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Cell morphology drives spatial patterning in microbial communities William P. J. Smitha, Yohan Davitb, James M. Osbornec, Wook Kimd,1, Kevin R. Fosterd,2, and Joe M. Pitt-Francisa,2

aDepartment of Computer Science, University of Oxford, Oxford OX1 3QD, United Kingdom; bInstitut de Mecanique´ des Fluides de Toulouse (IMFT), Universite´ de Toulouse, Centre National de la Recherche Scientifique (CNRS), Institut National Polytechnique de Toulouse (INPT), Universite´ Paul Sabatier (UPS), F-31400 Toulouse, France; cSchool of Mathematics and Statistics, University of Melbourne, VIC 3010, Australia; and dDepartment of , University of Oxford, Oxford OX1 3PS, United Kingdom

Edited by Roman Stocker, Eidgenossische¨ Technische Hochschule Zurich,¨ Zurich, Switzerland, and accepted by Editorial Board Member Edward F. DeLong November 15, 2016 (received for review August 5, 2016) The clearest phenotypic characteristic of microbial cells is their cells and surfaces (20, 21). The resulting orientational order shape, but we do not understand how cell shape affects the affects how cell groups expand in microfluidic channels and dense communities, known as biofilms, where many microbes enables motile cells to swarm together in raft-like collectives live. Here, we use individual-based modeling to systematically (22, 23). Aligned cells are also subject to buckling interactions, vary cell shape and study its impact in simulated communities. which fold neighboring cell groups into one another to form We compete cells with different cell morphologies under a range fractal-like interdigitations (21, 24), and differences in cell sizes of conditions and ask how shape affects the patterning and evo- may drive depletion effects that lead to genetic demixing (25). lutionary fitness of cells within a community. Our models predict These studies suggest that, by influencing biomechanical inter- that cell shape will strongly influence the fate of a cell lineage: actions between microbes, shape may have far-reaching con- we describe a mechanism through which coccal (round) cells rise sequences for the properties and prospects of a cell within a to the upper surface of a community, leading to a strong spatial community. structuring that can be critical for fitness. We test our predictions Individual-based modeling has emerged as a powerful way to experimentally using strains of Escherichia coli that grow at a sim- study biofilms. These models serve as a testing ground to study ilar rate but differ in cell shape due to single amino acid changes how phenotypes, including adhesion, antibiotics, and extracel- in the actin homolog MreB. As predicted by our model, cell types lular polymeric substances (EPSs), affect individual strains and strongly sort by shape, with round cells at the top of the colony biofilms as a whole (26–31). However, the majority of individual- and rod cells dominating the basal surface and edges. Our work based models do not allow cell shape to be altered (32). We have suggests that cell morphology has a strong impact within micro- therefore developed a flexible simulation framework that allows bial communities and may offer new ways to engineer the struc- us to incorporate cell shape alongside cell division, physical inter- ture of synthetic communities. actions, and metabolic interactions via nutrient consumption. Our analyses identify a mechanism by which different cell shapes biofilms | cell morphology | biophysics | self-organization | can self-organize into layered structures, thereby providing par- synthetic ticular genotypes with preferential access to favorable positions in the biofilm. We test our model predictions with experiments ingle-celled such as bacteria display signif- in which mutant Escherichia coli strains of different shapes are Sicant morphological diversity, ranging from the simple to the complex and exotic (1–3). Phylogenetic studies indicate that Significance particular morphologies have evolved independently multiple times, suggesting that the myriad shapes of modern bacteria may be adaptations to particular environments (4–6). Microbes can Microbial communities contain cells of different shapes, and also actively change their morphology in response to environ- yet we know little about how these shapes affect community mental stimuli, such as changes to nutrient levels or predation biology. We have developed a computational model to study (7, 8). However, understanding when and why particular cell the effects of microbial shape in communities. Our model shapes offer a competitive edge remains an unresolved question predicts that shape will have strong effects on cells’ posi- in microbiology. tioning, and, consequently, their survival and reproduction. Previous studies have characterized selective pressures favor- Rod-shaped cells are better at colonizing the base of the com- ing particular shapes (7, 9–11): for example, highly viscous envi- munity and its expanding edges, whereas round cells dom- ronments may select for the helical cell morphologies observed inate the upper surface. We show that the same patterns in spirochete bacteria (12). Thus far, these studies have predom- occur in colonies of Escherichia coli, using strains with dif- inantly focused on selective pressures acting at the level of the ferent shapes. Our work suggests that cell shape is a major individual cell. However, many live in dense, surface- determinant of patterning and evolutionary fitness within associated communities known as biofilms, which are fundamen- microbial communities. tal to the biology of microbes and how they affect us—playing major roles in the microbiome, chronic diseases, antibi- Author contributions: W.P.J.S., Y.D., J.M.O., K.R.F., and J.M.P.