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Applied and Environmental Microbiology, December 2008, p. 7329-7337, Vol. 74, No. 23
0099-2240/08/$08.00+0 doi:10.1128/AEM.00177-08
Copyright © 2008, American Society for Microbiology. All Rights Reserved.
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BioTechnology Institute, University of Minnesota, St. Paul, Minnesota 55108,1 Department of Biochemistry, Molecular Biology and Biophysics, University of Minnesota, Minneapolis, Minnesota 55455,2 Department of Civil Engineering, University of Minnesota, Minneapolis, Minnesota 55455,3 Department of Microbiology, University of Minnesota, Minneapolis, Minnesota 554554
Received 18 January 2008/ Accepted 21 September 2008
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This electron transfer capability has recently been utilized in devices known as microbial fuel cells (MFCs), where electrodes serve as electron acceptors to support growth (11, 18, 35, 36, 62). However, variations in electrode surfaces, operating temperatures, electron donor concentrations, and culture conditions limit comparison between electrode-reducing bacteria. In addition, MFCs aim to maximize electrical power production per unit volume, using large anodes consisting of carbon felt (19, 39, 50) or carbon paper (43) in small reactors (with surface/volume ratios between 25 and 640) (19, 25, 29, 43). In such systems, the actual surfaces accessible to bacteria are not known, multiple "dead zones" or diffusion-limited regions exist (19), high-surface-area electrodes increase capacitive current and reduce the sensitivity of analyses (53, 68), and irregular surfaces prevent mathematical modeling or imaging of attached biomass (22).
Electrochemical techniques typically used to study purified redox proteins (3, 4, 7) and cell extracts (26, 45) could likely be adapted for the study of metal-reducing bacteria. While protein voltammetry is limited by the success of purification and immobilization of enzymes (17, 49), metal-reducing bacteria represent a self-assembling multienzyme system that naturally interfaces with electrodes. In this report, we describe procedures for analysis of G. sulfurreducens biofilms on small carbon electrodes of defined roughness in potentiostat-controlled three-electrode cells. Several direct current and alternating current techniques could be applied to the characterization of the biofilm-electrode interface and have produced insights into electron transfer mechanisms between living cells and electrodes. Application of these techniques in routine characterization of other living bacteria and biofilm communities will allow quantitative comparisons between electron transfer rates and mechanisms used by these organisms.
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Electrode preparation.
Glassy carbon (Toko America, New York, NY) was machine cut into 2- by 0.5- by 0.1-cm electrodes. Freshly cut glassy carbon electrodes were polished using aluminum oxide-silicon carbide sandpaper with a grit designation of between P400 and P4000 (3M, Minneapolis, MN), as indicated in the ISO/FEPA standard (http://www.fepa-abrasives.com/). Mirror-polished electrode surfaces were obtained with 0.05-µm alumina powder (CH Instruments, Austin, TX). Polished electrodes were sonicated to remove debris, soaked overnight in 1 N HCl to remove metals and other contaminants, washed twice with acetone and deionized water to remove organic substances, and stored in deionized water. After each experiment, electrode surfaces were cleaned with an additional 1 N NaOH treatment (to remove biomass), and the entire surface was refreshed through sandpaper polishing and cleaning as described above to remove immobilized electron transfer agents. These working electrodes were attached to 0.1-mm Pt wires via miniature nylon screws that ensured electrical contact throughout the experiment.
Electrode cell assembly.
Platinum wires from the working electrode were inserted into heat-pulled 3-mm glass capillary tubes (Kimble, Vineland, NJ) and soldered inside the capillary to copper wires. Counter electrodes consisted of a 0.1-mm-diameter Pt wire (Sigma-Aldrich, St. Louis, MO) that was also inserted into a 3-mm glass capillary and soldered to a copper wire. The resistance of each electrode assembly was measured, and electrodes with a total resistance of higher than 0.5
were discarded. Reference electrodes were connected to bioreactors via a salt bridge assembled from a 3-mm glass capillary and a 3-mm Vycor frit (BioAnalytical Systems, West Lafayette, IN). Electrode capillaries were inserted through ports in a custom-made Teflon lid that was sealed with an O ring gasket. This lid fit onto a 20-ml conical electrochemical cell (BioAnalytical Systems, West Lafayette, IN), which had been previously washed in 3 N HNO3 (Fig. 1A).
