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Applied and Environmental Microbiology, September 2005, p. 4998-5003, Vol. 71, No. 9
0099-2240/05/$08.00+0 doi:10.1128/AEM.71.9.4998-5003.2005
Copyright © 2005, American Society for Microbiology. All Rights Reserved.
Institute of Food Research, Norwich NR4 7UA, United Kingdom
Received 4 November 2004/ Accepted 29 March 2005
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For the sake of simplicity we will define the lag time for spores as the time from which a dormant spore is exposed to conditions suitable for growth to the start of exponential growth. Germination and outgrowth of spores follow an ordered sequence of steps (10). Initially, spores may be activated, which can increase their ability to germinate. Germination is an irreversible cascade of degradative steps using preformed enzymes in which a dormant spore is transformed to a metabolically active cell. During germination, spores rehydrate and irreversibly loose their extreme heat and chemical resistance. In suitable conditions, metabolism is initiated, and the germinated spores begin macromolecular synthesis and start to grow. Eventually, the spore coats are shed, and a young cell emerges. Synthesis continues until cells obtain the full complement of molecules found in adult cells. Mature cells continue to increase in size and proceed to cell division.
To date, kinetic studies have been concentrated on only one part of the lag time, germination. For example, Billon et al. (6) examined germination of individual proteolytic Clostridium botulinum spores. However, germination is only part of the lag time; the lag also includes outgrowth. Knowledge of all stages in lag and the relationships between these stages is necessary if mechanistic models are to be produced. The distributions of times associated with the various stages and the relationships between the stages have not been determined previously.
C. botulinum is a group of spore-forming anaerobic bacteria that produce the extremely potent botulinum neurotoxin, the causative agent of botulism (7). While food-borne botulism is rare, the severity of the disease means that the prevention of outbreaks is a major aim of regulators and industry. Nonproteolytic C. botulinum is a particular concern for the safety of mildly heat-treated, refrigerated foods (11). C. botulinum spores are widespread in the environment but are usually present at low concentrations (7). Consequently, any growth in food packs is likely to initiate from just a few spores. It has been shown that decreasing the number of spores increased the uncertainty of estimation of time to observable turbidity in broth inoculated with spores of nonproteolytic C. botulinum (17). The authors suggested that this resulted from spores having a distribution of germination times, with larger populations more likely to have at least one spore with a shorter germination time present to initiate growth. Quantifying lag times from individual spores is important not only for estimating times to growth from small initial numbers but also for estimating uncertainty. It has also been shown that variability in lag times of individual spores is an important component in risk assessment for products contaminated at low levels (5). Knowledge of the distribution of lag times for individual spores should help refine risk assessment for such foods. Such distributions cannot be derived from observations made at the population level; instead, they must be determined from studies of individual spores.
The aim of this work was to determine both the biovariability of individual spores of nonproteolytic C. botulinum strain Eklund 17B and the relationships between different stages in germination and subsequent growth. Previous studies of single spores have focused only on germination. In this study we examined the time to germination (tgerm), the time to emergence (temerg), the times to growth to the length of one (tC1) and two (tC2) mature cells, and the time to turbidity, as well as the relationships between these stages of C. botulinum spore outgrowth.
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Time to turbidity measurement.
The time to turbidity was studied using a Bioscreen C automated turbidity reader (Lab Systems, Finland) installed in an anaerobic cabinet. All manipulations were performed in the anaerobic cabinet under a headspace consisting of 5% carbon dioxide, 10% hydrogen, and 85% nitrogen. Spores were diluted to 20 ml1 in PYGS broth, and then 50 µl of the spore suspension and 350 µl of PYGS broth were dispensed into each of the 200 wells of the Bioscreen plates. Filled plates were placed into the Bioscreen C reader and incubated at 22°C for 2 days. Optical density at 600 nm (OD600) was measured, and readings for each well were taken every 10 min for 48 h. The time to detectable turbidity (tdet) was defined as the time taken for the measured OD600 to reach 0.14 U. Blank medium had an OD600 of around 0.10 U. The detection limit was 3 x 105 CFU ml1, as determined from a calibration curve of cell number versus OD600. The specific growth rate of nonproteolytic C. botulinum 17B in PYGS broth at 22°C was determined from plate count measurements obtained during exponential growth. Plate counts were determined from appropriate dilutions of cells spread on PYGS agar and incubated under a headspace consisting of 90% hydrogen and 10% carbon dioxide for 2 days at 30°C.
