Summary
In uncertain environments, phenotypic diversity can be advantageous for survival. However, as the environmental uncertainty decreases, the relative advantage of having diverse phenotypes decreases. Here, we show how populations of E. coli integrate multiple chemical signals to adjust sensory diversity in response to changes in the prevalence of each ligand in the environment. Measuring kinase activity in single cells, we quantified the sensitivity distribution to various chemoattractants in different mixtures of background stimuli. We found that when ligands bind uncompetitively, the population tunes sensory diversity to each signal independently, decreasing diversity when the signal ambient concentration increases. However, amongst competitive ligands the population can only decrease sensory diversity one ligand at a time. Mathematical modeling suggests that sensory diversity tuning benefits E. coli populations by modulating how many cells are committed to tracking each signal proportionally as their prevalence changes.
Introduction
While navigating their environments, organisms sense and respond to signals embedded in a complex backdrop of other stimuli. Behavioral decisions thus require sensory systems capable of parsing these rich signal mixtures to control subsequent responses. In fly olfaction for example, relatively few olfactory receptors (∼50) are used to encode and identify an enormous range of stimuli to drive a highly olfaction-dependent lifestyle.1-4 Similarly, many bacteria use a small set (∼3) of quorum-sensing receptors to drive the switch between biofilm and planktonic lifestyles as the ratio of signals secreted by self and other bacteria changes.5,6 In both of these cases, a downstream network – neural for the fly and transcriptional for quorum sensing – parses the integrated signals and prevents signal cross-talk.
One of the most-studied sensory systems for navigation is the chemotaxis network of Escherichia coli. In this relatively simple signaling network, five chemoreceptor species that mix within allosterically coupled signaling complexes detect many different extracellular chemicals.7 Ligand-receptor binding then modulates the activity of the kinase CheA, the sole output of the complex, which phosphorylates a response regulator CheY that controls the direction of flagellar rotation.7,8 Thus, a multitude of extracellular signals are integrated into the activity of a single kinase and downstream effectors. In these receptor-kinase complexes (Figure 1A), ligand binding at one receptor is thought to not only change the conformation of the kinase associated with that receptor, but also its neighbors, leading to amplification of the signal generated by small changes in ligand concentration.9,10
In addition to cooperative receptor clusters, the chemotaxis network includes two proteins (CheR and CheB) that post-translationally modify receptors by respectively adding and removing methyl groups, to increase or decrease their activity in a way that opposes the current state of CheA activity.7 This negative feedback allows kinase activity to precisely adapt to sustained changes in attractant concentration, returning to the same steady-state activity over a wide concentration range.7,11,12 Adaptation has been shown to only be precise in receptor clusters containing multiple receptor species.13 Additionally, transient cross-methylation of receptors in the presence of a non-cognate ligand can occur.14-16 Despite decades of study, our understanding of cooperativity, adaptation, and signal integration within chemosensory arrays comprising multiple receptor species remains far from complete. Consequently, it remains challenging to explain, let alone predict, how E. coli navigate complex environments where they encounter and adapt to many signals at the same time.
Isogenic cell populations could generate individuals with diverse sensitivity to different stimuli to hedge their bets against changes in available attractant gradients and effectively explore complex environments.17-19 Developments in single-cell fluorescence resonance energy transfer (FRET) have allowed this diversity to be probed at the signal-transduction level by measuring FRET between CheY-mRFP1 and CheZ-YFP fusions to quantify kinase activity in individual cells.20-23 These studies revealed diverse sensitivities to various attractants, and confirmed cell-to-cell variability in kinase activity fluctuation.24-26
Recently, using single-cell FRET to measure kinase activity, we discovered that the degree of cell-to-cell variation in sensitivity to an attractant strongly depends on its background concentration.27 When the background concentration of a chemoattractant is low, sensitivity to the attractant varies greatly from cell to cell. However, after the cells have adapted to a sufficiently high background of the attractant, the degree of variation in sensitivity within the clonal population is strongly attenuated. This background stimulus dependent “diversity tuning” occurs without changes in gene expression. It was hypothesized that diversity tuning could play a role in a population’s ability to switch between different navigational strategies depending on the availability of environmental cues. When the information about the environment is scarce, populations can hedge their bets by diversifying their sensitivities to stimuli. However, after detecting a sufficiently strong signal, the population can shift to a tracking strategy where each individual is tuned to the ambient signal level, and primed to detect changes from the background signal level.
The diversity-tuning phenomenon was observed for the responses to alpha-methyl-aspartate (MeAsp) and serine, cognate ligands of the two major chemoreceptors Tar and Tsr, respectively, in settings where only a single ligand species is presented to cells at a time. However, whether and how diversity tuning applies to more ecologically relevant scenarios, where multiple ligands are present simultaneously, remains unknown. Does adding one stimulus to the environment affect the ability of the population to modulate the sensitivity distribution for other stimuli? Are there different effects when the ligands presented bind the same receptor or different receptors?
We hypothesized that, due to strong cooperative interactions within the receptor cluster28, the presence of one background ligand species could affect diversity-tuning of the sensitivity to other (foreground) ligand species. To test this hypothesis, we combined microfluidics and single-cell FRET to measure the distribution of sensitivities for various foreground ligands after allowing cells to adapt to different background conditions. We further reasoned that the binding mode of the foreground and background ligands – binding different receptors, binding one receptor competitively, or binding one receptor uncompetitively – could play an important role. Accordingly, we performed experiments for all three cases.
We found that the sensitivity distributions for ligands which bind uncompetitively, whether on the same receptor or different, despite strong allosteric coupling in the receptor cluster, can be tuned independently. However, when ligands compete for binding sites, response diversity that has collapsed upon adaptation with respect to one ligand can be restored by addition of a competitive ligand to the adapted-state background. Lastly, we explore through mathematical modeling the consequences of diversity tuning on chemotactic performance during navigation and how similar diversity tuning might arise in other systems.
