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A decay effect of the growth rate associated with genome reduction in Escherichia coli

BMC Microbiology201818:101

https://doi.org/10.1186/s12866-018-1242-4

©  The Author(s). 2018

  • Received: 22 May 2018
  • Accepted: 20 August 2018
  • Published:

Abstract

Background

Bacterial growth is an important topic in microbiology and of crucial importance to better understand living cells. Bacterial growth dynamics are quantitatively examined using various methods to determine the physical, chemical or biological features of growing populations. Due to methodological differences, the exponential growth rate, which is a parameter that is representative of growth dynamics, should be differentiated. Ignoring such differentiation in the growth analysis might overlook somehow slight but significant changes in cellular features of the growing population. Both experimental and theoretical investigations are required to address these issues.

Results

This study experimentally verified the differentiation in growth rates attributed to different methodologies, and demonstrated that the most popular method, optical turbidity, led to the determination of a lower growth rate in comparison to the methods based on colony formation and cellular adenosine triphosphate, due to a decay effect of reading OD600 during a population increase. Accordingly, the logistic model, which is commonly applied to the high-throughput growth data reading the OD600, was revised by introducing a new parameter: the decay rate, to compensate for the lowered estimation in growth rates. An improved goodness of fit in comparison to the original model was acquired due to this revision. Applying the modified logistic model to hundreds of growth data acquired from an assortment of Escherichia coli strains carrying the reduced genomes led to an intriguing finding of a correlation between the decay rate and the genome size. The decay effect seemed to be partially attributed to the decrease in cell size accompanied by a population increase and was medium dependent.

Conclusions

The present study provides not only an improved theoretical tool for the high-throughput studies on bacterial growth dynamics linking with optical turbidity to biological meaning, but also a novel insight of the genome reduction correlated decay effect, which potentially reflects the changing cellular features during population increase. It is valuable for understanding the genome evolution and the fitness increase in microbial life.

Background

Bacterial growth dynamics have been intensively studied at both the experimental and theoretical levels [1–4] due to their broad applications in the food and medical industries and because of the simplicity of the fundamental investigation of determining living systems [5–7]. It is well-known that bacterial growth commonly follows an S-shaped curve on a two-dimensional plane over time the bacterial population. To describe and/or predict S-shaped growth curves, a number of bacterial growth models were proposed, revised and expanded repeatedly to better understand the biological process of bacterial growth under varied conditions and/or forms [8–13]. Although the growth curve of the most representative bacterium, Escherichia coli (E. coli), has been examined since the 1930s [14], the indescribable complexity of the growth dynamics of E. coli remain and are still under investigation with other models to understand the differential growth dynamics [15, 16]. Despite the variation in either experimental techniques or theoretical models, the growth rate during the exponentially growing phase is the most important parameter and has a high biological impact; this rate represents the genetic and environmental influences on the bacterial growth dynamics [17–19]. Thus, precise evaluation on the growth rate is highly required for better understanding of growing cells and populations.

Experimentally, bacterial growth rate is quantified by varied techniques and is dependent on different principles of chemistry, physics and biology [20, 21], such as assays of optical turbidity, colony formation, cellular adenosine triphosphate (ATP) and particle counts [22–25]. The most commonly used method is the conventional method to measure the optical turbidity of a bacterial culture (optical density at a wavelength of 600 nm, OD600) due to its easy manipulation. To date, this method seems to be the most frequently used tool for assessing high-throughput assays of bacterial growth in microplates and colonies [4, 6, 26, 27], and for computational and systematic analyses of bacterial growth dynamics [26, 28, 29]. These up-to-date studies are largely based on fitting the logistic model [30, 31] to experimental data acquired from temporal reads of optical turbidity (OD600). Since the measurement of OD600 detects light transmitted through a cell culture by a spectrophotometer, the changes in absorbance may not always accurately correlate to the changes in the number of living cells. Although the optical turbidity was confirmed to be reliable for estimation of bacterial growth rate, the calibration of the optical measurements was required [32]. Taking account of these issues, the growth data reading OD600 might neglect potential changes in the cellular features occurred during population increase.