Slide preparation for microscopic observation.
Slides were prepared by placing a suspension of spores in a defined area on the surface of an electrostatically charged Superfrost Plus microscope slide to obtain a concentration between 1,200 and 3,000 spores mm2. After 30 min of contact time in a humid chamber at 1°C, each slide was washed in distilled water to remove any unattached spores, air dried in a fan-powered incubator at 30°C, and stored in an anaerobic cabinet for at least 16 h to remove any traces of oxygen from the slide. At time zero, the deoxygenated spores attached to the slide were overlaid with 8 µl of molten anaerobic PYGS medium containing 0.5% (wt/vol) agar. A coverslip (18 by 18 mm) was pressed onto the agar to create a thin film and was sealed in place with aluminum tape to prevent desiccation and oxygen ingress. The slide was transferred from the anaerobic cabinet to the microscope stage, and measurement was started.
Microscopy.
Spore outgrowth was observed by phase-contrast microscopy at a magnification of x40 (Leica x40/0.70 numerical aperture, PL FLUOTAR objective) with a Leica DMRB optical microscope. Samples were maintained at 22°C using a stage-mounted peltier device (Linkham Scientific Instruments, Tadworth, United Kingdom) with a temperature controller (Linkham PE60). The microscope was fitted with an XYZ stage (Marzhauser, Wetzlar-Steindorf, Germany) with an H128 motor controller (Prior Scientific Instruments, Cambridge, United Kingdom) controlled by Image-Pro Plus image analysis software (Media Cybernetics, Silver Spring, MD) so that the stage could be returned repeatedly to multiple set positions during each experiment. Images of each field of view were captured every 5 min for 15 h using a JVC KY-F70 three-charge-coupled device color digital camera. Individual images were compiled to give a sequence of frames for each field of view. This allowed the same spore to be monitored throughout the entire experiment. Spore data were collected from 11 replicate experiments.
Image processing.
The image sequences followed individual spores through dormancy, germination, emergence, elongation, and eventually cell division. The individual images were analyzed using Image Pro Plus image analysis software to determine the maximum pixel intensity and length of each spore or cell in each captured field of view. Images were sharpened to enhance intensity differences between neighboring pixels using two passes at strength 10 for a 7 x 7 kernel size and then outlined as objects with pixel intensities less than the mean background intensity minus three times the standard deviation. Each outline was checked by eye, and alterations, such as separation of touching objects or addition of nonoutlined areas, were made before the outline was saved. The outline was then overlaid on the raw image, and the maximum pixel intensity and the length of the object were measured.
Quantification of germination and outgrowth events.
For all measurements, time zero was defined as the time of nutrient addition. Germination was determined from when a spore changed from phase bright to phase dark, as measured by a decrease in pixel intensity. Maximum pixel intensity was plotted versus time and fitted with a linear triphasic model using Dmfit (www.ifr.ac.uk/safety/DMfit). The three lines represented the spore during periods of high (phase-bright), decreasing, and low (phase-dark) pixel intensity. Time to germination was defined as the time at the midpoint of the line representing decreasing pixel intensity. Time to emergence was defined as the time when a new cell was first observed emerging from the spore coats. Newly emerged spores do not contain the full complement of macromolecules found in adult cells and thus are smaller. The time to a mature cell was measured by determining the time that it took a cell to reach the length of a single mid-exponential cell in broth culture (found to be 5.5 µm in PYGS at 22°C). It was difficult to determine the time to cell division as septation and cell constriction were not always obvious microscopically; cells often appeared to elongate to many times their initial length before separation into multiple cells. It was decided that doubling time would be measured by determining the time that it took a cell to increase from the length of one mid-exponential cell to the length of two mid-exponential cells. DMfit was used to generate a best-fit curve for cell length versus time, and the times that it took to reach 5.5 µm and 11 µm were recorded as the times that it took to reach the lengths of one (tC1) and two (tC2) mature cells, respectively.
Statistical analysis.
The data sets were analyzed using an in-house program (Varifit) written in Visual Basic. The homogeneity of distributions was analyzed using a chi-square test, and a Bartlett test was used to compare the variances of the distributions. Pearson coefficients were calculated to study the correlation between growth event times and intervals during germination and subsequent growth.
