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# Simulations suggest a constrictive force is required for Gram-negative bacterial cell division

## Abstract

To divide, Gram-negative bacterial cells must remodel cell wall at the division site. It remains debated, however, whether this cell wall remodeling alone can drive membrane constriction, or if a constrictive force from the tubulin homolog FtsZ is required. Previously, we constructed software (REMODELER 1) to simulate cell wall remodeling during growth. Here, we expanded this software to explore cell wall division (REMODELER 2). We found that simply organizing cell wall synthesis complexes at the midcell is not sufficient to cause invagination, even with the implementation of a make-before-break mechanism, in which new hoops of cell wall are made inside the existing hoops before bonds are cleaved. Division can occur, however, when a constrictive force brings the midcell into a compressed state before new hoops of relaxed cell wall are incorporated between existing hoops. Adding a make-before-break mechanism drives division with a smaller constrictive force sufficient to bring the midcell into a relaxed, but not necessarily compressed, state.

## Introduction

Bacterial cells are protected from turgor pressure by a peptidoglycan (PG) cell wall that is composed of long glycan strands crosslinked by short peptides1. This relatively rigid sacculus allows cells to adopt specialized shapes, such as the rod shape of many Gram-negative bacteria. In order for the cell to change size or shape during growth and division, the pressurized sacculus must be carefully remodeled. This is accomplished by a set of cell wall remodeling enzymes including transglycosylases, transpeptidases, and endopeptidases. Experimental insights into the exact molecular mechanisms of these remodeling enzymes and how their functions are coordinated remain limited. Previously, we gained insight into these questions by building simulation software, REMODELER 1, to study cell wall synthesis during cell elongation2. In this software, a cylindrical cell wall is coarse-grained as chains of tetrasaccharide beads running circumferentially around the cylinder and connected by peptide crosslinks. The functions of transglycosylases, transpeptidases, and endopeptidases are explicitly modeled as beads. Using this software, we found that in order to maintain the integrity and rod shape of the cell, these remodeling enzymes have to coordinate with one another locally in synthetic complexes, but that no long-range coordination of the independent complexes is required. We also found that these complexes must contain a lytic transglycosylase to remove long, uncrosslinked glycan tails to clear the path for enzyme movement2. (Such an enzyme was independently identified experimentally3.) How cells set their diameter over thousands of generations remains unclear, however. A recent study reported that the activities of the Rod system composed of RodA, class B penicillin-binding proteins (PBPs), and MreBCD reduce the diameter, while those of class A PBPs have the opposite effect4. It will be interesting to learn the molecular mechanisms of these two diameter-changing strategies and whether they alone set the cell diameter.

During cell elongation, the diameter of a rod-shaped cell is conserved. In contrast, during division, the diameter of the cell wall at the division site must become smaller and smaller. How the cell overcomes turgor pressure to remodel its cell wall to a smaller diameter remains unclear5. It is unlikely to be due to a fundamentally different mode of synthesis, since (a) partially overlapping and homologous sets of enzymes mediate remodeling in cell growth and division6; (b) these PG synthesis enzymes were shown to move around the cell’s circumference during both elongation7,8 and division9,10; and (c) in purified sacculi, glycan strands exhibit similar circumferential orientation throughout the length of the cell11,12.

The protein FtsZ, a tubulin homolog found in nearly all bacteria and many archaea, forms filaments at the midcell during cell division13,14,15,16. It has been proposed that these filaments exert a constrictive force on the membrane and serve as a scaffold for the cell wall synthesis machinery17. Based on cryo-electron microscopy images of dividing cells, it has been proposed that GTP-hydrolyzing FtsZ filaments can generate a constrictive force either by switching conformation from straight to curved14 or by overlapping to form a closed ring, which then tightens to constrict the membrane15. Alternatively, a recent study posited that FtsZ simply serves as a scaffold and that the constrictive force on the membrane is provided by the inward growing cell wall18. This model was suggested by the observation that the rate of inward cell wall growth is limited by the rate of cell wall synthesis, but not by the GTP hydrolysis rate of FtsZ.

