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Opinion

Predicting the Hydraulic Conductivity of Metallic Iron Filters: Modeling Gone Astray

by
Chicgoua Noubactep
1,2,3
1
Department of Applied Geology, Universität Göttingen, Goldschmidtstraße 3, Göttingen D-37077, Germany
2
Comité Afro-européen, Avenue Léopold II, Namur 41-5000, Belgium
3
Kultur und Nachhaltige Entwicklung CDD e.V., Postfach 1502, Göttingen D-37005, Germany
Water 2016, 8(4), 162; https://doi.org/10.3390/w8040162
Submission received: 28 January 2016 / Revised: 31 March 2016 / Accepted: 13 April 2016 / Published: 20 April 2016

Abstract

:
Since its introduction about 25 years ago, metallic iron (Fe0) has shown its potential as the key component of reactive filtration systems for contaminant removal in polluted waters. Technical applications of such systems can be enhanced by numerical simulation of a filter design to improve, e.g., the service time or the minimum permeability of a prospected system to warrant the required output water quality. This communication discusses the relevant input quantities into such a simulation model, illustrates the possible simplifications and identifies the lack of relevant thermodynamic and kinetic data. As a result, necessary steps are outlined that may improve the numerical simulation and, consequently, the technical design of Fe0 filters. Following a general overview on the key reactions in a Fe0 system, the importance of iron corrosion kinetics is illustrated. Iron corrosion kinetics, expressed as a rate constant kiron, determines both the removal rate of contaminants and the average permeability loss of the filter system. While the relevance of a reasonable estimate of kiron is thus obvious, information is scarce. As a conclusion, systematic experiments for the determination of kiron values are suggested to improve the database of this key input parameter to Fe0 filters.

1. Introduction

Due to their low-cost components, metallic iron-based filtration systems (Fe0 filters) have a broad range of applications from small-sized units for the production of safe drinking water in remote and/or low-income communities (e.g., Africa, Latin America and South-East Asia) to large-scale reactive walls for groundwater remediation, progress in numerical simulation of such systems may reasonably be expected to increase the application potential of this proven environmentally-friendly technology.
Predicting the service life of Fe0 filters is a fundamental aspect in discussing the suitability of this technology, both in terms of affordability and (long-term) efficiency [1,2,3,4]. The present state of the art has been shown to be unsatisfactory [3,5,6,7,8,9,10,11,12]. This situation is caused by several reasons. One reason is a misinterpretation of the essential reaction causing contaminant removal. A reduction reaction implying electrons transfer from Fe0 to the contaminants (e.g., RCl = chlorinated hydrocarbon, cf. Equation (1)) can be at best a side reaction under environmental conditions [13,14,15,16,17,18,19].
Fe0 + RCl + H+ ⇒ Fe2+ + RH + Cl
Iron corrosion by water (cf. Equation (2)) is spontaneous and quantitative.
Fe0 + 2H+ ⇒ Fe2+ + H2
Iron corrosion is well-known as a major nuisance reaction in the present iron-based world causing billions of Euro of damage per year [20]. This reaction is quantitative even in situations where water is present as moisture only [21]. It is therefore clear that iron corrosion by water has to be considered as a major reaction in a context (water treatment or Fe0/H2O system) where water is the solvent ([H2O] = ~55.5 mol L−1). Even if more powerful oxidizing agents (e.g., CrVI, Cu2+, NO3, O2, RCl) should be present as solutes (even at the mg L−1 level), Equation (2) still needs to be considered a dominant reaction in Fe0/H2O systems.
It has been unambiguously demonstrated that contaminant reduction in Fe0/H2O systems is mediated by (i) FeII species (Equation (3)) and H2 (Equation (4)), which are primary corrosion products and (ii) secondary and tertiary corrosion products, including Fe3O4 and green rusts [10,11,22,23,24,25,26].
2 Fe2+ + RCl + H+ ⇒ Fe3+ + RH + Cl
H2 + RCl ⇒ RH + HCl
The fact that the Fe0 surface is constantly shielded by a multi-layered oxide scale (see [11] and the references cited therein) implies that, even under oxic conditions (O2 is available), Fe0 oxidizes according to Equation (2). This reaction is even accelerated if reaction products (e.g., FeII species) are consumed (Le Chatelier’s principle). Further details about this aspect of the iron corrosion process are summarized in [21].
The presentation above clearly shows that rate constants for modeling contaminant reductive transformations in Fe0/H2O systems should be exclusively based on Equations (3) and (4). Alternative strategies have been discussed in [16,19,27,28,29,30]. These alternative strategies are based on Equation (1) and mentioned herein for the sake of completeness.
Electrochemical reduction alone (Equation (1)) cannot explain all reported observations as (i) the generation of iron hydroxides and oxides for As or U removal [31,32] or (ii) the porosity loss of Fe0 beds flushed with distilled water [33,34]. These obvious discrepancies between various modeling approaches for Fe0 filters, however, had been a motivation for the discussion herein.
The following four facts suggest that it may be sufficient to characterize the long-term behavior of Fe0 corrosion while considering the coupled removal efficiency of selected species added as contaminants to have a realistic picture of Fe0 filters [10,11,25]: (i) Fe0 corrosion by water is quantitative; (ii) contaminants are chemically reduced by some iron corrosion products; (iii) contaminants are present in trace amounts; and (iv) contaminants without redox properties are quantitatively removed. Thus, the most important parameter to design a Fe0 filter is the long-term corrosion rate (kiron; cf. Section 2) of the material to be used.
The aim of the present communication is to demonstrate that no reliable model for Fe0 filters can be presented without relevant kiron values. Domga et al. [35] recently summarized the results of mathematical modeling of the spatial description of the process of permeability loss in Fe0 filters. Herein, it is shown that related temporal changes depend on kiron values that are yet to be determined. The significance of kiron will be first presented, followed by the specificity of Fe0 materials as used in water treatment and environmental remediation.

