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Biophys J, April 2000, p. 1748-1764, Vol. 78, No. 4

Biophysical Characterization of Changes in Amounts and Activity of Escherichia coli Cell and Compartment Water and Turgor Pressure in Response to Osmotic Stress

D. Scott Cayley,* Harry J. Guttman,* and M. Thomas Record Jr.*#

Departments of  *Chemistry and  #Biochemistry, University of Wisconsin-Madison, Madison, Wisconsin 53706, USA

    ABSTRACT
TOP
ABSTRACT
INTRODUCTION
MATERIALS AND METHODS
RESULTS
ANALYSIS
DISCUSSION
REFERENCES

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.

    INTRODUCTION
TOP
ABSTRACT
INTRODUCTION
MATERIALS AND METHODS
RESULTS
ANALYSIS
DISCUSSION
REFERENCES

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 gsim  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 Delta Osm and turgor pressure Delta Pi  = RTDelta Osm across the cell wall are maintained, and/or ii) by allowing Delta 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.

    MATERIALS AND METHODS
TOP
ABSTRACT
INTRODUCTION
MATERIALS AND METHODS
RESULTS
ANALYSIS
DISCUSSION
REFERENCES

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 (<A><AC>V</AC><AC>&cjs1171;</AC></A>cellwa) and cytoplasmic water (<A><AC>V</AC><AC>&cjs1171;</AC></A>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 <A><AC>V</AC><AC>&cjs1171;</AC></A>cellwa and <A><AC>V</AC><AC>&cjs1171;</AC></A>cytowa (in µL/mg DW) as described previously (Cayley et al., 1991). Measurements of <A><AC>V</AC><AC>&cjs1171;</AC></A>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, <A><AC>V</AC><AC>&cjs1171;</AC></A>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 <A><AC>V</AC><AC>&cjs1171;</AC></A>cytowa, showing that any deprivation of oxygen or nutrients that occurred during preparation of suspensions did not lower <A><AC>V</AC><AC>&cjs1171;</AC></A>cytowa. All steps after cell growth were performed at room temperature.

In NaCl plasmolysis titrations to determine the passive responses of <A><AC>V</AC><AC>&cjs1171;</AC></A>cellwa and <A><AC>V</AC><AC>&cjs1171;</AC></A>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 <A><AC>V</AC><AC>&cjs1171;</AC></A>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) <A><AC>V</AC><AC>&cjs1171;</AC></A>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 <A><AC>V</AC><AC>&cjs1171;</AC></A>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 <A><AC>V</AC><AC>&cjs1171;</AC></A>cytowa of cells plasmolyzed with 1 M NaCl. Use of taurine therefore introduced no systematic errors in determinations of <A><AC>V</AC><AC>&cjs1171;</AC></A>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 <A><AC>V</AC><AC>&cjs1171;</AC></A>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; rho  = 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 (rho  = 1.038 g/mL) was greater than for silicon oil (rho  = 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 <A><AC>V</AC><AC>&cjs1171;</AC></A>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 <A><AC>V</AC><AC>&cjs1171;</AC></A>periwa determined in this study and in Cayley et al. (1991). Values of <A><AC>V</AC><AC>&cjs1171;</AC></A>periwa were converted to volumes of free periplasmic water (<A><AC>V</AC><AC>&cjs1171;</AC></A>peri,fwa) by subtracting an osmolality-independent estimate of the volume of bound water of hydration of periplasmic biopolymers (<A><AC>V</AC><AC>&cjs1171;</AC></A>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 (Delta Pi MDO) is given by
&Dgr;&Pgr;<SUB><UP>MDO</UP></SUB>≅RT[C<SUB><UP>MDO</UP></SUB>+(Z<SUP><UP>app</UP></SUP><SUB><UP>MDO</UP></SUB><SUP>2</SUP>C<SUP>2</SUP><SUB><UP>MDO</UP></SUB>+4C<SUP>2</SUP><SUB><UP>X</UP></SUB>)<SUP>0.5</SUP>−2C<SUB><UP>X</UP></SUB>], (1)
where R = 0.0821 liter atm mol-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 Delta Pi MDO = RTCMDO for CX CMDO and Delta Pi 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.