-F. designed research; W.P.J.S. and W.K. performed research; W.P.J.S., Y.D., J.M.O., W.K., K.R.F., and J.M.P.-F. analyzed otic resistance, biofouling, and waste-water treatment (13–17). data; and W.P.J.S., Y.D., J.M.O., W.K., K.R.F., and J.M.P.-F. wrote the paper. As a result, there has been an intensive effort in recent years to The authors declare no conflict of interest. understand how the biofilm mode of growth affects microbes and This article is a PNAS Direct Submission. R.S. is a Guest Editor invited by the Editorial their (18, 19), but we know very little of the importance Board. of cell shape for biofilm biology. 1Present address: Department of Biological Sciences, Duquesne University, Pittsburgh, PA In biofilms, microbial cells are often in close physical con- 15282. tact, making mechanical interactions between neighboring cells 2To whom correspondence may be addressed. Email: [email protected] or particularly significant. Recent studies have suggested that rod- [email protected]. shaped cells can drive collective behaviors in microbial groups This article contains supporting information online at www.pnas.org/lookup/suppl/doi:10. because of their tendency to align their orientations with nearby 1073/pnas.1613007114/-/DCSupplemental.

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MICROBIOLOGY BIOPHYSICS AND PNAS PLUS Fig. 3. Cell morphology influences strain fitness within colonies. (A) Competition between different cell shapes is simulated by growing biofilm sections under nutrient-limited conditions. Nutrients are supplied either from above the colony (first row) or from below (second row). Cells on the left side of the colony are colored by their growth rate, showing that rapid cellular growth is limited to a thin layer at the top or at the base of the colony, in the two scenarios, respectively. Contours on the nutrient field (background) correspond to u/u0 = 0.25, 0.50 and 0.75. (B) Volume-weighted histograms (P(z)) of cell heights in nutrient-limited SL colonies show similar layering effects to those created under homogeneous growth conditions, with S cells (red) growing atop L cells (blue). (C) Bar plots of strain fitness show that coccal morphologies outcompete rod-like morphologies in scenarios where nutrients are delivered from above the colony, but the reverse is true when nutrients are delivered from below. There were 10 simulations per case.

vertical strain distributions seen in SS and LL control colonies Shape-Driven Layering Alters Strain Fitness. Next, we examined are identical, confirming the absence of layering. This effect can the consequences of layering phenomena on strain competition be reproduced in 3D simulations, where cell centers and axes are within the biofilm environment. Because biofilms are typically not confined to the xz plane (Fig. 2 B and C). characterized as highly heterogeneous environments, systematic In SI Appendix, we discuss further simulations carried differences in the positioning of bacterial strains could lead to out to interrogate the mechanism of the layering effect (SI significant differences in their fitness, offering a competitive Appendix, Figs. S1–S7 and Movie S2). We hypothesize that advantage to particular cell morphotypes (39–41). layering occurs because groups of rod-shaped cells form wedge- To examine this hypothesis, we repeated our 2D and 3D like structures, which, guided by the basal surface, collectively biofilm growth simulations under nutrient-limited conditions. burrow beneath groups of coccal cells. The necessary group Instead of allowing all cells to grow at the same rate as before, structure is, in turn, produced by steric interactions between we coupled each cell’s growth rate µi to the local concentration neighboring cells and the basal surface, which produce nematic u of a rate-limiting nutrient field, evaluated at that cell’s centroid ordering in rod-shaped cells but not in coccal cells. pi . As in previous studies (26, 28, 42, 43), we model this coupling We also report tests that verify that the layering effect is robust using the Monod equation µi = µmaxu(pi )/(K + u(pi )), where with respect to changes in simulation boundary conditions (SI µmax and K are the maximum specific cell growth rate and the Appendix, Fig. S9), relative cell size (SI Appendix, Fig. S7A), uptake saturation constant, respectively. By imposing