Results
Measuring the distribution of chemotactic response sensitivities
We set out to measure the distribution of sensitivity for one ligand species in the presence of different background ligand species. In our experimental setup, the ligand whose concentration is dynamically modulated in an experiment is called the foreground ligand, and the ligand whose concentration is fixed to a constant level is called the background ligand. Following preceding works,21,27 we defined ‘kinase activity’, a, as the relative FRET level normalized within individual cells: zero and one activity correspond to the minimum and maximum FRET level, respectively. The minimum FRET levels are observed immediately following addition of a stimulus large enough to saturate the response, and the maximum FRET is observed after removal of this stimulus. We quantified sensitivity for a foreground ligand by the K1/2, which we defined as the ligand concentration where kinase activity reached half of its steady-state value. For simplicity, we focused on ligands that bind the two highest-expressed receptors in E. coli: Tar and Tsr.7
For a given combination of foreground and background stimuli, we measured the K1/2 distribution using an extension of previous methods, where cells expressing sticky FliC (FliC*) adhered to the bottom of a microfluidic device are exposed to constant flow of stimuli dissolved in motility buffer (STAR Methods).27 We developed a microfluidic device with seven input channels (Figure 1B; Figure S1A-D) which allowed us to alternate between flows of six different stimulus solutions and a background solution over a field of immobilized cells. Each stimulus solution was presented to cells multiple times in a single experiment to reduce the statistical uncertainties originating from measurement noise and temporal variations in kinase activity by allowing within-cell averaging of the FRET responses to each stimulus (Figure 1C, D). The time to fully exchange the media in a field of view is ∼200 ms (Figure S1A-D), enabling quantification of kinase activity responses to small stimuli without the confounding effects of response adaptation, which occurs on the order of 10 seconds for sub-saturating step stimuli.22 Each foreground stimulus lasted for 5 seconds with time-lapse FRET measurements conducted every 0.5 seconds starting 5 seconds before the stimulus onset and lasting 10 seconds total. We waited 30 seconds between consecutive foreground stimuli to allow kinase activity to adapt back to its steady-state level. Cells were not imaged during these adaptation periods to minimize photobleaching. This stimulus protocol gives quasi-stationary distributions of responses over the course of an experiment (Figure S2A). Data collected from at least two biological replicates were included in each analysis to increase the number of cells per data point.
Using this experimental setup, we measured the K1/2 cumulative distribution function (CDF) for one combination of foreground and background ligands in a single experiment. The CDF of K1/2 can be extracted from the distribution of post-stimulus kinase activity normalized by its steady-state level, R (Figure S1F). As described previously, for a population of bacteria, the value of the CDF of the K1/2 is given by the fraction of responses R smaller than 0.5 (Figure S1E, F).27
Also in agreement with previous work, the K1/2 CDFs were well approximated by a lognormal distribution (Figure S2B, C).27 To quantify the variation in the magnitude of sensory diversity we use the coefficient of variation (CV) of the K1/2 distribution, which is defined as the standard deviation divided by the mean. Note that the is also monotonically related to the standard deviation of the distribution of log K1/2.
Orthogonal diversity tuning for ligands that bind different receptors
We first investigated how adaptation to a background ligand that binds one receptor species affects the K1/2 distribution for foreground ligands that bind a different receptor species (Figure 2A). Previous population-averaged FRET experiments found that prior adaptation to serine, which binds Tsr with high affinity (K1/2 ≈ 10−1µM) and Tar with low affinity (K1/2 ≈ 101µM), does not significantly affect the population-averaged K1/2 of MeAsp, which primarily binds Tar.29,30 However, at the single-cell level, whether this independence extends not only to the mean but also the variance of the K1/2 distribution remains unknown.
To address this question, we measured the K1/2 distribution for MeAsp and serine in four background conditions: no-background (plain motility buffer), 100 µM MeAsp, 1 µM serine, and a mixture of 100 µM MeAsp and 1 µM serine. These concentrations were chosen because 100 µM MeAsp and 1 µM serine were previously shown to collapse the width of MeAsp and serine K1/2 distributions respectively upon adaptation to a background of the same signals.27
We observed a broad K1/2 distribution at zero-background (CV = 0.74 ± 0.12), and adaptation to 100 µM MeAsp led to a collapse in the K1/2 diversity (CV = 0.037 ± 0.004) for MeAsp (Figures 2B; Figure S2DE). However, adaptation to 1 µM serine did not significantly affect the K1/2 distribution for MeAsp, even in the mixed background condition (Figure 2C; Figure S2FG). Similarly, while adaptation to 1 µM serine background collapses the serine K1/2 diversity (Figures 2D), adaptation to 100 µM MeAsp did not significantly affect the serine K1/2 distributions (Figures 2E; Figure S2FG).
These experiments show that in addition to maintaining the same mean sensitivity for MeAsp (serine) in the presence of serine (MeAsp), the bacterial populations also maintain the degree of variability in sensitivity. As such, even though receptor clusters inside individual cells comprise a mixture of receptor species that signal cooperatively, populations of E. coli can independently tune the K1/2 distributions for ligands that bind different receptor species.10,16,31
Diversity tuning when ligands bind the same receptor
Having seen that two ligands that primarily bind different receptor species have no effect on each other’s K1/2 distributions, we next asked how K1/2 diversity is affected when background and foreground ligands bind the same receptor. To that end, we sought to measure the K1/2 distribution for MeAsp before and after adaptation to other Tar-binding ligands.
The amino acids L-aspartate (L-asp), glutamate, and MeAsp all bind directly and competitively to the Tar receptor (Figure 3A). We first measured the K1/2 distribution for each of these ligands with no background stimulus, and found that, despite differences in the average sensitivity for each ligand, the degree of K1/2 diversity was similar for each ligand (Figure 3B, see Figure S3A-C for plots of the CV values). We then measured the MeAsp K1/2 distribution after adaptation to various concentrations of glutamate or L-asp (Figure 3C; Figure S3D-F). Although the average K1/2 for MeAsp increased in the presence of these competing background ligands, there was no significant change in the MeAsp K1/2 CV (Figure S3E). While adaptation to an L-asp or glutamate background will lead to methylation of the Tar receptor, these receptor modifications appear to have had no effect on K1/2 diversity for MeAsp.
To separate the effects of receptor modification and competition for binding sites, we measured responses to MeAsp after adaptation to maltose, which binds Tar indirectly through the maltose binding protein. Population-averaged maltose responses are known to be independent of the ambient MeAsp concentration (Figure 3D).29 We first verified that responses to maltose undergo diversity tuning similar to directly binding ligands. In the absence of background stimuli, variation in maltose K1/2 was similar to that of MeAsp (CV = 0.85 ± 0.11; Figure 3E; Figure S3A-C). After adaptation to 1 µM maltose, there was a significant decrease in the Maltose K1/2 CV (CV = 0.25 ± 0.026; Figure S3B). We attempted to measure K1/2 distributions at higher backgrounds, but due to saturation of the maltose binding protein, were unable to detect responses above 10 µM, consistent with previous population-level assays.29
When we measured the MeAsp K1/2 distribution in the presence of 1 µM maltose, we found no significant change in the MeAsp K1/2 distribution (CV = 0.55 ± 0.12; Figure 3E; Figure S3E). Similar to when serine, which binds at a different receptor, was present in the background, even in a mixed 100 µM MeAsp + 1 µM maltose background, the MeAsp K1/2 distribution was similar to when there was a 100 µM MeAsp background alone (CV = 0.026 ± 0.002; Figure 3E). These results suggest that the shift in average K1/2 when the background is competitive is due to lower binding site availability and not receptor modification (see model and discussion below).