To estimate how much difference in growth rates could be caused by the difference in methods, the growth rates of various E. coli strains were evaluated by varied methods in parallel. Furthermore, to see whether the improved evaluation of growth dynamics would identify any overlooked cellular features of the growing population, a large data set composed of hundreds of growth curves of an assortment of E. coli cells carrying reduced genomes were analyzed. As a consequence, the commonly used growth model of the logistic equation was revised by introducing a new parameter of biological importance, and a correlation between genome reduction and the logistic parameters was observed for the first time, owing to the modified logistic model. In a word, this study offers an improved growth model based on optical turbidity and a novel finding of the correlation between genome reduction and the growth related parameters, which are linked to the changes in the cellular features.

Results

Lower growth rates evaluated by the optical turbidity

The wild-type E. coli strain W3110 was cultured in minimal medium M63 and was temporally sampled in three different assays to measure the optical turbidity (OD600), colony formation (colony forming unit, CFU) and ATP abundance, which are based on the physical, biological and chemical properties of the growing cell population, respectively. Although these three methods are well established and widely used in experimental and theoretical studies on bacterial growth, it is unclear whether they result in a common conclusion regarding bacterial growth. The three methods of measuring the OD600, CFU and ATP represent the density of the biomass, number of living cells and cellular activity, respectively. The growth dynamics represented by the changes in these different parameters must be varied in consequence. To verify this assumption, we performed three assays in parallel on identical cell cultures. According to the growth curves generated from the OD600, CFU and ATP, the growth rates were calculated by regression toward the time sampling records during the exponential growth phase and as described in the Materials and Methods. Repeated cell cultures (N = 3~ 5) showed significant differentiation of the growth rates estimated by measuring the optical turbidity (OD), colony formation (CFU) and ATP abundance (Fig. 1). The growth rates estimated by measuring the CFU and ATP were comparable, whereas those from OD600 were lower (p < 0.05), regardless of identical population growth. The results demonstrated that the bacterial growth dynamics, which are represented by changes in optical turbidity, were different from those evaluated by changes in the number of active cells, consistent to the previous report [32]. How and what caused the differences in growth rates and whether the differences were common under other conditions were further investigated by comparing two representative methods, OD600 and CFU.
Fig. 1
Fig. 1

Lower estimated growth rate by means of optical turbidity. The differentiation in the growth rates were evaluated by the three methods. The mean growth rates repeatedly evaluated by means of the OD600 (blue), CFU and ATP (orange) are shown. The standard errors of biological replication are shown. Asterisks indicate statistical significance (P < 0.05)

Decay effect in optical turbidity triggered the lower estimated growth rate

A decay effect was observed when the optical turbidity results were compared to the records of colony counts and OD600 values. Both the CFU assay (Fig. 2a, upper) and OD600 reads (Fig. 2a, middle) were performed in parallel to monitor the same population growth. The temporal changes in both records were supposed to be similar. Nevertheless, a temporal decrease in the ratio of the OD600 reads and CFU counts was observed (Fig. 2a, bottom). Since the decrease was initiated from the early exponential phase, the growth rates evaluated by optical turbidity (μOD) were lower than those evaluated by colony formation (μCFU) (Fig. 1b); this decrease was considered to be due to the decay effect of the OD600 values. It was carefully tested whether the decay effect was caused by limitations of the optical measurement. No significant differentiation in the optical reads were detected during the exponential growth phase (OD600 < 0.5) compared with the significant decrease in the reads of OD600 during the stationary phase (OD600 > 1) (Additional file 1: Figure S1). It was verified that the decay of the OD600/CFU ratio during the exponential phase was not attributed to mechanical errors of the optical reads but was mainly due to biological issues, such as a difference in cellular properties.
Fig. 2
Fig. 2

