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Applied and Environmental Microbiology, January 2009, p. 83-92, Vol. 75, No. 1
0099-2240/09/$08.00+0 doi:10.1128/AEM.01799-08
Copyright © 2009, American Society for Microbiology. All Rights Reserved.

Department of Marine Sciences, University of Georgia, Athens, Georgia 30602,1 Department of Civil Engineering, Middle East Technical University NCC, Kalkanli, Guzelyurt TRNC, Mersin 10, Turkey,2 Department of Chemistry, Indiana University Bloomington, Bloomington, Indiana 474053
Received 4 August 2008/ Accepted 3 November 2008
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To predict how bacteria regulate their activity and grow in situ, it is necessary to quantitatively understand the complex and dynamic interactions between the numerous concurrent biogeochemical processes involved, which requires the use of mathematical models. While subsurface reactive transport models generally contain a comparatively sound description of the physical transport processes (3, 34), they often do not explicitly account for the dynamics of microbial populations that mitigate the majority of biogeochemical processes (18, 48). When included, microbes are typically represented as functional groups, with growth dynamics depending linearly on substrate availability or following Monod kinetics (27, 38, 44), an approach that has been successful in describing geochemical contaminant plume dynamics (7). However, lacking a realistic representation of microbial metabolism, such models are limited in their capability of reflecting microbial dynamics and forecasting the response to changing environmental conditions, which restricts their predictive power at the macroscale and their usefulness, for example, in the assessment of conditions that optimize in situ bioremediation (22).
With the advent of genome sequencing, over the last decade, the biological revolution has led to the characterization of cellular metabolic networks and to the development of mathematical models at the cell scale (41), ranging from descriptions of network topology (20, 45) to constraint-based models for different organisms (13, 33, 42) and fully kinetic approaches (e.g., see references 2, 30, and 50). Integration of such models of environmentally important groups of bacteria in reactive transport simulations would clearly benefit forecasting biogeochemical responses to changing macroscopic conditions. The gammaproteobacteria Geobacteraceae constitute such an abundant and environmentally important group in both pristine and contaminated sediment environments (22). Geobacter species are metabolically diverse and can grow with numerous electron donors and acceptors, including acetate or H2, and Fe(III), fumarate, or malate, respectively (8, 23). They have been shown to be enriched when Fe(III) reduction is promoted in a petroleum-contaminated sandy aquifer (39) and to mediate the reduction of U(VI) to U(IV) (25), converting the soluble form to the insoluble form and effectively removing the uranium from the groundwater (51). Geobacter shapes biogeochemical cycling directly through its metabolic activity, as well as indirectly, such as via the effect of iron (hydr)oxide reduction on the motility of sorbed trace metals and on pH.
In this study, we present a kinetic cell model of Geobacter sulfurreducens metabolism and its application in the simulation of a subsurface contaminant plume with the following goals: (i) to assess the kinetic description of central cellular metabolism and the growth efficiencies emerging under a range of substrate conditions by comparing them to observational data; (ii) to quantify the sensitivity of model results to the parameterization of the enzymatic reactions of the tricarboxylic acid (TCA) cycle and gluconeogenesis considered here; (iii) to compare and contrast different cell model approaches; (iv) to introduce a coupling approach between cell metabolic expressions and macroscopic reactive transport models; and (v) to assess the potential and the limits of macroscopic models that parameterize microscopic intracellular processes. Our cell model is validated against growth efficiencies obtained in chemostat experiments (12) and is compared to the flux balance (FB) model developed by Mahadevan et al. (26) who—based on an extensive genome analysis—used a constraint-based modeling approach to estimate steady-state intracellular fluxes and metabolite exchange with the environment. To assess the role of microbial dynamics in the environment, an acetate plume is studied in a heterogeneous porous medium, for which simulations with a full coupling between the environment and the cell model are contrasted with several simplified parameterizations, including commonly used Monod approximations.
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) followed by a slow dissociation (
), where Qf is the equilibrium constant for the fast reaction and k and kQs are the backward and forward rate constants for the slow reactions, respectively.
