloglucan galactosylation. This resulted in a novel xyloglucan that was intermediate in structure between that of Arabidopsis and Solanaceous species. The mur3/xlt2 mutants, which produced xyloglucan made only of XXXG subunits, were shorter than the wild type and had reduced wall extensibility. This phenotype may stem from dysfunctional xyloglucans within the wall or from detrimental effects on Golgi function (Tamura et al. 2005). The transgenic plants produced xyloglucan containing XXSG subunits (S indicates a xylose-arabinose side chain). This change restored growth and wall extensibility to wild-type levels. The results suggest that the length of the xyloglucan side chain may be more important than the specific type of sugars used. Thus the era of ‘designer xyloglucans’ is upon us, and this platform may prove useful in the future for creating additional novel xyloglucan variants to explore more detailed structure–function relationships of xyloglucan. Complementary to these biosynthetic enzymes, plants also have a suite of glycosidases that can trim xyloglucan side chains after deposition to the cell wall (Pauly et al. 2001, Sampedro et al. 2010). Such enzymes may be involved in turnover or recycling of sugars from non-structural xyloglucans in the cell wall. As mentioned above, galactose residues in xyloglucan are acetylated in Arabidopsis (Gille and Pauly 2012). Forward genetic approaches identified a pair of related multidomain transmembrane proteins named AXY4 and AXYL as essential for galactose acetylation (Gille et al. 2011). These proteins are part of a flexible O-acetylation mechanism that transfers acetyl groups to a number of polysaccharides and that is conserved across kingdoms (Gille and Pauly 2012). The targeting of acetylation, e.g. to the glucan backbone in xyloglucans of grasses or solanaceaous species, or to the galactose side chain in Arabidopsis and other species, or to other targets, is apparently well regulated but not understood in detail. One notable disparity in the literature is the remarkably small size of xyloglucans isolated from the Golgi (9 kDa) (Talbott and Ray 1992a, Thompson and Fry 1997) compared with the much larger size of xyloglucans extracted from cell walls (Mr in the range of 100–300 kDa or larger). One possible explanation for this disparity is that xyloglucan is synthesized in the Golgi as smaller units that are secreted to the wall and subsequently linked together to make longer chains. Such ligations are possible through the action of members of the xyloglucan endo-transglucosylase/hydrolase (XTH) family (Thompson et al. 1997, Thompson and Fry 2001, Rose et al. 2002), potentially generating the stepwise distribution of xyloglucan lengths observed by McCann et al. (1992). The same enzyme might also underlie other dynamic shifts in xyloglucan size (Talbott and Ray 1992a, Talbott and Pickard 1994), but this has not been established. If mature xyloglucans are indeed enzymatically assembled in the cell wall from small segments, the process could have a major impact on the topology of xyloglucan within the wall, probably resulting in complex entanglements; this could explain the need for a high NaOH concentration to extract xyloglucan from cell walls, whereas xyloglucan bound to cellulose in vitro is released at much lower concentrations. Interactions of Xyloglucan with Cellulose In Vitro and In Silico Early studies established that xyloglucan bound tightly but noncovalently to cellulose (Aspinall et al. 1969, Bauer et al. 1973). This was confirmed and extended by later studies, eventually leading to the ‘tethered network’ concept that xyloglucan extensively coats cellulose surfaces and tethers microfibrils together (Hayashi 1989, Pauly et al. 1999). Xyloglucan binding in vitro to cellulose has been explored with several physical and biological techniques. Many such studies have used commercially available tamarind seed xyloglucan, which differs in size, acetylation and side chain composition from xyloglucans typical of primary cell walls. Moreover, the forms of cellulose used for in vitro studies often differ from native cellulose from primary cell walls. It has become evident that these structural differences could impact the applicability of the results for understanding the state of xyloglucans in native cell walls. For instance one study found that the relative binding capacity for fucosylated and de-fucosylated xyloglucans differed according to cellulose source (Chambat et al. 2005). The two forms of xyloglucan bound equally to cellulose prepared from primary cell walls, but binding differed 2-fold with cellulose from secondary cell walls of flax. The lesson is clear: the biological source of cellulose and its processing can substantially influence xyloglucan binding. Native cellulose from primary cell walls takes the form of 3 nm wide