Differentiated growth rates estimated by means of the optical turbidity and colony formation. a. Repressed increase of OD600 in comparison to that of CFU. The temporal changes in CFU (upper), OD600 (middle), and the ratio of the two reads (bottom) of identical population growth are shown. Error bars indicate the standard errors of the assays. b. The growth rates under varied growth conditions. Growth of the same wild-type E. coli cells growing under the different conditions (D3, D4 and Cm) was analyzed in parallel by the two methods. D3 indicates that the cell growth that started from the pre-culture reached the stationary phase with a 1000-fold dilution in fresh medium. D4 indicates that the cell growth that started from the pre-culture remained in the exponential phase with a 10,000-fold dilution in fresh medium. Cm refers to cell growth in the presence of a low concentration of antibiotics (15 μg/mL chloramphenicol). The growth rates evaluated by OD600 and CFU are indicated as μOD and μCFU, respectively. c. The growth rates of the various genotypes. The growth dynamics of E. coli cells of four reduced genomes were analyzed by the two methods in parallel. Strain Nos. 7, 14, 20 and 28 indicate multiple deletions of approximately 251, 710, 899 and 982 kbs from the wild-type genome W3110, respectively. The standard errors of the biological replication are indicated, and asterisks indicate the statistical significance (P < 0.05)

The lower estimated growth rate according to optical turbidity was also detected either under other growth conditions or in other genotypes. Wild-type E. coli cells W3110 grown under various conditions (D3, D4 and Cm described in the figure legend) also showed lower growth rates (N = 3, P < 0.05) estimated by OD600 (Fig. 2b). In addition, the growth dynamics of four different E. coli strains with reduced genomes (Strain Nos. 7, 14, 20 and 28), which were previously constructed [33] and characterized [34], were assayed by the two methods (N = 3~ 4). Similarly, the values of μOD tended to be smaller than those of μCFU (P < 0.05) regardless of the multiple deletions of genomic sequences (Fig. 2c). The results indicated that the lower growth rates estimated by optical turbidity, which is the most commonly used method in bacterial growth studies, frequently occurred in different genotypes and under various growth conditions. Collectively, a lower μOD than μCFU was found to be common, which indicated the growth associated cellular changes might occur.

A decay rate introduced into the logistic model offset the decay effect

Considering the cellular changes that accompanied growth, a modified logistic model is proposed in the present study by introducing a novel parameter, the decay rate. The theoretical revision differed from the previous study that applying a numeral calibration of the measurements [32]. The logistic equation is the most popular model that is used to represent bacterial growth dynamics. This equation is commonly applied to fit growth curves based on optical turbidity, especially in systems and computational biology to understand the dynamics of living systems. Considering the decay effect in OD600 during population growth, the logistic model was revised. A new parameter, the decay rate (d), was defined, which has the same unit of h− 1 as the growth rate.

Logistic model:
$$ N(t)=\frac{K}{1+\frac{K-N0}{N0}\times {e}^{- rt}} $$
Modified logistic model:
$$ N(t)=\frac{K}{1+\frac{K-N0}{N0}\times {e}^{-r\left(1- dt\right)t}} $$

where N0, K, r, and d represent the initial cell concentration, saturated cell concentration, growth rate, and decay rate, respectively.

To evaluate whether the modified logistic model was applicable, a large number of growth data sets were fitted to the two logistic equations. A total of 710 precisely measured growth curves from 29 different E. coli strains in either rich (Luria-Bertani broth, LB) or poor (M63) medium were subjected to the theoretical fitting. The histograms of parameter K estimated by the two models were completely overlapped (Fig. 3a). However, the histograms of the growth rate, r, were different between the two models (Fig. 3b). The mean growth rates estimated by the modified logistic model were larger and with a larger variation. The results indicated that the addition of the decay rate d in the logistic model did not influence K, the saturated population density or the carrying capacity, but contributed to the growth rate r independent of the nutritional conditions for population growth (Additional file 1: Figure S2).
Fig. 3
Fig. 3

Growth parameters estimated by the two logistic models. a. Histograms of the saturated density K estimated by the two models. b. Histograms of the growth rate r estimated by the two models. Transparent blue and orange colors represent the theoretical fitting of experimental data with the logistic and modified logistic models, respectively. The number of growth curves is also indicated

Intriguingly, the modified logistic model presented improved goodness of fit compared to the original model. The residual errors, which were designated as the sum of the squared errors (SSE), of fitting the total 710 growth curves to the modified logistic model were smaller than those from the original model (Fig. 4a). Thus, the goodness of fit (R2) was better for the modified logistic model (Fig. 4b), independent of either the genotype or medium (Additional file 1: Figure S3). The results showed that the modified logistic model better explained the growth dynamics of bacterial cells, which strongly indicated that the revision of the logistic model was theoretically practical. Considering the fact that the increase in OD600 was decided not only by exponential changes in the number of cells but also by unclear changes in the cellular contents, such as the cell size and macromolecular abundance, revision of the logistic model by introducing an additional parameter of the decay rate was also biologically reasonable.
Fig. 4
Fig. 4

