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J Bacteriol, February 1998, p. 547-555, Vol. 180, No. 3
0021-9193/98/$04.00+0
Copyright © 1998, American Society for Microbiology. All rights reserved.
Bacillus subtilis Cell Cycle as Studied by
Fluorescence Microscopy: Constancy of Cell Length at Initiation of DNA
Replication and Evidence for Active Nucleoid Partitioning
Michaela E.
Sharpe,1
Philippe M.
Hauser,1,
Robert G.
Sharpe,2 and
Jeffery
Errington1,*
Sir William Dunn School of Pathology,
University of Oxford, Oxford OX1 3RE,1 and
Tessella Support Services plc, Abingdon OX14
3PX,2 United Kingdom
Received 4 September 1997/Accepted 17 November 1997
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ABSTRACT |
Fluorescence microscopic methods have been used to characterize the
cell cycle of Bacillus subtilis at four different growth rates. The data obtained have been used to derive models for cell cycle
progression. Like that of Escherichia coli, the period
required by B. subtilis for chromosome replication at
37°C was found to be fairly constant (although a little longer, at
about 55 min), as was the cell mass at initiation of DNA replication.
The cell cycle of B. subtilis differed from that of
E. coli in that changes in growth rate affected the average
cell length but not the width and also in the relative variability of
period between termination of DNA replication and septation. Overall
movement of the nucleoid was found to occur smoothly, as in E. coli, but other aspects of nucleoid behavior were consistent with
an underlying active partitioning machinery. The models for cell cycle
progression in B. subtilis should facilitate the
interpretation of data obtained from the recently introduced
cytological methods for imaging the assembly and movement of proteins
involved in cell cycle dynamics.
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INTRODUCTION |
The bacterial cell cycle
incorporates two important, discontinuous processes, DNA replication
and cell division or septation. Many of the genes and proteins involved
in these processes have been identified and characterized previously.
In general, they are highly conserved across the eubacterial
subkingdom, though much of what is known has been derived from studies
of Escherichia coli (recently reviewed in detail in
references 18, 26, and 29).
During each cell cycle, the chromosome, usually in the form of a single
circular molecule, needs to undergo a single complete round of
replication. Regulation is mainly exerted at the level of initiation,
and over a range of growth rates, this seems to occur when the cell
attains a critical mass, relative to the number of copies of the origin
of replication (oriC) it contains. Originally, this
"initiation mass" (Mi) was thought to be
constant (5), but more recent measurements suggest that it
decreases slightly with increasing growth rate (52).
Following initiation, DNA replication proceeds bidirectionally from
oriC. At all reasonably rapid growth rates (doubling time, <100 min), the time taken to replicate the chromosome (the C period) is more or less constant, at about 40 min. When the forks meet, in the
terminus region, diametrically opposite to oriC on the E. coli chromosome map, termination occurs. This is followed
by decatenation of the interlinked daughter chromosomes and, if
necessary, resolution of chromosome dimers which may have arisen by
homologous recombination.
During the remainder of the cycle, the chromosomes need to move apart
(partition) so that when division occurs, they are segregated into the
daughter cells. The mechanism of partitioning is poorly understood
(reviewed in reference 50). One school of thought supposes that the nucleoids are moved apart by a relatively passive mechanism, mediated by the many transient interactions that occur between the DNA and the cell envelope, as a result of the coupled transcription and translation of secreted proteins. An alternative view
is that partitioning is effected by an active, specific partitioning machinery, perhaps analogous to the mitotic apparatus of eukaryotic cells.
The period between the termination of DNA replication and septation,
sometimes known as the D period in E. coli, is also
relatively constant, at about 20 min (18). During this
period, the cell prepares for division by assembling a multicomponent
"divisome" comprising several proteins. The major component of this
assembly is a tubulin-like protein, FtsZ, which forms a ring at the
site of septation that is thought to contract to bring about division (reviewed in reference 26). The extent to which the
division and DNA replication cycles are coupled or interconnected is
not yet clear (34).
Aside from E. coli, little work has been done on cell
division in any other bacterium except Bacillus subtilis. An
important advantage of B. subtilis for cell cycle studies
lies in its ability to sporulate. This occurs in response to
starvation, and it begins with a reorganization of the cell cycle to
produce a modified, asymmetric cell division (10, 45). Thus,
the mechanisms controlling both the timing and positioning of the
septum are under inducible control. The few studies that have been done
on cell cycle progression in vegetatively growing B. subtilis (e.g., see references 2, 19, and
32) have detected only small differences from the E. coli paradigm. The most overt of these lies in the
tendency of sister B. subtilis cells to remain connected in
cell chains for a significant but variable period after formation of
the division septum (19, 36). Thus, the D period of B. subtilis, as formally defined, is highly variable.