microfibrils, consisting of cellulose crystalline domains and less ordered regions (Thomas et al. 2013, Cosgrove 2014). The degree of crystallinity is low, with estimates as low as 20–40% (Chambat et al. 2005). This contrasts with celluloses from secondary cell walls or bacterial sources which have much higher crystallinity and may aggregate into larger ordered structures. The crystalline regions have surfaces with distinctive physical properties: surfaces with exposed sugar rings form a dominantly hydrophobic planar surface populated by axial CH groups, whereas the other surfaces are populated by equatorial OH groups extending from the sides of the stacked glucan chains, and consequently are hydrophilic (Fig. 2A). The two surfaces probably interact in different ways with water, matrix polymers, enzymes and small molecules. As illustrated in Fig. 2, the ratio of hydrophilic to hydrophobic surface depends on the shape of the microfibril cross-section. This is an important, but poorly characterized, aspect of microfibril structure 185 Y. B. Park and D. J. Cosgrove | Xyloglucan interactions in growing cell walls Fig. 2 Cross-sectional shape and width of cellulose microfibrils affect the relative surface area with hydrophobic (blue) and hydrophilic (yellow) character. Left: a 24 chain microfibril with a truncated diamond shape. Right: an 18 chain microfibril with a rectangular shape. A xyloglucan chain is shown bonded non-covalently in an extended conformation on the upper hydrophobic surface of each microfibril. (Newman et al. 2013). Presumably the same kinds of surfaces are found in non-crystalline regions of cellulose, but there seems to be little evidence regarding this point. Two crystalline allomorphs (cellulose Ia and Ib) are synthesized by plants, algae and bacteria. They differ slightly in the alignment of adjacent glucan chains in the crystal. Land plants produce predominantly the cellulose Ib form, while algae and bacteria produce mostly cellulose Ia (Atalla and Vanderhart 1984, Lee et al. 2014), but the functional significance of this difference is unclear. Although celluloses from different sources are chemically identical, their physical forms may differ, potentially influencing xyloglucan binding (Chambat et al. 2005). The degree of crystallinity and the specific surface area are key factors, but other aspects may also be involved. Regenerated cellulose surfaces and amorphous cellulose particles lack the repeating organized structure of the cellulose microfibril. So-called amorphous cellulose, produced in vitro by swelling or dissolving crystalline cellulose, probably differs in surface structure from the noncrystalline portion of cellulose found in primary cell walls. A commonly used form of ‘microcrystalline cellulose’ branded as Avicel contains crystalline regions of Ib cellulose, but its physical form is an irregular, porous particle of acid-washed, pulverized woody cell wall aggregates (Supplementary Fig. S1). Smaller xyloglucan polymers can penetrate deeper into the Avicel particle than can larger polymers, which are restricted to the larger pores. Because the effective surface area for binding varies with xyloglucan size, binding kinetics are complicated and partly limited by size-dependent xyloglucan diffusion into the pores of the particles. These geometrical issues probably account for the markedly higher binding of Avicel for smaller xyloglucan polymers reported by Lima et al. (2004). In studies that used less porous cellulose, the binding capacity showed little dependence on xyloglucan size or increased with the size of the xyloglucan chain (Hayashi et al. 1994, Lopez et al. 2010), indicative of a surface topology with loops and coils. To obtain forms of cellulose more closely resembling native surfaces, cellulose has been isolated from primary walls (Hayashi et al. 1987), but treatment with strong alkali to remove hemicelluloses would have caused swelling of cellulose and 186 converted it to a different crystalline isomorph (cellulose II), in which the glucan chains are said to run antiparallel rather than parallel as in the native form (cellulose I). Hydrolysis with HCl has also been used (Chambat et al. 2005). This treatment may avoid the swelling problem, but it hydrolyzes some noncrystalline regions of the microfibrils, producing more tractable cellulose nanofibrils or nanocrystals which may partially resemble primary cell wall cellulose, but probably differ in some structural aspects. In other studies, nanocrystalline cellulose has been made by digestion with sulfuric acid, which is problematic because it esterifies the surface cellulose chains with sulfate groups, leaving a large negative charge on the surface (Gu et al. 2013). The sulfate esters may be removed by subsequent treatment with NaOH. These practical complexities of cellulose structure do not negate