Improved fitting efficiency of the modified logistic model. a. A comparison of the fitting residual errors between the two models. The fitting errors are represented by the sum of squares error, SSE. b. A comparison of the goodness of fit between the two models. The goodness of fit is represented by the coefficient of determination, R2. The broken red lines indicate the equivalent fitting efficiency of the two models. The number of growth curves used is also indicated

A correlation between the decay rate and the genome reduction in a nutritional dependent manner

Interestingly, a correlation between genome reduction and the decay rate was observed when applying the modified logistic model to the experimental bacterial growth data. Fitting the growth data of the reduced genomes to the modified logistic equation, as described above, resulted in the estimated constants of r and d, which are the growth and decay rates, respectively. Both the mean growth rates and mean decay rates of the repeated growth assays (N = 12~ 28) were calculated for a total of 29 strains (Nos. 0~ 28). The results showed that a decrease along with a genome reduction was detected not only in the growth rates but also in the decay rates (Fig. 5a). The larger the genome reduction, the lower the detection of decay. This finding was supported by the fact that the changes in growth rates evaluated by OD600 and CFU were smaller with the genome reduction (Fig. 5b). Fewer changes between μOD and μCFU resulted in a smaller decay effect in OD600. Reduction of the genome size might change the cellular properties that are linked to population growth.
Fig. 5
Fig. 5

Correlation between the genome reduction and decay rate. a. Genome reduction dependent changes in both growth and decay rates. The mean growth rates (r, upper) and mean decay rates (d, bottom) are a result of the fitting of the growth curves in M63 with the modified logistic model and are shown based on the order of the strain No. The genomes of strain Nos. 1~ 28 stand for reduced genomes, and No. 0 indicates the wild-type genome W3110. The standard errors of the growth curves/tests (N = 12~ 28) of the same strain are indicated. The broken lines in red represent the linear regression. b. The difference between the growth rates evaluated by CFU and OD600. The growth rates evaluated by OD600 and CFU are indicated as μOD and μCFU, respectively. The changes in growth rates were calculated according to the results from Fig. 2c. The reduced genomes are shown as strain Nos. 7, 14, 20 and 28 in the order of the length of the genome reduction from short to long

A correlation between the growth rate and genome reduction has been previously reported according to the manual calculation [34]. The same conclusion was drawn from the theoretical fitting suggested here, and the modified logistic model was applicable. Notably, an additional conclusion of the correlation between the decay rate and genome reduction was drawn based on the modified logistic model. The Pearson correlation coefficients of the genome size to the decay rate were highly significant (cor = 0.684, p = 4e-5) and were comparable to the growth rate (cor = 0.772, p = 6e-7). This result indicated that the changing cellular features that accompanied the population growth disturbed the optical properties. Note that the decline in the decay rates of the reduced genomes was significantly detected in the cell growth in the M63 medium but not LB medium (Additional file 1: Figure S5), which indicated that the nutritional richness affected the significance of the cellular changes that contributed to the decay rate. This finding agreed with the result that the difference of the fitting goodness between the two models was slight in LB but significant in M63 (Additional file 1: Figure S3).

