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Journal of Bacteriology, December 1998, p. 6364-6374, Vol. 180, No. 23
0021-9193/98/$04.00+0
Copyright © 1998, American Society for Microbiology. All rights reserved.
Effects of Chromosome Underreplication on Cell
Division in Escherichia coli
Emilia
Botello
and
Kurt
Nordström*
Department of Microbiology, Biomedical
Center, Uppsala University, S-751 23 Uppsala, Sweden
Received 5 May 1998/Accepted 30 September 1998
 |
ABSTRACT |
The key processes of the bacterial cell cycle are controlled and
coordinated to match cellular mass growth. We have studied the
coordination between replication and cell division by using a
temperature-controlled Escherichia coli intR1 strain. In
this strain, the initiation time for chromosome replication can be displaced to later (underreplication) or earlier (overreplication) times in the cell cycle. We used underreplication conditions to study
the response of cell division to a delayed initiation of replication.
The bacteria were grown exponentially at 39°C (normal DNA/mass ratio)
and shifted to 38 and 37°C. In the last two cases, new, stable, lower
DNA/mass ratios were obtained. The rate of replication elongation was
not affected under these conditions. At increasing degrees of
underreplication, increasing proportions of the cells became elongated.
Cell division took place in the middle in cells of normal size, whereas
the longer cells divided at twice that size to produce one daughter
cell of normal size and one three times as big. The elongated cells
often produced one daughter cell lacking a chromosome; this was always
the smallest daughter cells, and it was the size of a normal newborn
cell. These results favor a model in which cell division takes place at
only distinct cell sizes. Furthermore, the elongated cells had a lower
probability of dividing than the cells of normal size, and they often
contained more than two nucleoids. This suggests that for cell division
to occur, not only must replication and nucleoid partitioning be
completed, but also the DNA/mass ratio must be above a certain
threshold value. Our data support the ideas that cell division has its
own control system and that there is a checkpoint at which cell
division may be abolished if previous key cell cycle processes have not
run to completion.
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INTRODUCTION |
The cell cycles of all organisms
contain key events that occur only once during each doubling in mass,
replication of the genome, separation of the daughter genomes, and cell
division. These events are carefully coordinated with each other and
controlled to match the increase in cell mass. In eukaryotic cells,
there seem to be two independent, alternating processes, genome
replication (S phase) and separation of the daughter genomes (M phase);
each S phase requires a preceding M phase and vice versa
(27).
During the bacterial cell cycle (for reviews, see references
15, 24, 30, and 38), there are
three recognized periods at a slow growth rate, B, C, and D
(20). Chromosome replication occurs during period C, and
nucleoid partitioning and cell division take place during period D. The
length of C plus D can be much longer than the generation time,
. To
accommodate this, there may be up to three overlapping replication
cycles at a rapid rate of growth. Hence, alternations between periods C
and D cannot occur in bacteria as they do in eukaryotic cells.
Therefore, under different growth conditions, replication initiates and
partitioning occurs at different times in the cell cycle and can take
place at any time from birth to cell division. Since there may be
overlapping replication cycles, there cannot be a requirement for
completed nucleoid partitioning before the next replication cycle is
initiated. Cell division does not seem to be required for the two other
key events, and thus, inhibition of cell division leads to the
formation of filaments with 2, 4, 8, 16, etc., separated nucleoids.
Damage to the DNA or other effects that slow down replication induce systems, such as the SOS system, that transiently delay cell division in order to allow replication to be completed before the cell divides.
Inhibition of initiation of chromosome replication reduces the
frequency of, but does not totally block, cell division, which leads to
the formation of elongated or filament cells; the residual cell
division causes the formation of DNA-less cells. This and other pieces
of information indicate that initiation of chromosome replication,
nucleoid partitioning, and cell division have independent control
systems that link these processes to cell mass (for reviews, see
references 15, 24, 30, and 38).
This requires that within a single cell cycle there are checkpoints
that ensure that chromosome replication is finished before nucleoid
partitioning and cell division take place.
To address the questions of the number of control points in the cell
cycle of Escherichia coli and their molecular basis, we have
constructed so-called int strains (4, 17, 23,
29). In these strains, a 16-bp deletion in the leftmost 13-mer of
the chromosomal replication origin, oriC, which is crucial
for the initial opening of the origin at initiation of replication, has inactivated oriC (8). Plasmid replicons have been
inserted into oriC. Thereby, chromosome replication is
controlled by the plasmid replicon and independent of the normal cell
cycle controls. The copy number of plasmid R1 is about the same as that
of oriC at moderate and high growth rates (18)
and is essentially regulated by two transcription rates, that of the
mRNA for the rate-limiting initiator protein (RepA) and that of the
antisense RNA (CopA) that negatively controls the efficiency by which
the RepA mRNA is translated (28). We have constructed
intR1 strains in which both of these transcription rates are
controlled by temperature such that the chromosome content is normal at
39°C, lower (underreplication) at lower temperatures, and higher
(overreplication) at temperatures above 39°C (4, 6). This
corresponds to increasing or decreasing the initiation mass, which is
the same as moving the time of initiation of replication to later or
earlier times in the cell cycle compared to the normal situation (see
Fig. 1).
These int strains have been used to study how nucleoid
partitioning and cell division are controlled (1-3, 5, 6,
13). By using the temperature-controlled intR1 strains
under conditions of overreplication, we have been able to show that
cell division does not seem to be triggered by chromosome replication
but rather that it has its own, independent means of control
(3). This system was also used to switch off initiation of
replication, allowing ongoing rounds of replication to proceed to
completion, and afterward to switch on a single or multiple rounds of
replication in order to study the correlation between chromosome
replication and cell division (6). Several other groups have
studied the effects on cell division of inhibition and switching on of
DNA replication by using temperature-sensitive dna
mutants (see reference 20, p. 1635 to 1636).
