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Biophys J, April 2000, p. 1748-1764, Vol. 78, No. 4
Departments of *Chemistry and #Biochemistry, University of Wisconsin-Madison, Madison, Wisconsin 53706, USA
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ABSTRACT |
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To obtain turgor pressure, intracellular osmolalities, and cytoplasmic water activity of Escherichia coli as a function of osmolality of growth, we have quantified and analyzed amounts of cell, cytoplasmic, and periplasmic water as functions of osmolality of growth and osmolality of plasmolysis of nongrowing cells with NaCl. The effects are large; NaCl (plasmolysis) titrations of cells grown in minimal medium at 0.03 Osm reduce cytoplasmic and cell water to ~20% and ~50% of their original values, and increase periplasmic water by ~300%. Independent analysis of amounts of cytoplasmic and cell water demonstrate that turgor pressure decreases with increasing osmolality of growth, from ~3.1 atm at 0.03 Osm to ~1.5 at 0.1 Osm and to less than 0.5 atm above 0.5 Osm. Analysis of periplasmic membrane-derived oligosaccharide (MDO) concentrations as a function of osmolality, calculated from literature analytical data and measured periplasmic volumes, provides independent evidence that turgor pressure decreases with increasing osmolality, and verifies that cytoplasmic and periplasmic osmolalities are equal. We propose that MDO play a key role in periplasmic volume regulation at low-to-moderate osmolality. At high growth osmolalities, where only a small amount of cytoplasmic water is observed, the small turgor pressure of E. coli demonstrates that cytoplasmic water activity is only slightly less than extracellular water activity. From these findings, we deduce that the activity of cytoplasmic water exceeds its mole fraction at high osmolality, and, therefore, conclude that the activity coefficient of cytoplasmic water increases with increasing growth osmolality and exceeds unity at high osmolality, presumably as a consequence of macromolecular crowding. These novel findings are significant for thermodynamic analyses of effects of changes in growth osmolality on biopolymer processes in general and osmoregulatory processes in particular in the E. coli cytoplasm.
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INTRODUCTION |
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Escherichia coli grows over
more than a hundred-fold range of external osmolality (Osm), extending
from as low as 0.015 Osm (Baldwin et al., 1995
) up to ~1.9 Osm
(McLaggan et al., 1990
; Cayley et al., 1991
) in minimal medium and up
to ~3.0 Osm in rich medium (Record et al., 1998a
). To grow over this
range of external water activity (1.0 > aH2O
0.95, where
aH2O = e
Osm/55.5) requires a high degree of
thermodynamic sophistication. In general, growing cells may adapt to
changes in osmolality of the growth medium i) by making compensating
changes in the intracellular osmolality by changing the amounts of
water and/or solutes in the cytoplasm and periplasm, so that the
osmolality difference
Osm and turgor pressure 
= RT
Osm across the cell wall are maintained, and/or ii) by
allowing
Osm to change so that turgor pressure changes with external
osmolality (Record et al., 1998a
). E. coli makes large and
systematic changes in the amounts of cell and cytoplasmic water and in
the amounts of periplasmic and cytoplasmic solutes in response to
changes in osmolality of growth (reviewed by Record et al., 1998a
;
Csonka and Epstein, 1996
). How do these changes affect the activity of
cytoplasmic water? Of particular relevance for the present study are
observations that the amount of periplasmic membrane-derived
oligosaccharide (MDO, heterogeneous anionic glucose oligomers that are
too large to pass through pores in the outer membrane; Kennedy, 1996
)
increases as the osmolality of growth decreases for all wildtype
E. coli K-12 strains examined (Kennedy, 1982
; Kennedy and
Rumley, 1988
; Sen et al., 1988
; Lacroix et al., 1989
). Do these changes
in amount of periplasmic MDO demonstrate that turgor pressure changes
with osmolality of growth? Knowledge of turgor pressure as a function
of osmolality of growth is the only way to determine the physiological
range of cytoplasmic water activity, which, in turn, is needed for
analyses of the thermodynamics of cytoplasmic biopolymer processes as a
function of growth osmolality.
The activity of a small subset of genes and gene products
varies with the osmolality of the growth medium, although the nature of
the signal(s) controlling these osmoregulated changes is not well
understood (Wood, 1999
). Changes in turgor pressure have been
considered as a possible osmoregulatory signal (Wood, 1999
; Csonka and
Epstein, 1996
). Few estimates of turgor pressure of E. coli
are available under any conditions, however, and the questions of
whether turgor pressure exists only across the cell wall/outer membrane
or across the inner (cytoplasmic) membrane and whether turgor pressure
changes with osmolality of growth have been controversial and
unresolved. Studies of osmotic and Donnan properties of nongrowing suspensions of the closely-related bacterium Salmonella
typhimurium led Stock et al. (1977)
to conclude that the cytoplasm
and periplasm are isoosmotic, and that turgor pressure is maintained
across the cell wall. However, studies of the osmoregulation of the
expression of the kdpABC operon in E. coli have
been interpreted as indicating that changes in turgor pressure are
sensed by the cytoplasmic membrane-bound kdpD sensor kinase (Laimins et
al., 1981
). Phase and electron microscopy studies of growing cells have
led to the proposal that turgor pressure is maintained across the
cytoplasmic membrane (Koch, 1995
, 1998
).
To address these issues, we have indirectly quantified the variation of turgor pressure with external osmolality by measuring the effects of osmolality of growth and of plasmolysis with NaCl on the volumes (i.e., amounts) of cell, periplasmic, and cytoplasmic water, and by analyzing the dependence on growth osmolality of the concentration of periplasmic MDO, calculated from published amounts of MDO and from our measurements of periplasmic volume. We interpret the observed changes in amounts or volumes of water and in concentration of periplasmic MDO in terms of simple physical models. We conclude that the periplasm and cytoplasm are isoosmotic and that E. coli systematically varies turgor pressure with external osmolality.