2. The Rate Constant of Iron Corrosion (kiron Value)

2.1. Descriptive Aspects

Kinetic studies on contaminant reductive transformation in Fe0/H2O systems currently use relationships like the following based on reactions similar to Equation (5):
d [ RCl ] dt = k × [ RCl ] × [ H + ]
Following this approach, k values for individual contaminants (e.g., kRCl) have been determined and partly tabulated for modeling purposes [16]; however, considering that Equation (1) is faulty as Equations (3) and (4) are the main sources of electrons for any contaminant in a Fe0/H2O system (indirect reduction). Accordingly, properly modeling the kinetics of any reductive transformation in Fe0/H2O systems depends on the accurate characterization of the kinetics of the production of Fe2+ and H2 or the determination of the kinetics of Fe0 corrosion by water (Equation (6)). The relationship defining kiron can be written as:
d ( Fe 0 ) dt = k iron × [ H + ] 2
where kiron is the rate of iron corrosion and [H+] the concentration of protons. Reardon [36,37] has positively correlated kiron and the volume of H2 generated in the Fe0/H2O system. However, properly correlating both values depends on the description of individual systems and the characterization of possible H2 sinks [38]. In other words, characterizing the kinetics of iron corrosion (at pH > 4.0) by determining the volume of generated H2 is just an approximation. This approach is arguably nearer to reality than any reasoning based on Equation (5) [39].
The abundant literature on aqueous iron corrosion reveals that there are three basic kinetics laws that characterize the oxidation rates of Fe0: (i) the parabolic rate law; (ii) the logarithmic rate law; and (iii) the linear rate law. These laws are modeled respectively as follows [40,41]:
x2 = Kp × t + x0
x = Kp × log(c × t + b)
x = KL × t
where x is the thickness of the oxide scale on Fe0; Kp is the parabolic rate constant for scale growth; KL is the linear rate constant for scale growth; t is time; a and c are constants. As a rule, the x values (scale thickness) are correlated to the Fe0 weight loss (metal loss) without considering the presence of individual corrosive species (e.g., Cl, CO2, H2O, H2S, O2). The parabolic rate law assumes that the concentrations of diffusing species at the oxide/metal and oxide/water interfaces are constant and that the oxide scale is uniform, continuous and of the single phase type [41]. This law is applicable to high temperature engineering problems and is recalled here only for the sake of completeness. The logarithmic and the linear rate laws are more likely to be applicable to Fe0 water filters and are both empirical relationships. It is essential to notice that the corrosion rate (kiron) is not investigated as a function of the amount of individual corrosive species (e.g., Cl, contaminants, H2S), but rather as the extent of iron corrosion as influenced by these and all other operational parameters (flow velocity, system design, temperature). In other words, considering that contaminants are the main corroding agents for Fe0 is alien to corrosion science [10,13,14,25,40,41].