Under typical natural subsurface conditions, the oxidation of acetate in Geobacter—initially activated through the combined actions of acetate kinase (AK; EC 2.7.2.1) and phosphate acetyltransferase (10)—is coupled to the reduction of Fe(III) (24), which is believed to take place on the extracellular membrane (21). Thus, the kinetic cell model encompassed the uptake of acetate and its incorporation into biomass via gluconeogenesis or its complete oxidation in the TCA cycle (10, 14) (Fig. 1). Two compartments—one extracellular and the other intracellular—were considered. The extracellular compartment accounted for species concentrations that represented environmental conditions, while the intracellular one accounted for enzymatic reactions and resource allocation in cellular metabolism. Reactions were formulated using mass action kinetics:
![]() | (1) |
l denotes stoichiometric coefficients, and Np and Nr are the number of products and number of reactants, respectively. Model parameters were derived from the literature and are given in Table A1. As the literature rarely contains enzymatic forward and reverse rate constants, model parameters were typically derived from enzyme turnover numbers, specific activities, and substrate affinities. Details of the procedures and sources for model parameterization are given in the Appendix.
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FIG. 1. Structure of the kinetic cell model and FB models. The kinetic model focuses on the fate of acetate in the metabolism of Geobacter sulfurreducens through incorporation into biomass from gluconeogenesis or energy production from the TCA cycle. All reactions are assumed to be intrinsically reversible, and the rates are computed using the parameter values listed (for data sources, see the Appendix). The FB model is described in a study by Mahadevan et al. (26) and encompasses some 500 reactions and species.
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View this table: [in a new window] |
TABLE A1. Values used for the parameterization of the reaction networkf
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![]() | (2) |
Cellular energy dynamics.
Cellular energy dynamics were accounted for through reactions utilizing and producing AMP, ADP, and ATP. In addition to the energy used in the phosphorylation of acetate and pyruvate (Fig. 1, reactions 2 and 9), ATP is also produced through the reactions of the TCA cycle and consumed through cell growth and reactions required for cell maintenance according to the following equation:
![]() | (3) |
T and
D reflect the presence of ATP and ADP, respectively (1 if present, 0 otherwise). ATP, ADP, and AMP values were further constrained through a fast exchange of ATP + AMP = 2ADP that mimicked the balance between adenosine phosphates not modeled at the process level (29). Levels of other substances involved in intracellular energy regulation, such as NAD-NADH, NADP-NADPH, CO2, and phosphates (Pi, PP), were assumed to be constant (Fig. 1).
Acetate uptake.
Acetate uptake rates for the kinetic cell model were formulated using the four-state model for a facilitated diffusion carrier kinetics (2), in which the flux of acetate across the cell membrane, Jac (mol liter–1 s–1), is described by
![]() | (4) |
![]() | (5) |
is set to 0 for symmetric cross-membrane transport of acetate. Cell area was calculated based on G. sulfurreducens cell size (37), assuming a cylindrical shape. Maximum acetate exchange (Y = 1.20 x 10–4 dm s–1) was set to match the results from Geobacter chemostat experiments (12).
Growth efficiency was calculated from the acetate uptake flux and the flux of acetate through phosphoenolpyruvate (PEP) with the following equation: geff =
pepβ/Jac, where
pep is the molar concentration of PEP produced per unit of time and β describes the grams of dry weight of biomass produced per mole of PEP created. β was calculated from a growth efficiency of 4.4 x 10–3 gdw mmolacetate–1 at a cell-specific growth rate, µ, of 0.06 h–1 and an acetate flux to gluconeogenesis (Q) of 0.30 molacetate gdw–1 h–1 (26). Taking into account the 2-to-3 acetate-to-PEP carbon ratio, β = 2µ/3Q = 0.3 gdw mmolPEP–1.
Flux balance model.