Background on passive and active responses of E. coli to changes in external osmolality
The cytoplasm of E. coli exhibits both passive and
active responses to changes in external osmolality with NaCl or other
cytoplasmic membrane-impermeable solutes (Record et al., 1998a
). As an
example of a passive response, consider a so-called plasmolysis
titration (Cayley et al., 1991
, 1992
) in which a fresh, nongrowing cell suspension harvested from exponential growth in minimal medium at low
osmolality (e.g., 0.1 Osm) is titrated with NaCl. Na+ and
Cl
equilibrate across the outer cell membrane, subject to
the Donnan distribution for ionic species, which results from the
presence of outer-membrane-impermeable anions in the periplasm (Stock
et al., 1977
; Sen et al., 1988
; and see below). Because the cytoplasmic membrane is impermeable to NaCl and incapable of supporting an osmotic
pressure difference, the cytoplasm loses water to increase its
osmolality to that of the periplasm; this passive response reduces the
amount of cytoplasmic water at 1.0 Osm to ~30% of its original value
without changing the amounts of any cytoplasmic solutes (Cayley et al.,
1991
; Record et al., 1998a
). (Plasmolysis beyond 1.0 Osm results
eventually in removal of all unbound [osmotically active] water from
the cytoplasm.) To recover from the plasmolyzed state at 1.0 Osm and
resume growth requires an active osmoregulated response, initiated by
increased uptake of extracellular K+, with the end result
(in minimal growth medium without added osmoprotectants) that
cytoplasmic amounts of K+, glutamate
(and
other organic anions), trehalose, and water increase, and the amount of
cytoplasmic putrescine (2+) decreases (cf., Csonka and Epstein, 1996
;
Record et al., 1998a
for reviews). We propose that the fundamental
reason for the increases in amounts of cytoplasmic K+,
glutamate
, and trehalose is to allow the cell to increase
the amount of cytoplasmic water (by almost twofold over that
characteristic of the nongrowing plasmolyzed state at 1.0 Osm) and
thereby achieve the highest growth rate possible in a minimal medium
without osmoprotectants at this osmolality (Cayley et al., 1991
, 1992
;
Record et al., 1998a
).
In the present study, we use suspensions of E. coli lacking external K+ to prevent cells from adapting to osmotic stress, and analyze measurements of the passive changes in cell and compartment volumes in plasmolysis titrations of cells with NaCl to quantify their osmotic properties. This novel analysis provides the basis for our use of cell and cytoplasmic volume measurements to determine the osmotic properties and intracellular water activity of E. coli as a function of osmolality of growth.
The balloon model for turgor pressure of E. coli: why measurements of cell volume provide information about turgor
The bacterial cell wall has been considered balloon-like (Doyle
and Marquis, 1994
) because it can stretch under pressure. Outwardly
directed turgor pressure (the osmotic pressure difference between the
cell interior and the external medium) is the analog of the difference
in air pressure, which inflates a balloon. Turgor pressure stretches
the peptidoglycan of the E. coli cell wall (Woldringh, 1994
and references therein) elastically (Koch and Woeste, 1992
) relative to
the unstressed state existing in the absence of an osmotic pressure
difference. E. coli has two compartments (periplasm and
cytoplasm) with different permeabilities to solutes, so osmotic
responses of both compartments must be considered to interpret effects
of osmotic stress on cell volume. In this work, we provide additional
evidence that the periplasm and cytoplasm are isoosmotic, in agreement
with the conclusion of Stock et al. (1977)
and Sen et al. (1988)
, which
simplifies the physical situation. Thus, the balloon analogy is
instructive, and serves as the qualitative basis for our model that
changes in cell volume reflect changes in turgor pressure.
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MATERIALS AND METHODS |
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Bacterial strain, growth media, buffers, and chemicals
All experiments were performed with E. coli K-12
strain MG1655. Cells were grown aerobically at 37°C in a very low
osmolality MOPS (3-(N-morpholino)-propanesulfonate)-buffered
glucose minimal medium (VLOM; 0.03 Osm; Capp et al., 1996
), in the
MOPS-buffered glucose minimal medium (MBM; 0.1 Osm; Cayley et al.,
1989
), or in MBM with NaCl used to adjust osmolality of the growth
media. Wash buffer is growth medium in which all K+
(present as KH2PO4) and glucose were replaced
by an isoosmotic amount of NaCl. Plasmolysis buffer is wash buffer with
additional NaCl to increase the osmolality.
3H2O (1 mCi/g) and
[3H] polyethylene glycol (1.51 mCi/g) were
obtained from DuPont (Boston, MA). [14C] sucrose (621 mCi/mmol), [14C] inulin (9.4 mCi/mmol), [14C] urea (54.0 mCi/mmol), and [3H] sucrose (12.0 Ci/mmol) were obtained from Amersham (Arlington Heights,
IL). All radiochemicals except 3H2O and
[14C] urea were purified of radiolabeled contaminants
that interfere with volume measurements by preincubation with cell
slurries as previously described (Cayley et al., 1991
, 1992
).
NH4OH (5.08 N in water), 1-bromododecane, and silicone oil
were obtained from Aldrich (Milwaukee, WI).