Recently, the subcellular localization of many proteins involved in
cell division of both E. coli and B. subtilis has
been determined by application of newly developed cytological methods (reviewed in reference 42). In the case of B. subtilis, interpretation of the results of these experiments would
be greatly facilitated by a better knowledge of cell cycle progression
in this organism. Several of the methods routinely used to measure cell
cycle parameters in E. coli are unsuitable for B. subtilis because of the tendency of the cells of the latter to
form chains. However, this problem can be overcome by the use of
fluorescence microscopy (15). This work describes an
analysis of cell cycle progression of B. subtilis under four
different growth conditions. Several similarities and differences
between cell cycle dynamics in B. subtilis and E. coli have been detected. The availability of four different well-characterized growth conditions should be of considerable use for
future studies of the regulation and subcellular assembly of the
machineries responsible for DNA replication, chromosome partitioning,
and cell division.
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MATERIALS AND METHODS |
Bacterial strains.
B. subtilis SG38 trpC2
amyE (11) was used for all the experiments described in
this work. Strain L5481 dnaB19(Ts) xin-15 flaD1
(49) was used for the internal standard of DNA content in
the digital image analysis. Strain 1.5 (trpC2 spoIIAC1
[12]) was used to prepare chromosomal DNA for use as a
standard for the quantitative DNA-DNA hybridization.
Media and growth conditions.
S medium contained
(NH4)2SO4 (0.2% w/v),
K2HPO4 (1.4%), KH2PO4
(0.6%), sodium citrate (0.1%), Mg2SO4
(0.02%), MnSO4 (0.056%), and glucose (0.5%). TS medium
was S medium supplemented with L-glutamate (0.5%) and
Difco yeast extract (0.001%). CH medium (which contains 10% casein
hydrolysate) was as specified in detail previously (32a; modified as described in reference
35). CHG medium was CH medium containing glucose
(0.5%). All media were supplemented with tryptophan (20 µg/ml). A
single colony of SG38 was inoculated into 5 ml of each medium, diluted
5,000-fold into a further 5 ml, and incubated overnight at 30°C. For
S medium, the overnight culture was supplemented with 15 µl of CH
medium to prevent sporulation. In the morning, each culture was diluted
back in fresh prewarmed medium to an optical density at 600 nm
(OD600) of 0.1. The cultures were incubated with shaking at
37°C until they reached an OD600 of 0.7 to 0.8, at which
point they were harvested for DNA analysis or fixed for microscopy. A
plot of log OD600 against time was used to ensure that the
cultures were growing exponentially when harvested (not shown).
Measurement of cell length, cell width, nucleoid length, and DNA
content by digital image analysis.
The microscopic methods of
Hauser and Errington (15) were used. Briefly, the cells were
fixed with ethanol and the DNA was stained with DAPI
(4',6-diamidino-2-phenylindole). Phase contrast and epifluorescence
images of fields of cells were captured and analyzed electronically. To
randomize the sampling, all cells within a field, except those in
aggregates were analyzed. Cell length and cell width were measured
directly from images. The DNA content of nucleoids in individual cells
was measured by its fluorescence intensity relative to that of standard
nucleoids containing single complete chromosomes. By this method, DNA
content is underestimated because the DNA is more condensed in the
sample nucleoids than in the standard nucleoids. The approximate extent of this underestimation is given by the ratio of the maximum pixel brightness of the nucleoid to that of the standard nucleoids
(15). This ratio (1.2 to 1.5) was calculated for each field
of cells from the mean maximum pixel brightness of all of the nucleoids (standard deviation, ~10%) and was used as a correction factor for
the DNA content measurements. The average of the measurements obtained
did not differ significantly from the average DNA content of the
population measured by a direct chemical method (see below). The images
in Fig. 5 were obtained as described by Glaser et al. (13).
Preparation of chromosomal DNA, probes, and filter
hybridization.