Taken together, our experiments with Tar-binding background ligands suggest that adaptation to a background ligand that binds one receptor, only affects the K1/2 distribution of other ligands which bind the same receptor through competition for binding sites. This is in contrast to the case where the ambient concentration of the foreground ligand itself is increasing, which leads to a decrease in K1/2 diversity. To interpret this result, we turned to mathematical modeling of the chemoreceptor cluster.
The standard allosteric model of chemotaxis captures K1/2 diversity tuning with mixed background stimuli
We asked to what extent our results can be recapitulated by the simple Monod-Wyman-Changeux (MWC) modeling framework for chemoreceptor clusters, which has been the standard model of chemotaxis for the past decade.32-35 In this model, receptor-kinase clusters switch in an all-or-none fashion between a kinase activating ‘on’ state, and a deactivating ‘off’ state (Figure 4A). The free energy difference between these two states is determined by the concentration of all ligands in the environment, the methylation level of the receptors, and the degree of cooperativity between neighboring receptor-kinase units. Stronger cooperativity between neighboring receptor-kinase units leads to larger gain and a more nonlinear response.9,10,36 The model assumes precise adaptation of kinase activity,37,38 i.e., the change in free energy due to methylation always compensates for prolonged changes in ambient ligand concentration, ensuring that the average steady-state kinase activity is independent of the background ligand concentration. We also assume that the cluster contains two receptor species Tar and Tsr, that contribute ntar and ntsr cooperative units to the cluster.
In a previous study, we showed that when just one ligand species is used as both the foreground and background stimulus, the MWC model can quantitatively recapitulate the observed K1/2 distributions of adapted populations by assuming cell-to-cell variation in only one parameter, the number of cooperative units of the cognate receptor (ntar for MeAsp, ntsr for serine).27 Here, we ask what this model predicts for the K1/2 CV in the more general case where the background can be a mixture of multiple ligand species. Motivated by our measurements, we solved the MWC model for the CV of the K1/2 distribution for a foreground ligand L, as a function of its background concentration L0 as well as the concentrations of all other competitive ligands Ll (with l = 1, 2, 3, …) present in the background (Figure 4B, STAR Methods): where σ0 and K0 are the standard deviation and mean of the K1/2 distribution for the foreground ligand in the absence of any background stimulus, Ki is the dissociation constant of the foreground ligand for the inactive receptor state, and C = ∑l Ll/Kl is the sum of all competing background ligand concentrations scaled by their respective dissociation constants Kl (STAR Methods).
This simple expression for response diversity derived from the standard MWC model of bacterial chemotaxis captures the essential features of our experiments.33 First, the CV of the K1/2 distribution does not depend on the concentration of uncompetitive ligands because their effect is canceled out by adaptation (STAR Methods). The concentrations Ll of uncompetitive ligands therefore do not appear in equation (1), which implies that they should have no effect on each other’s K1/2 diversity, as experimentally demonstrated in Figure 2CE. Second, equation (1) predicts that when the foreground ligand species is absent from the background (L0 = 0), the CV and hence K1/2 diversity should be invariant under changes in either the dissociation constant Ki or the amount of competitive background ligands C, consistent with our experiments in Figure 3BC.
Equation (1) makes several predictions. For a population adapted to a background ligand concentration L0 sufficient to collapse the K1/2 diversity for the ligand L, addition of a competitor to the background (positive change in C) should actually increase K1/2 diversity. To test this prediction, we measured the MeAsp K1/2 distribution after adaptation to two different backgrounds: 10 μM MeAsp alone, and 10 μM MeAsp in combination with 10 μM L-Asp (Figure 4B). Adapting to 10 μM MeAsp alone led to a collapse of the K1/2 diversity (CV = 0.055 ± 0.007). However, in the mixed background, the K1/2 distribution widened (CV = 0.44 ± 0.05), qualitatively consistent with the model.
To test the quantitative agreement between model and data, we measured the MeAsp K1/2 CV and L-asp K1/2 CV across a range of mixed backgrounds containing different concentrations of MeAsp and L-asp. We jointly fit the model to both datasets (Figure 4CD) with the K0, σ0, and Ki values for MeAsp and L-asp (6 parameters total) as free parameters. We generally found good agreement between the data and the model fit to both datasets (Figure 4CD) with reasonable parameter values (Table S1). Using the model, we were able to predict the full K1/2 distributions for MeAsp and L-asp in most background conditions (Figure S4). The model slightly underpredicts the mean K1/2 for MeAsp in high L-asp concentrations (Figure S4J-L), and the diversity of L-asp K1/2 values with MeAsp present (Figure 4D). E. coli were previously shown to respond to L-asp even with mutant Tar receptors lacking the ligand binding domain,30 possibly through interactions with the phosphotransferase system.39 Such effects are not accounted for by the MWC model, and may be a source of the deviations from the model we observe.
Impact of sensory diversity tuning on navigation in chemical gradients
With a quantitative understanding of how chemosensory diversity is affected by adaptation to different background stimuli, we wondered whether this property of the K1/2 distribution could have tangible effects on navigation. Conceptually, the impact of diversity tuning on navigation can be understood by considering a population climbing an exponential attractant gradient (Figure 5A). In such a gradient, the fold-change in stimulus concentration during a typical movement within the gradient is constant40. For a pure log-sensing system, this would mean the perceived change in signal is constant in the gradient, so if sensitivities to the gradient are diverse, they should remain diverse at all concentrations. However, for a system which displays diversity tuning, this is not always the case. At low ligand concentrations, cells will have diverse abilities to detect the gradient. Meanwhile, at high ligand concentrations, cells with different sensory capabilities will perceive similar signals. Our experiments suggest that the presence of other ligands in the environment should not affect this overall strategy, but can only, in the case of competitive ligands, change the concentration where this transition from diverse to near-uniform sensitivity occurs. We hypothesized that diversity tuning allows populations to benefit from high-performance cells at low concentrations, while attenuating the performance penalty of low-sensitivity cells as signal intensity increases.