However, with our intR1 system, it is possible to
study populations growing exponentially at reduced DNA/mass
ratios, i.e., without switching off replication during the experiment. Hence, there will not be any disruption of the cell cycle, and the physiology of the cells will be less disturbed than
it is in the switch-off/switch-on experiments referred to above. This
allows studies of more aspects of the cell cycle, e.g., the correlation
between the timing of initiation of chromosome replication and nucleoid
processing-cell division, the requirement of factors other than
completed replication for cell division, the causes for inhibition of
cell division at increased initiation mass, and the location of cell
divisions in elongated and filamented cells, etc.
We have used the intR1 system to study the effects of
underreplication (reduced DNA/mass ratio) on key cell cycle events
during exponential growth. The ratio between CopA RNA and RepA mRNA
sets the DNA/mass ratio at levels that deviate from the normal value. Shifts from 39°C to lower temperatures lead to exponential growth with new, reduced DNA/mass ratios, because the rate of synthesis of
CopA RNA is increased. A reduction in the DNA/mass ratio corresponds to
movement of initiation of replication to later-than-normal times (Fig.
1). The question of how nucleoid
partitioning and cell division respond to this arises. Will the length
of the D period be kept constant and the cells divide at continuously
increasing sizes as the delay in replication increases
("Under-replication-I" in Fig. 1), or do the cells omit cell
division and wait until they are twice the normal septating size
("Under-replication-II" in Fig. 1)? Our data are essentially in
accord with the latter.

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FIG. 1.
Over- and underreplication during the cell cycle. B, C,
and D designate the different cell cycle periods. Under-replication-I
and -II, working hypotheses about the effects of chromosome
underreplication on cell division.
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MATERIALS AND METHODS |
Strains.
The E. coli K-12 strains used in this
study were EC1005 (metB1 nalA relA1 spoT1
r
F
) (19) and its intR1 derivative
EC::71CW/pOU420Aps (6).
Chromosome replication in the
intR1 strains is controlled by
a plasmid R1 replicon, which is inserted into
oriC (
4,
23,
29). R1 replication is controlled by the RepA protein and the
CopA antisense RNA. RepA is required for initiation of replication
from
oriR1, and it is rate limiting for this event, while CopA
controls R1 replication by inhibiting the synthesis of RepA
(
28).
The construction and characterization of the
intR1 strain EC::71CW/pOU420Ap
s have
been described previously (
6). In this
intR1
strain,
the synthesis of RepA and CopA is thermodependent and CopA is
produced from the R1 derivative replicon inserted into
oriC
as
well as from the plasmid pOU420Ap
s. By decreasing the
growth temperature a few degrees, from 39°C
to 38, 37, or 36°C,
increasing amounts of CopA antisense RNA and
decreasing amounts of RepA
protein are simultaneously produced
(
6).
Media and growth conditions.
Bacteria were grown in M9
medium supplemented with 0.2% glucose, 50 µg of methionine per ml,
and 1 µg of thiamine per ml (M9 glucose medium) (32). To
EC::71CW/pOU420Aps cultures, 20 µg of
ampicillin and 50 µg of chloramphenicol were added per ml.
The cultures were incubated in thermostatically controlled water baths
(Heto) with a maximum deviation of 0.2°C from the set
temperature.
Growth in mass was monitored by the absorbence of
the culture at 550 nm
(
A550), using a Novaspec II spectrophotometer
(LKB). Exponentially growing cultures were obtained from overnight
cultures after the appropriate dilution to allow at least 10 generations
of growth in fresh medium before the temperature shifts. At
the
moment of the temperature shifts, the cultures had an
A550 of
between 0.02 to 0.04, and culture
samples for microscopic analysis
were taken at an
A550 of between 0.25 and 0.45 (3, 4, and 5 h
after the shift from the cultures at 39, 38, and 37°C,
respectively).
Flow cytometry.
Flow cytometry was essentially performed as
described by Skarstad et al. (35). Samples from the
bacterial cultures were collected, and the cells were directly fixed in
ethanol by mixing 0.1 ml of a culture growing in M9 glucose medium with
1.75 ml of ice-cold 74% ethanol (70% ethanol [final
concentration]). Fixed cells were stored at 4°C. For staining,
7.6 × 106 to 1.7 × 105 cells were
pelleted by centrifugation. The cells were washed in 1 ml of cold
staining buffer (10 mM Tris, pH 7.4; 10 mM MgCl2), and
after centrifugation the cells were carefully resuspended in 70 µl of
the same buffer. An aliquot of the cell suspension (65 µl) was mixed
with an equal volume of a staining solution (40 µg of ethidium
bromide per ml and 200 µg of mithramycin A per ml, dissolved in the
staining buffer). The analysis was performed with a Bryte HS flow
cytometer using the software Win-Bryte version 1.06 (Bio-Rad). The
measurements were carried out with the flow cytometer being triggered
on light scattering. Thus, particles below a certain size were not
recorded, and in this way it was possible to separate sample debris
from small cells and the fluorescence of all particles above the
threshold for light scattering was detected. Plastic calibration beads
(Bio-Rad) with a diameter of 1.5 µm were used to monitor instrument
performance and to standardize the scale for between-sample comparisons.
Cell size (light scattering) and DNA content (fluorescence)
distributions obtained by flow cytometry were analyzed either
directly
(see Fig.
3 and
4) or after obtaining average values
in the population
for this parameters (see Fig.
2B and Table
1).
To calculate the average
cell size and DNA content values, the
histogram curves were integrated
by using the software Win-Bryte
version 1.06.
Analysis of chromosome replication kinetics by flow
cytometry.
