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Applied and Environmental Microbiology, March 2004, p. 1627-1632, Vol. 70, No. 3
0099-2240/04/$08.00+0 DOI: 10.1128/AEM.70.3.1627-1632.2004
Copyright © 2004, American Society for Microbiology. All Rights Reserved.
Department of Earth Science, Rice University, Houston, Texas 77005,1 Jet Propulsion Laboratory, California Institute of Technology, Pasadena, California 911092
Received 12 May 2003/ Accepted 17 November 2003
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However, there exists a large pool of abiotic mineral dissolution data, which has facilitated our understanding of dissolution kinetics exclusive of the quantifiable effects of organisms (11, 14, 24, 30). Historically, these studies have focused on the dissolution of carbonate minerals such as calcite or dolomite (26). Dissolution rates have typically been measured indirectly, by using mineral powders or single crystal weight loss techniques (reference 32 and citations therein). Direct studies have been performed using atomic force microscopy to gain much more detailed insight into step movement on crystal surfaces (8, 12, 13). Recently, crystal dissolution rates have been measured directly by vertical scanning interferometry (VSI) (1, 23, 24). These studies, in combination with a dissolution stepwave model (see below) (14, 15), help to explain the importance of "large-scale" direct observations at the crystal surface. Here, we extend this work, incorporating the critical effect of microorganisms on the dissolution of calcite.
Studies of surface interactions between microbes and carbonate minerals have traditionally focused on carbonate precipitation rather than dissolution (4, 28, 29). From such studies, it is generally agreed that carbonate precipitation is the result of chemical alteration of the aqueous environment (19). On the other hand, interactions between microbes and carbonates during mineral dissolution are less well documented. Organisms that can bore into carbonate rocks (7) are known; they are thought to do so via the excretion of organic acid. In general, organisms that excrete either CO2 or organic acids could impact the dissolution kinetics of carbonates via local changes in pH, acting via the following reaction:
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It was this type of mineral dissolution that we reasoned might be occurring if organisms were to attach to the surface of carbonate mineralsthe copious excretion of CO2, leading to carbonate breakdown. We elected to test our hypothesis with the environmental microbe Shewanella oneidensis MR-1, an organism known to attach to many substrates of no metabolic significance, e.g., glass and plastic. MR-1 attachment to carbonate, to our knowledge, had not been studied previously, and such carbonate dissolution via local pH alteration, should it occur, would be in marked contrast to the better-known mineral dissolution abilities of MR-1, which involve redox changes during the reduction of iron or manganese oxides (18, 20, 27).
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The goal of our studies was distinctly different. Dissolution of carbonate minerals should occur via a nonredox mechanism, with no apparent (energetic) advantage to the organism catalyzing the dissolution. Thus, we set out asking some simple questions about MR-1, with the expectation that local dissolution might occur as a result of localized CO2 and/or organic acid accumulation. (i) Is MR-1 able to attach to the calcite (10
4) cleavage surface at all? (ii) If so, can MR-1 recognize and respond positively or negatively to the high surface free energy sites at which etch pits typically form? ("Positively" means that MR-1 would be attracted by these surface sites; "negatively" means that MR-1 would avoid the sites.) (iii) Can MR-1 impact the rate of calcite dissolution or precipitation?
All calcite cleavage fragments [Miller index value, (10
4)] used in these experiments were split from a single natural, untreated crystal of optical-quality calcite. This calcite is well characterized and has been used in a variety of experimental dissolution studies before (1, 16, 17). Mirror-image pairs of crystal samples were created by cleaving a large single crystal along a (10
4) cleavage plane. This procedure of sample generation facilitated the exposure of equivalent sites on the surface of each of the two crystal samples (Fig. 1). We assume that the outcrops of line defects, e.g., screw dislocations, within the crystal lattice on one cleavage face will occur in a mirror pattern at the other cleavage face, too. The topographies of all (10
4) sample surfaces were then characterized with a VSI. VSI is a noninvasive technique used to quantitatively map the topographies of surfaces that reflect light (1, 23-25). By use of a Mirau interferometric objective with a magnification of x50, the MICROXAM MP8 (ADE-Phase Shift) provides a field of view of 164 by 124 µm per measurement. The system's vertical resolution is better than 2 nm if a white light source is used. Resolution improves to 0.7 Å if a narrow band of green light, i.e., 550 ± 10 nm, is used. Under these conditions, the lateral resolution is about 0.5 µm. A single vertical scan of a 4-µm height difference takes less than 2 s (scan rate, 2.1 µm/s) and gathers as many as 100,000 height data at a time.