    RESULTS
TOP
ABSTRACT
INTRODUCTION
MATERIALS AND METHODS
RESULTS
ANALYSIS
DISCUSSION
REFERENCES

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 (Vcellwa) 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, Vcellwa = 2.96 ± 0.10 µL/mg DW. Numerically, values of Vcellwa 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 Vcellwa of these cells monotonically to a high osmolality minimum value (designated Vcell,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 Vcellwa 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 Vcellwa 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 Vcellwa 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 Vcell,minwa of 1.56 ± 0.05 µL/mg DW. This plateau value is significantly less than the value of Vcell,minwa obtained from plasmolysis titrations of cells grown at 0.03 Osm (1.90 ± 0.05 µL/mg DW).



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FIGURE 1   Reduction in water-accessible cellular volume Vcellwa of suspensions of cells grown at 0.03 Osm (in VLOM; open circle ) and at 0.83 Osm (in MBM+0.4 M NaCl; ) with increasing plasmolyzing osmolality adjusted with NaCl. Each point shows the average (±1 SD) of 2-7 independent determinations, each performed in triplicate on separate cultures. The curves are empirical hyperbolic best fits to the data, and were used to estimate Vcell,minwa.


                              
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TABLE 1   Dependence on growth osmolality of volume accessible to water, growth rate, and amounts of protein and water per E. coli cell

To verify that the variation of Vcell,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 Vcytowa = 2.53 ± 0.08 µL/mg DW and Vperiwa triple-bond  Vcellwa - Vcytowa = 0.43 ± 0.13 µL/mg DW. As the concentration of NaCl is increased, Vcytowa 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 Vcellwa with plasmolyzing osmolality from Fig. 1 is also shown in Fig. 2.) Plasmolysis of cells grown at 0.03 Osm affects Vcytowa much more than Vcellwa, reducing Vcytowa to less than 20% of its initial value, whereas Vcellwa is reduced to 60% of its original value. Consequently Vperiwa (the difference between Vcellwa and Vcytowa) 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 Vperiwa 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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FIGURE 2   Reduction in water-accessible cytoplasmic volume (open circle ) and increase of water-accessible periplasmic volume (triangle ) of cells grown at 0.03 Osm (in VLOM) with increasing plasmolyzing osmolality adjusted with NaCl. Each point shows the average (±1 SD) of 6-12 measurements performed on 2-4 cultures. The curve through the Vcytowa data is an empirical best-fit hyperbolic function. The corresponding fit to the Vcellwa data for cells grown at 0.03 Osm from Fig. 1 is shown for comparison. Periplasmic data points were obtained by subtraction of cytoplasmic volumes from cell volumes. The periplasmic volume curve was determined by subtraction of the fitted curves for cell and cytoplasmic volumes.

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.


                              
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TABLE 2   Water-accessible volumes (µL H2O/mg DW) of the cell and compartments of growing cells and of centrifugally harvested suspensions

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 Vperi,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, Vperi,fwa increases slightly as osmolality of growth increases, in agreement with previous measurements of Vperiwa (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 Vperi,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.



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FIGURE 3   Reduction of the amount and concentration of periplasmic MDO with increasing osmolality of growth. Panel A plots the amounts of MDO (nMDO) in nmol/mg cell DW calculated as described in Methods from the analytical data of Kennedy (1982; open circle ) and Lacroix et al. (1989; triangle ) versus growth osmolality. The curve is the empirical best hyperbolic fit to all the data. Panel B plots the volumes of free periplasmic water Vperi,fwa (determined as described in Methods) in µL/mg cell DW versus osmolality of growth. The line is the best linear fit to the data and is shown for purposes of interpolation. Panel C shows the decrease in concentration of periplasmic MDO (cMDO) (in mol/L free periplasmic water) calculated from values of nMDO (A) and interpolated values of Vperi,fwa (B) with increasing osmolality of growth.