To analyze the kinetics of chromosome replication by
flow cytometry, 200 µg of rifampin and 50 µg of cephalexin were
added per milliliter to the cultures and samples were collected at
different time points after addition of the drugs. Rifampin blocks the
initiation of chromosome replication from oriR1, as well as
from oriC, while allowing ongoing rounds of replication to
be completed (9, 14). Cephalexin blocks cell division
(7, 21). Addition of cephalexin to the cultures at the same
time as rifampin allows a correct determination of the number of
replication origins per cell (35). Inhibition of replication
initiation, but not of elongation, results in cells containing fully
replicated chromosomes after the replication runout. The DNA histograms
will then display peaks corresponding to fully replicated chromosomes.
Therefore, by flow cytometry it is possible to follow the appearance of
peaks in the fluorescence histograms during the replication runout. In
this way the speed of replication fork movement can be estimated (33, 34).
To compare the rates of chromosome replication progression of different
cell populations, the evolution of the coefficients
of variance for
chromosome peaks during replication runout were
analyzed. We determined
the coefficients of variance (CVs) for
the upper half of the peaks
(CV-half values) corresponding to
four chromosomes per cell, and these
values versus the time of
sampling were plotted. The curves showed two
parts, a fast decrease
in the beginning that was followed by a
stabilization at a certain
level of resolution. The values for the
slope of the first part
of the curves and the intersection point, in
the
x axis, between
both parts of the curves were compared
for the different populations
under study (see Fig.
4B).
Microscopic studies.
Cells, fixed in the same way as for
flow cytometry analysis (70% ethanol [final concentration]) were
pelleted and then resuspended in 0.9% NaCl. Aliquots (5 to 10 µl)
were spread on microscope slides covered with thin layers of 1% agar
containing 0.9% NaCl and 0.5 µg of 4',6-diamidino-2-phenylindole
(DAPI) per ml. With this staining technique, extensive nucleoid
condensation and fusion are avoided (2, 37).
The cells were analyzed under a Nikon Optiphot-2 combined
phase-contrast and fluorescence microscope. The images were digitalized
by using a charge-coupled device camera (Sony Instruments) connected
to
a computerized image analysis system (software and hardware
from
Bergström Instruments). Cell length measurements, analysis
of
septating cells, and determination of the number of nucleoids
per cell
were performed manually from the digitized images, using
length
measurement as well as profile tools provided with the
software. The
digitized images were transferred to Adobe Photoshop
3.0 and printed
with a dye sublimation
printer.
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RESULTS |
Underreplication levels during exponential growth.
By
decreasing the growth temperature of the intR1 strain
EC::71CW/pOU420Aps, it was possible to reduce
its normal DNA/mass ratio, which at 39°C was close to that in the
parental strain replicating from oriC, and to stabilize new
ratios during a period of exponential growth.
EC::71CW/pOU420Ap
s and its
oriC parental strain, EC1005, were grown exponentially
in M9 glucose medium at 39°C for at least
10 generations. At an
A550 of between 0.02 and 0.04, the cultures
were
split, and the parental strain was shifted to 37°C and the
intR1 strain was downshifted to 38, 37, or 36°C. The
growth in
mass was monitored by measuring the
A550 (Fig.
2A;
Table
1).
Cells were collected from the
cultures growing at 39°C and at
different times after the temperature
shift to 38, 37, or 36°C,
fixed in ethanol, and analyzed by flow
cytometry and microscopy
(Fig.
2B and
3;
Table
1) (see also Fig.
5). The DNA/mass ratios
in the cultures at
different incubation temperatures were estimated
from the
flow-cytometric data (Fig.
2B; Table
1).

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FIG. 2.
Growth curves (A) and DNA/mass ratios (B) of
EC::71CW/pOU420Aps. The strain was grown
exponentially for at least 10 generations in M9 glucose medium at
39°C ( ), and at time zero different parts of the culture were
shifted to 38°C ( ), 37°C ( ), or 36°C ( ). The growth in
mass was monitored by measuring absorbance
(A550), and the DNA/mass values were obtained
from flow-cytometric measurements (see Materials and Methods). DNA/mass
ratios are expressed relative to the values obtained at 39°C.
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TABLE 1.
Physiological and cell division parameters for strain
EC::71CW/pOU420Aps at different levels
of replicationa
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FIG. 3.
Cell size (light scatter; left columns) and DNA content
(fluorescence; right columns) distributions of EC1005 and
EC::71CW/pOU420Aps growing exponentially in M9
glucose medium at 39°C (A) and of
EC::71CW/pOU420Aps at different times after the
shift to 37°C (B) or 38°C (C).
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The control strain, EC1005, had a mean doubling time ± standard
deviation of 40 ± 2 min (
n = 6) at 39°C, and
the growth rate
was essentially the same after the shift to 37°C
(data not shown).
Strain EC::71CW/pOU420Ap
s grew
with a doubling time of 53 ± 2 min (
n = 10) at
39°C. For
more than 1 h after a temperature downshift, the
culture's doubling
time remained the same as it had been at 39°C;
this was followed
by a transition period during which the growth rate
decreased.
Then, the different cultures reached a new rate of
exponential
growth in mass. Thus, around 90 min after the shift to
38°C, the
culture grew with a doubling time of about 66 ± 6 min
(
n = 7)
for approximately three generations, and 140 min after the shift
to 37°C, the culture reached 110 ± 30 min
(
n = 10) of doubling
time, with that rate being
maintained for about two cell generations
(Fig.
2A; Table
1). Following
the shift from 39 to 36°C, the
culture did not undergo exponential
growth for enough time to
be analyzed systematically in the present
study (Fig.
2A) (see
also Fig.
6).