Measurement of amounts of cellular and cytoplasmic water in nongrowing cell suspensions
Volumes of cell water (
cellwa)
and cytoplasmic water (
cytowa) in
units of µL per mg cell dry weight (µL/mg DW) of fresh nongrowing cell suspensions were obtained from comparisons of the volume of cell
pellets accessible to 3H2O to that of
14C inulin (a polymer that is outer-membrane impermeable)
or 14C sucrose (which freely diffuses into the periplasm
but is not transported into the cytoplasm) using the method of Stock et
al. (1977)
as described previously (Cayley et al., 1991
, 1992
). (These volumes are equivalent to amounts of water in mg water/mg DW assuming a
density of intracellular water of 1.0 g/mL). Briefly, cells were
harvested from exponential growth (at ~3 × 108
cells/mL, <0.2 mg DW/mL) by centrifugation at 7,000 × g for 8 min. Cell pellets were suspended in isoosmotic wash
buffer, recentrifuged, resuspended to a final cell density of ~5 mg
DW/mL with wash buffer and swirled periodically for the ~30 min
typically needed to complete a series of measurements. Three
µCi/mL of 3H2O and 0.2 µCi/mL of either 14C sucrose or
14C inulin were then added per mL of suspension, after
which the samples were immediately centrifuged at 12,000 × g for 30 s (a sufficient time to pellet cells
completely). The cpm in samples of the supernatant and cell pellets
were then assayed by dual isotope scintillation counting and used to
determine
cellwa and
cytowa (in µL/mg DW) as described
previously (Cayley et al., 1991
). Measurements of
cytowa immediately after harvest and
40 min after harvest were the same, demonstrating that the amount of
cytoplasmic water did not vary during the time needed to perform a
series of measurements. In addition,
cytowa was independent of time of
incubation of 14C sucrose in suspensions before volume
assay for at least 10 min, the longest time tested. Control experiments
showed no significant differences in volumes determined with
3H PEG instead of 14C inulin or with
14C taurine instead of 14C sucrose or
3H sucrose, indicating the absence of any specific
interactions of these probes with cell components. Bubbling suspensions
with O2 or incubation with 5 mM fructose, 11 mM glucose or
1.3 mM KH2PO4 for five min prior to assay did
not affect
cytowa, showing that any
deprivation of oxygen or nutrients that occurred during preparation of
suspensions did not lower
cytowa. All
steps after cell growth were performed at room temperature.
In NaCl plasmolysis titrations to determine the passive responses of
cellwa and
cytowa to increases in external
osmolality, suspensions of cells grown at 0.03 Osm (in VLOM) or at 0.83 Osm (in MBM+0.4 NaCl) were assayed as described above except that,
immediately before addition of radiochemicals, samples were diluted
fivefold with plasmolysis buffer to achieve the desired range of final
NaCl concentrations and a final cell density of ~5 mg DW/mL.
Most previously published values of
cytowa (Cayley et al., 1991
, 1992
)
referred to in this paper were determined using 14C taurine
in place of 14C sucrose. McLaggan and Epstein (1991)
found
that taurine can be accumulated with a KM of ~30 mM at
high osmolality by strains of growing E. coli defective in
the osmotically regulated accumulation of cytoplasmic trehalose.
However, in addition to controls that previously demonstrated that
neither purified 14C taurine (typically used at a
concentration of 0.28 mM) nor 14C sucrose is accumulated by
nongrowing suspensions of our wild-type strain under the conditions of
our volume assays (Cayley et al., 1991
, 1992
), we observe that 1)
cytowa of suspensions measured with
purified 14C sucrose or 14C taurine for cells
grown in MBM+0.5 M NaCl are the same within error, 2) dilution of
14C taurine to 1 mM with unlabeled taurine does not alter
measured values of
cytowa of cells
grown in MBM+0.2 M NaCl, and 3) variation of the concentration of
14C taurine from 0.1 mM to 1 mM does not significantly
affect measured values of
cytowa of
cells plasmolyzed with 1 M NaCl. Use of taurine therefore introduced no
systematic errors in determinations of
cytowa.
We also tested whether the centrifugal harvest method used to prepare
suspensions caused physiological changes relative to growing cells.
Upon completion of a volume assay with suspensions of cells grown at
0.1 Osm, samples examined in a phase microscope exhibited motility,
indicating that these suspensions retained and were capable of
utilizing endogenous energy reserves. Cell viability (the number of
colony forming units determined by plating on LB agar) and
cytowa also remained constant over
the course of an assay, as determined by comparison of these values
before and after a series of volume measurements. Moreover, cell
suspensions had not entered stationary phase by completion of a typical
volume assay, because suspended cells resumed a normal growth rate
immediately, with no observable lag, upon dilution into fresh growth
medium, and the thermotolerance of centrifugally-harvested suspensions
grown at 0.1 Osm (determined by the reduction in viability with time
after heating at 48°C; see Hengge-Aronis et al., 1991
) was identical
to that of growing cells and not enhanced as it was in cells grown into
stationary phase at 0.1 Osm (data not shown).
Measurements of amounts of cellular and cytoplasmic water and of protein in growing cells
Volumes of water in growing cells were determined by measuring
the distribution of radiolabeled probes in pellets of cultures harvested by brief centrifugation through oil. Briefly, 2 µCi/mL of 14C inulin, 14C
sucrose, or 3H2O was added to midlog phase
cultures growing in MBM (0.1 Osm, an osmolality at which the density of
cells is ~1.08-1.09 g/mL; Baldwin et al., 1995
) immediately before
centrifuging 1.4 mL aliquots in microfuge tubes containing 200 µL of
1-bromododecane (BDD;
= 1.038 g/mL) at 12,000 × g for at least 90 s. (Centrifugation for less than
~90 s incompletely pelleted cells, whereas results were independent
of centrifugation times longer than 90 s). After removing 100 µL
of supernatant from each tube, the remaining supernatant and BDD was
carefully removed by aspiration, the pellets suspended in 100 µL of
water, and the cpm in the supernatant and pellet samples determined by
scintillation counting. (The cpm in the suspended pellets ranged from
~1,000 cpm for samples containing 14C inulin up to
~2,000 cpm for samples containing 3H2O, and
no cpm was detected in the discarded BDD). The amount of protein in
each sample was determined by comparing the A550 of the
culture at the time of assay to a standard curve of mg protein/mL of
culture versus A550 determined separately on multiple cultures grown in MBM, using the assay of Lowry et al. (1951)
with BSA
as standard as previously described (Cayley et al., 1991
). Values were
normalized to the dry weight of samples using measurements of the
protein/dry weight ratio determined separately. Volumes of cytoplasmic
and cellular water (in µL/mg dry weight) were then calculated as for
suspensions by subtracting the sucrose- or inulin-accessible volumes,
respectively, from the water-accessible volume. In experiments to
control for the effects of centrifugation of suspensions through BDD,
the procedure used for assaying volumes of suspensions was used except
that, after radiochemical addition, samples were centrifuged in tubes
containing 200 µL of BDD for 120 s.
