Achieved results will be first discussed separately for each reactor, and thereafter, they will be compared and interconnected.
CSTR R1
R1 of the 5CSTR cascade is devoted to balanced biomass growth and cell division. C. necator DSM 545 is characterized by considerable PHB synthesis when exposed to excess carbon source even without simultaneous nitrogen and/or phosphate limitation. TEM pictures of the culture from R1 were successfully processed by ImageJ software to facilitate cell and granule counting and to enable distinguishing and measuring of footprint areas of cells and PHB granules. Digital imaging turned out to be a convenient method to convert to binary (black/white) images (Fig. 1, upper left and related right group of four pictures). Applying this procedure, all blurred silhouettes of cells that were not in focus of the microscope were removed in order to correctly interpret the ImageJ results: only those objects with sharply outlined edges of cells and the corresponding PHB granules were taken into account. In Fig. 1 (upper left group of four pictures), some cells are visible that are in late stage of cell division, as well as pronounced elongated cells without clear evidence of septum formation. Both of these cell types were counted as one individual cell, until the clear separation of daughter cell from mother cell occurs. It can be seen that in all these cells, PHB granules are not bigger and not higher in number per cell than in average. For typically elongated cells without clear evidence of a septum, it was difficult to state about their “status,” e.g., are these cells in division process with (for unknown reason) stopped septum synthesis or do these cells (trichomes!) have interrupted nucleoid division, as described by Jendrossek et al. (2007) and Wahl et al. (2012). Elongated cells with higher number of PHB granules than average but with significantly bigger PHB granules than presented in Fig. 1 were evidenced for cultivation of C. necator H16 by Mravec et al. (2016). It is not clear if this difference between results of Mravec et al. (2016) and the work at hand results from intrinsic strain properties. Here, it is necessary to mention that Mravec et al. (2016) hypothesize that there is no evidence for a direct control between cell size and number of PHA granules and suppose that “both PHA biosynthesis and cell length are influenced by the same factors (e.g. nutrient limitation).”
As the ImageJ software offers an opportunity for the determination of minimal, maximal, and average size of sharply edged objects of whole cell populations, it was used for statistical analysis of imaged footprint areas of whole cells, PHB granules, and the number of granules per cell (Table S1). In this reactor, 55.8 % of cells contained PHB granules, 30.9 % were equipped with one granule, and 17.3 % with two granules. It was very interesting to analyze the position of granules for the mentioned two groups of cells. When two small granules were found, they were dominantly located close to the nucleoid (frequently on opposite sites and rarely on the same side). This is in accordance with findings of Wahl et al. (2012) for R. eutropha H16 but different to results for B. indica achieved by Jendrossek et al. (2007) where the granules were located at the cell poles. In the same analysis, it was observed that those cells harboring one PHB granule are characterized by relatively large granules, presumably because 5.88 h of τ for R1 is long enough to provide the progression of PHB biosynthesis. These granules were large enough to be at the same time instantaneously in the vicinity of the nucleoid as well as close to the plasma membrane, so a connection with the plasma membrane cannot be deduced.
Resulting values of interdependence of cell/granule sizes for R1 and related distributions are presented in Figs. 2, 5, and 6. At first, it was intended to find out if the size of granules correlates to the size of cells and if the number of granules per cell depends on the cell size. Figure 2 (left picture) presents results obtained by correlating the PHB granule size to the whole cell size. Here, it is well visible that a clear correlation only exits for relatively small cells (<0.8 μm2), whereas with increasing cell size, scattering of results enormously increases. This is valid for both applied best fit straight lines (with and without forcing to the origin of the coordinate system). The “origin included” straight line refers to the assumption that PHB granules grow in parallel with cellular growth, whereas the “origin excluded” straight line hypothesizes that a certain cell size must be achieved before PHB synthesis starts. Because of the only minor difference between the Pearson’s correlation coefficients obtained for these two lines (R
2 = 0.2434 and 0.215, respectively), it is not easy to conclude which of the two assumptions more realistically reflects the real situation. In addition, the rather low values of these coefficients indicate the high heterogeneity (in terms of the ratio of PHB granule size to cell size) of the bacterial population growing under nutritionally balanced conditions. Furthermore, the number of individual granules per cell cannot be related to the cell size for the balanced cultivation condition present in R1. Here, the number of granules per cell rarely exceeds the value of 3. Cells without PHB, as well as with one, two, or three granules, are practically uniformly distributed among the whole size range of cells (Fig. 2, left picture, triangle symbols).