The DNA/mass ratio in EC::71CW/pOU420Ap
s was
monitored after the temperature downshifts. Immediately after a shift,
the DNA/mass
ratio started to decrease, and it reached the minimum
values of
around 0.67 during the first hour after the shift to 38°C
and
of 0.52 2 h after the shift to 37°C. Then, an incrementation
and
stabilization of this ratio followed, with fairly constant levels
of around 0.83 3 h after the shift to 38°C and of around 0.60
4 h after the shift to 37°C being reached (Fig.
2B; Table
1).
Flow-cytometric analysis showed that EC1005 and
EC::71CW/pOU420Ap
s cultures growing
exponentially at 39°C displayed similar cell
size and DNA content
distributions and average values (Fig.
3A).
Three hours after the shift
to 37°C, flow-cytometric distributions
of EC1005 cultures were very
similar to those seen during exponential
growth at 39°C (data not
shown). After the shift of EC::71CW/pOU420Ap
s to
37°C (Fig.
3B), the first effect that could be observed by
flow
cytometry was the reduction in the frequency of chromosome
initiation,
while the ongoing rounds of replication continued
to completion. This
could be deduced from the appearance of distinct
peaks in the DNA
content distributions, corresponding to one and,
mainly, to two
(55% of the population) chromosome equivalents
per cell, 30 min after
the downshift. During the first hour after
the shift, the cell size
distribution and the average cell size,
as well as the generation time
of the culture (Fig.
2A), were
constant; therefore, cell division took
place as in the control
situation. As a result of ongoing cell
division, 1 h after the
shift the fraction of cells with one
chromosome became more abundant
than that with two chromosomes. The
rapid effect of the temperature
downshift on replication could be
ascribed to the sudden incrementation
of the thermodependent production
of CopA from the plasmid pOU420Ap
s as well as from the R1
copy present in the chromosome of the
EC::71CW/pOU420Ap
s strain. Two hours after the
shift, the majority of the cell population
(56%) contained one
chromosome, and it could be observed that
replication resumed and some
cells (25%) contained more than one
chromosome but less than two. At
this time, an initial effect
on cell division could be detected because
the cell size distribution
got broader and the average size increased;
thus, cell division
started to be abolished. Three hours after the
shift to 37°C,
the doubling time for the culture increased (Fig.
2A)
and replication
resumed (Fig.
3B). Distinct peaks corresponding to
cells with
one, two, three, or four chromosomes could be distinguished
instead
of a more continuous distribution. The appearance of distinct
peaks in the DNA content distribution indicated that a shorter
period
of time was spent on the replication process, relative
to the whole
cell cycle, at 37°C than at 39°C. The presence of
a peak
corresponding to cells that contained one chromosome confirmed
that the
temperature shift resulted in an increase in cell mass
required for
initiation of chromosome replication. At this stage,
the percentage of
chromosomeless cells started to increase. By
this time, the cell size
distribution shows two overlapping cell
populations: one with a cell
size corresponding to that of the
culture growing at 39°C (45% of
the population) and the other
with a cell size approximately twice as
big (55% of the population)
as a result of cell division
blockage.
After this transition period, a new state in the population was reached
and held for the next 3 to 4 h (Fig.
3B, from 4 to
6 h).
Replication continued at an underreplication level, as could
be deduced
from the presence in the population of a fraction of
cells with an even
lower DNA content than the cells with a low
DNA content at 39°C. As
time passed, the fractions of cells with
no and one chromosome
increased slowly in the population, each
accounting for 20% of the
total population 5 to 6 h after the
temperature shifts (Fig.
3B;
Table
1). Cell sizes were distributed
in two overlapping populations,
and whereas the small cells got
slightly smaller than in the initial
distribution, the bigger
ones had a larger average cell size (see the
average mass/cell
ratios for the population in Table
1). The percentage
of the
smaller cells increased with time to represent around 60% of
the
population 5 to 6 h after the temperature shift. The
distributions
of the cell sizes and DNA contents were almost identical
5 and
6 h after the downshift. The distribution changed after
7 h, when
the culture started to reach the stationary phase (data
not shown).
Hence, the inhibition of chromosome replication led to an
abolishment
of cell division, and the achievement of a new level of
replication
allowed cell division to
resume.
In general, the effects on the cell population after the downshift to
38°C, as observed by flow cytometry, were essentially
the same as
those occurring after the shift to 37°C (Fig.
3C).
However, the
changes were less drastic and the new stable state
was reached more
quickly. The cell size distribution was similar
to that at 39°C until
2 h after the shift. At later times, the
cell population consisted
of a majority of cells with the average
cell size of the 39°C culture
and a group of bigger cells; their
proportions were 80 and 20%,
respectively, 4 h after the shift
(mass/cell ratios in Table
1).
From the DNA content distribution,
the same sequence of events as that
occurring after the shift
to 37°C could be observed; thus,
replication resumed 2 h after
inhibition of initiation of
replication following the shift, and
the new level was maintained
during the following 3 h. In this
case, when the population attained
the new constant underreplication
level, a percentage of the cell
population with an even lower
DNA content than the cells with a low DNA
content in the 39°C
culture could be detected, but the distribution
did not present
as distinct peaks as it had at 37°C. At the stable
level, around
65% of the cell population contained from one to two
chromosome
equivalents per cell. In this case, the number of
chromosomeless
cells did not increase significantly, and thus the
proportion
moved from around 4.5% after the shift to around 7.5%
after 4
h at 38°C (Fig.
3C; Table
1).
Since the proportion of chromosomeless cells increased in
EC::71CW/pOU420Ap
s over time after the temperature
shift down to 37°C, representing
20% of the population 5 h
after the shift, the doubling time obtained
by measuring the increment
in absorbance in these cultures overestimates
the real generation times
(Table
1).
Replication speed during underreplication.