Preliminary experiments showed that the error in the measurements of
volumes of growing cells assayed as above was much lower in cells
centrifuged through BDD than in cells centrifuged in the absence of
BDD. Preliminary experiments also showed that the firmness of pellets
and reproducibility of results obtained with cells spun through BDD
(
= 1.038 g/mL) was greater than for silicon oil (
= 1.050 g/mL). Evaporation of 3H2O was an
insignificant source of error because the membrane-permeable solute
14C urea (which readily equilibrates into cytoplasmic
water; Mitchell and Moyle, 1956
) gave results that were identical to
those obtained with 3H2O as long as sufficient
time (~90 s) was allowed for urea to diffuse into the cytoplasm of
cells before centrifugation of samples through BDD.
Calculations of periplasmic MDO concentration and of the contribution of MDO to turgor pressure
To calculate concentrations of periplasmic MDO at different
osmolalities of growth, molar amounts of MDO in E. coli K-12
from the data of Kennedy (1982)
and Lacroix et al. (1989)
were divided by the corresponding amounts of free water in the periplasm obtained from our volume measurements. Kennedy (1982)
and Lacroix et al. (1989)
measured the relative amounts of MDO (in cpm/mg DW, using 3H-glycerol to label MDO) as a function of growth
osmolality varied with NaCl. Values of the radioactivity of the
extracted MDO taken from Fig. 1 of Kennedy (1982)
were corrected for
non-MDO material by subtracting the reported osmotically-invariant
amount of non-MDO radioactivity in MDO extracts. Lacroix et al.
(1989)
reported relative amounts of MDO determined after purification
from non-MDO-labeled material. The relative amounts of MDO from Kennedy
(1982)
were normalized to nmol MDO/mg DW using the value of 136 nmol
MDO glucose/mg DW determined by Kennedy and coworkers in cells grown at
0.07 Osm and their assumption of 9 glucose/MDO (Rumley et al., 1992
). The relative amounts of MDO from LaCroix et al. (1989)
were converted to nmol MDO/mg DW using their value of 125 ± 20 nmol MDO
glucose/mg DW determined in cells grown at 0.07 Osm and by assuming 9 glucose/MDO. (The principal MDO species have 8-9 glucose monomers;
Kennedy, 1996
).
To calculate periplasmic concentrations of MDO (CMDO,
expressed as moles of MDO per L of free periplasmic water), the amount of periplasmic water
periwa (in
µL/mg cell DW) as a function of osmolality were obtained by
interpolation of the linear fit (cf., Fig. 3 B below) of
measurements of
periwa determined in
this study and in Cayley et al. (1991)
. Values of
periwa were converted to volumes of
free periplasmic water
(
peri,fwa) by subtracting an
osmolality-independent estimate of the volume of bound water of
hydration of periplasmic biopolymers
(
peri,bwa = 0.09 µL/mg cell
DW) obtained by assuming that periplasmic biopolymers are hydrated to
the same extent as cytoplasmic biopolymers (0.5 g H2O/g
biopolymer; Cayley et al., 1991
, 1992
) and that the protein/DW ratio of
the periplasm and cytoplasm are the same. Periplasmic protein was taken
as 20% of cell protein (Ames et al., 1984
; Cronan et al., 1987
).
The contribution of periplasmic MDO (concentration CMDO and
apparent valence ZMDOapp) to turgor pressure
across the cell wall as a function of salt concentration was calculated
from a Donnan equilibrium analysis, in which the osmotic pressure
difference across the cell wall is ascribed to anionic MDO in the
periplasm and to the unequal distribution of salt ions between the
periplasm and the external solution required for periplasmic
electroneutrality. For this calculation, the ionic composition of the
minimal growth medium with added NaCl was approximated as that of a
univalent salt with an anion concentration CX
equal to the sum of the anion concentrations in the growth medium
(primarily Cl
and the MOPS
anion). Then the
MDO contribution to turgor pressure (
MDO) is given by
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(1) |
1
deg
1 and T is Kelvin temperature. In Eq. 1,
nonideality effects are neglected. Subject to this approximation, Eq. 1
is valid over the entire range of concentration ratios
CMDO/CX, and gives the
correct limiting results 
MDO = RTCMDO for CX
CMDO and 
MDO = RT(|ZMDOapp| + 1)CMDO for CMDO
CX.
Other methods
The osmolalities of the growth media, wash buffer, and
low-osmolality plasmolysis solutions (
0.1 Osm) were measured using a
Wescor model 5520 vapor pressure osmometer. Osmolalities of other
plasmolysis buffers were calculated assuming additivity of osmotic
contributions from the wash buffer and added NaCl. The latter
contribution was calculated using osmotic coefficients of NaCl from
Robinson and Stokes (1959)
. This procedure was verified to be accurate
to within 1% for representative samples measured by osmometry. All
fittings were performed using the program NONLIN (Johnson and Frasier,
1985
; Straume et al., 1991
), a nonlinear functional-form, least-squares
fitting program. All errors reported for fittings were obtained from
NONLIN using a 67% confidence probability.