To test this idea, we solved a mathematical model of chemotactic migration (STAR Methods) that takes into account the cooperativity of the receptor cluster41,42. This model is a simple Keller-Segel drift-diffusion equation, where the drift velocity is proportional to the perceived chemotactic signal. This perceived signal is calculated using the MWC model41,43, which, as we have seen above, exhibits sensory diversity tuning. Solutions were analytically tractable with exponential attractant gradients for a bounded arena with reflecting boundary conditions.
We defined the chemotactic performance of a phenotype as the average ligand concentration over the population density at steady state, relative to the average concentration over a density of cells incapable of sensing the gradient. Solving for this performance as a function of receptor cooperativity n revealed three performance regimes characterized by the concentration scale of the gradients (Figure 5B). At low concentrations, the chemotactic performance is a convex function of the cooperativity n over the entire range of n values. As the concentration increases, the performance curve enters a sigmoidal regime, and eventually a convex regime at high concentrations. These same concentration-dependent performance regimes were also found numerically for other gradient shapes including a Gaussian ligand profile (Figure S5C). These three regimes of the performance curve suggest that, due to Jensen’s inequality44, over any fixed interval of receptor cooperativities, the average performance of a population with diverse cooperativities can exceed the performance of the average phenotype in low concentration gradients, but may suffer a disadvantage when signals are strong.
While the qualitative effect of diversity on performance is predicted by the shapes of these performance curves, the actual magnitude of the advantage/disadvantage depends on the distribution of cooperativities, as well as the environmental stimulus field. To explicitly quantify such effects of diversity tuning on navigation performance, we utilized an agent-based simulation of chemotaxis to explore this effect in different environments with a distribution of sensory capabilities constrained by our measured K1/2 distributions. In the agent-based simulation, cells sense their environment using an MWC-type receptor cluster with cooperativity n. Receptor adaptation and flagellar motor behavior are simulated as previously described45,46 (STAR methods). We considered two populations: a diverse and a uniform population. In the diverse population, each cell’s cooperativity was sampled from a distribution approximated from the zero-background K1/2 distribution for MeAsp (Figure S5A). For simplicity, we assumed that all other phenotypic parameters did not vary. In the uniform population, each cell had the median cooperativity from this same distribution. In this way, we could compare the performance of a diverse population to the performance of the median phenotype.
For each population, we simulated 10,000 cells for 1500 seconds in three dimensions with an exponential gradient that decreased in one dimension, and a reflecting plane at x = 0 (Figure 5C). The concentration of the gradient reaches a maximum value [L]max at this barrier. As in the analytical model, we defined the performance of a population as the average over the set of ligand concentrations corresponding to the set of final positions of cells in the population. We computed the performance of the diverse and uniform populations in attractant gradients with different maximal concentration in the environment, and various length scales. With all length scales tested, we found that when [L]max was low, the performance of the diverse population exceeded that of the uniform population. As [L]max increased, there was a regime in which the diverse population was at a slight disadvantage. At very high [L]max, the performances of both populations were similar (Figure 5D). In simulations within arenas with two separate Gaussian attractant peaks, we observed qualitatively similar performance curves when the attractants bound uncompetitively, and competitively (Figure S5D-H).
Both the analytical model and agent-based simulations demonstrate that diversity tuning can play a role in chemotactic navigation. Variation in phenotypic parameters will generate cells with variable chemotactic ability. However, diversity tuning allows the variation in chemotactic ability to change with the environment without changes in the underlying phenotype distribution. When signals are weak, the convex phenotype-performance map leads to a regime where performances are variable and the population can benefit from rare high-sensitivity cells. When signals are very strong, the phenotype-performance map flattens, leading to similar performance of all phenotypes.
Diversity tuning beyond chemotaxis
Given the navigational performance benefits suggested by our mathematical analysis and simulations above, we next asked if analogous diversity tuning arises in more general adaptive signaling systems beyond bacterial chemotaxis and the allosteric MWC model. In the STAR Methods, we present a mathematical analysis that identifies a general class of sensory systems, which includes the MWC model of chemotaxis, in which background-dependent sensory diversity tuning arises. In particular, we demonstrate that a sufficient condition for sensory diversity tuning is that the sensory system in question demonstrates upon adaption to a background input level L0 a dose-response relation that can be written as a function where f is a monotonic invertible function with phenotypic parameters θ which vary from cell to cell, A and B are positive constants analogous to dissociation constants, and L is the foreground input level. This generic dose-response relation, which could arise from a variety of underlying mechanisms, demonstrates two sensory regimes. When L0 is low relative to B, the system senses linear changes in ligand concentration. However, when L0 greatly exceeds B the system responds to the fold-change in ligand concentration relative to the background. For systems with such dose-response curves, we define a sensitivity KR analogous to the K1/2 but for arbitrary response level R. The coefficient of variation in KR can be shown in general to decrease as the background ligand concentration increases. Furthermore, if A = B, the system is now precisely adapting over all background stimuli, and the CV of KR is exactly equation (1) in the absence of a competitive background species (STAR Methods). As an illustrative example, we show how a dose-response curve in the form of equation (2) can arise in simple adaptive feed-forward and feed-back networks in the STAR Methods.
While equation (2) is a sufficient condition for tunable diversity, the dynamic range of the sensory diversity (i.e. the maximal achievable contrast in the KR CV) does depend on the specific form of f. Specifically, fractional change in sensory diversity as the population adapts to large backgrounds depends on the average zero-background sensitivity relative to the dissociation constant A (STAR Methods). In the case of chemotaxis, what this implies is that if cells are on average more sensitive than individual receptors (K0 < Ki), then sensory diversity will change significantly as the population adapts to large background stimuli. However, if cells are not more sensitive than individual receptors (K0 ≈ Ki) the change in diversity as cells adapt will be small. In the case of E. coli chemotaxis, high sensitivity is accomplished by cooperativity in the receptor cluster. This suggests that both the transition from linear to fold-change detection, and high cooperativity may be important for sensory diversity tuning.