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FIG. 1. Cartoon of three-electrode bioelectroreactor (A) and connection scheme to multichannel potentiostat (B).
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Autoclaved bioreactors flushed free of oxygen, filled with sterile growth medium, and incubated at 30°C were analyzed before each experiment to verify anaerobicity and the absence of redox-active species. Electrochemical cells showing residual peaks in differential pulse voltammetry (DPV), anodic current in cyclic voltammetry (CV), or baseline noise were discarded as having possible electrode cleanliness or connection noise issues. These autoclaved, verified bioreactors were then used for growth of G. sulfurreducens cultures.
A typical bioreactor was inoculated with 40% (vol/vol) of stationary phase G. sulfurreducens cells. After inoculation, a potential step of 0.24 V versus the standard hydrogen electrode (SHE) was applied and the reactors were incubated until the current stabilized (
72 h). The potential step was
200 mV higher than the midpoint potential, sustaining a half-maximal anodic current (as determined by preliminary CV; see below) (9).
Electrochemical instrumentation.
A 16-channel potentiostat (VMP, Bio-Logic, Knoxville, TN) was connected to the three-electrode cells described above (Fig. 1B). Software from the same producer (EC-Lab v9.41) was used to run simultaneous multitechnique electrochemistry routines, which include CV, DPV, and chronoamperometry (CA). Scan rates higher than 100 mV/s and all electrochemical impedance spectroscopy (EIS) experiments were performed using a Gamry PCI4 Femtostat (Gamry Instruments, Warminster, PA), and EIS data fitting was performed with E-Chem Analyst v5.1. Postacquisition analysis of CV data was performed with the software Utilities for Data Analysis (UTILS), kindly provided by D. Heering (v1.0; University of Delft, The Netherlands [http://www.tudelft.nl/]). All measurements, with the exception of CA, were performed in succession without stirring enabled. The parameters for DPV were as follows: Einitial (Ei) = –0.558 V versus SHE and Efinal (Ef) = 0.242 V versus SHE; pulse height, 50 mV; pulse width, 300 ms; step height, 2 mV; step time, 500 ms; scan rate, 4 mV/s; current averaged over the last 80% of the step (1 s, 12 points); accumulation time, 5 s. The parameters for CV were as follows: equilibrium time, 5 s; scan rate, 1 mV/s; Ei = –0.558 V versus SHE; Ef = 0.242 V versus SHE; current averaged over the whole step (1 s, 10 points). For CA, the parameters were Eapplied (E) = 0.242 V versus SHE.
EIS was conducted while maintaining a direct current voltage between the working electrode and the reference electrode (potentiostatic EIS) as electron transfer processes by Geobacter isolates were observed to be voltage dependent (62). EIS was performed at four potentials, 0.04, –0.06, –0.16, and –0.26 V versus SHE, with a perturbation amplitude of 10 mV. The frequency was varied from 105 to 0.01 Hz, as most biological charge transfer phenomena are observed in this range (10). Data were then fitted with a simple empirical model (62), using a constant phase element to account for irregularities in the morphology and chemistry of the glassy carbon surface. EIS was typically performed only at the end of incubations as extensive characterization required electrodes to be held at multiple potentials for long periods of time.
Confocal and SEM analyses.
A S3500N scanning electron microscope (SEM) (Hitachi, Japan) was used to image freshly polished (SEM) electrodes. After being thoroughly cleaned with deionized water, 2- by 0.5- by 0.1-cm graphite electrodes freshly polished with P400 and P4000 sandpapers were air dried and fixed through graphite tape to a sample stub. The sample stubs were placed directly into the SEM vacuum compartment and examined at an accelerating voltage of 5 kV.