The cell samples were lysed and chromosomal DNA was
extracted as described previously (15). For preparation of
the standard DNA from strain 1.5, a 150-ml culture of the strain was
induced to sporulate, as described by Partridge and Errington
(35). Twenty-two hours after the initiation of sporulation,
the sporlets (representing about 95% of the population) were harvested
and isolated by differential centrifugation, as described by Magill and
Setlow (27). The sporlets were lysed and their DNA was
purified as described for the DNA samples from vegetative cells. The
chromosomes of sporlets are generated by a mechanism similar to that of
spores (41, 55) and so are expected, like spores
(16), to contain single completed chromosomes, but their DNA
is much easier to extract than that of mature spores. The
concentrations of the chromosomal DNA stocks were estimated by
absorbance at 260 nm, and then they were diluted in TE buffer (10 mM
Tris-HCl, 1 mM EDTA, pH 7.5) to a final concentration of 50 µg/ml.
For filter hybridization (17), the DNA stocks were further
diluted in denaturing buffer (1 N NaOH, 3 M NaCl in TE buffer), such
that 20 µl contained 0.15 µg of DNA. (Samples of 0.05 µg of DNA
were also hybridized to check that the probe was saturating.) The DNA
was applied to a nylon membrane with a dot blot apparatus, denatured
with 0.5 M NaOH-1.5 M NaCl (2 min), and then neutralized with 0.5 M
Tris-Cl-1.5 M NaCl, pH 7.5 (5 min). The filter was briefly immersed (5 s) in 2× SSPE (1× SSPE is 0.18 M NaCl, 10 mM
NaH2PO4, and 1 mM EDTA [pH 7.7]) and baked at
80°C for 120 min. After soaking in 6× SSC (1× SSC is 0.15 M NaCl
plus 0.015 M sodium citrate), prehybridization was for 2 h at
42°C in 5× SSPE, 50% (vol/vol) formamide, 0.001% (wt/vol) sodium
dodecyl sulfate (SDS), 0.001% (wt/vol) Ficoll, 0.001% (wt/vol)
polyvinylpyrrolidine, and sonicated veal thymus DNA (0.1 mg/ml).
Hybridization was done in the same buffer containing the appropriate
labelled probe. Table 1 shows the primers
used in the PCRs to generate the 3-kbp probes from various regions of
the B. subtilis chromosome. The probes were radiolabelled by using the Random Primed DNA Labelling Kit (Boehringer Mannheim) and
[
-32P]dATP (Amersham). Following hybridization, the
filters were washed twice for 15 min (ambient temperature) in buffer 1 (2× SSC, 0.1% SDS) and once for 30 min (65°C) in buffer 2 (5× SSC,
0.1% SDS). The membrane was cut into rectangles, each containing a
single DNA dot, and placed into 2 ml of H2O in a
scintillation vial. Samples were counted for 5 min in the energy window
for 3H (Cerenkov effect).
Determination of DNA content in cultures.
The biochemical
quantitation of the total DNA content of cultures was as described
previously (15). The cell concentration was determined by
directly counting ethanol fixed cells in a Petroff-Hausser counting
chamber (average of three estimations). Each estimation was based on
the average number of cells in 20 ruled squares, each with a volume of
50 pl.
Calculation of the cell length distributions.
The
distribution of cells as a function of cell length was modelled
according to a newly derived model developed for this work (see the
Appendix). The major difference between the new model and the
Collins-Richmond approach (4) is that we assume that the
spectra of lengths at birth and septation do not overlap significantly. It is known that in E. coli there is a narrow distribution
of cell lengths at septation, and overlap is, therefore, unlikely. This
allows the probability of a cell having a given length at birth to be
calculated directly by using equation 8 in the Appendix; no iteration
is required.
In order to use this equation, we assume that the length probability
distribution at birth is a Gaussian distribution with average
and variance (
l)2:
where l is the cell length. Similarly, we assume that
the length probability distribution at septation is a Gaussian
distribution with average 2
and variance
2(
l)2:
Thus, there are only two parameters in the model: the average
length at birth,
, and the normalized variance of the
birth probability distribution,
(
l/
)2. With normalized
variances of the birth probability distribution in the range 0.01 to
0.20, it is found that equation 8 predicts that there is a 57% ± 1%
probability of finding a cell with length
1.4 regardless of the value
of the normalized variance. Thus, the experimentally measured length
distribution can be examined to find the length,
lC, at which the probability of any cell having length
lC is 57%. Then, the average length at
birth,
, is (lC/1.4). This
leaves the normalized variance of the birth probability distribution as
the only free parameter of the model, which may be varied to attempt a
variety of fits to the experimental data.