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RESULTS |
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Variation of the volume of cell water of E. coli in NaCl titrations of cells grown at very low (0.03) and moderately high (0.83) osmolality
Figure 1 plots the volume of cell
water (
cellwa) per unit DW of
E. coli grown at 0.03 Osm (in VLOM) and during the
subsequent course of plasmolysis titrations with NaCl. At the growth
osmolality of 0.03 Osm,
cellwa = 2.96 ± 0.10 µL/mg DW. Numerically, values of
cellwa correspond to amounts of cell
water in mg water/mg DW, assuming a density of 1 mg/µL. Figure 1
shows that addition of NaCl reduces
cellwa of these cells monotonically
to a high osmolality minimum value (designated
cell,minwa) of 1.9 ± 0.05 µL/mg DW, attained within error at plasmolyzing osmolalities in
excess of ~1 Osm. Figure 1 also plots the behavior of
cellwa in plasmolysis titrations of
cells grown at 0.83 Osm (in MBM+0.4 M NaCl), at which osmolality the
amount of periplasmic MDO is very low (Kennedy, 1982
; Lacroix et al.,
1989
). The initial value of
cellwa is
much smaller for cells grown at 0.83 Osm than at 0.03 Osm (cf., Fig. 1
and Table 1), in agreement with previous
observations (summarized in Table 1) that
cellwa decreases with increasing
osmolality of growth (Richey et al., 1987
; Larsen et al., 1987
; Cayley
et al., 1991
). Notably (cf., Fig. 1), after plasmolysis to any
osmolality greater than 0.83 Osm, the amount of water remaining in
cells grown at 0.83 Osm is always significantly less than the amount of
water in cells grown at 0.03 Osm. Figure 1 shows that, for cells grown
at 0.83 Osm and titrated with NaCl, increasing external osmolality
reduces the volume of cell water to a high osmolality minimum value
cell,minwa of 1.56 ± 0.05 µL/mg DW. This plateau value is significantly less than the
value of
cell,minwa obtained
from plasmolysis titrations of cells grown at 0.03 Osm (1.90 ± 0.05 µL/mg DW).
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To verify that the variation of
cell,minwa with osmolality of
growth is only the result of changes in the volume of water per cell,
and not in the amount of dry weight per cell, we examined whether the
dry weight per cell varies with osmolality of growth. Table 1 lists the
growth rate and mass of protein per viable cell for cultures grown from
0.1 to 1.0 Osm. Whereas the growth rate exhibits a maximum near 0.28 Osm, the amount of protein per viable cell shows no systematic
variation with osmolality and has an average value of 0.41 ± 0.03 pg per cell, which is within the range of published values for E. coli B/r (Bremer and Dennis, 1996
). Because the protein/DW ratio
of cells grown over this range of conditions is 0.68 ± 0.07, independent of osmolality (Cayley et al., 1991
), the dry weight per
cell is therefore also constant over the range of osmolalities and
growth rates examined.
Table 1 also lists volumes of water per viable cell, calculated from
determinations of the amount of protein per viable cell, the protein/DW
ratio, and the volume of cell water per mg DW. The calculated amount of
H2O per cell decreases from ~1.8 fL for cells grown at
0.03 Osm to ~1.1 fL for cells grown at 1.0 Osm (Table 1). For cells
grown at 0.1 Osm (in MBM), the volume of water per cell is ~1.5 fL.
Because the water-inaccessible volume of these cells is 0.63 ± 0.09 µL/mg DW (or ~0.4 fL per cell), independent of osmolality
(Cayley et al., 1991
), therefore, the total volume of the average cell
grown at 0.1 Osm is ~1.9 fL per cell. The corresponding dimensions of
a cell with this volume, assuming a cylindrical shape with
hemispherical ends and an overall 2:1 length:width ratio, is
approximately 2.2 µm × 1.1 µm, consistent with accepted
dimensions of E. coli (Neidhardt et al., 1990
).
Changes in water-accessible cytoplasmic and periplasmic volume during NaCl plasmolysis titrations of E. coli grown at very low osmolality (0.03 Osm)
Figure 2 plots the volumes of
cytoplasmic and periplasmic water of E. coli grown at 0.03 Osm and subsequently plasmolyzed with NaCl. The initial volumes of
water in these compartments are
cytowa = 2.53 ± 0.08 µL/mg DW
and
periwa
cellwa
cytowa = 0.43 ± 0.13 µL/mg
DW. As the concentration of NaCl is increased,
cytowa decreases monotonically to an
apparent plateau volume of ~0.4 µL/mg DW, approached at
plasmolyzing osmolalities in excess of 3 Osm. (For reference, the curve
for the reduction in
cellwa with
plasmolyzing osmolality from Fig. 1 is also shown in Fig. 2.)
Plasmolysis of cells grown at 0.03 Osm affects
cytowa much more than
cellwa, reducing
cytowa to less than 20% of its
initial value, whereas
cellwa is
reduced to 60% of its original value. Consequently
periwa (the difference between
cellwa and
cytowa) increases during these
plasmolysis titrations by more than 300%, to a plateau value of
approximately 1.45 ± 0.07 µL/mg DW. This increase in
periwa indicates that outer-membrane
impermeable periplasmic solutes (including MDO) are diluted to about
30% of their initial concentration upon plasmolysis with high
concentrations of NaCl. The observed variations in cell and compartment
volumes in NaCl plasmolysis titrations are larger but otherwise quite
analogous to those reported by Stock et al. (1977)
for sucrose
plasmolysis titrations of cells grown at 0.14 Osm.
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Volume measurements on fresh cell suspensions are applicable to growing cells
K+-deprived suspensions of cells were used in the
plasmolysis titrations to study the passive response of cells to
osmotic stress, because increased uptake of K+ from the
medium is the initial response required for adaptation of E. coli to hypertonic shock (Csonka and Epstein, 1996
). The suspensions also lacked glucose to prevent new synthesis of organic osmolytes, further ensuring that plasmolyzed cells are unable to
respond to increases in external osmolality by active osmoregulated mechanisms, and, instead, exhibit only the passive response of loss of
cell water. The absence of an active response in plasmolyzed cell
suspensions was verified by our observation (data not shown) that the
amount of cytoplasmic water in cells after plasmolysis with 1 M NaCl
remained unchanged for at least 15 min, the longest time tested.