A Nikon C1 spectral imaging confocal microscope (Nikon, Japan) with a x60 lens was used to image biofilm-covered electrodes. Immediately following harvesting, the biofilm-covered electrodes were gently washed in growth medium to remove planktonic cells and then stained with the LIVE/DEAD Baclight bacterial viability kit (Invitrogen Corp., Carlsbad, CA), incubated for 15 min in the dark, rinsed with growth medium, and placed on a microscope slide. The coverslip was supported by glass spacers thicker than the electrode to prevent damage to biofilm structure. Two laser wavelengths, 488 and 561 nm, were used to excite the two stains.
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After inoculation, the potential step was applied, and a rapidly increasing anodic (oxidation) current was detected (Fig. 2). As this rate of increase was many times higher than what could be explained by known growth rates of G. sulfurreducens, it was likely due to cell attachment to the electrode. The attachment phase was most rapid when fumarate-limited cells (compared to mid-log-phase cells) were used as the inoculum, consistent with reports linking acceptor limitation to the expression of enzymes important to metal reduction (21, 23). This was followed by a growth phase, characterized by an exponential increase in current, which doubled at a rate typically observed for G. sulfurreducens reducing Fe(III)-citrate or fumarate (doubling time,
7 h).
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FIG. 2. Characteristic growth curve for G. sulfurreducens inoculated into a bioreactor containing a 2.5-cm2 glassy carbon electrode (P400 grit polishing treatment). "Analysis" breaks indicate when CV and DPV were performed. "Medium change" breaks indicate where planktonic cells and culture medium were removed and replaced with fresh medium. Raw data are shown with no smoothing or noise-reduction transformations.
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15 µm with few structural features such as pillars (see Fig. S1 in the supplemental material). During the attachment and growth phases, electrodes were tested for the effect of voltammetry analyses on the rate of growth or current plateau. Repeated CV and DPV (see Materials and Methods) did not alter key midpoint potentials, colonization rates, or final current densities (Fig. 2). In order to minimize contribution of other electron transfer agents, we used a medium lacking redox-active species, such as vitamins (i.e., riboflavin), redox indicators (resazurin), and chemical reductants (cysteine and dithiothreitol) (47, 64). In our recent study (47), we showed that flavin concentrations in the nM range can be detected under the experimental conditions applied in the present work. When the medium in reactors was replaced, removing planktonic cells and any potential microbially produced soluble electron transfer agent, the electron transfer rate to electrodes remained unchanged. In addition, removal of nitrilotriacetic acid-chelated minerals from the medium (once electrode colonization had occurred) did not affect current production. These findings created stringent conditions for collection of baseline data in the absence of most common soluble redox-active compounds. A systematic examination of the effects of commonly present redox species on electron transfer by Geobacter spp. will be the focus of a future report.
The effect of microscale surface roughness on bacterial attachment and direct electron transfer has not been reported. Figure 3 shows the surface features of carbon electrodes polished with different sandpapers. When G. sulfurreducens biofilms were grown on electrodes polished with increasing grit size, the maximum current density increased over 100% for the same geometric area (Fig. 3). Polishing with particles smaller than
5 µm did not significantly reduce the maximum current. Therefore, even micrometer scale features have to be controlled to allow reproducibility and comparisons between cultures and electrodes in this and future studies.
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FIG. 3. SEMs of glassy carbon polished with P400 versus P4000 grit treatment (top). Bar graph (below) shows maximum current measured (n = 2 for each roughness) during CA after 72 h of growth. Also indicated ( , right y axis) is the average grit size of each polishing treatment.