different simulation parameters such as the rate of division noise injec- boundary conditions on the nutrient reaction-diffusion equation, tion (SI Appendix, Fig. S7B), and changes in initial cell align- we created opposing perfusion scenarios: one in which nutrient ment (SI Appendix, Fig. S7B). However, we find that layering is was supplied from above the colony and another in which sup- completely dependent on the presence of the basal plane, con- ply came from below. In each simulation, we measured the fit- firming its importance in the layering mechanism (SI Appendix, ness of each strain, ωstrain, by computing the number of division Fig. S7B). events per unit time, ωstrain = log2(Vstrain(tend)/Vstrain(0))/tend. Overall, these observations suggest that individual cell shape Here, Vstrain(tend) refers to the total cell volume of a strain at is capable of driving significant structural changes in the the endpoint of the simulation tend. The results of these simu- wider biofilm environment—and, in particular, that combina- lations are shown in Fig. 3. Nutrient field parameters are listed tions of differently shaped cells can drive the formation of lay- in SI Appendix, Table S3; these are chosen so as to create thin ered structures, as reported previously in multispecies biofilms growth layers of similar thicknesses in the two perfusion sce- (36–38). narios. In both cases, the Damkohler¨ number D (the ratio of

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A53K .coli E. ± µ tan:the strains: is 0.007 0. 519 h −1 ± natfc rdcdb h ursetlbln scheme. labeling fluorescent the by not is produced layering artifact that an demonstrating 5B), (Fig. pro- second result labels same the color the the by duces Reversing predicted 3. as Fig. in base, over- shown colony an scenario the modeling see at also cells we rod colony, of the growth below nutrients agar Because the colony. from the supplied in are depths increasing at taken projec- side slices from both confocal visible is of effect tions This colony. show from the (red) we cells of 5A, AK base Fig. shorter the displace In blue) cells. in longer (shown cells of WT top that on lying structures, cells layered of shorter emergence with the in result can together strains composi- edge. the colony affect the can of com- tion shape In shape cell other dimension. that for images demonstrating fractal the colony binations, lower additional in show a as we S12, with patterns Fig. fractal-like but generating case, interme- mixing, WT an of produces again column) level center column), 4, diate (Fig. LL interme- shape The cell 2, (24). AS studies diate (Fig. previous of model findings the the recapitulating interstrain in smooth seen show fractal-like interdigitations the colonies reproduce to mixtures AK-AK WT-WT Similarly whereas column), boundaries, row). (SS (bottom con- sections 2 shows and edge 4 Fig. row) colony Fig. of (top ratio. images colonies aspect focal complete cell of (red-blue) on images interstrain dependent epifluorescent (AK-AK, of strongly morphotype degree is that mixing one showed only WT-WT) of AS-AS, composed colonies in Firstly, Patterning Drives coli Morphology are Cell details Further blue. in shown in cells sig- provided fluorescence GFP-labeled the with from microscopy. pseudocolor, nal in scanning are imaged shown laser being images confocal The before and markers, flu- epifluorescence GFP red using or with labeled (RFP) strains, using protein three grown orescent these were of Colonies pairing possible comparison. each visual for strains these eetknatr4 fgot nec ae Saebr:tprw mm; 1 row, top 44. bars: ref. (Scale from case. permission with each taken in 20 growth of row, Images h bottom colonies. behavior, 48 WT after in intermediate than taken display dimension were fractal colonies lower of AS extending patterning colony. cell showing boundaries blue the group and simulations: smoother through red show our vertically between colonies (bot- of AK mixing projections predictions whereas fractal-like groups, orthogonal complex, the show corroborate alongside colonies images shown WT These are row). sec- colony edge tom each of images of confocal Inset representative (Center tions magnification, ratio higher aspect At cell rate. in differ WT which of (AK), composed colonies compares coli morphotype- row E. of top test The experimental an relationships. as patterning culture, solid in together grown are i.4. Fig. u xeiet lovrf htmxn ogadsotcell short and long mixing that verify also experiments Our ooisrpoue eea e rdcin formodel. our of predictions key several reproduced colonies ihtoeo ci ooo mutants homolog actin of those with loecnl labeled Fluorescently aeil n Methods. and Materials . hs-otatcl mgs(fwdh3.5 width (of images cell Phase-contrast µm.) o o)adfo horizontal from and row) top 5A, (Fig. z-stacks PNAS .coli E. | ulse nieDcme 0 2016 30, December online Published tan ihdfeetcl morphologies cell different with strains .coli E. mreB u rwa h same the at grow but ) A53S Colonies. A)and (AS) IAppendix, SI )were µm) mreB The | E283 A53K E.