Cellular metabolic rates under a range of acetate uptake fluxes were calculated using the FB model of G. sulfurreducens metabolism by Mahadevan et al. (26), which estimated intracellular fluxes and metabolite exchange with the environment for a given acetate uptake. The metabolic fluxes (reaction rates f) were sought, where for a network described by a stoichiometric matrix S,
![]() | (6) |
f
upper bound. Maximization of biomass production rate was used as an objective function, which had been shown to lead to results in agreement with experimental data (26). The FB model was implemented in MATLAB, and growth efficiencies were calculated from the ratio of growth rate (fgrowth) and acetate uptake (fac) as geff = fgrowth/fac.
Coupled environment-cell model.
Representations of Geobacter metabolism were coupled to simulations of a dynamic environment through incorporation into a reactive transport model. The two models were connected such that the reactive transport model was used to evaluate the transport of substrate and biomass while the cell model provided the cell-specific reaction rates under the environmental conditions at a given time and location. These cell-specific rates were then used to compute the reaction rates in the macroscopic reactive transport model. For dissolved constituents, the governing equation is
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| (7) |
is porosity, t is time, C is concentration, v is pore water velocity, D* is the dispersion tensor implemented with dependence on v as described by Scheidegger (36), and
R is the net reaction rate. Flow velocities were computed from an imposed pressure gradient using a Darcy model (40).
In our implementation, the cell model was driven by the availability of acetate as the substrate, whose spatiotemporal dynamics proceeded via
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| (8) |
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| (9) |
is the rate of acetate uptake, and Rferm is a source of acetate from the breakdown of high-molecular-weight organics. The model was solved numerically using sequential noniterative operator splitting. In each time step,
t, first the pressure and flow field were determined, which were then used to calculate the net transport for each of the chemical species. Subsequently, concentration changes due to reactions were evaluated by solving a set of coupled ordinary differential equations at each node. Reaction parameters that depend on the cell model (i.e., geff,
) were computed for a given environmental condition and cell state, reflected by the intracellular concentrations, and were assumed constant over a time step. Cell death was considered through negative growth efficiencies, which were obtained when the ATP produced did not completely account for cell maintenance demands and the existing pool of ATP was insufficient to meet the cellular energy requirements. In that case, the use of biomass resources was considered to meet ATP demands (a · Rg; see equation 3). |
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90% of the acetate uptake flux, with an additional
8% of acetate flowing through the TCA cycle being used for amino acid and lipid production, and the remainder of the acetate uptake flux passed through the pentose-phosphate pathway and gluconeogenesis. Along with the FB model, the kinetic model predicted that for lower acetate uptake rates, acetate is channeled preferentially into the TCA cycle, leading to low growth efficiency. Both the kinetic and the FB models showed nearly identical responses of the TCA cycle to acetate uptake, with a nearly linear increase in the TCA cycle with increasing acetate uptake rates (not shown). Both models reproduced the general trend in growth efficiencies seen in the literature as a function of the acetate uptake rate (Fig. 2), reflecting that at elevated uptake rates, the portion of acetate following the growth reaction pathway increased relative to that for the TCA cycle.
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FIG. 2. Growth efficiency in gdw molacetate–1 at a given acetate uptake rate (Raccell) for the cell model, FB model, and measured chemostat data (12). Error bars for the kinetic cell model represent the 25% and 75% quartile ranges, as determined in the sensitivity analysis (see the text). Inset: Acetate uptake flux at a given extracellular acetate concentration computed with the kinetic model along with measured data (chemostat data depicted with filled rectangles indicate measured acetate concentrations below the detection limit of 10 µM).
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, and using steady-state cell model results, one obtained vmax = (19.54 ± 0.04) mmolac gdw–1 h–1 and Km(acetate) = (10.24 ± 0.11) x 10–6 mol liter–1, consistent with half-saturation constants and maximum uptake rates derived from experimental data (12).
The kinetic model also provides estimates of intracellular metabolite concentrations, which can be used as diagnostics to experimentally assess its validity and limitations. Under steady-state conditions, the cell model predicted malate concentrations in the mM range, consistent with predictions of high malate concentrations based on the thermodynamics of the malate dehydrogenase reaction (5). Several other substances, including oxaloacetate, citrate, isocitrate, and succinate were predicted—depending on growth conditions—to be present in the micro- to millimolar range and to increase by a factor of 10 to 30 between no-growth and maximum-growth conditions. Succinyl coenzyme A (CoA) concentration was predicted to be relatively constant, while significant variations under changing growth conditions were computed for pyruvate and
-ketoglutarate, with lower concentrations at higher growth rates.