Use of the cell length distributions derived with this new model as the
initial input to the iterative Collins-Richmond method
(
4)
revealed no significant discrepancies between the two methods.
Determination of average DNA content at any point in the cell
cycle.
We assume that an "ideal" cell is born with the average
birth length,
, and with average DNA content at
birth, yo chromosome equivalents, and
that it septates (after a period of time equal to the generation time,
) with length equal to the average septation length,
2
, and average DNA content,
2yo chromosome equivalents. Migration
of DNA replication forks are assumed to occur linearly with time, at a
rate determined by the C period,
C. If no chromosomal
growth occurs between termination of replication and initiation (i.e.,
C), then the DNA content of an ideal cell as a
function of time, y(t), can be calculated as
follows:
If dichotomous replication occurs (i.e.,
C/2
C), then:
Calculation of average cell length at nucleoid transition.
The percentage of the cell population in each nucleoid state class
(mononucleate monolobed, mononucleate bilobed, binucleate monolobed,
binucleate bilobed, and tetranucleate monolobed) was calculated
directly from the measured data. The cell length at which the
transition between any two consecutive nucleoid states occurs was
estimated by calculating (from the best fits [see the Appendix] shown
in Fig. 1) the cell length at which the
cumulative probability of a cell having a cell length less than the
transition length is equal to the cumulative probability of a cell
existing in the preceding state.

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FIG. 1.
Characterization of exponentially growing cells in CHG
(A), CH (B), TS (C), and S (D) media by digital image analysis. The
cells were categorized according to cell length (frequency within the
population) and to nucleoid conformation and number (lightest to
darkest bars, monucluceate, mononucleate bilobed, binucleate,
binucleate bilobed, and tri- or tetranucleate, respectively). The solid
and dotted lines show ideal cell length distributions calculated as
described in the Appendix, using values for the normalized variance of
the birth probability distributions,
( l/ )2, of 0.03 and 0.06, respectively. Data are from >400 individual cells from each medium.
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RESULTS AND DISCUSSION |
Measurement of cell cycle parameters in four different media.
To determine the average cell cycle for B. subtilis cells
growing in various media, affording generation times between 30 and 73 min, we used the light microscopic methods of Hauser and Errington
(15). Some of the data for one medium, CH, were described previously (15). In Fig. 1 and
2, data from 200 or more individual cells
growing in each of the four different media are summarized. For each
cell the state of the nucleoids (number and conformation) were compared
with cell length and DNA content per cell (see Materials and Methods).
To check the accuracy of the fluorimetric DNA estimations, we measured
the DNA concentration of each culture by a direct chemical method and,
having determined the cell number by direct microscopic counting,
calculated the average DNA content per cell. As shown in Table 2, the
values obtained differed only by about 10% from the average DNA
content per cell obtained by fluorescence microscopy. An error of this
magnitude would have little effect on the cell cycle modelling
described below.

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FIG. 2.
Relationship between DNA content and cell length for
populations of cells grown in CHG (A), TS (B), and S (C) media. DNA
content (expressed as chromosome equivalents per cell) was measured and
plotted against cell length. The standard regression line for each plot
is shown. Data are from about 200 individual cells from each medium.
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The mean cell size of the population increased with increasing growth
rate (Table
2), in agreement with
previous studies
(
37,
38). In all four media, the shapes of
the cell length
frequency distributions, with a high proportion of
small newborn
cells and a decrease in frequency with increasing cell
size, were
generally characteristic of an asynchronously growing
population
dividing by binary fission (
20,
21). In all
media, the longest
cells were always more than twice the length of the
smallest.
This probably arises through slight variations in cell length
at septation, as described previously for
E. coli (
20,
39,
53). Apparently, the smallest cells at birth have a longer
subsequent
cell cycle and vice versa for the longer cells
(
22).
As with cell size, the mean DNA content increased with increasing
growth rate. The plot of DNA content against cell length
gave a linear
relationship in all media (Fig.
2 and reference
15),
indicating that within each population DNA replication
is tightly
coupled to cell growth. The regression lines had small
intercept values
in accordance with the expectation that both
DNA content and cell
length tended to be halved at septation.