The aim of the
present work was to analyze the effects of a delay of the initiation of
replication on cell division. Although a delay in the time of
initiation of replication
that is to say, an increase in the average
initiation mass
was detected by flow cytometry during periods of
underreplication in EC::71CW/pOU420Aps after
temperature downshifts (Fig. 3), a larger C/
ratio could be an
additional cause for the decrease in the DNA/mass ratio (10,
12). If an extension of the C period were the case, a delay in
the time of cell division could be ascribed to the replication period
being longer than in the control situation whenever a completed chromosome replication and correct partitioning are required for cell
division. Hence, it was important to determine the length of the C period.
Addition of rifampin inhibits initiation of replication but allows
ongoing replication to proceed to completion (runout replication)
(see
Materials and Methods). The kinetics of chromosome replication
was
determined by following the runout of chromosome replication
by flow
cytometry as described by Skarstad and Wold (
34).
Rifampin
(200 µg/ml) and cephalexin (50 µg/ml) were added to
EC::71CW/pOU420Ap
s cultures growing
exponentially at 39°C and 5 h after the shift
from 39 to 37°C.
Samples for flow-cytometric analysis were collected
at different time
points after the addition of rifampin and cephalexin
until the
replication runout was completed. The replication kinetics
for both
situations were compared (Fig.
4). The amounts of time
required for narrow peaks, representing fully replicated chromosomes,
to appear were similar in the two cases. The DNA histograms of
each
culture showed that in both cases, the majority of the population
contained fully replicated chromosomes 60 min after the addition
of the
drugs and that the best resolution was obtained at 120
min, when even
peaks for more than four chromosomes per cell became
defined (Fig.
4A).
The resolution of the peaks corresponding to
four chromosomes per cell
at the two temperatures was analyzed
by calculating the CV peaks (see
Materials and Methods). The CV-half
values versus the sampling time
were plotted (Fig.
4B). The values
of the slopes for the first part of
the curves represent the speed
of resolution, and the
x
values for the crossing point after extrapolation
of both parts of the
curve correspond to the time required for
the resolution of the peak.
The values obtained for the slopes
were

0.726 min
1 at
39°C and

0.794 min
1 at 37°C, and the crossing point
was at 57 min in both cases.
Similar results were obtained in an
analysis of the two-chromosome
peaks (data not shown).

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FIG. 4.
Kinetics of DNA synthesis during replication runout in
EC::71CW/pOU420Aps. The strain was grown
exponentially in M9 glucose medium at 39°C, and at an
A550 of 0.029, part of the culture was shifted
to 37°C. At an A550 of 0.29 at 39°C, and
5 h after the shift to 37°C (A550, 0.28),
rifampin (200 µg/ml) and cephalexin (50 µg/ml) were added to the
cultures (time zero). At different time points, samples were collected
and analyzed by flow cytometry. (A) DNA histograms during replication
runout at 39°C (left column) and 5 h after the shift to 37°C
(right column). The figure shows the distribution of DNA content in
samples collected before (time zero) and at the indicated times after
addition of the drugs. (B) Progress of the coefficient of variance
(CV-half) for the four-chromosome peak during the runout of replication
at 39°C ( ) or 5 h after the shift to 37°C ( ). Notice
that more experimental data are taken into account in panel B than are
shown in panel A.
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The similarity of the values for these parameters in the two situations
indicates that the replication speed was approximately
the same at
39°C and after the shift to 37°C. Therefore, this
result ruled out
any effect of the length of the C period on the
decline in the DNA/mass
ratio as well as on the cell division
pattern under these
conditions.
It should be noted that replication runout was more complete at 39°C
than after the shift to 37°C, according to the resolution
of the
peaks in the DNA content distributions (Fig.
4A, 180 min);
this effect
was mainly observed in cells with more than three
chromosome
equivalents.
Cell division during underreplication.
The effects of
underreplication levels on cell division were studied in
EC::71CW/pOU420Aps at different and stabilized
DNA/mass ratios. With this analysis, we addressed two main questions
regarding the control of cell division in bacteria: when and where cell
division takes place.
Three hours after the temperature shifts from 39°C, 4 h after
the shift to 38°C, and 5 h after the shift to 37°C, samples
from the different cultures were collected and the cells were
fixed in
70% ethanol. These cell populations were studied under
the microscope
after DAPI staining (see Fig.
5A). We analyzed
1,000 cells in the total
population, or 250 cells in the case
of septating cells, by
phase-contrast and fluorescence microscopy
and image analysis, and we
determined the cell length, position
of the incipient septum, and
number of nucleoids per cell (see
Materials and
Methods).
Microscope images showed a homogeneous population of cells growing at
39°C, with an average normal cell size distribution
and one or
two nucleoids per cell (Fig.
5A, upper panel). After
the temperature downshifts, the cell size and nucleoid distribution
of
the population became more heterogeneous. Cultures growing
at
38 and 37°C 4 and 5 h after the shift, respectively, contained
filamented cells as well as cells of normal size (Fig.
5A, middle
and
lower panels). At 38°C, many cells were slightly bigger than
the
average size at 39°C, and some filaments were present. The
proportion
of filamented cells in the population increased as
the replication
level decreased. Thus, at 37°C, many real filaments
could be
observed. Filamented cells frequently contained more
than one or two
nucleoids, generally having around four, which
were clearly separated,
and large DNA-free areas. At 37°C, DNA-less
cells of normal size were
frequently found. Therefore, the abolishment
of cell division during
underreplication that had been detected
by flow cytometry was easily
observed by microscopy (Fig.
3 and
5A; Table
1). This effect could be
quantified by determining
the increase of the average mass/cell ratio
and cell length in
the population (Table
1).

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|
FIG. 5.