Model sensitivity.
The sensitivity analysis based on
1,000 realizations for a given extracellular acetate concentration, which was sufficient to establish the probability distribution of the model response, allowed the identification of the reactions affecting growth efficiency most strongly (Fig. 3). The extent to which a parameter affected growth efficiency varies with the acetate uptake rate. For example, at low acetate uptake rates, growth efficiency was most sensitive toward parameters describing the acetate-CoA transferase (ACT; EC 2.8.3.8) reaction. In general, however, growth efficiency, over the range of acetate uptake rates, was most sensitive to cell model parameters associated with the activation of acetate to acetyl-P catalyzed by AK (Fig. 3), a reaction essential to the use of acetate in biomass production, as all acetate incorporated into cell biomass must go through this reaction (26). Increasing the forward rate constant kf—corresponding to an increase in enzyme concentration (ET), maximum enzyme activity (vmax), or higher substrate affinity (lower Km)—involved in the reaction catalyzed by citrate synthase (CS; EC 2.3.3.1) decreased growth efficiencies as more acetyl-CoA is shifted to the TCA cycle. For the same reason, increasing the parameters associated with the reaction catalyzed by succinate dehydrogenase (SDH; EC 1.3.99.1) resulted in a decrease in growth efficiency, and increasing parameters associated with pyruvate ferredoxin oxidoreductase (PFO; EC 1.2.7.1), a reaction involved in growth, resulted in an increase in growth efficiency. The variation in growth efficiency due to small—on the order of 5%—variations in forward and backward reaction rate constants can largely (>95%) be explained by the linear model (equation 2). Uncertainties in ET, vmax, and Km, however, tend to result in larger uncertainties in growth efficiencies due to error propagation, but the same reactions are found to have the most decisive impact (not shown).
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FIG. 3. Sensitivity, sj, of growth efficiencies to perturbations in the cell model parameters as a function of acetate uptake rates (equation 2). Labels AK, CS, ACT, SDH and PFO along the bottom of the figure denote the reactions promoted by the respective enzymes (see Fig. 1). kb, kf, and Q values denote the model parameters. Large absolute values of sj indicate a strong impact of a model parameter on resulting growth efficiencies (see the text for details).
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; equations 8 and 9) can be expressed by Monod kinetics, with Km(acetate) = 10.24 µM and vmax = 19.54 mmol gdw–1 h–1, as derived above. Finally, a third approximation employed both a constant growth efficiency and a constant acetate uptake rate as long as acetate was present (model III), with a cell-specific acetate uptake rate of 9 x10–3 molacetate gdw–1 h–1 and a growth efficiency of 3.3 gdw molacetate–1 (12). In order to quantify the impact of microbial dynamics and the substrate dependence of growth efficiencies under environmental conditions, simulations were performed in a domain that was 10 cm long and 6 cm high. The porous medium consisted of permeable sand (k = 10–11 m2) into which a less permeable section was embedded (k = 10–13 m2) as depicted in Fig. 4. No-flow conditions were set at the upper and lower domain boundaries, and a positive pressure gradient was imposed across the horizontal x-direction. The inflowing fluid was set to contain 0.76 µM acetate and 0.03 gdw m–3 biomass. After a period of constant input that allowed the establishment of a steady substrate and biomass distribution, the concentrations in the inflowing fluid were ramped up over a duration of 1 h to an inflow concentration of 1 mM acetate and 0.3 gdw m–3 biomass, reflecting a plume of dissolved organic carbon (16), and were held constant at high levels thereafter.