Interestingly, the regression
lines in all four media were not
significantly different, suggesting
that the ratio of DNA content
to cell length is constant, at least over
this range of growth
conditions. This was unexpected, because it
suggested that
B. subtilis compensates for an increased
growth rate solely by increasing
its length rather than by altering
both length and width, as is
the case for
E. coli
(
7). Indeed, we were unable to detect
significant changes in
cell width across the range of growth rates
tested (Table
2), in
agreement with previous reports (
40,
47).
This observation
has important implications for measurement of
the
Mi for DNA replication, as discussed below.
Measurement of the B. subtilis C period.
The
ratios of chromosomal markers close to oriC and
terC in the various cultures were determined by quantitative
DNA-DNA hybridization (Table 3), and
these values were used to calculate C periods (Table 3). The results
were similar to each other, from 50 to 58 min, and were close to
previously published values (8). It is interesting that the
C period of B. subtilis is significantly longer than that of
E. coli (about 42 min over this range of generation times
[18]). Thus, DNA replication forks in B. subtilis apparently migrate at only about four-fifths of the rate
in E. coli.
Cell cycle models.
To derive models for cell cycle progression
we needed to determine, in addition to the generation time and C
period, the average length and DNA content at birth. For the cell
length at birth, the data described above were treated with an
algorithm developed for this purpose, which is described above and in
the Appendix. The solid and broken lines shown in Fig. 1 show predicted
ideal cell length distributions, using two possible values for the only free parameter, the normalized variance of the birth probability distribution (0.03 and 0.06). As shown, variation of this parameter had
little effect on the shape of the plot. For the purposes of all
subsequent analyses, a value of 0.03 was used.
Values for the average lengths at birth and septation (assumed to be
twice that at birth) calculated in this way are shown
in Table
2. Cell
size at birth and, hence, septation increased
with increasing growth
rate. This was in accordance with previous
descriptions of the
E. coli cell cycle except that, as discussed
above, both length and
width vary (and indeed maintain a fairly
constant ratio in
E. coli [
7]). The main factor responsible
for the
marked effects of growth rate on the average dimensions
of bacterial
cells may be the relative constancy of the C period.
Because initiation
occurs at a relatively fixed cell mass irrespective
of the growth rate
(see below) and division can occur only after
a round of DNA
replication has been completed, rapidly growing
cells reach a much
greater size at division than more slowly growing
cells.
The average DNA content of newborn cells (Table
2) was determined
directly from the regression lines in Fig.
2 and the results
of Hauser
et al. (
15), and as expected, this content increased
with
increasing growth rate. The relationships between cell length,
DNA
content and time were calculated from the various measured
and derived
parameters (see Materials and Methods), allowing models
for progression
through the
B. subtilis cell cycle at the four
different growth rates to be derived (Fig.
3).

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FIG. 3.
Models for cell cycle events progression in B. subtilis growing at four different rates. Shown are the major
events during the cell cycle: birth (b), initiation (i), termination
(t), binucleation (bi), and septation (s). Dots indicate the initiation
of DNA replication. The cell length is shown on the scale below the
models.
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Initiation of replication.
The initiation of DNA replication
is a key event in the bacterial cell cycle. The point in the cell cycle
at which initiation occurred was calculated from the average DNA
content at birth and the C period (Table 2). In all cases the observed
DNA content of cells at the initiation length was consistent with the
predicted value (compare Fig. 1 and 2 with Table 2). For cells in which the generation time was greater than or equal to the C period (S or TS
media), initiation of DNA replication occurred in fully replicated
chromosomes. The DNA content of such cells was two chromosome
equivalents rather than one, because the products of the previous round
of DNA replication did not segregate into separate cells until later in
the cycle. It is interesting to compare this with E. coli,
in which slow-growing cells (e.g., doubling time, 70 min) tend to
initiate DNA replication soon after birth. Termination then occurs soon
enough in the cycle for the nascent sister chromosomes to segregate
immediately at the forthcoming division (18). B. subtilis thus tends to maintain a higher chromosomal copy number than E. coli.
For cells with a generation time of less than the C period, new rounds
of replication began before the previous rounds had
terminated,
resulting in dichotomous (multifork) replication.
Therefore, the DNA
content at initiation of replication was usually
greater than two.
Moreover, at the growth rates sustained by CH
or CHG media, the cells
in which initiation occurred would divide
twice before the round of DNA
replication terminated and the newly
formed sister chromosomes could
segregate. Thus, in these media,
initiation occurred in much larger
cells containing four replication
origins (Table
2).