Phase-contrast and fluorescence photomicrographs
(A), cell length distributions (B), septum localization patterns (C),
and nucleoid distributions (D) for
EC::71CW/pOU420Aps. The strain was grown
exponentially in M9 glucose medium at 39°C, and at an
A550 of between 0.02 to 0.04, the culture was
split and downshifted to 38 and 37°C. Three hours after the shift
from 39°C (upper panels), 4 h after the shift to 38°C (central
panels), and 5 h after the shift to 37°C (low panels), cells
from the cultures growing at the different temperatures were collected
and fixed in ethanol (70%, final concentration). (A) After DAPI
staining (0.5 µg/ml), the cell populations were analyzed by combined
phase and fluorescence microscopy (see Materials and Methods). One
thousand cells from the total population and 250 septating cells from
each culture were analyzed. Bar, 5 µm. (B) Cell length distributions
in the total population (continuous lines) and of septating cells
(broken lines). (C) Septating cells with (from the top to the bottom of
the bars) one ( ), two ( ), three ( ), four ( ), or five and
more ( )
nucleoids. (D) To represent the localization of the septum, the lengths
of the two future daughter cells produced in each septation event were
plotted against each other, with the shorter cell always being chosen
for the x axis. The dotted lines represent different
daughter cell length ratios. Closed circles represent the cells which
would give two nucleated daughter cells after division, and open
circles represent the cells which would give one nucleated and one
nucleoid-free daughter cell. In the latter case, the anucleate cell was
always the shorter one.
|
|
The frequency of cell division was determined by counting the
number of septating cells among 1,000 cells from the total population.
The septation frequency observed in exponentially growing cultures
of
EC::71CW/pOU420Ap
s with a normal DNA content was
essentially maintained under moderate
levels of underreplication (at
38°C). However, below some threshold
level of replication (at
37°C), cell division was partially abolished
and the frequency of
septating cells was reduced (Table
1). The
reduction in cell division
frequency was also reflected in the
increase of the average mass/cell
ratio and cell length in the
population (Table
1; Fig.
3 and
5A and
B).
To determine when cells divide, the cell length of septating cells was
measured (Fig.
5B). The distribution of the length
of septating cells
at 39°C showed a single peak, with a mean length
± standard
deviation of 4.5 ± 0.7 µm (Fig.
5B, upper panel; Table
1,
eighth column). After the shift to 38°C, the length distribution
of
the septating cells was essentially the same as that at the
normal
level of replication (at 39°C); thus, 80% of the cells
were grouped
around a mean length of 4.9 ± 0.8 µm, but the remaining
20% of
the scored cells fell into a group with double the average
length
(10.0 ± 2.2 µm) (Fig.
5B, middle panel; Table
1). The
cell
length distribution of septating cells at 5 h after the shift
to
37°C was clearly different from the situation at 39°C (Fig.
5B,
lower panel). In this case, the distribution of cell length
gave two
distinct peaks, with average lengths of 6.5 ± 1.7 and
13.2 ± 1.6 µm for 63 and 25% of the scored cells, respectively.
A
minority of the cells, around 12%, were distributed in a more
dispersed group with a mean length of 21.6 ± 4.5 µm. These
distinct
peaks are more easily seen in the three-dimensional plot shown
in Fig.
6. The distinct peaks in the
length distribution of septating
cells at 37°C localized around one,
two, and four times the length
of the septating cells at 39°C,
suggesting that if cell division
cannot take place at the normal size,
a discrete cell length (two
or four times the normal cell size) is
required to allow cell
division.

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|
FIG. 6.
Three-dimensional plot of the length of the two future
daughter cells versus the number of cells obtained from length
measurements of septating cells of
EC::71CW/pOU420Aps growing at 37°C. The data are
the same as in the lower panels Fig. 5B (broken lines) and 5D.
|
|
By comparing the cell length distribution of septating cells to that of
the total population in EC::71CW/pOU420Ap
s (Fig.
5B), the potentials for cell division for cells of the
different
lengths were compared. At 39°C, cells longer than the
average
population length were able to divide (Fig.
5B, upper
panel). In the
cases of underreplication, the main population
divided with the same
capacity as that observed at 39°C, but although
they divided, the
filamented cells had a reduced potential to
carry out cell division
(Fig.
5B, middle and lower panels); this
is clear from the fact that
the ratios between the two histograms
are much higher at the cell
length of normal dividing cells than
at longer cell
lengths.
The nucleoid distribution in septating cells was analyzed, and the
numbers of nucleoids per cell for the different cell sizes
are
represented in Fig.
5C. At normal levels of replication, most
of the
dividing cells (around 90%) contained two nucleoids (Fig.
5C, upper
panel). The fraction of septating cells with more than
two nucleoids
was increased as the level of replication decreased.
Thus, after the
temperature shift to 38°C, only 75% of the septating
cells contained
two nucleoids, and after the shift to 37°C, this
proportion was
diminished to 55% (Fig.
5C, middle and lower panels,
respectively).
The septating cells with two nucleoids had average
lengths of 4.5, 5.2, and 7 µm at 39, 38, and 37°C, respectively.
Septating cells
containing more than two nucleoids were almost
always longer than
normal septating cells (Fig.
5C, lower panel);
in these cells, the
nucleoids were DNA masses well separated from
each other. Therefore, no
partitioning problems seem to cause
abolishment of cell division during
underreplication. This nucleoid
distribution in septating cells can be
considered as another result
of the abolishment of cell division. Since
the DNA/mass ratio
in these populations was reduced, the fact that
septating cells
contained more than two nucleoids indicates that not
only the
completion of chromosome replication and partitioning but also
a certain DNA/mass cell ratio is required to allow cell
division.
To study the pattern of cell division during underreplication, the
relative placement of the septa along the length axis of
the cell was
analyzed. The distance from each pole to the septum
was measured for
each cell, and the data were inserted in Fig.