MICROBIOLOGY BIOPHYSICS AND PNAS PLUS COMPUTATIONAL BIOLOGY Fig. 5. Mixed-morphotype colonies reproduce the layering phenomena predicted by simulations. (A) Pseudocolor confocal images show that GFP-labeled WT E. coli (shown in blue) are able to burrow beneath shorter, wider AK mutants (red), leading to the WT cells’ enrichment at the base of the colony. (B) The same is true when fluorescent labels are reversed. Images correspond to vertical colony sections (A and B, top row) and horizontal slices taken at successive depths (A and B, bottom row). (C) We quantify layering effects by measuring the volume fraction of GFP-labeled cells as a of depth in the colony, using automated image segmentation (Materials and Methods). (D) The gradients of these traces, corresponding to the percentage gain (or loss) of GFP signal per unit depth, are compared for various binary shape combinations. Cell micrographs in A, B, and D are taken with permission from ref. 44. (Scale bars: 20 µm.) Confocal images and data taken after 48 h of growth.

In Fig. 5C, we use automated image analysis to quantify the ing of the functional value of cell shape, both as a competitive layering effect. By counting the number of blue pixels in each phenotype in the biofilm context and as a means for bacteria to layer of the stack (Materials and Methods), we estimate the vol- influence their environment through collective action. ume fraction of AK (top row) or WT (bottom row) cells as a From an evolutionary perspective, our work suggests that the function of depth in the colony. These traces show an approxi- biofilm environment may select for particular cell shapes in spe- mately linear reduction in the AK cell fraction (and correspond- cific environments because of the ways in which they collec- ing increase in WT fraction) within the first 15 µm below the tively influence biofilm architecture. Given the predominance of colony surface, which is in agreement with the cell arrangements the biofilm environment for microbial (18, 19), any selective predicted in Figs. 2 and 3. effect produced might be expected to have a strong impact on the Finally, we repeated this analysis with images taken from evolution of bacterial morphology. In natural biofilms, rapid cell colonies of other morphotype combinations, including the con- growth is often limited to the upper regions of a biofilm (28, 41), trol colonies shown in Fig. 4. In each case, we quantified inter- which will select for coccal morphologies. Indeed, this selective strain layering using the average slope of the GFP fraction traces, pressure provides a rationale for morphological transitions asso- such as those shown in Fig. 5C, using linear fitting. Example ciated with biofilm development (46–48) and may partly explain image segmentations, along with the complete set of GFP frac- the ubiquity of the coccal morphology despite disadvantages, tion traces, are provided in SI Appendix, Fig. S13. The degree of such as decreased nutrient absorption area (7). layering for each type of mixture is shown in Fig. 5D. As pre- In reality, microbial communities are far more intricate dicted by the model, we observe a strong relationship between than the description used in our simulations. Like all mod- differences in cell shape and the degree of layering in the colony els, our framework makes simplifying assumptions: we deliber- across these different genotypes. Our experiments, therefore, ately neglect the role of cell motility, detachment, and shear support multiple predictions of our model (Figs. 4 and 5). More- forces from the liquid surrounding the colony (42, 43, 49). over, this support came without needing to tune conditions; Our representation of EPS secretions—a hallmark of microbial we performed the experimental tests after the modeling. This biofilms—is purely implicit, whereas the inclusion of explicit EPS observation suggests that the effects we report in this study particles has been shown to influence colony structure in previ- are robust to experimental conditions and may be common to ous studies (25, 41). Our model also neglects adhesive interac- many existing experimental systems that use mixtures of different tions, which could inhibit the layering effect if coccal cells were cell shapes. irreversibly attached to the basal surface. However, these omissions allow a degree of realism to be Discussion traded for additional control and tractability. Rather than We have used simulations and experiments to show that cell attempting to reproduce the exact dynamics of colony growth, shape can be a determinant of both spatial patterning and com- our simulations instead predict the rich dynamics that can position within a microbial community. In particular, we find emerge when nonspherical cell shapes are introduced to existing that mixtures of rod-shaped and coccal cells can produce layered modeling paradigms (28, 50). The fact that these predictions are colony structures, as observed previously in both biotic and abi- corroborated by our experiments demonstrates the usefulness of otic environments (36, 45). This result extends our understand- this approach.