    ANALYSIS
TOP
ABSTRACT
INTRODUCTION
MATERIALS AND METHODS
RESULTS
ANALYSIS
DISCUSSION
REFERENCES

Analysis of Vcytowa 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 Vcytowa in plasmolysis titrations to obtain both the volume occupied by bound water of hydration Vcyto,bwa and the amount of osmotically-significant solutes phi cyto(Sigma  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
&Dgr;&Pgr;=RT(<UP>Osm</UP><SUB><UP>cyto</UP></SUB>−<UP>Osm</UP><SUB><UP>ex</UP></SUB>). (2)
The osmolality of the cytoplasm is related to the molar amount of cytoplasmic solutes (Sigma  nj)cyto and to the volume occupied by free (unbound) cytoplasmic water (Vcyto,fwa) by
<UP>Osm</UP><SUB><UP>cyto</UP></SUB>=&phgr;<SUB><UP>cyto</UP></SUB><FENCE><LIM><OP>∑</OP></LIM> n<SUB><UP>j</UP></SUB></FENCE><SUB><UP>cyto</UP></SUB><FENCE><A><AC>V</AC><AC>&cjs1171;</AC></A><SUP><UP>wa</UP></SUP><SUB><UP>cyto,f</UP></SUB></FENCE>, (3)
where phi cyto is the osmotic coefficient of the cytoplasm (Cayley et al., 1991). In Eq. 3,
<A><AC>V</AC><AC>&cjs1171;</AC></A><SUP><UP>wa</UP></SUP><SUB><UP>cyto,f</UP></SUB>≡<A><AC>V</AC><AC>&cjs1171;</AC></A><SUP><UP>wa</UP></SUP><SUB><UP>cyto</UP></SUB>−<A><AC>V</AC><AC>&cjs1171;</AC></A><SUP><UP>wa</UP></SUP><SUB><UP>cyto,b</UP></SUB>, (4)
where Vcyto,bwa is defined as the volume occupied by bound cytoplasmic water (expected to be primarily water of macromolecular hydration; Cayley et al., 1991; Record et al., 1998a). Combining Eqs. 2-4 gives
 <A><AC>V</AC><AC>&cjs1171;</AC></A><SUP><UP>wa</UP></SUP><SUB><UP>cyto</UP></SUB>=<A><AC>V</AC><AC>&cjs1171;</AC></A><SUP><UP>wa</UP></SUP><SUB><UP>cyto,b</UP></SUB>+&phgr;<SUB><UP>cyto</UP></SUB><FENCE><LIM><OP>∑</OP></LIM> n<SUB><UP>j</UP></SUB></FENCE><SUB><UP>cyto</UP></SUB><FENCE>(&Dgr;&Pgr;/RT+<UP>Osm</UP><SUB><UP>ex</UP></SUB>)</FENCE>. (5)
Plots of Vcytowa 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) and at 1.02 Osm (Cayley et al., 1992) are linear for all plasmolyzing NaCl concentrations investigated, although the initial (unplasmolyzed) value of Vcytowa at 0.1 Osm deviates from the best fit line. Interpreted using Eq. 5, this linear behavior indicates most simply that Delta Pi /RT is negligible relative to Osmex in the range of plasmolyzing NaCl concentrations investigated, and that both phi cyto(Sigma  nj)cyto and Vcyto,bwa are independent of plasmolyzing NaCl concentration (Cayley et al., 1991). A similar plot of the Vcytowa 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 phi cyto(Sigma  nj)cyto and Vcyto,bwa, we therefore linearly fit Vcytowa versus 1/Osmex for cells plasmolyzed to an osmolarity exceeding 1 Osm to Eq. 5 assuming turgor pressure is zero. (Above 1 Osm, Vcellwa 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 phi cyto(Sigma  nj)cyto = 0.31 ± 0.04 µmol/mg DW and intercept Vcyto,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 Vcyto,bwa and phi cyto(Sigma  nj)cyto.) The value of Vcyto,bwa for cells grown at 0.03 Osm is within error of previous determinations of Vcyto,bwa of cells grown at higher osmolality (see Table 3). The value of phi cyto(Sigma  nj)cyto is approximately equal to that for cells grown at 0.1 Osm (Cayley et al., 1991), consistent with our previous conclusion (Capp et al., 1996; see also Record et al., 1998a) that the primary difference in the pool of cytoplasmic osmolytes in these cells is that cells grown at 0.03 Osm have ~0.04 ± 0.02 µmol/mg DW more putrescine(2+) and, thus, ~0.08 ± 0.04 µmol/mg DW less K+ than cells grown at 0.1 Osm.