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FIG. 1. Frequency distributions for tgerm, temerg, tC1, tC2, and tdet for single spores of nonproteolytic C. botulinum Eklund 17B in PYGS medium at 22°C.
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TABLE 1. Average times and standard deviations for events occurring during germination of, and subsequent growth from, spores of nonproteolytic C. botulinum Eklund 17B in PYGS medium at 22°C
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FIG. 2. Frequency distributions for times for germination (tgerm), outgrowth (tC1 tgerm), and first doubling (tC2 tC1) for spores of nonproteolytic C. botulinum Eklund 17B in PYGS medium at 22°C.
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TABLE 2. Pearson product moment correlations between pairs of variables representing times for events during germination of and subsequent outgrowth from spores of nonproteolytic C. botulinum Eklund 17B
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FIG. 3. Scatter diagram showing tgerm versus tC2 for spores of nonproteolytic C. botulinum Eklund 17B in PYGS agar at 22°C.
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The independence of different stages of lag phase indicates that the time for each stage is not related to a single factor but depends on many diverse factors. The lag phase for spores of nonproteolytic C. botulinum is a multistage process. Germination differs from other growth stages in that it is a series of degradative reactions in which preformed enzymes are used, while the later stages require macromolecular synthesis (10). It is likely that different metabolic processes are required at different times during emergence, outgrowth, and cell multiplication and also that these stages depend on nonmetabolic factors, such as the strength of the spore coat or the initial size or chemical complement of the spore. Adverse conditions or processes could add further complexity as they may affect each stage differently. For example, heat treatment is known to damage the spore germination system (13), and while the presence of oxygen does not affect germination of C. botulinum (15), it adversely affects subsequent stages that require active metabolism. This complexity ensures that mechanistic models have to be created specifically for spore inocula.
Strong correlations were found between the total times to different stages of the lag phase when the time for one stage formed a substantial component of the time for another stage. Correlation would be expected in these circumstances but does not necessarily allow one event to be predicted from the other. For example, tgerm was found to correlate strongly with tC2. The time to two cells depends on both tgerm and the time for growth from germination to two cells (tC2 tgerm). These intervals encompass different growth events and were shown to be independent of each other. The correlation between tgerm and tC2 depends on their relative magnitudes and occurs only when tgerm is a large proportion of tC2. Figure 3 shows that the correlation between tgerm and tC2 was strong only for slowly germinating spores, when an extended tgerm contributed a large proportion of tC2. The majority of spores (>50%) germinated within 1 h. For these rapidly germinating spores, tC1 was highly variable, ranging from 4.5 to 14.4 h, and correlated poorly with tgerm. Despite overall strong correlations, it is unwise to estimate time to late growth events from early growth events, such as germination, unless there is a mechanistic dependence.
Two independent methods were used to determine the shape of lag distributions in this study. Early stages in germination and outgrowth were measured using microscopy, and lag distributions were derived from times to detection in a Bioscreen automated turbidity reader. A previous study suggested that microscopy provided a more accurate estimate of Listeria monocytogenes cell lag times than the Bioscreen method (18). Using microscopy, individual lag times are determined directly. However, all spores are in a single chamber so they may interfere with each other, either spatially or chemically. With the Bioscreen method, spores are physically separated and thus unable to affect each other's lag times, but single lag times are not measured directly; the Bioscreen reader records detection times for populations originating from about one spore. Another difference between the methods was that turbidity measurements were made in broth media, whereas agar was added to the medium used in microscopic studies to keep individuals in a fixed location that allowed identification at multiple observation times. The time to a mature cell could be longer for attached spores in agar than for free spores in broth. Despite the differences between the two methods, the Bioscreen and microscopic methods produced distributions with very similar estimates of lag variability.