In order to explore these different conceptual models, we modified our simulation software for the Gram-negative bacterial cell wall, REMODELER 1, to create REMODELER 2, which allowed us to test different mechanistic hypotheses of how inward cell wall growth might occur during division. We found that simply restricting the enzyme complexes to the midcell results in elongation without constriction, even with a make-before-break mechanism of PG remodeling, suggesting that cell wall growth alone is not sufficient to drive Gram-negative bacterial cell division. We found that a constrictive force at the midcell results in cell wall division when the force is sufficiently large to initially constrict the midcell past the diameter of the unpressurized sacculus. If the constrictive force is slightly less, sufficient to constrict the midcell sacculus into a relaxed state, the addition of a make-before-break mechanism is now effective in facilitating division. These results are summarized in Supplementary Movie 1. Due to the difficulty of describing dynamic three-dimensional (3D) processes in words and static images, we recommend readers watch the movie in full before proceeding.

## Results

### Cell wall synthesis at the midcell

To adapt REMODELER 12 into REMODELER 2 to study cell division, we added several features: (1) PG synthesis complexes were organized at the midcell, (2) a constrictive force could be implemented, and (3) the enzymes could build a multi-layered cell wall.

### PG remodeling under a constrictive force

Since FtsZ filaments have been proposed to exert a constrictive force on the membrane, we implemented a constrictive force at the midcell to see if this allowed new PG to be incorporated in smaller hoops at the constriction site (see section “Methods/Constriction force”). Initially, the constrictive force made the midcell smaller before new PG was inserted (Fig. 2a). As new PG was inserted, further reduction of the midcell radius did not occur if Fc, the constrictive force divided by the sacculus circumference, was smaller than 20 pN/nm (Fig. 2b, d). The midcell did continue to reduce in size if Fc was larger than 20 pN/nm (Fig. 2c, d). We found that at the transition point Fc ~20pN/nm, the force initially constricted the midcell into a relaxed state where its radius was equivalent to that of an unpressurized cell, 127.5 nm (Fig. 2e). Therefore, a constrictive force alone can drive division if it is sufficiently large to initially bring the midcell into a compressed state, that is, reduce the midcell radius to less than that of a relaxed sacculus. Note also that our findings were limited to Fc less than ~32 pN/nm since a larger force buckled the cell wall, making the simulation unstable. We speculate that such a buckling force scales with turgor pressure and cell radius.

### PG remodeling under a make-before-break mechanism

Next, we explored if and how cell wall growth alone could be sufficient to drive cell division without the presence of a constriction force. Conceptually, this can occur with a make-before-break mechanism, in which the cell wall synthesis machinery adds one or several new PG layers that form a temporary septum underneath the existing PG layer (make) before hydrolases cleave the constraining peptide crosslinks above these new PG layers (break). If many layers are built in before any bond on the surface is hydrolyzed, the hoops of PG in the inner layer can potentially be made from fewer PG beads. While it is clear that Gram-positive bacteria divide by making a thick septum across the width of the cell, it has only recently been speculated that Gram-negative bacteria might also adopt this septation scheme, but with a thinner septum23. (For clarity, we use septum here to refer to the new PG layers beneath, but not including, the existing layer.) Upon examining our electron cryotomograms of dividing cells (see section “Can Gram-negative bacteria divide by a septation mechanism” for details), however, we concluded that if a thin septum exists at the dividing midcell, it must be thinner than ~4 nm, the resolution of the electron cryotomograms24. Accordingly, in our simulations, we limited septum thickness to one layer of PG and our findings are therefore limited to this assumption.