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FIGURE 4   Effects of periplasmic MDO on Vcytowa in a NaCl plasmolysis titration of cells grown at 0.03 Osm (VLOM). Contributions to turgor pressure Delta Pi from the Donnan osmotic pressure of periplasmic MDO as a function of Osmex were calculated with Eq. 1 using a lower bound estimate of nMDO = 15 nmol/mg DW (estimated by extrapolation of Fig. 3 A as described in the text), interpolated values of Vperi,fwa from Fig. 3 B, and several choices of MDO valence ZMDOapp. These contributions to Delta Pi were used in Eq. 6 to predict the behavior of Vcytowa versus 1/Osmex, where Osmex was varied with NaCl in a plasmolysis titration (cf. Methods). Curve A shows the linear fit to the data of cells plasmolyzed to ~1 Osm and above (see text). Curve B shows the fit assuming ZMDOapp = 0 to calculate Delta Pi ; curve C shows the fit assuming ZMDOapp = -3 to calculate Delta Pi ; curve D is the best fit of Eq. 6 to the data and corresponds to the situation in which |ZMDOapp| is initially 2 in unplasmolyzed cells and increases to 3 as the concentration of NaCl increases (see text). Inset: Reduction in turgor pressure of cells grown at 0.03 Osm (VLOM) with increasing osmolality of plasmolysis. Turgor pressure was predicted from the concentration of periplasmic MDO by Eq. 1 with a value of ZMDOapp that varied with [NaCl] as in curve D.


                              
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TABLE 3   Amounts of cytoplasmic water and osmotic properties of E. coli grown at different osmolalities*

The linearity of the high-osmolality region of the plasmolysis plot in Fig. 4 indicates that Vcyto,bwa and phi cyto(Sigma  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 (Sigma nj)cyto is constant throughout these plasmolysis titrations (see above), phi cyto is also constant at high plasmolyzing osmolalities. We assume that phi cyto does not vary at lower plasmolyzing osmolality, which is consistent with the K+-nucleic acid polyion model used to interpret phi cyto (Cayley et al., 1991). Because Vcyto,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 Vcytowa using
&Dgr;&Pgr;=RT<FENCE>&phgr;<SUB><UP>cyto</UP></SUB><FENCE><LIM><OP>∑</OP></LIM> n<SUB><UP>j</UP></SUB></FENCE><SUB><UP>cyto</UP></SUB><FENCE><A><AC>V</AC><AC>&cjs1171;</AC></A><SUP><UP>wa</UP></SUP><SUB><UP>cyto,f</UP></SUB>−<UP>Osm</UP><SUB><UP>ex</UP></SUB></FENCE></FENCE>. (6)
From the value of Vcytowa of unplasmolyzed cells (2.53 ± 0.08 µL/mg DW) and the values of phi cyto(Sigma  nj)cyto and Vcyto,bwa obtained above and tabulated in Table 3, the calculated turgor pressure of cells grown at 0.03 Osm is Delta Pi  = 3.1 ± 0.4 atm. This value significantly exceeds the turgor pressures calculated from Eq. 6 from the published values of phi cyto(Sigma  nj)cyto and Vcyto,bwa for cells grown at 0.1 Osm (MBM; Delta Pi  = 1.5 ± 0.3 atm) and at 0.28 Osm (MBM+0.1 M NaCl; Delta Pi  = 0.7 ± 1.1 atm, i.e., Delta Pi  ~<  1.8 atm; see Table 3 and Cayley et al., 1991).