5D. Despite the
disturbance of the cell length at the time of
septation, due to the
abolishment of cell division during underreplication,
the pattern of
division septum localization in the elongated cells
was
nonrandom.
At normal levels of replication, when the septating cells were grouped
in a single peak in the cell length distribution, the
majority of the
cells (around 94%) presented the incipient septum
in the center of the
cell, since they were grouped at around a
1:1 length ratio between the
daughter cells (Fig.
5D, upper panel).
In this case, a few daughter
cells (0.8%) were chromosomeless.
In the population growing for 4 h at 38°C after the shift from
39°C, 85% of the septating cells
fell into the 1:1 length ratio
class, but besides this, the septum was
located in a one-quarter
position in around 10% of the cells to give a
1:3 daughter length
ratio (Fig.
5D, middle panel). In the 1:3 group,
the shorter daughter
cell had the normal length of a newborn cell. The
frequency of
chromosomeless cells after the shift to 38°C was
essentially the
same as that for the septating cells growing at 39°C
(1.2% of
the daughter cells). The effect of underreplication on the
cell
division pattern was more drastic after the shift to 37°C; the
sizes of septating cells fell into distinct cell length classes.
With
regard to the septation pattern, two main groups could be
clearly
distinguished, corresponding to 1:1 and to 1:3 cell length
ratios (Fig.
5D, lower panel). A reduced proportion of the septating
cells belonged
to the 1:1 group (60%), and instead an increased
proportion of cells
presented an asymmetric septation pattern;
thus, in around 27% of the
cells, the septation event produced
a 1:3 daughter length ratio. A more
dispersed group of cells,
corresponding to 10% of the analyzed cells,
could be ascribed
to an 1:7 length ratio. The asymmetric septations
always produced
one daughter cell with about the same length as the
shorter daughter
cell formed at 39°C. Nevertheless, the length of the
shorter cell
slightly increased when the level of replication
decreased; thus,
the mean value for the length of the shorter cell,
when considering
only shorter cells smaller than 5 µm, increased from
2.2 ± 0.4
µm at 39°C to 2.5 ± 0.6 µm 4 h after
the shift to 38°C and to
2.9 ± 0.7 µm 5 h after the
shift to 37°C.
The cells with a central septum location (60%) could be divided into
two groups: cells with a size similar to that at 39°C
and a small
cluster (4% of the total number of analyzed cells)
with double-cell
size in which the septum still formed in the
middle position of the
lengthwise cell axis. In the culture growing
for 5 h at 37°C,
chromosomeless cells represented 9% of the daughter
cell population.
The majority of cells which, after septation,
would produce a
chromosomeless daughter cell (96%) were located
above the line of the
1:3 length ratio, and they accounted for
70% of the total cells in
this area (Fig.
5D, lower panel). Therefore,
the septation events which
led to the production of one chromosomeless
daughter cell took place in
the longer cells, which still could
form a visible septum, after an
asymmetric septation; that is
to say, when the shorter daughter cells
came from the longer mother
cells, they were almost always nucleoid
free. Chromosomeless cells
were always the shorter of the two cells
produced after the septation
event, and they had the same mean length
as the shorter cell formed
after the septation at 39°C (2.6 ± 0.5 µm for chromosomeless cells
at 37°C, compared to 2.2 ± 0.4 µm for the shorter cell at 39°C).
Therefore, although cells with different lengths could divide, the
septations at any level of replication resulted in a daughter
cell
length ratio of 1:1, 1:3, or 1:7. In no case was a cluster
of cells
found around the 1:2 length ratio. The proportions of
cells at the
different septation length ratios reflect a preference
for central
septations until a certain cellular length is reached.
The frequency of
the asymmetric septation increased as the level
of replication
decreased. It appears that when the delay in replication
does not allow
cell division at the normal cell length, asymmetric
septations (1:3 and
1:7) begin to occur (Fig.
5D).
 |
DISCUSSION |
We have used a so-called intR1 strain to vary the
initiation mass of E. coli from normal to higher values by
performing small changes in growth temperature. Shifting a culture
growing exponentially at 39°C to 38 or 37°C resulted in a
transition to new stable DNA/mass ratios, namely, about 80 and 60% of
the initial value, respectively. This corresponds to a delay in the
time of initiation of replication by 15 or 27% of the generation time
(see below) (Fig. 1). Under these conditions, the septating cells were
of two main classes, those that divided in the middle to give daughter
cells of about normal size and those that were twice as big and divided
to produce one daughter of normal size and one three times as big (1:3
ratio); some of the divisions resulted in one daughter (always the
smallest) being chromosomeless. Our data are in accord with the mode
denoted under-replication-II in Fig. 1. Under conditions of
underreplication there was a considerable fraction of the cells that
were elongated and contained more than two nucleoids. Hence, the direct
coupling of nucleoid partitioning and cell division was lost. This
suggests that cell division requires not only completed replication and nucleoid partitioning but also a DNA/mass ratio above a certain threshold value. Our main results, obtained under conditions of exponential growth, are similar to those reported by Bernander et al.
(6) when cell division was studied after synchronous initiation of replication in the same intR1 strain after
runout of replication by shifting exponentially growing populations to 36°C.
It should be stressed that Fig. 1 gives an idealized picture of the
cell cycle in int strains, since initiation of replication of the intR1 chromosome is random over time (23);
hence, the time of initiation varies within the population, but Fig. 1
describes the average situation. The randomness also explains why there was not a distinct shift from the normal cell division pattern to a new
one during underreplication. There will always be some cells in which
initiation of replication occurs early and that divide essentially normally.
The delay in initiation of replication caused by the transition from
39°C to 38 or 37°C can be calculated as follows. The average
number of genome equivalents per cell, G, present in an exponentially growing population is determined by the equation G = (
/C · ln2)[2(C + D)/
2D/
] (11),
in which C, D, and
are the lengths of the C and D periods and the generation time, respectively. A delay by x
min of initiation of replication would give the equation G = (
/C · ln2)[2(C + D
x)/
2(D
x)/
].