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Application of CV to living bacteria required limiting the potential range to prevent harmful oxidizing or reducing conditions, as well as selection of informative scan rates. While it is known that application of potentials can disrupt biofilms either by producing hydrogen (28) or by inducing unfolding/oxidation of adsorbed proteins at oxidizing potentials (52), G. sulfurreducens biofilms were not harmed by exposure to potentials between –0.55 and 0.24 V versus SHE. For example, routine CV did not slow or impede biofilm development, as the anodic current after such analyses was 100.1% ± 3.4% (n = 6) of the current recorded before analyses. This was not unexpected, as Geobacter spp. are commonly exposed to metals in this potential range. Future work with stricter anaerobes, or organisms adapted to higher-potential environments, should independently verify the potential range which is not harmful to electron transfer.
Stable catalytic features with a high signal-to-noise ratio were observed when CV was performed at low scan rates (1 mV/s). Under these conditions, the rate of electron transfer rose rapidly at a potential higher than –0.3 V, reaching a limiting current above a potential of –0.1 V (Fig. 4). This response, commonly called a "reversible catalytic wave" (7), indicated continuous regeneration of the entire series of proteins catalyzing electron transfer from the substrate to the electrode. In preliminary investigations, each increase in the scan rate significantly increased the ohmic current and shifted the location of peaks in voltammetric waves, as expected from kinetic effects (see Fig. S2 in the supplemental material). However, increasing the scan rate by fivefold did not significantly alter the limiting current, demonstrating that at low scan rates, conditions were within a timescale sufficient to establish sustained catalysis by cells at each applied potential. Since the most informative scan rate could vary for each experimental setup, scan rates used in this report should be taken only as an aid in choosing conditions for new organism or electrode surface studies.
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FIG. 4. (A) Low scan rate CV of G. sulfurreducens biofilms after inoculation (0 h) and at maximum current production (72 h). (B) First derivatives of cyclic voltammograms of biofilms (P400 grit polishing treatment) (n = 4) showing the midpoint potential detectable in catalytic waves of mature biofilms.
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Once a biocatalyst is adsorbed, it is also possible to determine its response to increasing concentrations of substrate (24). To test this approach, the electron donor was first removed from the medium, and electrodes were incubated at 0.24 V for 36 h until no residual anodic (oxidation) current was observed. At this point, the effect of lowering substrate concentrations could be determined. The anodic-limiting current at –0.1 V was determined from CV and was found to increase linearly with the acetate concentration when acetate was <200 µM. At acetate concentrations higher than 3 mM, the anodic-limiting current did not change (Fig. 5). The midpoint potential of catalytic waves remained centered at the same position for all concentrations, suggesting a similar electron transfer mechanism and rate-controlling reaction, even at low current densities. This dose-response test detected acetate at concentrations as low as 3.5 µM (signal-to-noise ratio, >3).
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FIG. 5. Low scan rate CV (1 mV/s) of G. sulfurreducens at different concentrations of electron donor. The biofilm was poised at oxidizing potential without an electron donor until no anodic current was observed. Then electron donor was added, and the limiting current was recorded (inset). The midpoint potential of catalytic curves was constant with increasing concentration of the electron donor.
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Preliminary experiments with G. sulfurreducens biofilms indicated that DPV could also be used to monitor biofilms nondestructively, across a range of scan rates (up to 50 mV/s) and pulse heights (up to 100 mV). The parameters chosen (see Materials and Methods) represent a compromise between the time of analysis and sensitivity. When performed on mature biofilms, DPV always revealed a broad peak, which increased in height with the age of the biofilm. These voltammograms were highly reproducible, with the peak centered at –0.105 ± 0.005 V versus SHE (Fig. 6).
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FIG. 6. (A) DPV (scan rate, 4 mV/s; pulse height, 50 mV) under catalytic (presence of acetate) conditions at inoculation and after 72 h of growth. (B) The shape of peaks and average potential for DPV of mature biofilms (72 h) between four independent biological replicates.
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EIS.