The decay rate was partially attributed to the changes in cell size

As the decay rate of the reduced genome was much smaller than that of the wild-type genome (Fig. 5), we investigated whether any biological features could be identified to explain the decrease in the decay rate. As the growth rate is often discussed with cell size [35] and the genome reduction was found to somehow contribute to the change in cell size [34], growth accompanying changes in cell size might be linked to the decay rate. To verify the assumption, cells carrying either the wild-type (No. 0) or the reduced (No. 28) genomes were cultured in M63 medium, and the size distributions at a varied population density were analyzed. Since the cell size of an identical population often showed a large variation (Fig. 6a), the median of the cell size of the population was used as a representative parameter [36]. The results showed that the median cell size was smaller compared to the increase in population density (Fig. 6b, triangle). The feature of a higher population density linked to a smaller cell size was clearly identified in the wild-type genome, but not in the reduced genome (Fig. 6b, circle). This result suggests that the population density dependent size effect became insignificant due to genome reduction, consistent with the findings of the decay rate, and significantly declined in the reduced genome (Fig. 5). Thus, cell size changes of the growing population might be one of the reasons that cause the decay effect in OD600. Population density dependent changes in cell size were supposed to happen during the stationary phase due to nutritional depletion [35, 37]; however, the results showed that the changes in cell size also occurred even in the exponential phase. This result agrees well with the temporal decrease in the ratio of OD600/CFU from the exponential phase (Fig. 2a).
Fig. 6
Fig. 6

Relationship between the cell size and population density. a. Size distribution of an identical cell population. A size distribution of more than 10,000 E. coli cells growing exponentially in M63 is shown as an example. b. The relationship between the population density and cell size. E. coli cells of either the wild-type (No. 0, triangle) or the reduced (No. 28, circle) genomes were grown in M63. The cell size of the culture at various population densities was measured, and the median size of the cell population was used for analysis. The red broken lines represent the exponential regression

Discussion

Growth assay on an assortment of E. coli strains observed a common feature of lower μOD than μCFU. This result was attributed to the repressed increase in the OD600 value during population growth, which suggests that the changes in the cellular features were not always strictly correlated to the changes in cell number or even during the exponential growth phase. This experimental finding raised the question of whether the theoretical models that use the reads of optical turbidity properly describe bacterial growth. Because the temporal assay using OD600 is convenient and because it is easy to perform continuous reads in theoretical studies, a revision of the existing growth model through a consideration of the decay in OD600 was examined for the first time. In comparison to the original model, the revised logistic model proposed in the present study showed a better fitting goodness, indicating that this modified growth model was practical.

In addition, although the parameter of r is known to be a constant value in the logistic model, the growth rate of μOD was somehow inconstant during the exponential phase when monitoring by the microplate reader (Additional file 1: Figure S4), probably due to the decay effect, which was consistent with the finding that the increase of OD600 was slower with population growth in comparison to that of CFU (Fig. 2a). Therefore, the parameter of r in the logistic equation, which presents the exponential changes of a population increase, might represent the growth rate of μCFU and changes in the number of cells without considering changes in cellular features. Because the logistic model was widely applied to growth data based on reads of OD600, the additional decay rate, which compensated for the decrease in μOD, met the decay effect and contributed to the effective logistic fitting of bacterial growth based on optical turbidity.

Systematic analyses on the growth dynamics of the E. coli cells holding the reduced genomes led to a new finding on the correlation of the decay rate to genome reduction. This finding evidently revealed the biological impact of the revision of the logistic model by incorporating the decay rate (d), which provided a better understanding of the bacterial growth dynamics in depth. Further investigation on the changes in cell size accompanied growth experimentally demonstrated the biological basis of the newly introduced parameter of the decay rate. The optical turbidity might reflect both the cell number and cell size. The decay rate (i.e., decay effect in optical turbidity) could be partially explained by changes in the cell size/volume accompanied by the population increase, and the significance of the cell size-mediated decay effect was genome/strain dependent. The modified logistic model included an additional parameter considering the cellular features, such as the cell size, to compensate for the original logistic model, which is often applied to population growth with the quantitative unit of the cell number.

Conclusions

The present study reconfirmed the methodology mediated variation in growth rates and provided the first example of that the precise growth analysis could bring new findings in bacterial growth. In summary, a decay effect in the bacterial growth rate evaluated by optical turbidity was detected according to the differentiation in growth rates caused by variations in methods. To compensate for the decay effect in OD600 reads, the commonly used growth model of the logistic equation was revised by introducing a new parameter, the decay rate, which was found to be dependent on both the genotype and medium and was partially attributed to changes in cell size. These new findings reveal the biological impact of considering the decay effect in the bacterial growth rate evaluated by optical turbidity. The novel finding of the correlation between genome reduction and the decay rates is highly intriguing and requiring further investigation. In addition, whether the decay rate is universal in bacteria is also a highly interesting question required to be addressed for a better understanding of bacterial growth dynamics.