We simulated a make-before-break mechanism by decoupling PG synthesis (transglycosylation and transpeptidation) from PG hydrolysis (endopeptidation). Specifically, cleavage of existing peptide crosslinks was blocked until complete hoops of new glycan strands were crosslinked into the PG network underneath these crosslinks (Fig. 4a–d). Note that how this might occur at a molecular level remains unclear. The rate of endopeptidases was controlled so that only about one layer of new PG was present underneath the existing layer (see section “Methods/Make-before-break mechanism”). To mimic the volume exclusion effect between the outer and inner layers, before existing peptide crosslinks were cleaved, a repulsive force between these crosslinks and the new glycan strands was applied to separate them to a distance of ds = 2 nm, the estimated thickness of one PG layer. To study the effect of the make-before-break mechanism alone, we did not apply a constrictive force.

Since cell expansion due to turgor pressure varies with cell size (Supplementary Figure 4A), the difference in radius of the cell wall Δr between a relaxed cell and a pressurized cell can be negligible for cells of sufficiently small sizes. For example, for cells with circumference of fewer than 150 tetrasaccharides (corresponding to a diameter of ~100 nm), Δr would be smaller than ds = 2 nm, which is the assumed thickness of one PG layer (Supplementary Figure 4B). In this case, a make-before-break mechanism could plausibly drive division in the absence of a constrictive force. In addition to cell width, turgor pressure may vary between cells. While most studies report turgor pressure in the range of 2–4 atm in Gram-negative bacteria25,26,27, a turgor pressure as low as 0.3 atm has been reported28. At this low turgor pressure, cells of circumference smaller than 300 tetrasaccharides would expand <2 nm in radius (Supplementary Figure 4B). Still, for a make-before-break mechanism to be effective in a cell the size of an Escherichia coli (~1500 tetrasaccharides in circumference), the turgor pressure would need to be on the order of 0.03 atm to make the radius expansion negligible (Supplementary Figure 4C).

### Make-before-break in the presence of a constrictive force

Our observations suggested that in order for the make-before-break PG remodeling mechanism to be effective in constriction, the midcell must be in a relaxed state. We reasoned that a constrictive force squeezing the midcell could create this condition by restoring the gaps between adjacent peptide crosslinks at glycan breaks from ~6.2 nm to their relaxed size of ~4 nm (Fig. 6a). Implementing a constrictive force divided by circumference Fc smaller than ~20pN/nm resulted in an initial constriction that did not completely relax the midcell. Predictably, in this scenario, insertion of new PG with a make-before-break mechanism did not cause further constriction (Fig. 6c). When Fc was 20pN/nm, the midcell was completely relaxed or even squeezed to a smaller radius than the unpressurized cell (Fig. 2e). As we expected, in this condition make-before-break PG remodeling could now reduce the midcell radius (Fig. 6b, c). Note that while the constriction force alone could drive division if the magnitude of Fc was larger than 20pN/nm, reducing the midcell to a compressed state (Fig. 2e), in the presence of the make-before-break mechanism, division started to occur at Fc = 20pN/nm since reducing the midcell to a relaxed state was sufficient.

### Can Gram-negative bacteria divide by a septation mechanism

While Gram-positive bacteria divide by building a septum across the cell, septation was observed in Gram-negative bacteria only when the cells were in abnormal conditions29,30. Erickson23 speculated, however, that it is possible for Gram-negative bacteria to cheat turgor pressure and build a temporary septum if the periplasm and cytoplasm are iso-osmolar23. Based on published electron tomograms of dividing Gram-negative bacteria, the author suggested such a septum might be built while hydrolases actively degrade outer layers of the advancing septum, keeping it thin. To determine if such a septum exists in dividing Gram-negative bacterial cells, we carefully examined 3D electron cryotomograms collected in our lab of intact frozen-hydrated cells of six species: Caulobacter crescentus, Escherichia coli, Proteus mirabilis, Myxococcus xanthus, Cupriavidus necator, and Shewanella oneidensis. In all cases, we could not discern any thickening of the wall at the dividing midcell that might indicate the existence of a thin septum (Fig. 7a; Supplementary Figure 5). We also observed that the distance between the inner and outer membranes remained constant throughout the midcell (Fig. 7b). We therefore concluded that if a thin septum exists at the dividing midcell, it must be thinner than ~4 nm, the resolution of the electron cryotomograms24.