In
E. coli growing at a reasonably rapid rate (e.g., more
than one doubling per h), the ratio of the cell mass at initiation
of
DNA replication (
Mi) to the number of chromosome
origins (
Ni)
is constant (see reference
5) or decreases slightly with increasing
growth rate
(see reference
52). Given the relatively constant
width of
B. subtilis cells (see above), cell length should
be
approximately proportional to cell mass. It is interesting that
for
three of the four media used, S, TS, and CH, the
Li (length
at initiation, per copy of
oriC) was fairly constant (Table
2),
whereas in CHG medium a
slightly smaller
Li was obtained. Thus,
it
appears that the initiation mass behaves similarly in
B. subtilis and
E. coli.
Termination of DNA replication.
The bidirectional replication
of the B. subtilis chromosome ends when the two replication
forks meet in the terminus region, located approximately opposite to
the replication origin (57). The timing of termination and
the cell length at which this occurs are determined by the time of
initiation of replication and the duration of the C period
(18). Therefore, it varied considerably from medium to
medium (Table 2). For more slowly growing cells (with a generation time
less than or equal to the C period) termination should coincide with
the cell's attaining a DNA content of two chromosome equivalents.
Thus, in cells growing in TS medium, in which the C period is more or
less equal to the generation time, initiation and termination should
occur almost simultaneously. In S medium, in which the generation time
is well in excess of the C period, a significant gap should occur
between termination of one round of replication and initiation of the
next. During this interval the DNA content should remain constant at
two chromosome equivalents, until the initiation mass is achieved.
However, we did not detect a clear gap in the S medium cell cycle,
presumably either because of the natural variation in the population of
cells or the relative insensitivity of our measurements. For cell
populations growing in CH and CHG with generation times less than the C
period, termination of replication occurred after the succeeding cell cycle had started and, hence, at a DNA content in excess of two chromosome equivalents.
The D* period.
In E. coli it has been shown that
there is a relatively fixed interval (the D period) between the
termination of a round of DNA replication and cell separation
(18). Measurement of this period in B. subtilis
is more complicated because septation and cell separation do not
coincide; indeed the time between these two events varies markedly
under different growth conditions (19). It seems that most
of the variation lies in the time taken to hydrolyze the thick
peptidoglycan layer (typical of gram-positive bacteria) that binds the
sister cells together after septation. We have therefore found it
useful to use the term D* for the period between termination of DNA
replication and formation of the corresponding division septum
(15). Our present data show (Table 2) that the D* period was
relatively constant in three of the media tested but that, as was the
case for the Li, it was somewhat reduced in CHG
medium. The possibility that the link between termination of DNA
replication and septation is less tight in B. subtilis than
in E. coli is supported by the observation (7a, 43,
56) that a delay in DNA replication in B. subtilis has
much less of an effect on septation than that in E. coli
(3).
Nucleoid separation.
While measuring cell length and DNA
content, we also recorded nucleoid appearance and number per cell (Fig.
1). At all growth rates tested, the cells showed either one or two
discrete nucleoids (i.e., were mononucleate or binucleate), with the
exception of a few of the largest cells in CH or CHG. In general, it
appeared from the distributions shown in Fig. 1 that the transition
from one to two nucleoids occurred progressively later in the cell cycle as the growth rate increased. Thus, in S medium, the cells were
mononucleate throughout most of the cycle, whereas in CH and CHG, the
cells were mainly binucleate. The average point of transition from the
mononucleate to the binucleate state was determined for each medium as
described in Materials and Methods. In the faster-growing cells (CH or
CHG medium), binucleation occurred at or soon after termination, in
accordance with previous observations for E. coli
(6). However, in more slowly growing cells (S or TS medium),
there was a significant delay between the two events. Interestingly,
nucleoid separation (binucleation) occurred at a cell length of about 3 µm in both of these media, which was similar to the length at
binucleation in CH medium (Table 2). It seemed possible that the
failure to observe nucleoid separation in cells of less than 3.0 µm
might reflect the minimum length of the nucleoid. To determine the
length of a nucleoid corresponding to a single unreplicated chromosome
we used a dnaB(Ts) mutant. At the nonpermissive temperature,
this mutant completes ongoing rounds of DNA replication but does not
initiate new rounds (49), so the cells arrest with single
completed chromosomes. (Such cells were used as a standard for the DNA
content measurements discussed above.) The average length of the
nucleoid in these standard cells was 1.5 ± 0.25 µm (200 nucleoids measured). This value suggests an obvious explanation for our
failure to detect nucleoid separation in cells of <3.0 µm.