Methods

Strains and media

The E. coli strain W3110 and its derivative strains [33, 34] used in the present study were acquired from the National BioResource Project (NBRP) of the National Institute of Genetics (NIG), Japan. E. coli cells were cultured in minimal medium M63, which contains 62 mM dipotassium hydrogenphosphate, 39 mM potassium dihydrogen phosphate, 15 mM ammonium sulfate, 15 μM thiamine hydrochloride, 1.8 μM Iron (II) sulfate, 0.2 mM magnesium sulfate, and 22 mM glucose. Preparation of the M63 medium was previously described in detail [27]. The colony formation was detected using LB broth agar, Miller (Sigma Aldrich).

Bacterial growth in the test tubes

A total of 43 mL of M63 medium was placed in a 50 mL Falcon (Watson) tube in which 100 μL of the E. coli glycerol stock stored at − 80 °C was added and well mixed using a vortex. A total of 5 mL of the mixture was dispensed into eight sterilized glass tubes and cultured at 37 °C and 200 rpm using a bioshaker (Taitec). The culture was temporally sampled from the late lag phase to the early stationary phase to detect the growing population using three different methods that relied on the physical, biological and chemical properties of bacterial cells, i.e., the optical turbidity, colony formation, and ATP abundance. Sampling was conducted by taking 1.2 mL of the culture from two out of eight glass tubes, and 1 mL of the sampled culture was placed in a cuvette to measure absorbance at OD600 (Beckman DU730), and the remaining volume was used for the other two assays. Time sampling was performed rotationally among a total of eight glass tubes, which led to a single growth curve based on the OD600 value. This time course of bacterial growth was conducted repeatedly (N = 3~ 5). The biological replications varied from the initial pre-culture.

Colony forming unit (CFU) assay

The colony formation (CFU) assay is a method of estimating the number of viable bacteria in a culture solution by counting colonies on the assumption that a microorganism colony that appears on agar medium is derived from one cell. According to the value of OD600, multiple dilution rates of the sampled culture, which varied in order, were performed to obtain 10 to 500 colonies per plate on which 100 μL of the diluted culture was plated. The media used for the dilution and the plating were M63 and LB, respectively. The plates were cultured overnight in an incubator (Yamato) at 37 °C, and then, a colony count was performed. At least four plates were used for each sampling point, and approximately 40 plates were used for a single growth curve based on the CFU. Three to five biological replications of the growth curves were performed for each strain or culture condition, which resulted in the consumption of approximately 2000 LB agar plates in the present study.

Measurement of the cellular ATP concentration

Six different concentrations of the ATP solutions were prepared for the standard curve by diluting 10.4 mg/mL ATP (Roche) 104~ 109-fold with M63 medium. After placing 100 μL of M63 medium or the six ATP solutions in 1.5-mL microtubes, 100 μL of BacTiter-Glo ™ Microbial Cell Viability Assay solution (Promega) was added to each microtube according to the manufacturer’s instructions. The fluorescence intensity was measured to prepare a calibration curve. A total of 10, 20, 50, and 100 μL of each sampled culture was measured similarly to estimate the amount of ATP in the growing cells. Based on the calibration curve, the cellular ATP concentration was determined. A growth curve based on the ATP concentration was made to calculate the growth rate.

Calculation of the growth rate

Growth curves based on three different methods were created according to the temporal measurements of OD600, CFU, and/or ATP as described above. A simple exponential regression toward the exponential growth phase in the growth curve was performed as follows.
$$ {N}_i={N}_0{e}^{\mu {t}_i} $$
where N, t and μ represent the population density (cell concentration), time (h) and growth rate, respectively. Regression resulted in an exponent of the exponential slope as the growth rate (h− 1). The growth rates calculated from the growth curves of OD600, CFU and ATP were named μOD, μCFU and μATP, respectively.