## Discussion

Together, our results demonstrate how 3D modeling of molecular details can provide insights into complex symmetry-breaking processes such as cell division. By simulating how rod-shaped Gram-negative bacteria could divide their cell walls, and within the assumptions of our model, we found that a constrictive force is the key factor driving constriction, while cell wall remodeling by a make-before-break mechanism can only facilitate the process. Our work advances understanding of how the molecular consequences of the make-before-break idea play out on a large scale, beyond individual glycan strands as originally described31,32.

Many factors involved in cell division remain unknown, however, and our model is a simple coarse-grained model that does not represent any particular bacterial species. It is a theoretical, simplified construct meant to explore the fundamental mechanistics ideas in the field. Future experiments will surely further clarify the situation. For example, the PG synthesis mode during cell division and that during cell elongation might be completely different, resulting in different architectures of cell wall, for example, different glycan strand length distributions. While the two major bifunctional transglycosylase/transpeptidase enzymes PBP1A and PBP1B of E. coli showed some overlapping roles33, the two monofunctional transpeptidases PBP2 and PBP3 (also known as FtsI), which are essential for cell elongation and cell division, respectively, are likely part of two different complexes, namely, an MreB-associated PG synthesis complex34 and an FtsZ-associated PG synthesis complex10. While during cell elongation, the circumferential movement of MreB was shown to be driven by PG synthesis and dependent on the activities of PBP235, during cell division, the speed of PBP3 was shown to depend on the treadmilling rate of FtsZ10.

To decrease the radius of the midcell, the cell needs to add smaller and smaller hoops of new PG. Conceptually, this can occur by at least three mechanisms. (1) Because existing PG hoops are stretched by turgor pressure, if by some unknown force new PG hoops are stretched even further at the time they are incorporated between existing hoops, the new hoops would have fewer PG beads and therefore become smaller as the system relaxes. (2) If a mechanism exists to initially compress existing hoops at the midcell to become even smaller than relaxed hoops and new, relaxed PG hoops are incorporated between these existing hoops, the new hoops would have fewer beads and remain small once the compressing force terminated. (3) If a mechanism exists to initially relax existing hoops at the midcell and new, also relaxed, PG hoops are made inside (at smaller radius—i.e., make-before-break) existing PG hoops, the new hoops would again have fewer beads. Note that in all three models, new PG and old PG are brought to a similar stretching degree before the former is inserted into the wall. Here we showed that Model 2 is plausible with a constriction force alone and Model 3 is plausible with a combination of a constriction force and a make-before-break mechanism. We did not simulate Model 1 as we judge it unlikely to occur in real cells. Nevertheless, we cannot currently rule out the possibility that an unknown force pulls the enzymes forward, stretching the new glycan strands before incorporating them. Such a PG pre-stretching mechanism would enable cell division with a much smaller constrictive force36 or in a combination with a make-before-break mechanism perhaps render a constrictive force unnecessary. Likewise, we cannot rule out the possibility that cells might divide by a completely different mechanism that has not yet been discussed in the literature. For example, while FtsZ treadmilling has been speculated to help distribute cell wall material evenly around the cell’s circumference9,10, such a directional movement of long filaments might cause constriction in an unknown mechanism.

What is the role of a constrictive force? FtsZ filaments have been shown to be able to constrict liposomes37, but it is unclear if they exert a constrictive force on the membrane in vivo and if this force is required for cell division. Here we found in silico that to make new PG hoops smaller than existing hoops, the midcell needs to be initially constricted to at least a relaxed state, with further constriction occurring only after new PG is inserted. In this model, the constriction rate is limited by the slower of either the force generator (presumably FtsZ) or the PG synthesis rate. Therefore, the finding by Coltharp et al.18 that the inward growth rate of the cell wall is limited by the rate of PG synthesis, but did not change even when the GTP hydrolysis rate of FtsZ was reduced 90%, might simply reflect that the PG synthesis rate is much slower than the action of FtsZ. Indeed, it has been reported that an FtsZ mutant with a GTP hydrolysis rate 3% that of wild-type FtsZ resulted in very slow growth of colonies38.