2.2. Corrosion Rate and Extent of Mass Loss

The extent of aqueous Fe0 corrosion under environmental conditions is generally expressed either in terms of [40,41] (i) the change in Fe0 weight (mass loss), (ii) the dimensions of the corroded crevices, (iii) the number and quantity of formed pits or (iv) the amount of corrosion products (e.g., the thickness of the oxide scale; Equations (7)–(9)). Equation (10) expresses the corrosion rate (kiron) in terms of mass loss:
k iron = K × m b   m a A × ρ × t
where kiron (mm/y) is the corrosion rate; mb (g) is the mass before exposure; ma (g) is the mass after exposure; A (mm2) is exposed surface area; t (years) is the exposure time; ρ (g/cm3) is density and K a constant. Expressing the time in years suggests that, to be relevant, experiments should ideally last for several years.
Another conventional way to access kiron uses the Faraday law. Here, kiron is quantified through the relationship between the corrosion current density and the extent of metal dissolution [41,42].

2.3. Oxide Scale Formation and Its Effects on kiron: Modeling Aspects

Equation (10) shows that kiron depends on Δm = mbma, A and t. Δm is related to the amount of corrosion products within the system or the thickness of the oxide scale (x value; Equations (7)–(9)). The time-dependent changes of Δm and A render corrosion processes very complex. Generally, one should consider the following processes [40,41,43]: (i) the Fe0 dissolution (anodic reaction) at the free metal surface; (ii) water reduction (cathodic reaction) at the Fe0 surface; (iii) the precipitation equilibria yielding the oxide scale on the Fe0 surface; (iv) the dissolution of the oxide scale (abiotic and biotic); (v) chemical reactions within the oxide scale (including Equations (3) and (4)); (vi) adsorption, co-precipitation and mass transfer across and within the oxide scale; and (vii) electro-migration (ionic transport) through the oxide-scale. The latter depends on the permeability and the surface charge of the precipitates building the scale [43].
A comprehensive model for the corrosion process should take into account all of these phenomena. Such a model would contain a large number of parameters. Relevant parameters could not be unequivocally determined on the basis of the limited amount of data that is available in the literature. This is an argument for new, holistic and systematic investigations. However, appropriate simplifications could be made. For example, Anderko and Young [44] considered that separate species form on the corroding Fe0 surface in order to derive a mathematical model that represents the effects of scale formation on corrosion rates. The time-dependent change of each Fe0 surface fraction is mathematical expressed. Similarly appropriate assumptions could be made on the reaction orders, the absorption behavior (e.g., Freundlich, Langmuir) and all other relevant aspects [44,45].
The approach conventionally used in the Fe0 water filtration literature [16,19,27,28,29,30] is not derived from Equation (10) and related simplifications. Moreover, the presentation above reveals that chemical reactions yielding contaminants reductive transformation in Fe0/H2O systems (Equations (3) and (4)) are included in just one of seven processes making up the dynamics of oxide scale formation and transformation. For this reason, it would be difficult to find a model really describing an actual Fe0/H2O system within the remediation literature.

3. Metallic Iron for Water Treatment

3.1. Major Characteristics of Fe0 Materials for Water Filters

Reactive Fe0 materials used for water filters are characterized mostly by their size/thickness of less than 5.0 mm [46,47,48,49]. A widely-used Fe0 sample from iPuTech (Rheinfelde, Germany) has a grain size varying from 0.3 to 2.0 mm [16,47]. This diameter represents less than 1/10 of the thickness of the buried cast iron pipes investigated by Mohebbi and Li [50]. The pipe presented pits having widths varying from 13 to 117 mm and depths from 1.6 to 9.1 mm after a service life of 90 years. From the study of Mohebbi and Li [50], an average rate constant (kiron) for a cast iron pipe under service conditions can be derived (Equation (10)), but such kiron values cannot be extrapolated to Fe0 materials for water filters, even when they result from the same cast iron. Many material and application-dependent kiron values can be found in the broad literature [51,52] using Fe0, but none of them can be adopted for Fe0 filters. Relevant fields include metal recovery by the cementation process, which was established in 1890s [53,54]. In the cementation process, metal (e.g., Fe0, Zn0) particles are used in technical devices for some weeks or months and the major (controlled) operating conditions (e.g., high temperatures or low pH values) are not comparable to those of water filters. In particular, high metal ion concentrations warrant the formation of an electronic conductive layer of recovered metals at the Fe0 surface, while in the water filtration industry, a multi-layered, nonconductive oxide scale (“passive” film) is inevitably formed [55], rendering quantitative direct reduction (electrons from Fe0) simply impossible.