A 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 phi cyto(Sigma  nj)cyto/Vcyto,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 Delta Pi . 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 Vcytowa 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 Vcytowa 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). Curve C provides a better fit than curve B to the Vcytowa data at 0.1 and 0.2 Osm, but deviates at lower osmolality, predicting values of Vcytowa 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 Vcytowa. We then let ZMDOapp vary with Osmex, and calculated the values of ZMDOapp that yield the observed values of Vcytowa (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 Vcytowa data of Fig. 4 requires that |ZMDOapp| congruent  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) and Sen et al. (1988) (see Discussion).

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 Delta Pi 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 Vperiwa 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 (Vcell,minwa) than cells grown at 0.03 Osm. This prediction was confirmed by our observation that Vcell,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 Delta Pi 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 Delta Pi at low growth osmolality (0.03-0.28 Osm) determined from measurements of Vcytowa in plasmolysis titrations (cf., Table 3) and values of Delta Pi 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 Delta Pi in cells growing above 0.8 Osm.



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FIGURE 5   Reduction in turgor pressure (Delta Pi ) with increasing osmolality of growth. (triangle ) Turgor pressure calculated with Eq. 6 from the cytoplasmic water-accessible volume Vcytowa determined for cells grown at 0.03, 0.10, and 0.28 Osm, using the values of phi cyto(Sigma  nj)cyto and Vb,cytowa in Table 3. Uncertainties in these values are ±(0.3-1) atm (Table 3). (black-triangle) Turgor pressures calculated with Eq. 1 from the values of cMDO from Fig. 3 C and from the variation of ZMDOapp with [NaCl] inferred from the best-fit curve D of Fig. 4; uncertainties in these values are approximately ±35%. (+) Turgor pressures determined by measuring collapse pressures of gas vacuoles in Microcystis sp. grown at 15 mOsm and 45 mOsm (Reed and Walsby, 1985). (×) Turgor pressure determined by measuring collapse pressures of gas vacuoles in Ancylobacter aquaticus grown at 0.1 Osm (Koch and Pinette, 1987), which has an error of ~15%. The osmolalities of the media used by Reed and Walsby (1985) and Koch and Pinette (1987) were estimated from their composition.

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 (Delta Pi ) and the corresponding changes in total cell volume (Delta Vcelltotal) have been related by the empirical equation (Broyer, 1952; Phillip, 1958; Zimmermann, 1978)
&Dgr;&Pgr;=ϵ&Dgr;<A><AC>V</AC><AC>&cjs1171;</AC></A><SUP><UP>total</UP></SUP><SUB><UP>cell</UP></SUB>/<A><AC>V</AC><AC>&cjs1171;</AC></A><SUP><UP>total</UP></SUP><SUB><UP>cell,0</UP></SUB>, (7)
where varepsilon  is the volumetric elastic modulus (Cosgrove, 1988), Delta Vcelltotal = Vcelltotal - Vcell,0total, and Vcell,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 (Vcellwa) and the water-inaccessible cell volume (Vcellwi)
<A><AC>V</AC><AC>&cjs1171;</AC></A><SUP><UP>total</UP></SUP><SUB><UP>cell</UP></SUB>=<A><AC>V</AC><AC>&cjs1171;</AC></A><SUP><UP>wa</UP></SUP><SUB><UP>cell</UP></SUB>+<A><AC>V</AC><AC>&cjs1171;</AC></A><SUP><UP>wi</UP></SUP><SUB><UP>cell</UP></SUB>. (8)
For the conditions of the present study, Vcellwi = 0.63 ± 0.09 µL/mg DW, independent of external osmolality (Cayley et al., 1991). The empirical elastic modulus varepsilon  is apparently independent of both Vcelltotal and of turgor pressure over a range of volumes and pressures for some plant cells (Cosgrove, 1988) and for the gram n