the value of in vitro binding studies but they do need to be kept in mind in evaluating the applicability of results for native wall structure. When applied in dilute aqueous solutions, xyloglucans bind to cellulose as a monolayer, meaning that xyloglucan does not stack on itself; the binding appears to be irreversible and the binding capacity—measured as the xyloglucan : cellulose ratio—increases as the fibril size is reduced, as would be expected for the trend of surface area : mass ratio (Hayashi et al. 1987, Chambat et al. 2005). Much attention has been given to the significance of terminal fucose residues on trisaccharide (F) side chains since an early computational study suggested that F side chains promote a xyloglucan conformation favorable for cellulose binding (Levy et al. 1991). Experimental work showed that fucosylated xyloglucan bound more rapidly to Avicel than did non-fucosylated xyloglucan (Hayashi et al. 1994, Levy et al. 1997), but a reverse trend was observed with other forms of cellulose (Chambat et al. 2005). These xyloglucans were isolated by extraction with alkali, and so would be de-acetylated. Xyloglucans bound to cellulose in vitro are readily solubilized with 0.25 M NaOH, which is much lower than the 4 M concentration required for extraction from native cell walls. This difference in extractability presumably stems from the more intricate interactions/entanglements of xyloglucans with cellulose and pectins in native cell walls, arising from the wall assembly process. Such interactions have been partially mimicked in multilayered assemblies of cellulose nanocrystals and xyloglucan (Cerclier et al. 2010) and in cellulosic composites produced by cellulose-synthesizing bacteria grown with xyloglucan in the culture medium (Whitney et al. 2006). By use of adsorption isotherms and isothermal titration calorimetry, a recent study explored the influence of chain length, side chain pattern and degree of acetylation on xyloglucan binding to nanocrystalline cellulose (Lopez et al. 2010). Celluloses were prepared from bacterial cellulose or filter paper by acid hydrolysis, so aspects of their structure may differ from cellulose in primary cell walls. Two stages of xyloglucan adsorption to cellulose were identified: an exothermic process attributed to hydrogen bonding at low xyloglucan concentration, and an endothermic process attributed to hydrophobic interactions and solvent reorganization at high xyloglucan oligosaccharide concentration. This study found that binding capacity increased with the size of the xyloglucan, Plant Cell Physiol. 56(2): 180–194 (2015) doi:10.1093/pcp/pcu204 that a minimum of 12 backbone glucosyl residues were needed for binding to crystalline cellulose surfaces, and that xyloglucan with fucose-terminated side chains bound at somewhat higher levels than did xyloglucan lacking fucose. These results are consistent with previous work (Hayashi et al. 1994). The minimum chain length for binding is similar to the persistence length of xyloglucan, suggesting that binding requires bonding between a relatively stiff xyloglucan segment and a flat cellulose surface. The enhanced binding of fucosylated xyloglucan was attributed to the trisaccharide character of the fucose-containing side chain—potentially providing more OH groups for hydrogen bonding to cellulose—rather than any particular influence of fucose on xyloglucan conformation. This inference was based on a computational analysis of xyloglucan–cellulose interactions (Hanus and Mazeau 2006) rather than experimental results. Acetylation did not influence xyloglucan binding to nanocrystalline cellulose. Lopez et al. also noted that xyloglucan binding did not involve a large change in enthalpy (heat), confirming an earlier study (Lima et al. 2004). The low enthalpic character of binding suggests that binding has a large entropy component, most probably by freeing water molecules constrained to an organized layer of water at cellulose surfaces. The entropy contributions for xyloglucan–cellulose binding require further study, especially in view of the crowded environment of the cell wall where molecular crowding might influence polymer interactions (Benton et al. 2012). It is notable in this context that amorphous cellulose is reported to have more hydrophilic and fewer hydrophobic surfaces exposed to aqueous solvent than does crystalline cellulose (Mori et al. 2012). This observation may be relevant to the mode of xyloglucan binding in primary cell walls where the majority of cellulose is microfibrillar but with low crystallinity. Xyloglucan binding to the distinctive surfaces of cellulose is difficult to distinguish experimentally, but insights may be gained from computational approaches. Early computational work simulated xyloglucan binding to cellulose without explicitly considering the contribution