Nucleoid length.
Woldringh and coworkers have argued that
chromosome partitioning is a relatively passive process driven by
multiple transient associations between the DNA and the cell envelope,
mediated by the coupled transcription and translation of secreted
proteins (summarized in reference 54). In support of
this view, they showed that in E. coli the nucleoids
increase in length smoothly and continuously during growth
(48). To test whether nucleoid expansion was also continuous
in B. subtilis, we measured the total length of the nucleoid
in the images of cells grown in the four different media and plotted
these relative to cell length (Fig. 4).
As for E. coli, a clear linear relationship was obtained in
all four media. Thus, overall movement of the nucleoid in both organisms appears to be continuous.

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FIG. 4.
Relationship between nuclear length and cell length over
a range of growth rates for cells growing in CHG (A), CH (B), TS (C),
and S (D) media. For each plot standard regression lines are shown. For
binucleate cells, nuclear length corresponds to the sum of the two
nuclei. Data are from 200 cells from each medium.
|
|
Despite the evidence for gradual overall movement of the nucleoid,
there is increasing support for the existence of more-active,
mitosis-like partitioning mechanisms in bacteria (
1,
13,
24,
25,
30,
33,
51). How can the passive and active
models for nucleoid
partitioning be reconciled? We suggest that
both mechanisms are used by
the cell. The active, mitosis-like
partitioning apparatus serves to
ensure that the
oriC regions
of newly replicated sister
chromosomes are driven apart by a significant
distance early in the DNA
replication cycle (
13,
24,
44,
51). The passive mechanism
would tend to move the bulk of each
sister nucleoid into a position
more or less centered on the fixed
oriC region, this
movement being facilitated by extension of the
cell envelope. Thus, the
active and passive mechanisms of chromosome
partitioning need not be
mutually exclusive.
Nucleoid bilobation.
Support for an underlying active
partitioning mechanism was obtained from the observation of cell
cycle-associated changes in nucleoid morphology. Figure
5 shows a compilation of images of cells
at different points in the cell cycle, from each of the four different
media. In general, small (i.e., newly separated) nucleoids had a
relatively uniform oval shape. However, larger nucleoids tended to
appear dumbbell shaped or bilobed. The frequency of bilobation was
greater at higher growth rates: at the lowest growth rate in S medium,
only 20% of the nucleoids were bilobed, whereas at the highest growth
rate tested (CHG medium) most of the nucleoids were bilobed (Fig. 1).
The time of transition to a bilobed state was measured for all four
cell populations and related to cell length and DNA content, as shown
in Table 2. For cells growing with doubling times greater than the C
period, the nucleoids became bilobed shortly before they divided to
produce two separate nucleoids in a binucleate cell. It is possible
that in these cells the bilobed appearance was due to the presence of
two completed but still overlapping nucleoids. As discussed above,
complete nucleoid separation is probably delayed as a function of the
overall dimensions of the cell at these low growth rates. However, in
larger cells, growing with generation times of less than the C period,
bilobation occurred relatively early in the cell cycle and well before
termination of DNA replication. From the average DNA contents at the
transition to the bilobed state (Table 2) it can be deduced
(46) that the ongoing rounds of DNA replication would have
progressed to about 60 (CH) or 75% (CHG). We suggest that in these
faster-growing cells, at least, the bilobed conformation is a
consequence of the active separation of the partially replicated
daughter chromosomes. If so, the data indicate that this partitioning
process is in progress or complete well before the round of DNA
replication finishes. The bilobed state probably reflects the active
separation of the oriC regions of the daughter chromosome
segments, which is mediated in part by the Spo0J-dependent chromosome
partitioning system (13, 24, 25, 51).

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|
FIG. 5.