3.2. Coping with the Singularity of Fe0 Filters

In order to assess the service life of Fe0 filters, it is imperative to determine corrosion rates (kiron) of relevant Fe0 materials over the long term and to develop models for Fe0 depletion to be correlated with the extent of contaminant removal under operational conditions. Although many studies have been performed to determine the rate constant of the degradation (chemical reduction) of individual contaminants (kcontaminant; based on reactions similar to Equation (1)) (Section 2), little research has been undertaken, which could be used to derive kiron values over longer time scale than days, weeks or a few months. The intention herein is to pave the way to fill the gap regarding the long-term corrosion rate of materials for Fe0 filters in the absence of historical data. Clearly, long-term experiments for the determination of kiron values are urgently needed to assist the development of reliable models to predict the service life of Fe0 filters and/or describe their operation.
It is understood that the kiron value is not an intrinsic property of the material, but depends on several inter-related site-specific parameters. For example, the same material will exhibit different kiron values in reactive zones containing the same amount of Fe0, but having different volumetric Fe0:sand ratios, e.g., 10:90, 25:75 and 50:50. The rationale is that the long-term kinetics of iron corrosion also depends on the pressure within the filter (PH2 in Equation (6)). The initial kiron value (k0iron) could be identical in the three systems, but with increasing service life, systems with higher Fe0 ratios will exhibit lower kiron values. Remember that in designing Fe0 filters, the goal is to work with the material, for which kiron value implies efficient decontamination under the operational conditions (e.g., bed thickness, flow velocity, water chemistry). Clearly, selecting an appropriate material for a given site is not seeking for the most reactive one.

4. Modeling Permeability Loss of Fe0 Filters

4.1. Lessons from Monitored Aquifer Recharge

In many regions of the world, monitored aquifer recharge (MAR) is applied as a tool to (i) overcome the over-exploitation of groundwater or (ii) store excess storm water in the subsurface [56,57]. While injecting water into an aquifer, clogging does often occur, possibly rendering MAR inefficient in the long-term. There are three clogging types: (i) biological clogging due to growing biofilms; (ii) chemical clogging due mostly to precipitation reactions; and (iii) physical clogging caused by suspended solids. In many cases, it has been demonstrated that physical clogging accounts for about 70% of the permeability loss [58].
A particular case of water injection into the aquifer is that of the re-circulation of iron-rich groundwaters. Here, the precipitation of FeII/FeIII mineral phases significantly reduces the porosity of the aquifer system after a certain operation duration. The removal of dissolved iron by several techniques was proven efficient in sustaining MAR operations [59]. In the context of Fe0 filters, dissolved iron generates and precipitates within the system (in situ). Accordingly, dissolved iron cannot be removed, but only properly considered. Thus, the two major lessons from the MAR technology are that: (i) suspended substances should be filtered out; and (ii) the generation, migration and transformation of Fe species should be carefully considered (mass balance, including volumetric expansion).