of water (Levy et al. 1991, Finkenstadt et al. 1995, Levy et al. 1997, Hanus and Mazeau 2006). In contrast, more recent studies included water and used different quantitative approaches based on more advanced molecular dynamics software (Zhang et al. 2011, Zhao et al. 2014), reaching somewhat different conclusions from the earlier work and showing that the influence of side chains on binding is more complicated than anticipated in earlier work. Inclusion of water substantially reduced the interaction energy calculated in the binding simulations. With xyloglucan oligosaccharides (glucan chain length = 9) bound to a hydrophilic surface of cellulose, galactosyl and fucosyl substitutions had little effect on binding strength, but xyloglucan conformation was affected (Zhang et al. 2011). When interaction energies were compared for xyloglucan bound to the hydrophilic and hydrophobic surfaces of cellulose in water, binding was seen to be much more favorable for the hydrophobic surfaces for most side chain configurations tested (Zhao et al. 2014). Such high-energy binding entailed removal of structured water from the cellulose surface and from half of the xyloglucan surface. Presumably such structured water pays an entropic penalty which would be redeemed upon its release by xyloglucan binding to the cellulose surface. Xyloglucan was much more rigid when bound to the hydrophobic surface than when bound to the hydrophilic surface, where binding was more disorderly and of lower energy. This computational study suggests a geometrical specificity of binding to cellulose surfaces that could be significant for the assembly of cell walls in vivo. In a similar vein, surface dehydration and hydrophobic interactions are considered important aspects of the formation and insolubility of cellulose microfibrils (Glasser et al. 2012, Medronho et al. 2012) and for binding of carbohydrate-binding modules to the hydrophobic surface of cellulose microfibrils (McLean et al. 2002, Georgelis et al. 2012). Another computational study based on coarse-grain modeling suggested that xyloglucan binding to cellulose would create tension in the polymer, i.e. tethered xyloglucans were seen to be self-tensioning (Morris et al. 2004). O’Neill and York (2003) proposed that the straightening and untwisting of xyloglucans tethered in two places would drive the polymer into a duplexed, coiled conformation. Self-tensioning and duplex formation has not been experimentally verified, but perhaps they contribute to force generation in tension wood (Baba et al. 2009). If such a self-tensioning process functioned in primary cell walls, tethers would adaptively unzip and zip (lengthen and shorten) to maintain a constant tension—an interesting concept that presents problems if xyloglucan function is to resist wall stresses originating from cell turgor pressure. Would typical wall stresses simply pull xyloglucan tethers off the cellulose surface, as occurs during single molecule AFM spectroscopy (Morris et al. 2004)? This possibility has not yet been assessed. Other physical studies indicate that xyloglucan has two apparently contradictory effects on cellulose composites in vitro: it reduces friction between cellulose surfaces while also increasing adhesion between adjacent fibril surfaces (Stiernstedt et al. 2006, Cerclier et al. 2010). These opposing effects depend on the duration of the interaction and the distances between cellulose surfaces. When xyloglucan was incorporated into bacterial composites, the material became very soft and extensible (Whitney et al. 2006); this effect was partly due to reduced friction between cellulose fibrils but mostly it was a consequence of large xyloglucan-organized domains of cellulose fibrils that could readily slip past one another. Slippage of large domains encounters less frictional resistance than nanoscale slippage of many randomly entangled fibers. These methods can reveal potential interactions that might occur in plant cell walls, but the differences in materials, structure and environment from bona fide cell walls may limit extrapolation of the conclusions to the biological realm where more organized assembly processes may dominate wall structure. Xyloglucan–Cellulose Interactions in the Primary Cell Wall We turn now to a more biological context. As described above, a long-standing view holds that xyloglucan binds tightly to 187 Y. B. Park and D. J. Cosgrove | Xyloglucan interactions in growing cell walls cellulose within the primary cell wall, coating most available cellulose surfaces, intercalating into microfibrils during their synthesis and tethering adjacent microfibrils to form the major load-bearing network in the growing cell wall. These concepts, illustrated in many depictions of the cell wall, are based upon several facts and assumptions (Hayashi 1989, Mccann et al. 1992): (i) that