Compilation of representative images of the different
cell types found in four different growth media S (A), TS (B), CH (C),
and CHG (D). DAPI fluorescence images are overlaid on phase-contrast
images. The nucleoids are the brightly stained objects within the dark
cell bodies. All of the images are at the same magnification. Scale
bar, 2 µm.
|
|
It is interesting that Wake and coworkers have demonstrated that
commitment to septation in germinating spores of
B. subtilis can occur when the first round of chromosome replication has progressed
about 70% to completion (
28,
56). It is therefore possible
that initiation of septation is coupled in some way to nucleoid
bilobation. This could be consistent with the proposal that initiation
of septation could be triggered by a DNA-free zone in the cell,
the
so-called "negative nucleoid effect" of Mulder and Woldringh
(
31).
There is presently much interest in following the subcellular
localization and assembly of proteins involved in cell division
and
chromosome partitioning in
B. subtilis (see, for example,
references
9,
13,
14,
23, and
25). The detailed descriptions
we have presented for
cell cycle progression in
B. subtilis at
four different
growth rates should be of considerable use in these
studies.
 |
APPENDIX |
Cell cycle model. (i) Basic assumptions. In order to
predict the probability that a given cell has a length inside the range
l to l + dl,
(l)
dl, four pieces of information are needed. First, the rate
of increase in the population with time is required. Assuming that the
rate of growth of the population is exponential with time, the number
of cells that exist at time t is given by:
|
(1)
|
where
No is the number of cells at time
(
t) zero and

is the generation time. Since cells divide
in two at septation, it
follows that the number of cells born in the
time interval
t'
to
t' +
dt' is:
|
(2)
|
Second, the rate of growth of the length of a given cell with
time is required. Assuming that the length of a cell grows
exponentially with time, then at time
t, the length of a
cell
born with length
l' at time
t' is:
|
(3)
|
In addition, the probability that a cell is born with a length
between
l and
l +
dl,
Pbirth(
l)
dl is required
probability
that a cell septates with a length between
l and
l +
dl,
Psept(
l)
dl is required.
In this model two further assumptions are made that are the key
difference between this model and earlier ones, e.g., the Collins-Richmond approach (4). (v) There is no significant overlap between the birth and septation probabilities. (vi) The probability of a cell septating at any length is not dependent on its
length at birth. These two assumptions enable the cell length
distribution to be calculated directly from the model parameters unlike
in the Collins-Richmond approach, where an iterative method is needed.
It can be shown that the distributions calculated from this model fit
the Collins-Richmond equation (4) well, thereby justifying
these additional approximations.
(ii) Model derivation. The number of cells born with a
length in the interval l' to l' + dl'
in the time interval t' to t' + dl'
is:
|
(4)
|
Provided that they do not septate, all the cells born with length
l' at time
t' will grow to length
l at
time
t while those
cells born with length
l' +
dl' at time
t' will grow to length
l +
dl at time
t (where
dl = (
l/
l')
dl'). Thus, the number of
cells with length
l to
l +
dl that exist at time
t which
were
born in the time interval
t' to
t +
dl' is:
|
(5)
|
where
is the probability that a given cell can grow to a length
l
without
septating. This equation implicitly assumes that there is a
negligible
overlap between the birth and septation probabilities and
that
the probability of a cell septating is not dependent on its birth
length as indicated above.
By integrating over all possible birth times, we obtain the total
number of cells with length l to l + dl that exist at time t:
|
(6)
|
Hence, the probability that the length of a given cell is
l to
l +
dl is:
|
(7)
|
The derivation of this equation has made no assumptions about the
rate of growth of cell length or about the birth or septation
probabilities. However, if the cells grow exponentially with time,
as
assumed above (equation 3), it follows that
N(
t')/
N(
t) =
l'/
l (by using equation 1),
l'/
l =
l'/
l, and
dt' = (

/ln2)(
dl'/
l').
Hence,
equation 7 becomes:
|
(8)
|
 |
ACKNOWLEDGMENTS |
M.E.S. and P.M.H. contributed approximately equally to this work.
We thank R. G. Wake for helpful comments on the manuscript.
This work was supported by grants from the Biotechnology and Biological
Sciences Research Council of the United Kingdom. P.H.M. was supported
by fellowships from the Swiss National Fund for Scientific Research and
EMBO.
 |
FOOTNOTES |
*
Corresponding author. Mailing address: Sir William Dunn
School of Pathology, University of Oxford, South Parks Rd., Oxford, OX1
3RE, United Kingdom. Phone: 44 1865 275561. Fax: 44 1865 275556. E-mail: erring{at}molbiol.ox.ac.uk.
Present address: Hospital Preventive Medicine, CHUV Hospital, 1011 Lausanne, Switzerland.
 |
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