Discussion
With decades of extensive characterization, E. coli chemotaxis provides an excellent testing ground for general principles of signal processing by living systems, and the role of cell-to-cell variation in population-level sensory strategies. In this study, we used single-cell FRET to measure the sensitivity distributions for several ligands after adaptation to different background stimuli. Consistent with previous studies, increasing the concentration of a particular ligand led to a decrease in the amount of K1/2 diversity for that ligand.27 Here, we found that if two ligands bind uncompetitively – on the same receptor or different receptors – sensory diversity for each ligand can be tuned in an orthogonal manner. That is, it is possible to be in the low-diversity regime for one ligand, and the high diversity regime for another ligand in the same environment. However, for ligands that compete for binding sites, increasing the background concentration of one ligand decreases K1/2 diversity for that ligand, while increasing the K1/2 diversity of its competitors.
Previously, we showed that the two diversity regimes are explained by the two regimes of allosteric receptor clusters. At low methylation levels, the K1/2 is strongly dependent on the receptor cooperativity. However, when receptors are highly methylated, the K1/2 depends weakly on the receptor cooperativity27,35. Our experiments and theory suggest that what matters for sensory diversity tuning is not simply the methylation level of the receptors, but the amount of receptor methylation that directly offsets the free energy contribution from each ligand species.
First, consider two ligands that bind uncompetitively such as serine and MeAsp. Increasing the background MeAsp concentration leads to receptor methylation to offset the effect of MeAsp on the kinase activity. The magnitude of this offset, as in the single species case, determines whether the population is in the high or low diversity regime.27,35 Adding serine to the background will cause additional receptor methylations that offset the serine concentration. If we change the MeAsp concentration however, responses will not be affected by these new methylations, since their effects are canceled out by the constant serine background. As such, the distribution of MeAsp sensitivities remains independent of the serine concentration. Only methylation due to the background MeAsp concentration affects the MeAsp K1/2 distribution.
The case of competing ligands is slightly more complicated. Consider MeAsp and L-Asp for example. Again, adapting to MeAsp leads to receptor methylations which offset the background MeAsp concentration. However, addition of a competitive background ligand, while leading to additional methylations, now also changes the effective affinity of MeAsp for the receptor due to reduced binding site availability. Due to this change in the effective affinity of the receptor for MeAsp, even though the total receptor methylation has increased, the total contribution of MeAsp to the free energy has decreased, and as such a smaller proportion of the total receptor methylation is offsetting its concentration. This decrease in methylation required to offset its concentration leads to an increase in the MeAsp K1/2 diversity.
Another, more general way, to understand sensory diversity tuning is in terms of the transition from a linear sensing regime, where cells sense the total change in ligand concentration, to a logarithmic sensing regime, where cells sense the fold-change in ligand concentration relative to the adapted background concentration. In bacterial chemotaxis, the implementation of this transition (see equation (2)) by receptor clusters as described above is sufficient to capture the K1/2 diversity as background conditions change. From this perspective, the reason for which sensory diversity can be tuned orthogonally for ligands that do not compete for binding sites is that the transition from linear to logarithmic sensing is also orthogonal for such ligands. However, for competitive ligands, previous theory showed that only one ligand species can be in the logarithmic sensing regime at a time.47 While there are likely milder conditions for diversity tuning than equation (2), dose-response relationships of this kind can emerge in some simple feed-forward and feed-back signaling pathways (STAR Methods),40,48 suggesting that diversity tuning may arise in adaptive signaling systems beyond chemotaxis.
Functionally, how might diversity in sensitivity (K1/2) and the ability to tune this diversity in different backgrounds benefit bacterial populations? Behavioral studies previously revealed diversity in the chemotactic gain, and suggested that maintaining poor navigators in a population can protect the population from catastrophic events.19 Additionally, within each cell, temporal fluctuations in gain have been theorized to improve resource exploitation in complex environments by preventing cells from getting trapped in local attractant maxima.17 One implementation of pathway gain diversity which is consistent with our model, may be variation in receptor cooperativity, which has been suggested by previous work.19,27
Our findings add context to these previous results. Variation in receptor cooperativity can generate rare high-sensitivity cells that can track weak signals. But as the signal prevalence increases, diversity tuning enables even rare low-sensitivity cells to track the same gradient. This perspective is supported by our mathematical modeling of chemotactic behavior where we challenged cells with diverse sensory capabilities to track an exponential gradient, or locate the center of two different gaussian attractant signals. When the attractant source is weak, a diverse population has higher performance than the median phenotype since rare high-gain cells can track the gradient. However, at high source strength, due to diversity tuning, the low-gain cells do not significantly hamper performance, and behavior is similar to that of the median phenotype.
Ultimately, our experiments and theory suggest that E. coli implement sensory diversity tuning in a manner that allows the population to simultaneously deploy a bet-hedging strategy for responding to some ligands while deploying a tracking strategy to climb gradients of others. This feature of the chemosensory receptor cluster could aid populations in making behavioral decisions. If weak signals appear, a small segment of the population will track them without committing the entire population to a potentially transient signal. Due to precise adaptation and the independence of the sensory diversity for different ligands, this behavioral strategy can be applied independently to different signals by the same population, at the same time.
Funding
This work was supported by NIH Awards R01GM106189 and R01GM138533. J.M. was supported by the NSF Graduate Research Fellowship Program under Grant No. DGE-2139841. K.K. was supported by the JST PRESTO grant, JPMJPR21E4, and the NSTC grant, 112-2112-M-001-080-MY3.
Author contributions
J.M., K.K. T.E., and T.S.S. designed the project. K.K. designed the experimental setup. J.M. and R.K. performed the experiments. J.M. performed the data analysis and mathematical modeling. J.M., K.K., R.K., T.E. and T.S.S. wrote the manuscript.
Declaration of Interests
The authors declare no competing interests.
Data and materials availability
All data needed to evaluate the conclusions in the paper are present in the paper and/or the Supplementary Materials. Additional data may be requested from the authors.
STAR Methods
RESOURCE AVAILABILITY
Lead contact
Further information and requests for resources should be directed to and will be fulfilled by the Lead Contact, Thierry Emonet (thierry.emonet{at}yale.edu).
Materials availability
This study did not generate new unique reagents or strains.
Data and code availability
All data needed to evaluate the conclusions in the paper are present in the main text and/or the supplementary materials. The datasets generated in this study have been deposited in the dryad database (doi: 10.5061/dryad.nvx0k6dzz). Codes used in this study are available on GitHub (https://github.com/emonetlab/SensoryDiversityTuningAnalysis). Any additional information required to reanalyze the data reported in this paper is available from the lead contact upon request.