xyloglucan binds tightly to cellulose surfaces; (ii) that the amount of xyloglucan in primary walls is sufficient to coat most or all accessible cellulose surfaces (this statement assumes xyloglucan has a fully extended conformation throughout its length); (iii) that a large portion of xyloglucan in the cell wall is recalcitrant to extraction except under conditions that swell cellulose, e.g. 4 M NaOH; (iv) that unextracted cell walls lack available sites for binding exogenous xyloglucan; (v) that direct cellulose–cellulose contacts do not occur in primary cell walls (a common assumption, but see discussion below); and (vi) that xyloglucan forms interfibril tethers with sufficient mechanical strength to withstand the tensile forces generated by turgor pressure. We first consider the concept that xyloglucan coats cellulose microfibrils, then assess the concepts that it intercalates within microfibrils and tethers microfibrils together. Coating microfibrils Contrary to the prediction of the conventional model, 13CssNMR analyses of complex cell walls showed that surprisingly little of the cellulose microfibril surface makes contact with xyloglucan (Bootten et al. 2004, Dick-Perez et al. 2011). In the study by Bootten et al., proton spin relaxation was combined with spectrum editing to identify xyloglucans of two different mobilities in mung bean cell walls. Xyloglucans with a rigid backbone comprised 27% of the xyloglucan; the rigid xyloglucans were assumed to be bound to cellulose microfibrils, whereas the majority of the wall xyloglucan was less rigid and surrounded by mobile polysaccharides. The authors calculated that <8% of the cellulose surface was coated with xyloglucan. Dick-Perez et al. (2011) reached a similar conclusion by use of two- and three-dimensional ssNMR to detect cross-peaks (spin transfer) between cellulose and matrix polysaccharides of Arabidopsis cell walls. Extensive interactions (spin transfer) of the cellulose surface chains were observed for pectins (rhamnose and galacturonic acid residues), but not for xyloglucan. Cross-peaks between interior cellulose chains and xyloglucan were seen, suggesting that some xyloglucan may be entrapped within cellulose microfibrils. Because xyloglucan is the dominant hemicellulose in dicot primary cell walls, these studies concluded that cellulose surfaces in these growing walls are largely free of tightly bound hemicellulose. At first glance, this conclusion is perplexing. Where is all the xyloglucan in the wall, if it is not coating cellulose? If there is plenty of free cellulose surface in the wall, why doesn’t xyloglucan bind it? There is no dispute about the strong binding interaction between xyloglucan and cellulose. Studies in which fluorescently labeled xyloglucan was used to stain growing pea epicotyl cells observed extensive binding when endogenous xyloglucan was previously removed from cell wall ‘ghosts’, but found negligible staining of walls not pre-extracted to remove 188 xyloglucan (Hayashi et al. 1987). This result was interpreted to mean that most of the cellulose was natively coated with xyloglucan. Does this contradict the NMR results? The 2D and 3D ssNMR studies identified spin transfer between pectin and cellulose surfaces as well as between pectin and xyloglucan (Dick-Perez et al. 2011, Dick-Perez et al. 2012, Wang et al. 2012). Such transfer requires close proximity and relatively slow molecular motions, which is indicative of stable interactions but not necessarily tight binding. Why were xyloglucan–cellulose interactions in low abundance, given the well-documented affinity of xyloglucan for cellulose surfaces? Two factors may limit xyloglucan–cellulose interactions within the cell wall: xyloglucan selectivity for binding to the hydrophobic surface of cellulose and steric hindrance by pectins. Regarding steric hindrance, we note that the cell wall matrix is a crowded space. Pectins may physically block access to cellulose surfaces and may also interact directly with xyloglucan, limiting the ability of entangled xyloglucan chains to align to the hydrophobic surface of cellulose. Pectin content is approximately 3-fold that of xyloglucan in Arabidopsis cell walls (White et al. 2014), which is typical of many species. Hence crowding, limited diffusion and entanglement by the pectin network may kinetically limit xyloglucan access to cellulose. Additionally, as discussed above, the high-affinity binding sites for xyloglucan binding may be restricted to the hydrophobic surface, which may be a small percentage of the total cellulose surface. In contrast, cellulose surface chains identified by NMR include both the hydrophobic and hydrophilic surfaces. Xyloglucan could occupy most of the hydrophobic surfaces while still leaving the majority of cellulose surface chains without rigidly bound xyloglucan. Xyloglucans