To test directly whether the amounts of cell and cytoplasmic water in cell suspensions and in growing cells are the same, we used a radiochemical method to measure volumes of growing cells harvested by brief centrifugation through BDD oil as described in Methods. Table 2 shows that the water-accessible cell and cytoplasmic volumes of mid-log phase cells growing at 0.1 Osm are the same, within error, as in fresh suspensions, indicating that fresh suspensions have the same osmotic properties as growing cells (and see Discussion). Table 2 also shows that centrifugation of cells through BDD per se does not perturb the amount of intracellular water, because cell and compartment volumes of suspensions assayed by centrifugation through BDD are the same as suspensions assayed without BDD. A bathing atmosphere of medium must therefore accompany cells as they sediment through BDD, a conclusion verified by our observation that the extracellular (i.e., inulin-accessible) volume in pellets of samples spun through BDD contained ~1.8 µL extracellular water/mg total cell protein. Although significantly less than the ~2.5 µL extracellular water/mg protein of samples of pellets spun in the absence of BDD, the 1.8 µL/mg protein greatly exceeds that estimated for a monolayer coverage (~0.02 µL/mg protein) of a smooth surface with the dimensions of the E. coli cell.
|
The equivalence of the amounts of cell and cytoplasmic water in fresh
suspensions and growing cells validates our use of suspensions in this
study. Measurements on suspensions are preferable to measurements of
growing cells because they are of higher accuracy (see Table 2), in
large part because the cell density of log phase cultures is ~25-fold
lower than that of suspensions. Moreover, to measure only the passive
response of cells to osmotic stress, plasmolysis titrations must be
performed on nongrowing samples lacking extracellular K+,
because the initial active response to the increase in external osmolality of increased uptake of K+ from the medium
(Csonka and Epstein, 1996
) begins immediately after external osmolality
increases (Epstein and Schultz, 1965
).
Variation of periplasmic MDO concentration with osmolality of growth: implications for turgor pressure
Figure 3 A summarizes
amounts of MDO calculated by us as described in Methods from the data
of Kennedy (1982)
and Lacroix et al. (1989)
for E. coli K-12
strains grown at various osmolalities. Amounts of MDO decrease
monotonically from ~15 nmol MDO/mg DW at 0.07 Osm to very low levels
at high osmolality. Figure 3 B shows our determinations of
the volume of free periplasmic water
peri,fwa, obtained from the
difference between measured volumes of cell and cytoplasmic water as a
function of osmolality of growth as described in Methods. At least
above 0.3 Osm,
peri,fwa
increases slightly as osmolality of growth increases, in agreement with
previous measurements of
periwa
(Richey et al., 1987
; Larsen et al., 1987
). The experimental uncertainty is too large to allow us to conclude whether a different behavior occurs at lower osmolality, and, consequently, we have fit all
these data to a line for purposes of interpolation. Interpolated values
of
peri,fwa (Fig.
3 B) were used with determinations of
nMDO (Fig. 3 A) to estimate
concentrations of MDO (cMDO; see Methods) in the
free water of the periplasm as a function of the osmolality of growth.
Figure 3 C shows that cMDO decreases
from ~0.05 mol/L at a growth osmolality of 0.07 Osm to ~0.003 mol/L
at a growth osmolality of 0.8 Osm. Uncertainties in absolute MDO
concentrations are approximately ±35%; this uncertainty, although
large, has no effect on the semiquantitative conclusions obtained from
analyses of these results below. (The trend in relative amounts of MDO
is known to higher accuracy; Lacroix et al., 1989
). In particular, the
contribution of MDO (which Kennedy [1996] concluded are free and not
bound to other periplasmic components) to turgor pressure across the
cell wall may be estimated from these cMDO and
from the concentration of anions of the medium, as described in Methods
and analyzed below.
|
| |
ANALYSIS |
|---|
|
|
|---|
Analysis of
cytowa in
plasmolysis titrations of cells grown at low osmolalities (0.03 Osm to
0.28 Osm) demonstrates that turgor pressure decreases with increasing
osmolality of growth
For cells grown at 0.1 and 0.28 Osm, Cayley et al. (1991)
quantitatively analyzed the behavior of the volume occupied by
cytoplasmic water
cytowa in
plasmolysis titrations to obtain both the volume occupied by bound
water of hydration
cyto,bwa
and the amount of osmotically-significant solutes
cyto(
nj)cyto (see below) in the cytoplasm. Here, we extend this analysis to determine turgor pressure of these cells and of cells grown at 0.03 Osm. Turgor pressure is fundamentally related to the difference between
the osmolality of the cytoplasm (Osmcyto) and the external medium (Osmex) by
|
(2) |
nj)cyto
and to the volume occupied by free (unbound) cytoplasmic water
(
cyto,fwa) by
|
(3) |
cyto is the osmotic coefficient of the
cytoplasm (Cayley et al., 1991
|
(4) |
cyto,bwa is
defined as the volume occupied by bound cytoplasmic water (expected to
be primarily water of macromolecular hydration; Cayley et al., 1991
|
(5) |
cytowa versus
1/Osmex for data obtained in NaCl plasmolysis titrations of
cells grown at 0.1 Osm and 0.28 Osm (Cayley et al., 1991
cytowa at 0.1 Osm deviates from
the best fit line. Interpreted using Eq. 5, this linear behavior
indicates most simply that 
/RT is negligible relative
to Osmex in the range of plasmolyzing NaCl concentrations
investigated, and that both
cyto(
nj)cyto and
cyto,bwa are independent of
plasmolyzing NaCl concentration (Cayley et al., 1991
cytowa data from Fig. 2 versus
Osmex
1 for cells grown at 0.03 Osm is highly
nonlinear (Fig. 4), indicating most
simply that residual turgor pressure is significant relative to
RTOsmex at low NaCl concentrations. To simplify
determination of
cyto(
nj)cyto and
cyto,bwa, we therefore
linearly fit
cytowa versus
1/Osmex for cells plasmolyzed to an osmolarity exceeding 1 Osm to Eq. 5 assuming turgor pressure is zero. (Above 1 Osm,
cellwa ceases to vary significantly
with Osmex, from which we deduce that residual turgor
pressure is insignificant relative to RTOsmex). These data
are well fit by a line (r2 = 0.99) with
best-fit slope
cyto(
nj)cyto = 0.31 ± 0.04 µmol/mg DW and intercept
cyto,bwa = 0.45 ± 0.03 µL/mg DW, labeled A in Fig. 4. (Fitting these data assuming cells grown at 0.03 Osm exhibit a small residual turgor pressure (~0.4 atm) at high plasmolyzing osmolalities (see below) yields insignificantly different values of
cyto,bwa and
cyto(
nj)cyto.)