In our model, the total initial constriction force needed to be at least ~15 nN (corresponding to a force divided by circumference Fc ~20pN/nm) to enable cell wall division. Assuming that the constrictive force is generated by FtsZ, each monomer of which has been estimated by molecular dynamics simulations to generate 30 pN39, our estimated force is equivalent to the action of 500 FtsZ monomers, which could form a continuous filament ~2.2 μm long or 15 filaments of an average length of 150 nm. This is reasonable, considering an estimated ~5000–7000 FtsZ molecules per cell measured in E. coli17 and the fact that our simulated sacculus is a third the size of an E. coli cell. Note that it has recently been speculated that excess membrane synthesis might also generate a constrictive force5.

Can cell wall growth alone drive constriction? While cell wall growth has been speculated to partially or primarily drive constriction during cell division18,21, our simulations showed that cell wall growth via a make-before-break mechanism failed to cause cell division in the absence of a constriction force. We found that for the make-before-break mechanism to have an effect, the new PG hoops must be made inside relaxed existing hoops and therefore a constriction force is needed to initially relax the midcell. In theory, the need for a constriction force could be bypassed if the enzymes could make a multi-layered septum. Once the septum thickness was equal to or larger than the difference in radius between the pressurized cell and the relaxed cell, the innermost layer of the septum would be in a relaxed state, allowing the next PG layer to be made of hoops containing fewer PG beads (Supplementary Figure 6). For this scenario to occur, in the case of our modeled cell wall, which had a radius of 127.5 nm when relaxed and 137.5 nm when pressurized, the septum would have to contain at least five PG layers (assuming each layer is 2 nm thick). By this logic, a cell the size of an E. coli, whose circumference is ~1500 tetrasaccharides, would need a septum ~65 nm thick for this mechanism to drive division (Supplementary Figure 4A–B). However, we saw no such septa in our electron cryotomograms of dividing cells. We therefore think it unlikely that this mechanism is the primary driver of cell division.

## Methods

### Simulation of cell wall synthesis

Here we only briefly describe our simulation system. For a more detailed description, please see our previous papers2,40. The source code of our simulations is provided with the manuscript as Supplementary Software.

### Cell wall

$$F(x) = k_{\mathrm{WLC}}\left[ {\frac{{L_{\mathrm{c}} - x_0}}{{4\left\{ {1 - \left( {x - x_0} \right)/\left( {L_{\mathrm{c}} - x_0} \right)} \right\}^2}} - \frac{{L_{\mathrm{c}} - x_0}}{4} + x - x_0} \right],$$
(1)

where Lc = 4.8 nm is the contour length of the peptide crosslink and kWLC = 15.0 pN/nm is the force constant.

To build the initial cell wall cylinder, glycan strands were placed along circumferential hoops of the same radius, then opposing peptides on adjacent hoops were connected to form crosslinks40. Previously, in order to reduce the computational cost, most of our simulations started with a small sacculus with a circumference composed of 100 tetrasaccharides2. In the current simulations, to allow the midcell radius to constrict over time, we used a starting sacculus with a circumference of 400 tetrasaccharides. To reduce the computational cost, since PG remodeling only occurs at the midcell during cell division, we removed the two caps of the starting sacculus and built a cylinder only 40 glycan hoops wide.

### PG remodeling enzymes

One endopeptidase exists in each enzyme complex to cleave existing peptide crosslinks. In our previous simulations, when an endopeptidase diffused across a crosslink, the enzyme cleaved the crosslink with a probability of 0.1. To speed up our current simulations, every 10 time steps, if the distance from the endopeptidase to a crosslink is within 3.0 nm, the enzyme captures then cleaves the crosslink. If there are multiple crosslinks within this reaction distance, the probability of crosslink i being chosen is calculated as

$$P_i = \frac{{1/d_i^2}}{{\mathop {\sum }\nolimits^ 1/d_i^2}},$$
(2)

where di is the distance from the endopeptidase to crosslink i.