bound to the hydrophilic surfaces of cellulose are relatively mobile (Zhao et al. 2014) and may be gradually removed by the trimming action of XTH enzymes (Thompson and Fry 1997). Pectin binding, on the other hand, may be biased towards the hydrophilic surfaces (but this point has evidently not been investigated). Although pectin binds more weakly to cellulose than does xyloglucan (Zykwinska et al. 2008, Gu and Catchmark 2013), its greater abundance may result in preferential occupancy of the hydrophilic surfaces with pectin chains while at the same time sterically interfering with access by xyloglucan. An additional possibility is that interactions with pectins draw xyloglucans away from weak binding to the hydrophilic surface of cellulose. This possibility could be tested by computational approaches. The net result of all these effects would be stronger NMR cross-peaks between cellulose and pectin (Wang et al. 2012). The idea that there is sufficient xyloglucan to coat all cellulose surfaces assumes that xyloglucan has an extended shape, not the coiled shape that it has in solution (Hayashi 1989, Levy et al. 1997). What is the evidence that xyloglucan assumes a fully extended form in the wall? This concept is partly based on a questionable extrapolation of xyloglucan stiffness at the scale of its persistence length to longer scales. In addition, EM images of putative xyloglucan chains dried onto a mica surface show a highly extended shape (Mccann et al. 1992), similar to that Plant Cell Physiol. 56(2): 180–194 (2015) doi:10.1093/pcp/pcu204 observed with AFM (Morris et al. 2004). However, this extended conformation is an effect of interaction with the mica surface; conformation within the complex, hydrated cell wall may be quite different. At this point there seems to be no compelling evidence concerning xyloglucan conformation in the native wall. The fact that 38% of the xyloglucan in cell walls of pea stems could be solubilized by xyloglucan-specific endoglucanase (Pauly et al. 1999) suggests that much of the xyloglucan has an enzyme-accessible, well-solvated coil conformation. This percentage is probably an underestimate because the presence of other wall polymers reduces enzyme access to xyloglucan. Additional support for a coiled configuration comes from ssNMR studies of spin diffusion from water to cell wall polysaccharides in which xyloglucans (and pectins) were seen to be well hydrated (White et al. 2014). Xyloglucan tightly bound to cellulose would be at least partially dehydrated. When pectins were partially extracted by treatment with calcium chelator, water mobility increased and spin transfer from water to xyloglucan and to cellulose was greatly slowed. The conclusion was that the organization of water in the cell wall was controlled by pectins, which were in intimate contact with both cellulose and xyloglucan. Microfibril entrapment Several observations suggest that xyloglucans become entrapped by microfibrils during cell wall assembly: (i) extraction of xyloglucan from cell walls requires high alkaline conditions that swell cellulose, converting it to cellulose II, whereas xyloglucan that is bound to cellulose in vitro is solubilized with much lower alkaline solutions (Hayashi 1989); (ii) some xyloglucan in pea epicotyl walls was not released until the walls were completely digested by cellulase (Pauly et al. 1999); (iii) cellulose crystallinity is higher in a xyloglucan-deficient line of Arabidopsis mutant compared with the wild type (Dick-Perez et al. 2011); and (iv) NMR cross-peaks were detected between xyloglucan and internal cellulose chains (Dick-Perez et al. 2011). Xyloglucan entrapment during microfibril formation (Atalla et al. 1993) is a potential explanation of these observations. Consistent with this idea, cellulose crystallinity was reduced when cellulose-synthesizing cells of Gluconacetobacter xylinus were cultured in the presence of xyloglucan (Atalla et al. 1993, Whitney et al. 1995, Park et al. 2014). Tethering microfibrils Pauly et al. (1999) operationally defined three xyloglucan domains in cell walls from etiolated pea stems: (1) a domain that was solubilized by xyloglucan-specific endoglucanase (XEG), releasing 38% of the xyloglucan; (2) a domain solubilized by additional extraction with 4 M KOH (48% of the xyloglucan); and (3) a residual domain (14%) that was solubilized only upon digestion of the residue with cellulase. Domain (1) was assumed to comprise loops and tethers between microfibrils, forming the hypothetical load-bearing links between cellulose microfibrils. Domain (2) was considered to be xyloglucan strands tightly bound to cellulose surfaces, and domain (3) was proposed to be entrapped within or between cellulose microfibrils. The inference that cell wall strength depends on xyloglucan tethers between microfibrils was tested directly by