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FIG. 1. (10 4) Mirror cleavage faces of calcite as used in the experiments. For a detailed discussion of the use of mirror cleavage faces, see the text.
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h/
t is the surface-normal retreat (or advance) velocity (v) of dissolution (or growth) at the surface, expressed in meters per second. The rate constant, k, is then computed by dividing by the molar volume (AzV) of the material dissolved or grown, as follows:
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Organisms were prepared by inoculating 50% Luria-Bertani (LB) broth at 25°C with MR-1 cells from frozen (80°C) stock. After 24 h, these inoculants were split into separate 15-ml centrifuge tubes of 10% LB broth with the addition of 10 mM sodium lactate. These cultures were incubated for 48 h at 27°C.
pH measurements of the growth medium containing the MR-1 cells were taken before and after application to the calcite crystals with subsequent attachment of the microbes. The initial pH was 6.47. After a 30-min run duration, the pH of the fluid-organism suspension in contact with the calcite surface was substantially unchanged at 6.59.
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FIG. 2. (A) Three-dimensional height map of crystallographically defined rhombohedral etch pits in (10 4) cleavage faces of calcite. (B) False-color image (height map) of a calcite surface with MR-1. The image was taken with a 50x Mirau objective, i.e., the field of view is about 162 by 122 µm, and the height difference is about 1 µm.
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FIG. 3. Interferogram showing a large number of etch pits in a calcite cleavage face, representing a relatively high dislocation density. Note the typical shape of the pits as described, e.g., by Arvidson et al. (1) and Lea et al. (16).
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4) calcite cleavage faces, the microbes were exposed to a charge-neutral crystal surface. Thus, we did not introduce charge variables that would affect the sticking efficiency of the microbes (9). VSI measurements showed that MR-1 cells, when added to the solution, would quickly settle on and then attach to the calcite surface. Most surprisingly, the organisms had a dramatic inhibitory effect on the formation of etch pits (Fig. 2B), as seen by comparison to experiments without inoculation (controls). This unexpected result is consistent with MR-1 having the ability to detect the high-energy sites, attach to them, and inhibit the opening of the nascent etch pits. Recognition of and attachment to these energetically distinct sites must happen rapidly, before the individual etch pit opens from a hollow core (5, 6) or a point defect to a size larger than that of the individual organism. We know from the control experiments that after a run duration of about 10 min, the first generation of etch pits is significantly larger than the MR-1 organisms (diameter, approximately 600 nm; length, about 2 µm). Therefore, the edges of the pits could not be directly controlled by MR-1 after a 10-min run duration.
If we follow the model recently introduced by Lasaga and Lüttge (14, 15), the edges of etch pits are the sources of "dissolution stepwaves," i.e., trains of crystallographically determined steps that move across the crystal surface and cause its retreat. According to this model, the velocity and spacing of the stepwaves together with the formation of etch pits determine the overall abiotic dissolution rate of a particular crystal surface. Based on this model, it can be inferred that MR-1 inhibited not only the formation of etch pits but the entire abiotic dissolution mechanism of a calcite surface almost completely. Our VSI measurements presented here have confirmed this inference. To achieve the measurements of absolute surface-normal retreat (or advance), several micrometer-sized spots on the pristine calcite surface were covered (masked) with silicone rubber (Fig. 4A) (23) to protect parts of the pristine, untreated sample surface from dissolution and/or bacterial attack. These individual masks were taken off at later stages of the experiments. All vertical changes in the surface topography were then quantified by taking interferograms, which were digitized with a charge-coupled device camera and converted into topographic maps (Fig. 5). Each topographic map represents a part of the reacted crystal surface that includes at least one spot of the unreacted, pristine reference surface. By comparing the height of the reacted surface with the height of the reference spot(s), all measurements become absolute. For samples inoculated with MR-1, no measurable surface-normal retreat could be detected. That means that the presence of MR-1 reduced the calcite dissolution rate to values below the detection limit of the VSI method.