EXPERIMENTAL MODEL DETAILS
Bacterial growth conditions
All FRET experiments were performed with a derivative of E. coli K-12 RP437 harboring ΔCheYZ and ΔFliC mutations, and transformed with two plasmids: pSJAB106 from which CheZ-YFP and CheY-mRFP1 are expressed in tandem on an isopropyl-β-d-thiogalactopyranoside (IPTG) inducible promoter, and pZR1 from which ‘sticky’ FliC* is expressed on a sodium-salicylate (NaSal) inducible promoter.21 Cells were grown overnight in TB broth (1% bacto-tryptone, 0.5% NaCl), then diluted 1:100 into 10mL of fresh TB supplemented with 50µM IPTG to induce the FRET pair, and 3µM NaSal to induce sticky FliC* for cell adhesion to glass coverslips27, with 100ug/mL ampicillin and 34ug/mL chloramphenicol for plasmid retention. Cultures were grown at 33.5°C to an OD600 of 0.44-0.47 then washed once with 30mL motility buffer (10mM KPO4, 0.1mM EDTA, 1uM methionine, 10mM lactic acid) and suspended in 2mL of motility media. Suspensions were left at room temperature for 2hrs before imaging.
METHOD DETAILS
Microfluidics fabrication and operation
Microfluidic devices were constructed from PDMS with standard soft lithography methods.49 The master mold for the device was a silicon wafer with features created using ultraviolet photoresist lithography (Figure S1). To cast the device, the mold was coated with a 5 mm-thick layer of degassed 10:1 PDMS-to-curing agent mixture (Sylgard 184, Dow Chemical). Molds were baked at 80°C for 45 min. Devices were cut out of the mold and holes were punched into the inlets with a manually sharpened 20-guage blunt-tip needle. Then, PDMS devices were bonded to a 24mm X 60mm coverslip (#1.5). PDMS was cleaned with transparent adhesive tape (Magic tape, Scotch) then rinsed with acetone, isopropanol, methanol, and water. Coverslips were also rinsed with acetone, isopropanol, methanol, and water. Glass and PDMS were treated with plasma generated by a corona treater. Then, PDMS was laminated to the coverslip, and baked overnight at 80°C.
The microfluidic device has 7 inlets, an outlet at the end of the imaging chamber, and two side outlets of which only the right one is opened during cell loading (Figure S1). During operation, the inlets were connected to 7 reservoirs containing motility media supplemented with different attractant concentrations. Cells washed in motility medium were loaded into the device through the outlet channel, where they initially exit through one of the side outlets, which is plugged before imaging to induce flow towards the end outlet. Pressure in the inlet reservoirs was controlled by computer-controlled solenoid valves (MH1, Festo) that quickly switch between atmospheric pressure, and a source of 1kPa pressurized air as needed.
In-vivo single-cell FRET microscopy
Single-cell FRET and cell culture were performed as previously described.27 Cells were grown and washed as described above. FRET imaging was performed with an inverted microscope (Eclipse Ti-E, Nikon) equipped with an oil immersion objective (CFI Apo TIRF 60X Oil, Nikon). Yellow fluorescent proteins were illuminated with a light-emitting diode system (SOLA SE, Lumencore) through one excitation filter (59026x, Chroma), then another (FF01-500/24-25, Semrock) and a dichroic mirror (FF520-Di02; Semrock). Emission was fed into an emission image splitter (OptoSplit II, Cairn) where it was split into donor and acceptor channels with a dichroic mirror (FF580-FDi01-25×36, Semrock) and collected through emission filters (FF01-542/27 and FF02-641/75; Semrock) with a scientific CMOS camera (ORCA-Flash 4.0 V2, Hammatsu). Red fluorescent protein mRFP1 was imaged in the same way as YFP, except with a different second excitation filter (FF01-575/05-25) and dichroic mirror (FF593-Di03-25×36, Semrock). For both fluorophores, images were taken with 50 ms exposure time.
FRET data analysis
Single-cell fluorescent signals were extracted from fluorescence time-series as described previously.21,27,50 Images were segmented and single-cell fluorescent signals determined with in-house software. Photobleaching was corrected by fitting donor and acceptor time-series with a bi-exponential function and subtracting out the decay to yield donor D(t) and acceptor A(t) time-series.
To calculate FRET from fluorescence time-series, we used the E-FRET method.50 The E-FRET index is given by where IDA is FRET-acceptor emission intensity from donor excitation, IAA is acceptor emission with acceptor excitation, IDD is donor emission from donor excitation, with a, G, d being optical constants that depend on the FRET pair and optical setup which were determined by an independent experiment with strains that express only CheY-mRFP or only CheZ-mYFP.22
To convert FRET time-series to kinase activity, for each cell, FRET values were normalized by the minimum and maximum values measured during a saturating stimulus at the beginning and end of the experiment. For each experiment, the saturating stimulus was a mixture of the background stimulus, and a saturating amount of the foreground stimulus.
Determining K1/2 distribution from single-cell responses
After a saturating stimulus for response calibration, cells were adapted to the background for 3 minutes. Then, cells were presented with 5 different attractant concentrations in series with 5 second presentation time, and 30 seconds at the background level in between stimuli. This cycle through the stimulus levels was presented 7 times to allow within-cell averaging of the response amplitudes.
We extracted the K1/2 cumulative distribution function from the within-cell average responses using previous methods.27 Given a family of dose-response curves, for a given ligand concentration [L]i, the fraction of responses that are greater than half-maximal equals the fraction of cells with K1/2 < [L]i (Figure S1). Thus, by determining the fraction of half-maximal responses at a series of ligand concentrations, we can measure the cumulative distribution function (CDF) of the K1/2. For each measured point on the CDF, confidence intervals were determined by bootstrapping, both over cells and over the seven responses per re-sampled cell. Confidence intervals (95% CI) on the fitted lognormal parameters were estimated from the posterior distribution with lognormal priors and gaussian error using markov-chain monte carlo methods (Figure S2). For each CDF, cells from at least two independent biological replicates were pooled to increase the number of cells included in each analysis, since the number of cells measured in each experiment varied from day to day.