treatment of cell walls with substrate-specific endoglucanases in combination with biomechanical assessments of the cell wall (Park and Cosgrove 2012b). Three endoglucanases from glycosyl hydrolase family 12 (www.cazy.org) were used: XEG, which digests xyloglucan but not cellulose; CEG, which cuts unbranched glucans (cellulose) but not xyloglucan, and CXEG (Cel12A), which cuts both xyloglucan and cellulose. Of the three enzymes, only CXEG loosened the cell wall, assessed by cell wall creep and wall compliances. These results showed that XEG-accessible xyloglucan did not strengthen the wall. A combined treatment with CEG and XEG might be expected to mimic the effect of CXEG, but paradoxically such treatment did not loosen the wall. Resolution of this enigma led to the ‘biomechanical hotspot’ hypothesis: a small fraction of xyloglucan is interlaced with cellulose chains, forming relatively inaccessible adhesion zones linking two or more microfibrils (Fig. 3). Efficient digestion of such a structure would require an enzyme with both xyloglucanase and cellulase activity. This requirement explains why enzymes from the XTH family do not cause cell wall creep (McQueen-Mason et al. 1993, Saladie et al. 2006) and why XTH mutants exhibit negligible growth phenotype (Kaewthai et al. 2013, Hara et al. 2014). Genetic redundancy has sometimes been invoked to account for the lack of phenotype in XTH mutants, but Kaewthai et al. (2013) showed that XTH hydrolytic activity was completely eliminated in AtXTH31/AtXTH32 double knockout lines, yet they displayed negligible growth phenotype. Substantial wall loosening by CXEG was traced to the digestion of a specific component comprising <1% of the xyloglucan in the wall, indicating that very limited sites may control wall extensibility (Park and Cosgrove 2012b). The xxt1/xxt2 mutant lacked a creep response to CXEG, indicating that xyloglucan was necessary for the formation of these biomechanical junctions (Park and Cosgrove 2012a). Moreover, CXEG treatment solubilized some pectins as well as xyloglucan from Arabidopsis walls and increased water–pectin interactions (White et al. 2014), suggesting that pectins may be connected to the biomechanical hotspots in some way, as yet undefined. Recent cell wall cartoons have depicted both xyloglucan and pectins acting as parallel tethers between microfibrils (Zykwinska et al. 2007, Dick-Perez et al. 2012). To evaluate the relative significance of pectin and xyloglucan for wall extensibility, we used enzymatic and other biochemical treatments to loosen pectins or xyloglucans selectively in Arabidopsis cell walls and measured the biomechanical consequences (Park and Cosgrove 2012a). The results indicated that treatments targeting pectin had negligible effects compared with those targeting the xyloglucan–cellulose junctions. The effects of pectin loosening, however, were notably larger in cell walls of the Arabidopsis xxt1/xxt2 line, indicating that pectins have a greater mechanical role when xyloglucan is absent. One might expect a similar situation in celery parenchyma, which contains only 2% xyloglucan (Thimm et al. 2002), but this has not been tested. A recent mathematical model of 189 Y. B. Park and D. J. Cosgrove | Xyloglucan interactions in growing cell walls Fig. 3 Biomechanical hotspot model in which cellulose microfibril contacts are mediated by a subfraction of inaccessible xyloglucans. (A) Cellulose microfibrils are depicted as rods with hydrophilic (yellow) and hydrophobic (blue) surfaces; extended xyloglucan chains (intense green beads) are found in the cellulose–cellulose junctions while coiled regions act to disperse microfibrils. Pectins are not shown. (B) Computational model of a cross-section of a junction between the hydrophobic surfaces of two cellulose microfibrils (blue) glued together through a monolayer of xyloglucan. (C) Depiction of two lamellae in a primary cell wall. The cellulose is shown as an 18 chain rectangular model with yellow hydrophilic surfaces and blue hydrophobic surfaces. Pectin chains (orange/red) fill much of the space between cellulose layers and make extensive contracts with the hydrophilic surfaces of cellulose, whereas xyloglucans (green/blue) preferentially bind to the hydrophobic surfaces of cellulose in limited regions and form coils between microfibrils. Image B adapted from Zhao et al. (2014), copyright Springer Verlag, and used with permission. growing cell walls proposed pectins to be a key determinant of extensibility in yielding cell walls (Dyson et al. 2012), but experimental assessment of this idea is needed. Control of Wall Extensibility at the Meso-Scale The biomechanical hotspot hypothesis requires that cellulose microfibrils come into close contact with each other at limited mechanical junctions. This might be via a monolayer of xyloglucan binding the hydrophobic