CSTR R2
R2 acts as a “transient reactor” where the nitrogen source added to R1 gets finally depleted. Therefore, some cellular growth is still possible in R2, but the cells undergo a considerable change regarding their intracellular metabolic fluxes from biomass synthesis to PHB production. Again, TEM images of the bacterial population in R2 (Fig. 1, lower group of three pictures, left) were processed to binary images (Fig. 1, lower group of three pictures, right). In contrast to R1, both cell types, i.e., long cells with relatively small PHB granules and long cells with PHB granules close to average dimension, are present. The latter cell/granule type was also found by other authorships, e.g., Jendrossek et al. (2007), Wahl et al. (2012), and Mravec et al. (2016)). Similar to R1, results of measuring footprint areas of whole cells and PHB granules (Table S2) were used for statistical analysis. Sufficiently sharp and clear binary images were advantageous to distinguish between PHB and the residual cell fraction. Figure 2 (right picture) shows that the number of PHB granules per cell (i.e., 0–3) is homogenously distributed among the whole range of cell sizes, but the footprint area of PHB granules, if compared to the footprint area of whole cells, was significantly enlarged (Fig. 1). Less variance of results for the interdependence of PHB granule areas and related cell areas in R2 (Fig. 2, right picture) is observed than in R1 (Fig. 2, left picture). This is reflected by the values of the Pearson’s correlation coefficients obtained for the straight lines (R
2 = 0.5238 if including the origin of coordinate system and R
2 = 0.5770 without inclusion of the origin, respectively). Although at a first glance an interdependence of the mentioned variables seems to be obvious, the relatively low values of both correlation coefficients warn for vigilance. However, based on Fig. 2 (right picture), it can be concluded that PHB granules are exclusively visible in such cells of footprint areas exceeding 0.2 μm2.
CSTR R3
R3 is the first reactor along the cascade where no more growth of cells, but intensive PHB synthesis is expected. TEM images of the bacterial population from reactor R3 (Fig. 3, upper row, two pictures at the left) were transformed to binary images (Fig. 3, upper row, two pictures right) and statistically analyzed for footprint areas of whole cells and PHB granules (Table S3). In R3, the footprint area of PHB granules is already dominant over the footprint area of the PHB-free cell fraction. Here, it is striking that the number of elongated cells decreases if compared with R1 and R2; the cell shape becomes more ellipsoidal. Results presented in Fig. 4 (left picture) and Table S3 indicate that among the investigated cell size range, cells with zero or three PHB granules vanish in favor of cells harboring one or two granules (Fig. S1). This can be interpreted by the assumption that with increasing τ, those cells which in R1 and R2 were still PHB-free start to accumulate granules in R3, and those with three granules disappear because of steric hindrance of granules; here, granules seem to merge in only one carbonosomal space. If compared to the outcomes of R2, the variance of results for correlation of PHB size and cell size is slightly lower in R2, with somewhat higher Pearson’s correlation coefficients in R3, i.e., R
2 = 0.5867 with the origin included and R
2 = 0.6297 with the origin excluded, respectively. In addition, similar to the findings for R2, it is remarkable that granules are predominantly present in cells of footprint areas exceeding 0.2 μm2.
CSTR R4
TEM images of bacteria collected from R4 (Fig. 3, central row, two left pictures) were converted to binary formats (Fig. 3, central row, two right pictures). Statistical analysis was performed as described for R1–R3 (Table S4 and Fig. 4, central picture). These illustrations clearly show that the majority of cells contain one single big granule (52.3 % of all cells, 56.1 % of the individuals containing granules); most other cells contain two granules (24.4 % of the whole population), whereas cells with zero or three granules are rare. If compared with other reactors, the scattering of results related to dependence of PHB footprint area on the whole cell area (Fig. 4, central picture) is significantly lower, as indicated by Pearson’s correlation coefficients R
2 = 0.7662, if including the origin point of coordinative axes, and R
2 = 0.8119, if excluding the origin. Also for R4, it turned out that the majority of cells containing PHB granules have a footprint area exceeding 0.2 μm2.
CSTR R5
By analyzing the results presented in Fig. 3 (bottom row), Fig. 4 (right picture), and Table S5, it can be concluded that the number of PHB granules in the cells in most cases does not exceed the value of two. Notably, the footprint area of PHB granules, if compared to the whole cell’s area, is significantly higher than in the previous reactors R1–R4. The scattering of results presented in Fig. 4 (right picture) by correlation coefficients of R
2 = 0.8572 (origin point included) and R
2 = 0.8847 (origin excluded) is significantly lower than in all other reactors, indicating the high correlation between the two area types (PHB and PHB-free area).