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(2011) al. et P, mor- selected Vos of history 2. natural The diversity: Bacterial (1965) VBD Skerman MP, Starr 1. x ntotal, In interac- antagonistic only considers study our although Finally, and empirical further for need the highlight predictions Our iue Srne cec uiesMda odeh,TeNetherlands), The Dordrecht, Media, 601–610. Business & Science 3. Vol (Springer micutes bacteria. unusual phologically = 300 ,wees3 iuain sdacbia oanwt base with domain cuboidal a used simulations 3D whereas µm, ,0 oe iuain eepromdo w VDATesla NVIDIA two on performed were simulations model ≈3,000 L x eso httehr onayapprox- boundary hard the that show we S9, Fig. Appendix, SI = iuain eepromduig2 n Ddmis In domains. 3D and 2D using performed were Simulations L y = 40 .Smltoswr ntaie sn ninocu- an using initialized were Simulations µm. nuRvMicrobiol Rev Annu 19:407–454. a e Microbiol Rev Nat 3(8): eevdfnigfo h alv eerhCnr o vlto n Human Oxford). and Evolution College, for (Magdalen K.R.F. 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Image Confocal scan- mixed- laser inoculation, 57). confocal (41, following and described previously epifluorescence days as by microscopy Two ning imaged out. were from colonies carried reverse using culture are also experiments combina- sur- control study were each labels, the fluorescent this For labeling and glu- on volume. strains in cell between 1-µL volumes of reported difference at tion 10-µL data significant spotted or plates supplementation; no 1- glucose-supplemented observed lactose either We or plates. in cose DM spotted of then face and ratio, 1:1 plasmids. maintain 37 g 15 with (Thermo-Fisher (175 LB supplemented in (57), rpm medium 250 (DM) at 37 shaking cul- at grown routine were Scientific) For cells microscopy. liquid, confocal in and turing epifluorescence (44). for time strains phase three lag in the is marginally share A53S only strains differ and and (44). three rate morphology, protein all growth cellular Importantly, specific MreB same A53. widest the with of and compared residue shortest intermediate, acid the amino nonsynony- exhibits 53rd respective A53K the the at with mutation REL606 mous from constructed previously (REL606mreB were A53K A53. as here to referred Plasmids. and Strains Bacterial are assumptions, and equations model including in framework, provided details IbM Further 2015a. the Matlab using on out carried was results of postprocessing operation. norm and where o iuain nldn hm oacutfrtesohsi os terms criterion convergence noise the stochastic card using converged, the graphics Appendix measurements for GFX (SI account 4GB model To our K5000 in them. Quadro including NVIDIA simulations two for on and fields nutrient .Ksl T adc M acm D rnY 21)Dvriytkssae Under- shape: takes Diversity (2016) YV Brun PD, Caccamo AM, Bring- Randich DT, (2001) M Kysela Vicente A, 6. Valencia J, Mingorance M, Gonzalez-Moreno morphology. J, bacterial Tamames of mapping 5. Phylogenetic (1998) GE Fox JL, Siefert 4. vrih utrswr eilydltdi B,mxdtgte na in together mixed PBS, in diluted serially were cultures Overnight eitoue lsispaRPo mxF AaaLna noall into (Amaxa/Lonza) pmaxGFP or pmaxRFP plasmids introduced We the and 4.3.1, Paraview using checked and visualized were Simulations ogy tnigtemcaitcadaatv ai fbceilmorphology. bacterial of basis adaptive and 14(10):e1002565. mechanistic the standing shape. bacterial into order gene ing ◦  .Almdawr upeetdwt aayi t50 at kanamycin with supplemented were media All C. µg TOL 4 P 10):2803–2808. 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