surfaces of two microfibrils together (Fig. 3B, C). Such junctions are missing in common depictions of cell walls where microfibrils are drawn as well separated from each other and only linked via tethers. In contrast, recent AFM images of never-dried cell walls (Fig. 4) show that cellulose microfibrils do come into close lateral contact over short regions (Zhang et al. 2014). Because the walls in this AFM study were imaged under water and were never dried, artifactual aggregation that occurs during extraction and dehydration could be excluded. The idea of limited biomechanical junctions is also consistent with a low density of a-expansin 190 binding sites in the cell wall (McQueen-Mason and Cosgrove 1995). In Fig. 4 we have pictorially represented the density of expansin binding sites in the surface lamella of a primary cell wall. They are limited to a small fraction of the cell wall, although the exact spatial locations are unknown. A recent study used ssNMR to identify chemically expansin’s target in a complex cell wall (Wang et al. 2013). This is technically challenging because the low density of binding sites means the concentration of expansin in a wall sample, even at expansin saturation, is too low to detect by typical ssNMR methods. By combining 15N and 13C labeling with a sensitization method called dynamic nuclear polarization, it was possible to obtain an NMR spectrum of the polysaccharides within 13C spin-diffusion distance (1 nm) of recombinant expansin proteins bound to the cell wall. The NMR spectrum showed that the target was cellulose, but with a structure slightly different from bulk cellulose and with xyloglucan in close proximity. This characterization is remarkably similar to the hypothesized biomechanical hotspots, based on a completely different approach. These results lead to a more nuanced concept of the physical basis of cell wall extensibility. Conventional models have Plant Cell Physiol. 56(2): 180–194 (2015) doi:10.1093/pcp/pcu204 require a suite of new approaches, combining the power of genetic mutants with advances in imaging and labeling methods as well as physical characterization of the cell wall and additional approaches yet to be devised. Supplementary data Supplementary data are available at PCP online. Funding This work was supported by the US Department of Energy, Office of Science, Basic Energy Sciences as part of The Center for LignoCellulose Structure and Formation, an Energy Frontier Research Center under Award # DE-SC0001090. Fig. 4 AFM image of the recently deposited surface of an onion epidermal outer cell wall. The red ellipses illustrate the average density of a-expansin binding sites in the surface lamella, based on the binding studies of McQueen-Mason and Cosgrove (1995). The arrows indicate a few of the many regions where two microfibrils separate and come into close contact. Image credit: the AFM image is reprinted from Zhang et al. (2014), copyright Springer Verlag, and used with permission. envisaged the growing cell wall as a scaffold of cellulose microfibrils embedded in a polysaccharide matrix which acts to keep microfibrils apart and to link them via load-bearing polysaccharide tethers. For >40 years the focus has been at the molecular scale of microfibril–matrix–microfibril interactions, i.e. the nanometer scale, with the premise that the viscoelasticity of the matrix determines wall extensibility. The new model shifts focus to a larger scale and proposes that wall extensibility is controlled at limited sites where microfibrils make close contact. When these sites are loosened by the action of expansins or by CXEG-type enzymes, the microfibrils slide or separate, perhaps at a rate that is influenced by the bulk viscoelasticity of the microfibril–matrix network between biomechanical hotspots. Pectins are likely to play a major role in wall viscoelasticity. Figs. 3 and 4 graphically illustrate some of the key concepts of primary cell wall structure that probably impact cell wall extensibility. Perspective and Future Directions The ideas summarized above leave many questions for future inquiry. How are the biomechanical junctions formed? What is their structure and lifetime? Do non-crystalline or crystalline regions of the cellulose microfibril take part in junction formation? Is there more than one kind of such site in the wall? What is the relative significance of yielding by bulk wall viscoelasticity vs. yielding at the biomechanical junctions for wall extensibility and control of cell growth? The answers to these questions will Disclosures The authors have no conflicts of interest to declare. References Armstrong, J.K., Wenby, R.B., Meiselman, H.J. and Fisher, T.C. (2004) The hydrodynamic radii of macromolecules and their effect on red blood cell aggregation. Biophys. 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