There are three transpeptidases in each complex, one crosslinking the two new strands to one another and the other two crosslinking the pair to the existing network (Supplementary Figure 1). Previously, the probability of a transpeptidase capturing a peptide of a PG bead at a distance d was given as Ptp = (1 − d/d0)2, where d0 = 2.0 nm was the reaction distance. To speed up the current simulations, d0 is increased to 3.0 nm. Note that increasing the modeled rates of the enzymes did not change the principles driving cell wall remodeling in our simulations.

To constrain the enzymes into a complex, they were tethered such that a force, Fez = −kez(dez − D0), was applied to draw two enzymes closer together if their distance dez became larger than D0 = 1.0 nm. The force constant was chosen to be kez = 10 pN/nm. Since in real cells, enzymes are in the periplasm, we introduced a force normal to the surface, Fsurf = − ksurf(ds − ds0), on an enzyme if it moved a distance ds larger than ds0 = 3.0 nm away from the surface. The force constant ksurf was chosen as 500 pN/nm.

To model enzyme diffusion, a random force was applied to each enzyme every time step. Using the Box–Muller transformation45, two random numbers from a Gaussian distribution were generated as:

$$r_1 = {\mathrm{cos}}\left( {2\pi u_2} \right)\sqrt { - 2\,{\mathrm{ln}}\left( {u_1} \right)}$$
(3)

and

$$r_2 = {\mathrm{sin}}\left( {2\pi u_2} \right)\sqrt { - 2\,\mathrm{ln}\left( {u_1} \right)},$$
(4)

where u1 and u2 are two random numbers from a uniform 0–1 distribution. For N enzymes, 3N Gaussian random numbers were generated and then scaled by a force constant of 500 pN to obtain 3N Cartesian components of the random forces.

### Turgor pressure

To calculate the effect of turgor pressure, we first calculated the volume V enclosed by the pressurized sacculus. To do this, the surface of the sacculus was divided into a series of polygons whose vertices were at positions of the PG beads. Each polygon was further divided into a set of triangles, and each triangle together with the center point of the sacculus formed a tetrahedron40. In the end, the sum of the tetrahedrons’ total volume $$V = \sum V_{i}$$, where Vi was the volume of tetrahedron i.

The force on the sacculus was then calculated as Ftg = −Evol, where Evol = −PtgV is the work done by turgor pressure to inflate the sacculus. Specifically, the force on bead j was calculated as following:

$$F_j = P_{\mathrm{tg}}{\sum} {\nabla _jV_i}.$$
(5)

As in our previous simulations, turgor pressure was chosen to be Ptg = 3.0 atm.

### Constriction force

When a constriction force is applied at the midcell, it creates an inward pressure Pc satisfying

$$F_{\mathrm{c}} = {\int} {P_{\mathrm{c}}{\mathrm{d}}x_{\mathrm{m}}},$$
(6)

where Fc is the constriction force divided by the circumference and xm is the distance from the midcell. To model the force, if the absolute value of xm is <50 nm, a constriction pressure $$P_{\mathrm{c}}(x_{\mathrm{m}}) = P_0{\mathrm{e}}^{ - x_{\mathrm{m}}^2/\sigma ^2}$$ is applied, where σ = 10 nm and P0 is calculated using the following equation:

$$P_0 = \frac{{F_{\mathrm{c}}}}{{{\int} {{\mathrm{e}}^{ - x_{\mathrm{m}}^2/\sigma ^2}} {\mathrm{d}}x_{\mathrm{m}}}}.$$
(7)

### Make-before-break mechanism

To implement the make-before-break mechanism, existing peptide crosslinks are marked as “constraining crosslinks” once new glycan strands are formed underneath the crosslinks. Cleavage of a constraining crosslink is delayed for 106 time steps. After that, cleavage can occur by four scenarios: (a) an endopeptidase is within 2 nm of the constraining crosslink, (b) two PG layers exist beneath the crosslink, (c) a random cleavage with a probability of once every 107 time steps, or (d) the constraining crosslink has existed for 109 time steps. We found that these probabilities resulted in a septum ~1 PG layer thick.