To predict individual lag times from the tdet measured by the Bioscreen method, it is assumed that growth in each well arises from a single spore, the time from lag to detection is constant in identical conditions, and the growth conditions are identical in all wells. If these assumptions are true, the measured tdet distribution should be the same as the desired lag time distribution, simply shifted in time (8). One assumption made in the consideration described above is that growth originates from a single spore. As samples were prepared by dilution, the number of spores per Bioscreen well would have followed a Poisson distribution, so not all wells would have contained a single spore. The size of the inoculum used in the Bioscreen analysis was a compromise between the percentage of wells with a single spore and the number of wells in which growth occurred giving a distribution of the detection times. The dilution used resulted in growth in only 70% of the observed wells, so according to the Poisson distribution ca. 30% of the wells contained no spores, 36% of the wells contained one spore, 22% of the wells contained two spores, and the rest of the wells contained more than two spores. Computer simulations showed that this composition of inocula would still allow estimation of the distribution of single cell parameters (results not shown). It is therefore a reasonable assumption that the measured distribution approximated the distribution that would have been obtained using single spores. The agreement was also demonstrated by the finding that the variance in the distribution of lag times measured by the Bioscreen method was the same as that obtained microscopically. If the lag distributions measured microscopically and by the Bioscreen method were identical and growth after lag occurs at a constant rate, then the tdet distribution should be the same as the tC1 distribution simply shifted by the time required for 18.2 doublings. The mean observed tdet was 23.6 h, compared to 25.7 h estimated from the mean time to one cell plus time for multiplication from one cell to a detectable population calculated using a population doubling time of 0.99 h. Although there is a discrepancy of 2.1 h, this value is small considering that the doubling time was extrapolated over 18.2 generations.
The population doubling time of 0.99 h measured in broth culture was much shorter than the mean time required for a new cell to double in length (tC2 tC1) (1.50 h). The relationship between the doubling time of a population (td) and the mean generation time of the single cells within that population (tg) is not straightforward and depends on the distribution of single cell generation times (4). In the special case of all cells having identical generation times, td is equal to tg. When single cell generation times are exponentially distributed, the population doubling time is much shorter than the mean generation time, and td = ln2 x tg (4). In most cases, populations have distributions somewhere between these two special cases, and td has a value between ln2tg and tg. Using tC2 tC1 as a measure of average single cell generation time and assuming that the observed distribution of generation times is maintained for all generations throughout growth, it is possible to simulate a growth curve and estimate the population doubling time. The estimated td in this experiment was 1.30 h, which gives an estimate for tdet of 31.2 h. The difference between the population doubling time measured during exponential growth and that calculated from cells observed immediately after lag could arise from differences in the measurement techniques, as mentioned above, but it could also be because the assumption that the generation time distribution remains constant throughout growth does not hold. Recent work has suggested that the average and spread of generation times decrease during the first three generations after lag (9, 14). Further examination of growth kinetics for generations soon after lag is required if the real shape of growth curves originating from single cells is to be determined and times for small increases in cell numbers are to be predicted.
Knowledge of individual spore lag time distributions is an important component in quantitative risk assessment and process risk modeling of products containing low numbers of spores (5) and also is necessary for improved prediction of population lag (2). Population lag is traditionally determined as the breakpoint from the stationary phase of log cell count against time and can thus depend on the initial count. The relationship between population lag and the average lag of the individual cells in the population is not simple and again depends on the distribution of single cell lag times. This distribution can be determined only from observations of times to growth from individual cells as population lag is a stochastic process from which the underlying distributions cannot be determined (3). Determination of lag phase distributions as observed in this study should help the development of more mechanistic models to predict bacterial growth.
The distribution curves determined in this study highlight the finding that there is considerable heterogeneity within spore populations. The shape of the distribution of germination times was skewed with a long tail and was similar to the shape of distributions previously reported for proteolytic C. botulinum (6). The asymmetry of the distribution implies that mean germination time is not a good parameter to use in risk assessment work as it underestimates the number of spores germinating at times shorter than the mean time. In the present study, the mean germination time was 2.6 h, but 50% of the spores germinated within 1 h. Information on the shape of the distribution curve should be useful in refining estimates of germination.
Food-borne botulism is an intoxication. Consequently, the time to toxin is of paramount importance in food safety. In the absence of direct toxin measurements, safety is usually estimated from the time to growth. Comparison of the times for germination, outgrowth, and doubling show that the time between germination and outgrowth to a full-sized cell is a large part of the lag in good growth conditions. Using germination time as an estimate of lag time underestimates times to growth. This study also showed the distribution curves for germination, and subsequent stages of growth were not simply projections of each other shifted in time, so later events cannot be predicted by adding a constant value to earlier values. Knowledge of spore germination kinetics alone cannot be used to estimate time to growth or time to toxin.
We thank József Baranyi for useful discussions.
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