While originally applied to investigation of solid-solid interfaces, EIS is today the most common alternating current method applied to the characterization of aqueous biointerfaces (10, 13). In most EIS methods, a small sinusoidal potential perturbation is applied to the sample. The frequency of this perturbation is changed in the range between few mHz and 105 Hz. The resulting sinusoidal current is analyzed via fast Fourier transform techniques to calculate the impedance (Z) of the interface in the frequency domain to estimate charge transfer resistance (32), diffusion at surfaces covered by protein monolayers (20), charge transfer time constants (59), and mechanisms of electron transfer (8).
Applications of EIS are numerous in microbially influenced corrosion, in which the sample is studied at the open circuit potential (42, 51). However, we have shown that electron transfer processes by G. sulfurreducens are voltage dependent (example shown in Fig. 3). Thus, while EIS is typically performed at open-circuit potentials, potentiostatic EIS (where the sinusoidal potential is applied while maintaining a given potential at the working electrode) was more likely to reveal electron transfer characteristics of active cells attached to electrodes.
Figure 7 shows a comparison of a glassy carbon electrode before and after colonization by G. sulfurreducens. When EIS was performed at –0.16 V versus SHE, the presence of G. sulfurreducens reduced the charge transfer resistance (inferred from the Z value at low frequencies), with a main time constant in the 1 to 10 Hz frequency range. At high rates of electron transfer, a second, slower time constant was observed in the 0.01 to 0.1 Hz range. The addition of a second time constant to the model did not significantly improve the dispersion of residuals, likely due to the low frequency of the second time constant.
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FIG. 7. EIS of G. sulfurreducens biofilms at V = –0.16 V versus SHE; modulus of impedance (Z) after inoculation () and at 72 h ( ); phase angle V-I after inoculation ( ) and at 72 h ( ). Biofilm development results in lower charge transfer resistance at the electrode-biofilm interface, with two distinct charge transfer processes around 1 and 0.03 Hz.
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), double-layer capacitance (Cp = 3.0 ± 0.9 mF), and nonideality coefficient (a = 0.72 ± 0.06) did not change appreciably. These results again highlighted how data from one method (CV) could be used to select parameters in a complementary method (EIS). They also demonstrated the importance of investigating the proper analysis parameters for each bacterial system, as another strain with a different midpoint potential for its catalytic process would need to be studied at a different imposed voltage to obtain the fastest time constant.
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FIG. 8. EIS of mature G. sulfurreducens biofilms (72 h) performed at different potentials. (A) Bode plot. Modulus of impedance (Z) at 0.04 (filled black circles), –0.06 (filled red circles), –0.16 (filled blue circles), and –0.26 V (filled green circles) versus SHE; phase angle V-I at 0.04 (open black circles), –0.06 (open red circles), –0.16 (open blue circles), and –0.26 V (open green circles) versus SHE. Note that frequency of the major charge transfer process changes with applied potential. The second charge transfer process can be observed only at –0.16 V. (B) Nyquist plot. The relaxation times for the electron transfer process at the interface are summarized in Table 1.
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TABLE 1. EIS parameters for biofilms at 72 ha
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In particular, this study shows how the response of an intact film to a range of applied potentials can be measured systematically and analyzed to produce data that are easily compared between species, conditions, or electrode surfaces. As scan rates are lowered, electron transfer kinetic effects (rates of electron transfer between cell surfaces and electrodes) are minimized, and enzymatic effects (related to microorganisms' activity) become primary factors. As the goal was to initially characterize the catalytic behavior of the system, low scan rates (1 mV/s) were chosen, since they permitted reactions with a time constant on the order of
1 s to be active as turnover processes at each imposed potential step. At high levels of electron donor and low scan rates, catalytic voltammograms should therefore be representative of steady-state conditions. In addition, minimization of ohmic current aided in identification of inflection points in derivative analysis. The choice of a relatively low scan rate was also supported by data from EIS measurements, in which we found time constants on the order of 0.1 and 1 to 10 s. For a system such as this, with what appears to be sluggish interfacial electron transfer kinetics, the potential difference between anodic and cathodic peaks for a given redox couple could change significantly with even modest changes in scan rate. Future work will focus on the use of electrochemical techniques under nonturnover conditions to better elucidate these electron transfer kinetics for a more complete understanding of the interplay between microbial catalytic abilities and interfacial electron transfer.