In real cells, different PG layers would be separated due to the volume exclusion effect. To mimic this effect in our model, if a glycan strand is underneath a constraining crosslink and their separation d is less than the thickness of one PG layer ds = 2.0 nm, a repulsive force Fr = kr(ds − d) is exerted on the crosslink and the two PG beads that are closest to the crosslink, where the force constant kr was arbitrarily chosen to be 200 pN/nm.

### Langevin dynamics

The system was evolved using Langevin dynamics such that coordinate X(t) of a bead of mass m and interaction potential U was calculated as

$$m\frac{{{\mathrm{d}}^2X}}{{{\mathrm{d}}t^2}} = - \nabla U\left( X \right) - \gamma \frac{{{\mathrm{d}}X}}{{{\mathrm{d}}t}} + R(t),$$
(8)

where γ is damping constant and R the random force on the bead. For simplicity, we assumed the inertia of the bead was negligible, making the displacement dX a linear function of the total force Ftot on the bead as

$${\mathrm{d}}X = \frac{1}{\gamma }\left[ { - \nabla U\left( X \right) + R} \right]{\mathrm{d}}t = \frac{1}{\gamma }F_{{\mathrm{tot}}}{\mathrm{d}}t.$$
(9)

To prevent system instability, the maximum displacement of the PG beads, which corresponds to the maximum force Fmax, was set to be dmax = 0.01 nm. Displacement of bead i was then calculated as

$$d_i = d_{{\mathrm{max}}}\frac{{\gamma _{{\mathrm{max}}}F_{{\mathrm{tot}}}^i}}{{\gamma _iF_{{\mathrm{max}}}}}.$$
(10)

### Electron cryotomography

Bacterial strains were grown and imaged as described: Caulobacter crescentus16; Escherichia coli46; Myxococcus xanthus47; Cupriavidus necator48; Shewanella oneidensis49.

### Measurement of the distance between the inner and outer membranes

A tomographic slice 10 nm thick through a central plane along the long axis of the cell was captured using the IMOD software50. Each membrane (inner and outer) was manually traced and represented by a set of points evenly spaced along the line. This process was repeated for the membranes on the opposite side of the cell. The location of the midcell was determined by the shortest distance between the two traces of the inner membrane. The distance between the inner and outer membrane on each side was then calculated for points up to 500 nm from the midcell in both directions.

### Reporting summary

Further information on experimental design is available in the Nature Research Reporting Summary linked to this article.

## Code availability

The source code of our simulations is provided as Supplementary Software.

## Data availability

The data supporting the findings of this study are available within the paper and its Supplementary Information files.

Journal peer review information: Nature Communications thanks the anonymous reviewer(s) for their contribution to the peer review of this work. Peer reviewer reports are available.

Publisher’s note: Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.

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## Acknowledgements

We thank Martin Pilhofer for sharing the electron cryotomogram of an E. coli cell shown in Fig. 4, Debnath Ghosal for helpful discussions, and Andrew Jewett for assisting with membrane-tracing software. This work was supported by the National Institutes of Health (grant R35 GM122588 to G.J.J.).

## Author information

L.T.N. designed and ran simulations and wrote the manuscript. C.M.O. wrote the manuscript. H.J.D. ran simulations and did analysis of electron cryotomograms. M.K., Q.Y., Y.-W.C. and M.B. performed electron cryotomography. G.J.J. designed simulations and wrote the manuscript.

### Competing interests

The authors declare no competing interests.

Correspondence to Grant J. Jensen.