The value of
cyto,bwa for
cells grown at 0.03 Osm is within error of previous determinations of
cyto,bwa of cells grown at
higher osmolality (see Table 3). The
value of
cyto(
nj)cyto is
approximately equal to that for cells grown at 0.1 Osm (Cayley et al.,
1991
|
|
The linearity of the high-osmolality region of the plasmolysis plot in
Fig. 4 indicates that
cyto,bwa and
cyto(
nj)cyto for
cells grown at 0.03 Osm are independent of plasmolyzing osmolality.
Because we use nutrient-deprived suspensions to ensure that the sum of
the amount of cytoplasmic solutes
(
nj)cyto is constant throughout
these plasmolysis titrations (see above),
cyto is also
constant at high plasmolyzing osmolalities. We assume that
cyto does not vary at lower plasmolyzing osmolality, which is consistent with the K+-nucleic acid polyion model
used to interpret
cyto (Cayley et al., 1991
). Because
cyto,bwa is independent of
growth osmolality (see Table 3), we assume it is also independent of
low plasmolyzing osmolality. With these plausible assumptions, the
turgor pressure of these cells before or in the initial stages of
plasmolysis may be estimated from experimental values of
cytowa using
|
(6) |
cytowa of
unplasmolyzed cells (2.53 ± 0.08 µL/mg DW) and the values of
cyto(
nj)cyto and
cyto,bwa obtained above and
tabulated in Table 3, the calculated turgor pressure of cells grown at
0.03 Osm is 
= 3.1 ± 0.4 atm. This value significantly
exceeds the turgor pressures calculated from Eq. 6 from the published
values of
cyto(
nj)cyto and
cyto,bwa for cells grown at
0.1 Osm (MBM; 
= 1.5 ± 0.3 atm) and at 0.28 Osm
(MBM+0.1 M NaCl; 
= 0.7 ± 1.1 atm, i.e., 
1.8 atm; see Table 3 and Cayley et al., 1991A limitation of our plasmolysis titration method seen in these results
is that the propagated error becomes comparable to the turgor pressure
itself for growth osmolalities above 0.1 Osm, because the absolute
error in
cyto(
nj)cyto/
cyto,fwa
increases and the turgor pressure decreases with increasing osmolality. Hence, other approaches (developed below) are needed to establish whether turgor pressure varies with osmolality of growth above 0.1 Osm.
Contribution of MDO to periplasmic osmolality and turgor pressure as functions of the osmolality of growth and of plasmolysis
We evaluated periplasmic MDO concentration as functions of
osmolality of plasmolysis and growth from the amounts of MDO and volumes of unbound periplasmic water in Fig. 3. These values were then
used in Eq. 1 to quantify the effect of periplasmic MDO concentration CMDO, MDO apparent valence
ZMDOapp, and external salt (anion)
concentration CX on 
. These calculations, described below, make a strong case for our conclusions that 1) the
periplasm and cytoplasm are isoosmotic under all conditions, 2) the
turgor pressure exerted across the cell wall at any condition of
plasmolysis is primarily determined by CMDO, ZMDOapp, and CX, and
3) periplasmic MDO concentration and turgor pressure decrease together
with increasing osmolality of growth or of plasmolysis with NaCl.
Donnan analysis of effects of residual turgor from periplasmic MDO on the initial stages of a plasmolysis titration of cells grown at 0.03 Osm
In Fig. 4, the linear fit of the high osmolality data, where the effects of residual turgor are minimized as discussed above, is designated A. The large systematic deviations of the data of Fig. 4 from line A at low Osmex (i.e., high Osmex
1) are in the direction expected if cells
grown at 0.03 Osm have a large residual turgor pressure at low
plasmolyzing osmolality.
To assess whether the residual turgor pressure calculated from the
amount of periplasmic MDO can predict
cytowa over the entire range of
plasmolyzing osmolalities in Fig. 4 (and thus to test whether the
cytoplasm and periplasm are isoosmotic), we estimated the amount of MDO
in cells grown at 0.03 Osm by extrapolation of the empirical fit to the
data of Fig. 3 A to be ~18 ± 3 nmol MDO/mg DW. A
conservative lower-bound estimate of nMDO (15 nmol MDO/mg DW) was then used to estimate residual turgor from the
Donnan model (Eq. 1) for two choices of MDO apparent valence. Curve
B represents the case ZMDOapp = 0, corresponding to the situation in which MDO bear no net charge (for
example, as a result of Mg2+ binding). Although clearly
Curve B is an improvement over line A, it does
not fit the
cytowa plasmolysis data
below 0.2 Osm. Curve C was calculated assuming ZMDOapp =
3, corresponding to the
situation in which there is no cation binding to MDO and therefore MDO
have their full structural charge (the primary species of MDO have an
approximate structural charge of
3; Kennedy, 1996
cytowa data at 0.1 and 0.2 Osm, but
deviates at lower osmolality, predicting values of
cytowa that are significantly smaller
than those measured at 0.03 and 0.05 Osm. (The discrepancy increases if
higher values of nMDO or
ZMDOapp are assumed.) Despite this, Curve
C demonstrates unambiguously that the Donnan osmotic
pressure contribution of negatively charged MDO is more than sufficient
to account for the effects of turgor pressure on
cytowa. We then let
ZMDOapp vary with Osmex, and
calculated the values of ZMDOapp that yield
the observed values of
cytowa (Curve
D). We find that ZMDOapp in Eq. 1
must be smaller in magnitude at the low osmolality of growth than after
plasmolysis with high concentrations of NaCl. To fit the
cytowa data of Fig. 4 requires that
|ZMDOapp|
2 at the growth osmolality
of 0.03 Osm, but that |ZMDOapp| = 3 upon
plasmolysis of these cells with
0.05 M NaCl, an increase in
|ZMDOapp| which could result from
dissociation of bound Mg2+ (or other oligovalent cations)
from MDO with increasing NaCl concentration.