Comparative analysis of results for all reactors of the five-stage CSTR system
Statistical distribution of cell size (expressed as the footprint area of cells present in the 5CSTR devoted to production of PHB by C. necator in binary images) is presented in Fig. 5. The same was accomplished for PHB granule sizes (Fig. 6). Minimal, maximal, and average values of whole cell footprint areas as variables dependent on τ in the 5CSTR are shown in Fig. 7 (left picture). The same was accomplished for PHB granule areas (Fig. 7, central picture) and for the PHB-free parts of the cells (Fig. 7, right picture).
Concerning statistical distributions of cell sizes (Fig. 5), it can be concluded that the shape of distribution functions is fluctuating along the 5CSTR. The range of footprint areas of whole cells is 0.02–1.5 μm2. This variable can successfully be depicted by the log-normal distribution for reactors R1–R3 and for R5, whereas the population in R4 displays a slightly different characteristic. Here, small cells are present at relatively high share, and normal distribution best reflects the situation. Nevertheless, concerning the irregularity in height and disposition of the illustrated bars (Fig. 5, picture R4), this distribution appears rather questionable. In general, the comparison of cell size distribution along the 5CSTR leads to the conclusion that cell size is increasing with increasing τ (indicated by the increasing width of the distribution function on the right side towards higher values along the cascade). Similarly, footprint area values for maximal and average cell size by trend increase with increasing τ (except for the discrepancy observed for R4), and the approaching of a finite maximum value, pre-defined by biological and geometrical constraints, seems to be very likely. Regarding minimal values of cell sizes estimated in the 5CSTR, it is not possible to unambiguously conclude, due to its narrow range, if this variable has a tendency to increase with increasing τ.
A slightly different situation occurs for the size of PHB granules (Fig. 6). They are distributed according to a log-normal distribution (R2, R3, and R5) and according to a gamma distribution in the case of R1 and R4. Here, R4 features an exception by the striking presence of small granules, probably related to the share of small cells (see leftmost bar in Fig. 6; R4). This bar (and the irregularity in bars height through the size range) raises the questions about significance and validity of such distributions. In general, the footprint areas of PHB granules are in the range of 0.01 to 1.2 μm2. It can be seen that in R1 the share of small PHB granules is dominant, whereas in all other CSTRs, we witness a domination of big granules. The increasing of shape width of the distribution function towards the right side (i.e., towards higher values for PHB shape area) along the reactor cascade is also evident. This is in excellent agreement with the technological designations of the individual stages of the 5CSTR (R1, nutritionally balanced cellular growth; R2, transient reactor for metabolic switch; R3–R5, PHB synthesis under growth limitation). Analogous to cell size, the footprint area values for maximal and average PHB granule size (Fig. 7, central picture) by trend increase with increasing τ, but, moreover, they tend to approach a finite maximal value, indicating that the rise of PHB content in the cell volume is slowing down along the 5CSTR, probably by the action of spatial limitation. A certain discrepancy for R4 is also observed regarding average and maximal granule size. Values for minimal PHB granule size are very similar (Fig. 7, central picture), thus hampering the conclusion if they increase or not with increasing τ.
After the separate analysis of cell size and PHB granule size, it was a logical step to investigate the ratio of these variables along the 5CSTR. For this purpose, the ratio of related sizes was expressed as the ratio of footprint areas estimated from binary images. It can be concluded that the ratio of PHB granule to cell size is increasing until R5 (results not shown). The average value of PHB-free footprint areas by trend slightly declines with higher τ (Fig. 7, right picture). This trend is also visible for the minimal and maximal values of this variable. Such results had to be expected, as the free space in cells gets more and more “occupied” by the synthetized PHB during the time cells move further through the 5CSTR, especially in growth-limited reactors R3–R5. Special attention should be devoted to Fig. 8 which comparatively visualizes how the average value of whole cell’s footprint area linearly increases with increasing τ. Simultaneously with the progression of τ, the average value of PHB granule area is rising in accordance with logarithmic progression, so the remaining free space in cells is decreasing. At first, the ratio of footprint areas related to PHB and whole cells significantly increases (R1 and R2); thereafter, the increase slows down (R3 and R4), and, finally, the ratio reaches a constant value (R5).