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FIG. 4. (A) Reflected-light image showing MR-1 colonies and single individuals with superimposed interference fringes. (B) Two-dimensional false-color height map calculated from the interferogram. Three different terraces can be identified. At the upper part of the image, MR-1 has started successfully to establish a closed biofilm. (C) Interferogram showing a section of the calcite surface. The upper part of the image is covered with MR-1, while the lower part shows the pristine calcite surface after removal of the mask. No significant height difference was measured between the "reacted" and "pristine" parts of the surface, indicating that MR-1 had successfully blocked the global dissolution of this calcite face.
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FIG. 5. (A) Interferogram showing MR-1 colonies in height resolution. (B) Three-dimensional height map calculated from the interferogram. (C) Detail with strongly exaggerated z-scale. The image shows a shallow etch pit that is no longer deepening into the crystal surface because MR-1 has successfully blocked the high-energy site in the bottom of the pit.
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Here, we present results of additional so-called "live-dead" experiments, which we conducted to determine whether MR-1 cells have to be alive in order to prevent the etch pits from opening. MR-1 cells were killed by exposure to 20 µg of chloramphenicol/µl and 0.5 mM carbonyl cyanide m-chlorophenylhydrazone (CCCP; a protonophore) added to the growth medium (0.1% LB medium plus 10 mM sodium lactate) on a shaker platform for 15 min. The VSI maps in Fig. 6 summarize the results of these experiments after a 15-min run duration, showing convincingly that only living cells cause the inhibitory effects we are reporting. Similar results were achieved in experiments with a 3-h run duration. The control experiments without any cells confirmed the previous findings that the abiotic growth medium causes the formation of pits (Fig. 6A). The same solution with dead MR-1 cells added also causes the formation of pits in calcite (Fig. 6B). Only experiments with living MR-1 cells significantly reduced or even entirely prevented the formation of pits (Fig. 6C).
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FIG. 6. Results of live-dead experiments. (A) Etched calcite surface of the control experiment without MR-1 organisms; (B) calcite surface with dead MR-1; (C) calcite surface with live MR-1 organisms. Images were taken with a 50x Mirau objective. The total height difference was 1.60 µm for panel B and 1.65 µm for panel C; field of view, 162.4 by 122 µm.
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A final point noted was the unusual and complex morphology of the attached MR-1 cells as they grew on the calcite surface. According to our spectrophotometric measurements, the organisms used in the experiment are in late-log phase or early-stationary phase; that is, measurements with the spectrophotometer show maximal density. This being the case, it is interesting that the biofilm propagated rapidly enough on the calcite surface that it was already densely honeycombed after a 90-min run duration. Because the pH does not decrease in the medium supporting the organisms as they form a film on the crystal surface, one might speculate that the organisms are using the carbon and preventing the transport of CO2 into the bulk fluid. As expected, the cells divided in a polar fashion, forming strings of organisms (Fig. 5A and B), but they did not form rounded colonies as they might on an agar surface. Similar morphologies have been seen in early formation of Shewanella biofilms on metal oxides (K. H. Nealson, personal communication). In the case of metal oxides, strings of microbes eventually coalesce to form a continuous biofilm. In our experiment, the chains became entrenched, ultimately forming structurally complex colonies. One might surmise, for purely geometric reasons, that the trenches will ultimately coalesce, creating a very different surface topography underlying a continuous biofilm like that typically formed on metal oxide surfaces.
MR-1 substantially slows the dissolution rate of the calcite crystal. Therefore, we conclude that the MR-1 biofilm is the major factor controlling calcite solubility under experimental conditions. This surprising result provides a quantitative foundation for earlier speculations that microbes could have a substantial role in the stabilization of carbonates in an aqueous environment and that one should expect entirely different dissolution kinetics in an environment devoid of their presence. One might expect biofilms to stabilize other mineral surfaces rather than aid in their corrosion, and the experimental protocol that we have developed positions us to address such questions.
We thank K. H. Nealson, R. S. Arvidson, K. J. Davis, T. A. Fewless, M. S. Beig, and J. C. Liu for thoughtful discussions and two anonymous reviewers for insightful and helpful comments that significantly improved this paper.
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4) obtained by scanning force microscopy: microtopography-based dissolution kinetics on surface with anisotropic step velocities. Geochim. Cosmochim. Acta 62:941-947.
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