Taken together, the semiquantitative calculations in Fig. 4
show that a reasonable estimate of the amount and apparent valence of
periplasmic MDO is sufficient to satisfy the condition
Osmcyto = Osmperi. We therefore propose
that the Donnan osmotic pressure of charged MDO is the primary
determinant of turgor pressure for cells grown at 0.03 Osm and conclude
that the periplasm and cytoplasm are isoosmotic, in agreement with the
findings of Stock et al. (1977)Role of MDO as a determinant of the extent of cell wall stretch and cell volume in plasmolysis titrations
For cells grown at 0.03 Osm, the turgor pressure calculated from cMDO by Eq. 1 over the course of a plasmolysis titration does not reach zero, even at high osmolalities of plasmolysis. Plasmolyzed cells retain residual turgor pressure because the large amount of MDO in the periplasm of cells grown at 0.03 Osm is diluted no more than fourfold by plasmolysis. (The volume occupied by periplasmic water increases from 0.43 µL/mg DW to a maximum of ~1.45 µL/mg DW; see Fig. 2.) The inset to Fig. 4 plots the turgor pressure
predicted from CMDO and ZMDOapp as a function of plasmolyzing
osmolality, on the basis of the variation of
ZMDOapp with NaCl concentration, which
yields Curve D of Fig. 4. From the maximum value of
periwa obtained at high plasmolyzing
osmolality and the lower bound value of nMDO
estimated for cells grown at 0.03 Osm (~15 nmol/mg DW), we calculate
that cells grown at 0.03 Osm retain at least 0.3 atm of residual turgor
pressure at the highest plasmolyzing osmolality (6 Osm) employed. (This calculation is independent of the choice of
ZMDOapp because the Donnan
contribution of salt ions to turgor pressure is negligible in cells
suspended in plasmolyzing media of high [NaCl].)
If the large amount of MDO in cells grown at 0.03 Osm at high
plasmolyzing osmolality results in retention of significant residual
turgor at high plasmolyzing osmolalities, then cells grown at high
osmolality (a growth condition where cells contain very low amounts of
MDO; see Fig. 3 A) should exhibit negligible residual
turgor and completely unstretched cell walls after extensive plasmolysis with NaCl, and thus have a lower minimum cell volume (
cell,minwa) than cells grown
at 0.03 Osm. This prediction was confirmed by our observation that
cell,minwa of cells grown at
0.83 Osm is significantly lower than that of cells grown at 0.03 Osm
(see Fig. 1), consistent with our conclusion that the amount of MDO is
a primary determinant of periplasmic osmolality and therefore of turgor
pressure and cell wall stretch in E. coli K-12.
Contribution of MDO to turgor pressure as a function of growth osmolality
Figure 5 plots predicted turgor pressures of growing E. coli as a function of osmolality of growth. Figure 5 predicts a monotonic decrease in
from ~3
atm for cells grown at 0.03 Osm to less than 0.5 atm for cells grown at
0.8 Osm. Included in this figure are values of 
at low growth
osmolality (0.03-0.28 Osm) determined from measurements of
cytowa in plasmolysis titrations
(cf., Table 3) and values of 
predicted from contributions of
outer membrane-impermeable periplasmic solutes, including: the Donnan
contribution of the concentration of periplasmic MDO (calculated
assuming that the MDO apparent valence
ZMDOapp (Eq. 1) changes the same way with
[NaCl] for growth and for plasmolysis of cells grown at 0.03 Osm);
and an estimate of the contribution of periplasmic proteins (and any
other outer membrane-impermeable periplasmic solutes) to turgor
pressure, obtained from the analysis of the cell volume data (see
below). The latter effect is approximately 0.3 atm, and is therefore
predicted to become the dominant contribution to 
in cells
growing above 0.8 Osm.
|
Relationship between cell volume and turgor pressure
As an independent method of quantifying turgor pressure to compare
with our estimates based on analysis of periplasmic MDO concentration,
we applied an empirical relationship between changes in cell volume and
changes in turgor pressure previously used to characterize
turgor-volume relationships in plant (Zimmermann, 1978
; Cosgrove,
1988
) and microbial (Walsby, 1980
; Reed and Walsby, 1985
) cells.
Changes in turgor pressure (
) and the corresponding changes in
total cell volume (
celltotal) have
been related by the empirical equation (Broyer, 1952
; Phillip, 1958
;
Zimmermann, 1978
)
|
(7) |
is the volumetric elastic modulus (Cosgrove, 1988
celltotal =
celltotal
cell,0total, and
cell,0total is the total cell
volume in the zero-turgor reference state. Total cell volumes are
defined as the sum of the water-accessible cell volume
(
cellwa) and the water-inaccessible
cell volume (
cellwi)
|
(8) |
cellwi = 0.63 ± 0.09 µL/mg
DW, independent of external osmolality (Cayley et al., 1991
is apparently independent of both
celltotal and of turgor pressure over
a range of volumes and pressures for some plant cells (Cosgrove, 1988