Model of the chemotaxis pathway
Throughout the main text and STAR Methods, we use the standard model of bacterial chemotaxis32-35,51 where the cell relays sensory information to the flagellar motor through a signaling cascade triggered by binding of attractant to highly cooperative receptor arrays. Receptor clusters whose activity can be described by a two-state model where activity a ∈ [0,1] is determined by the free energy difference F (in units of kBT) between the active and inactive states
The free energy can be decomposed into two terms . The first depends linearly on the degree of receptor methylation m, such that Fm(m) = −nTα(m − m0) where nT is the total receptor coupling, and α and m0 are constants.52 The second term is the dependence of the free energy on ligand binding, where is a vector containing the concentrations of all ligand species in the environment. The form of FL (L) will depend on whether the ligands bind competitively or uncompetitively to the receptor cluster. For a receptor cluster with two receptor species - Tar and Tsr - that are allosterically coupled, and two ligands that bind either Tar or Tsr but not both, where ntar and ntsr are the number of cooperative Tar and Tsr units in the cluster with ntar + ntsr = nT, L1 and L2 are concentrations of ligands binding Tar and Tsr respectively with dissociation constants Ki and Ka to the inactive and active receptor states. The case where two ligands bind independently to the Tar receptor is identical to equation (S2) with ntsr = ntar. In cases where L1 and L2 both bind Tar in the same binding pocket,
As the external ligand concentration changes, receptors are methylated or demethylated to adapt to maintain an activity level a0 independent of the environment. To describe methylation kinetics, we used a similar approach as previous studies, where where V and (θ is the Heaviside function and a = 0.74, r = 4.0) are the methylation/demethylation rates for CheR and CheB with dissociation constants, KR and KB.18,33,52
We assume signal transduction to be fast compared to methylation, so that the active response regulator CheY-P concentration can be written, Y(a) = αya with αy constant. CheY-P binds the flagellar motor, changing the switching rate between clockwise (CW) and counter-clockwise (CCW) rotation. This switching is assumed to be a Poisson process with switching rates
Where with ϵ1, ϵ2, K constant.18,45,53 We assume that only a single motor switching from CCW → CW is sufficient to tumble, so for cells with only 1 flagellum, the rates above describe the run and tumble dynamics as a function of CheY-P.
Agent-based simulations of chemotactic behavior
Agent-based simulations were performed using Euler integration of the above model, as described previously.18,45,53,54 At each time-step, the cell either moves or stays in place depending on its motility state (run or tumble), which both have their own rotational diffusion coefficients DR and DT. After updating the position and local ligand concentration, the adaptation equation is integrated and the free energy of the receptors, and thus the CheY-P concentration and motor switching rates are updated. A random number is drawn to determine whether the flagellum state switches, with rules and parameters as in.53
Cells were challenged to navigate two different environments. The first is a simple exponential gradient extending in one dimension with a reflecting boundary at x = 0, maximum concentration Lmax, and length scale λ, given by L(x) = Lmaxe−x/λ. The second was an environment with two static gaussian gradients, given by , where L is the ligand concentration at the starting position, is the center of the gaussian, and r is the gradient ramp rate. The gradients were placed equidistant from the origin where cells were initialized. Additionally, for each cell, values of ntar and ntsr were drawn by sampling from the experimental K1/2 distribution for meAsp in 0-background, and using the conversion .35 For simplicity, the same distribution was assumed for both ntar and ntsr. Additionally, the distribution of ntar and ntsr was assumed to be independent since responses to the population average K1/2 were uncorrelated (Figure S5B). To isolate the effect of signal integration and diversity in receptor coupling, we assumed that methylation does not saturate, which would lead to imperfect adaptation as the population climbs the gradient.55,56
Quantitative model of the K1/2 CV as a function of background ligands
Here we derive the coefficient of variation (CV) of the distribution of K1/2 for the classic MWC model of bacterial chemoreceptor clusters. For a ligand L, assuming L ≪ Ka, the activity of the cluster is approximately where ϵ is the free energy of the cluster in the absence of all ligands, C = ∑l Ll/Kl is a constant that accounts for the presence of all background attractants that compete with L, and U is a constant that accounts for all uncompetitive ligands. C and U follow from equations (S2) and (S3) above. Note that U can take different forms depending on how the uncompetitive ligand binds. For example, if the second ligand L′ bound the same receptor as L with dissociation constant , then . However, if it bound a different receptor which contributed n′ cooperative units to the receptor cluster, then .
We assume that the receptor cluster adapts perfectly. This means that at steady state, any combination of ligands will result in the same activity, given by where ϵ0 is the adapted zero-background free energy difference. Now, we can define the K1/2 as the ligand concentration L where a(L, ϵ) = a0/2. We also write L = L0 + ΔL where L0 is the background concentration of L. To find the K1/2, we solve
Where and ϵeff = ϵ + In(U) + n ⋅ In(1 + C + L /K) = ϵ due to perfect adaptation. Continuing,
Thus, the K1/2 as defined above, is given by
In the zero-background condition, the sensitivity becomes
The K1/2 clearly depends on both the free energy of the cluster in zero background condition ϵ0, and the degree of receptor coupling, n. It also depends on the concentration L0 of ligand in the background, as well as on the presence of competitive ligand C = ∑l Ll/Kl in the background. However, the K1/2 is unaffected by the presence of uncompetitive ligands, whether the bind the same or different receptors. We assume that the receptor-ligand affinities Ki and Kl and concentrations L0 and Ll of the ligand and competitors in the background are the same for each cell. Thus, we can write the average K1/2 as and the standard deviation as
Where and are equivalent to the mean and standard deviation of the K1/2 distribution for ligand L in the absence of any background stimulus. Then, the coefficient of variation (CV = SD(K1/2)/⟨K1/2⟩) in K1/2 for ligand L in the presence of a background concentrations L0 of itself and background concentrations Ll of competitors is given by
By inspection and for increasing L0, the maximal CV is σ0/K0 and the minimal CV is σ0/(K0 + Ki). Given a particular competitive background C, the transition between the high and low diversity regimes as L0 increases occurs when
Diversity tuning emerges from the transition from linear to logarithmic sensing
The molecular details of the chemosensory network are not necessary to capture the essential diversity-tuning behavior of the chemotaxis pathway. A sufficient condition to have background dependent sensory diversity is that the dose-response relationship can be written as a function where A and B are positive constants, L0 is the background stimulus level, L is the foreground stimulus level, and f some monotonic invertible function with phenotypic parameters θ. Note that this function is always precisely adapting if A = B, but otherwise only precisely adapting when L0 ≫ A, B. Analogous to the K1/2, the stimulus level where activity is half of the steady state, we define a KR, which is the stimulus level where . We define the inverse of the monotonic function f at constant θ by . Solving for KR,
We define K0 = B ⋅ ⟨f−1(R; θ)⟩θ − A, which is the mean of the distribution of KR in zero-background (L0 = 0), and the subscript θ denotes an average over the distribution of phenotypic parameters θ. Similarly, we define σ0 = B ⋅ SDθ(f−1(R; θ)) which is the zero-background standard deviation of the distribution of KR, and SDθ is the standard deviation of the distribution of θ. In an arbitrary background, the . Using the definition of K0 and σ0 to replace ⟨f−1(R; θ)⟩θ and SDθ(f−1(R; θ)), we obtain which is a decreasing function of the background ligand concentration L0. If A = B = Ki, equation (S17) is identical to equation (1) from the main text in the absence of competitive background ligands.