Detection of the cell size

The cell culture (glycerol stock) was repeatedly diluted twofold with M63 medium, which led to a series of dilution rates from two to 1028-fold. A total of 2 mL of the diluted cell mixtures was loaded on a 24-well microplate (Iwaki). The microplate was incubated for 12 h in a microplate mixer (Taitec) with a rotation rate of 500 rpm at 37 °C as described previously [38]. All of the wells (cell cultures) were subjected to measurements by both optical turbidity and a cell counter to reach a correlation between the OD600 and the mean cell size of the cell population. OD600 was measured using a 1 mL cuvette as described above. The cell size (volume) of the growing E. coli cells were measured using a cell counter (Beckman, Multisizer 4) as described previously [34]. Each culture (well) was measured individually. The median size of 3000~ 30,000 cells in the culture (well) was calculated and used as the representative cell size of the culture, which provided a precise correlation between cell size and OD600 of the same cell population (culture).

Bacterial growth in a 96-well microplate

Glycerol stocks of the E. coli cultures collected at the early exponential phase (OD600 < 0.05) were diluted 100- to 1000-fold in M63 medium and well mixed using a vortex. The diluted cell mixture was loaded onto a 96-well microplate (Costar) in multiple wells at varied locations with 200 μL of mixture per well as previously described [27]. The 96-well microplate was incubated in a plate reader (Epoch2, BioTek) with a rotation rate of 600 rpm at 37 °C. Bacterial growth was detected at an absorbance of 600 nm and read at intervals of 5 min. The growth rates were calculated from every two reading points in a growth curve and according to the following equation.
$$ \mu =\ln \left(\frac{C_j}{C_i}\right)/\left({t}_j-{t}_i\right) $$
where Ci and Cj represent the two reads of OD600 values at two time points of tj and ti, respectively, which were discontinuous at an interval of 1 h (i.e., every 20 intervals), although the reads were at intervals of 5 min. Such discontinuously calculation largely masked the noisy records potentially occurred during the short interval measurements.

Computational analysis of the bacterial growth

The theoretical models for bacterial growth were evaluated using Python. The logistic and modified logistic models were fitted with 710 growth curves of 29 E. coli strains of various genome sizes growing in 96-well microplates. The raw data sets of these growth curves can be found at Springer Nature Research Data Support and can be accessed online via the following URL: https://doi.org/10.6084/m9.figshare.5918608. The details regarding the determination of the growth data set was previously described [27, 34], and the data sets of growth in M63 and LB media were used in the present study. Evaluation of the models (goodness of fit) was assessed based on the sum of squares, which were calculated according to the following equations.
$$ SSE=\sum {\left({y}_i-{\widehat{y}}_i\right)}^2 $$
$$ {R}^2=1-\frac{SSE}{SST},\kern0.5em SST=\sum {\left({y}_i-\overline{y}\right)}^2 $$

where SSE, SST and R2 represent the sum of squared errors, the sum of squares total, and the coefficient of determination, respectively. The script for the model regression can be freely requested at the following URL: http://www.trios.tsukuba.ac.jp/researcher/0000003489.

Abbreviations

ATP: 

Adenosine triphosphate

CFU: 

Colony forming unit

E. coli : 

Escherichia coli

LB: 

Luria-Bertani

OD600 : 

Optical density at a wavelength of 600 nm

SSE: 

Sum of the squared errors

Declarations

Acknowledgments

We thank the National BioResource Project and the National Institute of Genetics (Shizuoka, Japan) for providing the E. coli strains and the lab members for fruitful discussions.

Funding

This study was partially supported by the Tsukuba Basic Research Support Program (Type B). The funder had no role in the study design, data collection and interpretation or the decision to submit the work for publication.

Availability of data and materials

The raw data sets of the growth curves, which were used for the theoretical fitting, can be found at Springer Nature Research Data Support and can be accessed online via the following URL: https://doi.org/10.6084/m9.figshare.5918608.

Authors’ contributions

KT, MK and KA performed the experiments; YYC, TY and BWY performed the analyses; BWY conceived the research and wrote the paper. All authors read and approved the final manuscript.

Ethics approval and consent to participate

Not applicable.

Consent for publication

Not applicable.

Competing interests

The authors declare that they have no competing interests.

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Authors’ Affiliations

(1)
School of Life and Environmental Sciences, University of Tsukuba, 1-1-1 Tennodai, Ibaraki 305-8572, Japan
(2)
Institute of Biology and Information Science, East China Normal University, 3663 Zhongshan Road (N), Shanghai, 200062, China

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