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Journal of Bacteriology, January 2006, p. 820-822, Vol. 188, No. 2
0021-9193/06/$08.00+0 doi:10.1128/JB.188.2.820-822.2006
Copyright © 2006, American Society for Microbiology. All Rights Reserved.
Department of Chemistry and Biochemistry, University of Oklahoma, Norman, Oklahoma 73019
Received 22 July 2005/ Accepted 20 October 2005
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Relationship between growth rate and cell permeability of the wild type.
Starter cultures of E. coli MG1655 (CGSC 7740) for our study were grown to full yield at 37°C in Luria-Bertani (LB) medium, and after 15 h they were diluted 1:100 into the same medium to initiate the experiments. At 1-h intervals, 30 ml of the culture was centrifuged for 5 min at 10,000 x g at 5°C, the cell pellet was washed twice with 10 ml 100 mM (pH 7.4) phosphate-buffered solution (PBS), and the final cell pellet was resuspended in 30 ml PBS. The entire manipulation was complete, and permeability measurements were made within 10 min of sampling the culture. We employed a HI-TECH SF61 DX2 and stopped-flow methods to determine the permeabilities (1, 7). E. coli cells were subjected to an outwardly oriented osmotic gradient (see below), and the change in light scattering at
em = 600 nm was recorded as a function of time. Two features were observed in the transient spectra that followed mixing: a rapid exponential increase in scattering and a subsequent slower exponential decrease in scattering (data not shown). These events are attributed to egress of water from the cytoplasm and a subsequent slower movement of the osmolyte into the cytoplasm, as indicated by the direction of the change in scattering, the similarities of the observed rate of the first event to previous measurements of the egress of water from E. coli (1), and the insensitivity of the rate of the first event (and a sensitivity of the second event) to the chemical nature of the osmolyte (see below). The magnitude of change in scattering was proportional to the concentration of the cells, which was adjusted to permit the transmission of 60 to 80% of the light. Proline was selected as the osmolyte for our initial studies because it is considered to be a "compatible solute" (it can be accumulated to very high levels without disturbing cellular physiology), and as such it is frequently used to balance environmental osmolality (4). The measurements that are summarized in Fig. 1 and Table 1 are for the 1:1 mixing of cells suspended in PBS and 1 M L-proline in PBS (to give a final concentration of 500 mM L-proline in 100 mM PBS). To further improve the signal-to-noise ratio by reducing the basal water permeability, our initial measurements were carried out at 5°C. The emission/time traces that were used to determine the rate constants were the average of five mixing cycles. The standard deviations that are reported in Table 1 were obtained through statistical comparison of five independent averaged spectra. The change in scattering due to egress of water and influx of osmolyte were fitted to single exponential functions to give the pseudo-first-order rate constants kw and kp, respectively. The osmotic permeabilities (Pf) were computed using the following equation: Pf = [V0/(S x VW x
osM)] x d[V/V0]/dt, where the molar volume of water (VW) is 18 cm3/mol, the change in osmolality (
osM) is 5 x 104 mol/cm3, and d[V/Vo]/dt is kw/p. The initial volume (Vo) and surface area (S) of the cells were computed assuming a length of 5 µm and a diameter of 1 µm, which are average values for K-12 strains of E. coli grown in LB during exponential phase and at the beginning of stationary phase (10). Figure 1A illustrates the relationship between Pf for water at 5°C and the growth of E. coli MG1655 (wild type) in LB with aeration at 37°C. One observes an initial decrease in permeability of the cells during the transition from the lag phase to exponential growth, relatively little change in permeability during exponential growth itself, and then a rapid increase in permeability that coincides with the onset of the stationary phase. The initial decrease in permeability that is observed in Fig. 1A was eliminated in an experiment that was identical in every respect, except the experiment was initiated by subculturing a starter culture that was in the mid-exponential growth phase rather than one that was in late stationary phase. The observed relationships between the rate of growth and permeability in Fig. 1A, most notably the initial decrease in permeability and the lag that occurs between the observed increase in permeability and the onset of exponential growth, is consistent with the observation that transcription of an aqpZ-lac fusion on the chromosome of E. coli increases as the cells enter the stationary stage of growth (9).
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FIG. 1. Growth (open circles) of (A) MG1655 (wild type) and (B) NCM3306 ( aqpZ::Cam+) in LB with aeration at 37°C (optical density at 600 nm [OD600]) and osmotic permeability (open squares) for the efflux of water from cells suspended in PBS (100 mM NaxPO4, pH 7.4) upon 1:1 mixing with 1 M L-proline (in the same PBS) at 5°C as a function of time. The cultures were started by 1:100 dilution of a 15-h culture with fresh LB medium.
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View this table: [in a new window] |
TABLE 1. Rate constants for the egress of water (kw) and the influx of L-proline (kp) for MG1655 (wild type) and NCM3306 ( aqpZ::Cam+) for osM = 500 mosM at 5°C as a function of growtha
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aqpZ::Cam+) (9), a derivative of MG1655 in which the aqpZ gene is disrupted. The experiment was carried out using the same protocol as that for the wild type. In contrast to the marked effect the stage of growth has on the rate of water efflux for the wild-type (Fig. 1A), Pf remains essentially constant throughout the stages of growth for the aqpZ knockout (Fig. 1B). Effect of temperature on cell permeability. To confirm that permeability was constant during exponential growth and to ensure that the observed trends in permeability were not artifacts of the low temperature that was employed in our initial experiments (e.g., vis-à-vis phase transition of the lipids), in a subsequent experiment we collected more samples during exponential growth (at 15-min intervals instead of 1-h intervals) and the permeability measurements were carried out at 37°C. The more closely spaced sampling required a modification of our sampling protocols such that cell pellets were stored at 5°C until the permeability measurements could be made, typically within 45 min of sampling. The overall relationship between growth rates and permeability was similar at 37°C, although the basal and maximal permeabilities were somewhat higher, presumably due to greater passive diffusion of water. Figure 2 clearly demonstrates that basal permeability is maintained during the exponential growth of MG1655. A similar basal permeability was observed for NCM3306 at 37°C (data not shown).
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FIG. 2. Growth (open circles) of MG1655 (wild type) in LB with aeration at 37°C (optical density at 600 nm [OD600]) during the exponential phase of growth and osmotic permeability (open squares) for the efflux of water from cells suspended in PBS (100 mM NaxPO4, pH 7.4) upon 1:1 mixing with 1 M L-proline (in the same PBS) at 37°C as a function of time. The line was generated by least-squares fit of the growth data (which yields a generation time [g] of 30 min).
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View this table: [in a new window] |
TABLE 2. Basal and maximal osmotic permeabilities of MG1655 (wild type) and NCM3306 ( aqpZ::Cam+) for osM = 500 mosM at 37°C
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We thank Helen I. Zgurskaya and David P. Nagle, Jr., for stimulating discussion and Sydney Kustu for supplying NCM3306. We are also appreciative of the reviewers' comments.
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