An additional attempt was made to detect the correlation between experimentally determined volumetric PHB productivity [g/(L h)] and productivity determined by footprint areas related to PHB granules (Fig. 9). In Fig. 9 (left picture), data for R4 are excluded. During the experiment, in reactor R4, a period of low glucose concentration occurred; this period includes the time point 232 h, when samples for preparing the TEM pictures were taken. This fact has significantly influenced PHB synthesis, very likely explaining why data related to this reactor show so much deviation if compared with the others. Excluding these data drastically enhances Pearson’s correlation coefficient R
2 from 0.0071 (results not shown) to 0.8863 (Fig. 9, left picture). A similar result was obtained when the specific growth rate μ [g/(g h)], determined by gravimetric analysis, was compared with μ [μm2/(μm2 h)] estimated by footprint area analysis. In this case, R
2 values amounted to 0.0507 (results not shown) and 0.8970 when data for R4 were excluded (Fig. 9, right picture).
Results summarized in Table 1 allow comparing μ and π obtained by two different methods: by standard gravimetric procedure and by estimation of footprint area binary images. Independent on the applied method, μ estimated for R1 (0.17 h−1) was highest among all reactors, with an excellent agreement between both approaches. This result is a strong indication for the correctness of assumed linear relationship between real cell/granule sizes and related measured areas (i.e., its shape size) on binary images. This is well in accordance with results presented by Mravec et al. (2016), achieved by a similar technique. Based on these results, μ in continuous systems can in the future be simply and quickly estimated by digital imaging of stained cells/granules and by size estimation using appropriate software like ImageJ. For that purpose, the testing and comparison of light microscopy results with TEM technique should be performed. For other reactors than R1, values for μ are practically zero, independent on the applied method of estimation. This is in good relation with the central idea about the function of the individual stages of the 5CSTR system. Results for π obtained by the two different methods (Table 1) cannot display the same numerical values, because they differ in units. To still achieve comparable results, the footprint area of cells and PHB granules obtained from SEM pictures should be related to the volume of cells/granules first and, thereafter, should be multiplied by estimated densities of related materials. After that, π can be calculated as usual and compared with gravimetrically obtained data. Because of cell shape changes observed along the cascade (they were more similar to an ellipsoide than to cylinder), it was not possible to approach the cell volume by cylinder volume as shown by Mravec et al. (2016). So, in our case, it was not possible to calculate volumes; hence, π cannot be converted to mass units.
In addition to the cells and granule sizes, it was interesting to track the number of granules per cell along the cascade; related results are presented in Fig. S1. Under the cultivation conditions applied, the number of PHB granules per cell rarely exceeds three. The average number of granules per cell was less than two (in the range 1.59–1.81 for all reactors; see Table 1). Only in a few cases that five, six, or maximum seven PHB granules were evidenced. This is in contrast to the findings of Mravec et al. (2016) who reported that the average number of granules per cell during the PHA accumulation phase varied between 10 and 15 and neither in accordance with the results of Anderson and Dawes (1990) (10 granules on average) nor with the findings of Tian et al. (2005). Furthermore, Wahl et al. (2012) reported that PHB granules were “formed in aggregated clusters of in average 2–6 granules in most cells,” but, after 1 h of cultivation under conditions favoring PHB synthesis, the number changed to 12 granules for R. eutropha H16 or 1 to 4 granules for R. eutropha HF39, respectively. It cannot be deduced if this difference is a consequence of intrinsic strain properties (PhaM and PhaP5 regulations) or, less probably, the result of the cultivation technique. In Fig. S1 (supplementary file), it can be seen that the fraction of PHB-containing cells increases with τ in the system, reaching a maximum of 94.6 % in the population in R5. Interestingly, the fraction of cells with one PHB granule (among all cells harboring PHB) changes through the reactor system (maximum of 63.6 % reached in R3, then decrease to 33.7 % in R5). The fraction of cells harboring two or three PHB granules shows an opposed trend than those with one granule: they reached its maximum in R4 and R5. This can be explained rather by additional granule formation in those cells harboring one granule (under PHB synthesis favoring conditions in R4 and R5) than by assuming a merging of granules. In TEM images of R4 and R5 cultures, cells with two or three granules of different sizes are often detected. In this context, it seems that the average number of granules per cell (in the range of 1.59–1.81 granules/cell for all reactors, with slight tendency to increase with increasing τ) does not change too much along the cascade. It happens because of the mutual “covering” of categories along the reactor cascade, because of successive shift from one category to another (caused by rising of τ and by shift of cell fractions with zero, one, two, or three PHB granules towards those with higher number of granules). This means that the shift to the next category is compensated by the shift from the previous category. Using only the results presented in the present work, it is not possible to unambiguously conclude if the PHB granules (i.e., the carbonosome complex containing PhaC1 synthase, different phasins PhaP1-PhaP7, PhaM protein, and PHA depolymerase enzymes) will merge after detaching from nucleoid in the late phase of synthesis.