The values for the delay x cannot be calculated exactly
because D is not known. However, the data from Fig. 4 show
that the lengths of the C period at 39 and 37°C were
approximately the same. Hence, assuming that C and
D are 57 (Fig. 4) and 20 min, respectively, the value of
x can be calculated to be 10 and 30 min at 38 and 37°C,
respectively, or 15 and 27% of the generation times at these two
temperatures. It should also be stressed that the measured generation
times are overestimates of the real ones because DNA-less cells were
formed during underreplication.
During underreplication, the cell length distributions of the septating
cells were slightly broader than under normal conditions; this
broadening took place only at the large side of the cell length
distributions. This indicates that cell division could be postponed
when replication and nucleoid partitioning were slightly delayed and
that when the delay were longer, cell division would be omitted and
would not take place until one doubling in mass later (Fig. 5D). The
molecular nature of this putative cross talk between
replication-nucleoid partitioning and cell division is unknown.
Previous experiments showed that the SOS- and SfiA-mediated division
inhibition was not the main reason for the cessation of division that
was observed after runout of chromosome replication in this
intR1 strain (6). Under these conditions, some of
the divisions occurred at twice the normal mother length; in this case,
one of the daughter cells was of normal newborn size. This favors the
idea that cell division has got its own, independent control system. It
had been expected that the cells would divide in the middle. The 1:3
division pattern of elongated cells suggests that there is a size
window during which cell division is allowed. The maximum size that
still allowed cell division was about 25% bigger than the maximum size
of dividing cells at the normal DNA/mass ratio (Fig. 5D). If cell
division has not occurred at this size, it is omitted and a second
opportunity occurs one mass doubling later. However, the ability to
divide in the middle is lost, and cell division now takes place at new
sites one-fourth of the cell length from the poles. Hence, cell
division in some way seems to measure the distance from one of the
poles; according to Donachie et al. (16), cell division at
all growth rates initiates at a specific cell length rather than at a
specific cell mass. As a matter of fact, even when very long cells
divided, one of the daughters was of normal cell size, and although the
number of measured cells was small, our data suggest that division
occurs at a 1:7 ratio between the lengths of the two daughter cells. It
may be appropriate to mention that Raskin and de Boer (31) showed that the MinE protein forms a ring in the middle of the cell
very early in the cell cycle. They found that there were two MinE rings
in some elongated cells and that these rings were placed one-fourth of
the cell length from each cell pole, as if the ring in the middle had
disappeared. As a matter of fact, we observed that filamented cells
occasionally contained two septa at the cell quarters, with the normal
distance to each pole, and that only about 4% of the septating cells
at 37°C were twice the normal mother size and still divided in the middle.
Omission of one cell division led to the appearance of elongated cells
with more than two separated nucleoids. Hence, there was no tight
coupling between completed replication-nucleoid partitioning and cell
division; rather, for cell division to occur, not only must cells be of
an appropriate size and two separated nucleoids be present, but also
the DNA/mass ratio must be above a certain threshold value.
During underreplication, in a significant number of divisions of
filamented cells the smallest daughter did not contain chromosomal DNA.
Several groups have studied the cell size distribution of anucleate
cells formed after total inhibition of DNA replication by using
temperature-sensitive dna strains (20, 22, 25, 26,
36). The data are somewhat conflicting; some groups found that
the anucleate cell size distribution was narrow and comparable to that
of normal newborn cells (22, 36), whereas Mulder and Woldringh (25, 26) reported a more random
distribution. In our case, the anucleate daughter cells were of
normal size, supporting the idea of a nonrandom positioning of the
septa (see also reference 20, p. 1635 to 1636). We
have earlier favored the idea that the size of the nucleoid
determines the size of the daughter cells (2), but the size
of the DNA-less cells contradicts this and strengthens the conclusion
that cell division has its own control system also with respect to the
position of the division site.
When E. coli is grown in different media its generation time
varies. The dimensions of the cells, both diameter and length, increase
with increasing growth rate (16, 39). In the present study,
however, although there was a reduction in growth rate during
underreplication, the cell diameter did not change measurably (0.84 ± 0.08 µm at 39°C versus 0.88 ± 0.09 µm at
37°C) (Fig. 5A). Hence, it appears that the diameter of the cells is
set by the medium rather than by the growth rate.
In conclusion, our studies with intR1 strains under
conditions of both overreplication (3) and underreplication
(this paper) indicate that cell division has its own control system,
with respect both to its coupling to the cell mass and to the
positioning of the division sites, that is independent of chromosome
replication. The nature of this control system is not yet known.
 |
ACKNOWLEDGMENTS |
This work was supported by the Swedish Natural Science Research
Council and the Swedish Cancer Society. Grants from the Knut and Alice
Wallenberg foundation enabled us to purchase the microscope and the
image analysis equipment. E.B. acknowledges a fellowship from the
Swedish Institute.
 |
FOOTNOTES |
*
Corresponding author. Mailing address: Department of
Microbiology, Biomedical Center, Uppsala University, Box 581, S-751 23 Uppsala, Sweden. Phone: 46 18 471 45 26. Fax: 46 18 53 03 96. E-mail:
kurt.nordstroem{at}mikrobio.uu.se.
Present address: Departamento de Bioquímica y
Biología Molecular y Genética, Facultad de Ciencias,
Universidad de Extremadura, 06080 Badajoz, Spain.
 |
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Journal of Bacteriology, December 1998, p. 6364-6374, Vol. 180, No. 23
0021-9193/98/$04.00+0
Copyright © 1998, American Society for Microbiology. All rights reserved.
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