The high reproducibility between biological replicates and the ability to perform experiments with a range of electrodes provided a robust measurement of G. sulfurreducens current densities, which approached 2 A/m2 for electrodes polished with 35-µm-grit-size particles. The catalytic wave consistently observed for G. sulfurreducens is an independent demonstration that interior oxidative processes of this organism are linked via a continuous pathway to surfaces and that the entire collection of attached organisms (i.e., the biofilm) behaves as an adsorbed catalyst. The midpoint potential of the catalytic wave at –0.15 V supports a model with a dominant rate-limiting electron transfer reaction and shows that G. sulfurreducens respiration rate does not increase when cells are provided with an electron acceptor with a potential greater than 0 V. The latter result implies that the final step of electron transfer (e.g., between a terminal external protein and the electrode) is not rate limiting, as this process can always be accelerated by additional applied potential (as described by the standard rate law kf = k0 eß
E) (9). The midpoint and the limiting current potential found in this study are consistent with G. sulfurreducens being adapted for the reduction of iron oxides with a potential between –0.2 and 0 V versus SHE in the environment and suggest that cells do not derive any additional energetic benefit from higher-potential electron acceptors.
While the study of an intact electron transport chain in G. sulfurreducens represents perhaps a complex example of this electrochemical approach, similar methods have been used to characterize extracts from bacterial cells adsorbed onto, or incorporated into, electrode materials (26, 45, 46, 61). In addition, researchers have washed and concentrated whole cells for brief voltammetry analyses and detected possible redox-active agents on the external surfaces of cells (39). The benefits of using living cells in the work reported here include the lack of a protein purification step and the fact that cells are allowed to assemble the actual biofilm structure responsible for this unique extracellular electron transfer process.
The multiple peaks visible in both CV and DPV analyses also confirm the complexity of the G. sulfurreducens surface. Multiple cytochromes and redox proteins have been previously implicated in outer membrane-based electron transfer in proteomic and labeling studies (23, 36, 41). As most proteins implicated in electron transport by G. sulfurreducens contain multiple hemes or redox centers, the detected redox centers could reflect individual hemes, domains that act as a single center, or individual proteins. Recent work with the multiheme cytochrome MtrC (30) showed that multiheme proteins do not demonstrate classic, individual redox behavior for each heme but rather act as a cluster with a broader midpoint. In another study (67), the same protein was observed to behave as two pentaheme domains with broad midpoint potentials. Future work with specific mutants lacking key redox proteins in G. sulfurreducens will aid in identifying the origin of these peaks.
Based on the results reported here, voltammetric methods previously developed to characterize electron transfer phenomena by enzymes adsorbed at carbon electrodes can be extended to the characterization of viable biofilms. By choosing the appropriate conditions, these methods are not destructive and allow in vivo determination of electron transfer from whole cells to electrodes under conditions that are comparable to those encountered in natural environments. Both thermodynamic and kinetic parameters can be determined and used to define the phenotype of an organism for comparison with other strains or mutants. The proposed methods can be applied to well-defined pure cultures, as well as to complex microbial communities, and could allow for quantitative comparisons in the development of better microbial catalysts based on direct electron transfer between bacteria and electrodes.
We also thank Jeremy Alley for technical help with the experimental setup, Dirk Heering for suggestions in the interpretation of data, and Lewis Werner for the SEM images of bare electrodes.
Published ahead of print on 10 October 2008. ![]()
Supplemental material for this article may be found at http://aem.asm.org/. ![]()
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