The stated sufficient condition guarantees that the degree of cell-to-cell variability will vary with the background stimulus level. But is the change in variability always significant? It can be shown that the difference between the maximum and minimum levels of cell-to-cell variability depend only on the average sensitivity K0, relative to the dissociation constant A. As written above, the maximum CV occurs at L0 = 0, and the minimum CV occurs as L0 → ∞. These are,
To determine the relative difference between the maximum and minimum CV we compute which reveals that the contrast between the high and low diversity states (i.e. the significance of diversity tuning) depends only on K0/A, the average zero-background KR relative to the dissociation constant A. This leads to an intuitive understanding of the conditions for diversity tuning within this framework. If the cells achieve a sensitivity greater than the dissociation constant (K0 ≪ A), then adaptation can dramatically affect the KR distribution. However, if cells are far less sensitive than ligand binding alone (K0 ≫ A), then adaptation has a negligible affect on diversity.
It is easy to check that this theory applies to diversity tuning in chemotaxis. We start by re-writing the MWC model in the form of Equation (S15). Assuming L ≪ Ka, the activity of the receptor cluster can be written where, as before, we have decomposed L into its background concentration L0 and the change in foreground concentration ΔL, and defined . Assuming the activity adapts precisely to L0, ϵ will adjust until the sum is the steady-state free energy difference. From here we get
Therefore we have written the kinase activity a as a function of the form with A = B = Ki :
Given an activity level a = r the inverse of the function f at constant parameters θ = (n, ϵ0) is which can be used to calculate the ligand concentration L = KR needed to reach the activity a = r:
Here we are interested in the concentration L = K1/2 at which the activity is half its adapted value . Inserting in the above expression we recover the expression (S10) for the K1/2 derived earlier.
Two simple examples of adaptive signaling pathways with diversity tuning
To illustrate that diversity tuning can arise when equation (S15) is satisfied in systems beyond chemotaxis, we analyzed two simple adaptive signaling pathways. With mild assumptions, diversity tuning can be shown to arise in two basic adaptive network motifs: the incoherent feed-forward loop, and negative integral feedback. First, we will consider a simple incoherent feed-forward loop with three species: the output species Z, the input X which activates Z, and the adaptation species Y which deactivates Z but is itself activated by X. We can write a zero-order approximation for the Z and Y dynamics40,57-59 where kf and kr are rate constants, a and b are constants allowing constant basal production and destruction of Z, and τ is the timescale of Y equilibration. After adaptation to a constant background input X0, Y = X0.
Assuming adaptation is slow relative to the response of Z to change in X, the dose-response curve of Z activity is which is a function of the form of equation (S15), suggesting this system is capable of diversity tuning if kr and/or kf vary from cell to cell.
We can perform a similar analysis for negative feedback. For this case, we consider the same dynamics of Z, but different dynamics for Y. The negative feedback loop equations are thus
At steady state, assuming constant input X, Z = Z0, so , and the steady-state dose-response curve of Z is which is also a function in the form of equation (S15), and should also tune diversity due to variation in Z0 as the background input X0 changes.
Calculating chemotactic performance with diverse receptor cooperativity
To explore analytically the role of diverse receptor cooperativity in navigation, we used an extension of the classic Keller-Segel model.41,42 In this model, the bacterial cell density ρ(x, t) is governed by the partial differential equation where D is the diffusion coefficient, χ is the chemotactic coefficient, and f is the signal perceived by the cell. This perceived signal is the change in free energy of the chemoreceptor complex given a change in ligand concentration, which as in the MWC model can be expressed as
Assume a fixed ligand profile over the domain 0 ≤ x ≤ a and that L(x) ≪ Ka. Then the cell density reaches a phenotype dependent steady-state where C is the integration constant and η = nχ/D. It is convenient to define a conditional probability density of the cell position given phenotype η :
The cell density for phenotype η is then simply ρ(x|η) = NcellsP(x|η). We also see that when cells do not respond to the gradient or when they do respond but there is no gradient, i.e. L(x) = L0 is constant, then the conditional probability density of the cell position becomes a constant P0 :
In this case the cell density is uniform and becomes ρ = Nt°tP0 = Nt°t/a, as expected.
We now define the performance of a particular phenotype as the expected ligand concentration experienced by the cells with phenotype η normalized by expected ligand concentration experienced by the cells when they are not responsive to the ligand:
For an exponential gradient L(x) = Lmaxe−x/λ we calculate P(x|η) by changing variables from x to
Introducing (S37) in equation (S34) using the fact that we get: where S0 = S(0), Sa = S(a) and B is the incomplete Beta function. We can also define the probability density function
For the performance Q(η) we then use (S36-S39) to calculate the numerator of equation (S36) and the denominator
From this we obtain for the performance:
If we restrict the values of η to any interval, this performance has three regimes. At low values of Lmax (or S0), this performance curve is convex (Figure 5B). At intermediate values, the curve is sigmoidal, and at high values, the curve is concave. Because of Jensen’s inequality, which states that for a convex function Q(η), that Q(⟨η⟩) ≤ ⟨Q(η)⟩, in the convex regime, it is possible for the average performance of a population with diverse η to exceed the performance of the average phenotype, ⟨η⟩. Conversely, in the concave regime, the population may underperform the average phenotype.
QUANTIFICATION AND STATISTICAL ANALYSIS
All statistical testing was performed in Matlab (version R2020a). For each quantity, confidence intervals were calculated as described in the relevant figure caption. Data were quantified as described in the respective method subsections and/or figure captions.
Supplemental Materials
Acknowledgements
We thank JS Parkinson and V. Sourjik for providing strains, and we thank F. Avgidis, D. Clark, N. Dimitrova, and H. Mattingly for useful discussions.
Footnotes
↵5 Lead Contact
Main text figures 1-5 have been included above their figure captions.