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FIG. 4. Results of reactive simulations utilizing different representations of bacterial growth and acetate uptake. Steady-state acetate and biomass distributions under low (panels A to F) and high (panels G to L) input conditions for the dynamic cell model (panels A, B, G, and H), the Monod parameterization (panels C, D, I, and J), and simulations with fixed growth efficiency and acetate uptake rate (panels E, F, K, and L). The low-permeability zone is indicated by the boxes with dashed-line borders, and the arrows in panel A indicate the direction and magnitude of flow.
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Steady high substrate input stimulated microbial growth, reflected in the elevated biomass levels in both high- and low-permeability regions (Fig. 4H, J, and L). A clear distinction was visible between the results obtained with the dynamic cell model and the Monod approximations compared to the fixed growth efficiency description. The latter predicted biomass levels ranging from 0.3 to 1.2 gdw m–3 in the low-permeability zone (Fig. 4L), while the kinetic models suggested a region of higher biomass in the low-permeability zone adjacent to the more-permeable one (Fig. 4H and J). In the models that represented the cell in more detail, the maximum growth efficiencies exceeded the constant average value in the "fixed" model, leading to a buildup of biomass and the depletion of acetate in the low-permeability zone. The Monod parameterized model suggested acetate levels that are similar to those for the cell model (Fig. 4G and I). The cell model predicted the depletion of biomass in those low-permeability regions that exhibited low acetate concentrations (Fig. 4H). This pattern was less pronounced in the Monod model, which as a result of the missing feedback of substrate availability on growth efficiencies showed elevated biomass levels even where acetate levels approached zero (Fig. 4I and J).
Conclusion.
The kinetic representation of Geobacter sulfurreducens central metabolism, encompassing its TCA cycle and the use of pyruvate in gluconeogenesis, successfully reproduces measured growth efficiencies, with iron as electron acceptor over a wide range of extracellular acetate concentrations. Despite its limited scope, it predicts process rates that are in good agreement with results from a comprehensive FB model (26), as it includes feedback between metabolite levels and transformation rates which can accurately regulate the response over a range of substrate conditions.
The two main differences between these two modeling approaches are the extents of the network considered and the fact that the kinetic description provides explicit estimates of intracellular metabolite concentrations. The more comprehensive description inherent in FB models—possible because they do not require extensive parameterization—is an advantage as, intrinsically, it extends the range of applicability well beyond the acetate-limited environmental settings discussed here. However, the computation of metabolite levels in the kinetic approach allows for a mechanistic process description linking intracellular conditions to environmental conditions. In contrast, the FB approach requires a priori knowledge of uptake fluxes, which may restrict its use to settings at which they are constrained by experimental data.
While comparison of the fully coupled reactive transport model with the Monod type simulations shows that it is possible to approximate microbial distribution patterns without the explicit incorporation of cell models into reactive transport simulations, the parameterization has to reflect the response of intracellular processes. Process-level descriptions of microbial metabolism give rise to emerging properties, such as growth efficiencies, that are critical in the incorporation of microbial dynamics in reactive transport models. Hence, models aiming at describing in situ microbial functioning and at accounting for environmental feedbacks can benefit substantially from reflecting the growing knowledge on cellular metabolism, which in turn will bolster the predictive power necessary for their broad application.
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![]() | (A1) |
![]() | (A2) |
![]() | (A3) |
![]() | (A4) |
![]() | (A5) |
Concentrations of enzyme substrate complexes used in equation A5 are not measured directly and were calculated according to each enzyme's mechanism, which is separated into several fast components and one slow component (32):
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The enzyme substrate concentrations in the slow reactions were calculated following Purich and Allison (32):
![]() | (A6) |
![]() | (A7) |
![]() | (A8) |
![]() | (A9) |
for enzymes that employ an ordered bi-bi mechanism,
![]() | (A10) |
for enzymes that employ a ping-pong mechanism,
![]() | (A11) |
![]() | (A12) |
for a tri-ping-pong mechanism,
![]() | (A13) |
![]() | (A14) |
![]() | (A15) |
![]() | (A16) |
The values used for the parameterization of the reaction network are shown in Table A1.
We thank two anonymous reviewers, whose comments significantly improved the manuscript.
Published ahead of print on 14 November 2008. ![]()
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