4.2. Lessons from the Merrill-Crowe Process

The century-old zinc cementation for gold recovery from a pregnant leach liquor (the Merrill-Crowe process) reveals that clarification and deaeration (O2 removal) of the leach liquor are two decisive stages to optimize the efficiency of Fe0 filters. Clarification corresponds to the elimination of suspended substances (Section 4.1) to avoid physical clogging.
In its original version, the cementation process involved the filtration of a gold-bearing cyanide solution through a packed bed of zinc shavings. This operation was proven to have little efficiency because the reaction rate was very slow and the Zn0 surface was soon “passivated”. The problem of passivation was solved by the addition of a lead salt (e.g., Pb(NO3)2). This allowed a Zn0/Pb0 bimetallic system to form at the Zn0 surface (shavings), enabling continued gold cementation (deposition).
Two further improvements were realized later: (i) using zinc dust rather than shavings; and (ii) the deaeration of the gold-bearing solution to O2 levels lower than 1.0 mg L−1. Zn0 dust provided a much larger surface area (“A” in Equation (10)) for gold precipitation (Equation (11)), while the deaeration significantly reduced Zn0 consumption through O2. Clearly, a concurrent reaction for Zn0 consumption is eliminated.
Zn0 + Au2+ ⇒ Zn2+ + Au0
Replacing Zn0 by Fe0, in the context of Fe0 filters, iron corrosion by water (Equation (2)) is the main reaction and corresponds to Equation (11).
It has been established that disturbance through dissolved O2 results from the acceleration of Equation (2) by consumption of FeII species that are the effective reducing agents for O2. Considering permeability loss, Fe0 corrosion in the presence of O2 yields more voluminous FeIII oxides (e.g., Fe2O3, FeOOH) and hydroxides (Table 1). Table 1 summarizes the densities of iron corrosion products and the corresponding coefficient of volumetric expansion. If it is assumed that all oxidized Fe remains in the system (no transport of FeII/FeIII), then it becomes evident that, for a constant volume (initial porosity of a Fe0 filter), the systems with more oxygen will clog early [7,60].
The logical consequence of the presentation above is that the use of O2− poor leach liquors is a prerequisite for efficient Au recovery through Zn0 cementation in packed beds. This process is ultimately known as the Merrill-Crowe precipitation process. Coming back to Fe0 filters, it becomes evident that the analysis of the chemistry of the system would have enabled the proper consideration of the volumetric expansive nature of iron corrosion (Table 1) prompted at the start of the technology some 25 years ago.
The major lesson from the Merrill-Crowe precipitation process for Fe0 filters is that controlling the O2 level is essential for the efficiency of a filter. O2 accelerates corrosion and can be beneficial in some cases. Where necessary, even stronger oxidizing agents can be used [32,61]. However, it should be carefully considered that more corrosion products implies rapid clogging, such that it is certain that long-term permeable systems should operate at low O2 levels.

4.3. Conventional Approach

Conventionally, numerical models are used to predict the long-term behavior of Fe0 filters (see [19] and the references cited therein). Data for such models should be derived from well-designed laboratory column experiments performed under operational conditions (e.g., experimental duration, flow velocity, temperature and water chemistry) mimicking as closely as possible those expected in the field. However, such studies currently provide at best information for understanding the early service life of Fe0 filters (some months). In fact, experiments lasting for more than one year are very scarce [19,62,63], while it is not established that kiron determined under such conditions would describe the behavior of Fe0 filters for 10 or 15 years. Moreover, according to Alamilla et al. [51], it is even not likely that this will be the case because of the well-documented non-linearity of the kinetics of iron corrosion [64] (Section 2).
It has been unambiguously demonstrated that all tools used to accelerate lab-scale experiments collectively impair the reliability of the obtained test results [35,65,66,67]. Relevant tools include adding oxidizing agents to accelerate corrosion [58], increasing flow velocity [34] and using Fe0 of smaller particle sizes and/or rapid small-scale column tests [65]. For the early phase of column operation, methylene blue (MB) discoloration has been proven a powerful indicator of reactivity [68,69,70,71,72,73,74]. Actually, the longest experiment with MB in this context lasted only for 4 months [69]. Accordingly, the suitability of MB discoloration for characterizing the long-term behavior of Fe0 filters is yet to be investigated.
While the reliability of data currently used to model processes in Fe0 filters is questioned, there is evidence that used kiron values are inaccurate. For example, Moraci et al. [19] critically reviewed available approaches and presented a new modeling tool to simulate the permeability loss in Fe0 filters. The presented model takes into account: (i) the volumetric expansive nature of iron corrosion; (ii) the precipitation of foreign species; and (iii) gas formation. However, a look at the used kiron values suggests that there are still misunderstandings to be addressed before acceptable models are presented.

4.4. An Alternative Approach

The process of permeability loss should be investigated at the micro-scale [35]. The size of the Fe0 particles, the volume of the space between individual grains and their modifications with the service life of the filter should be simultaneously considered.

4.4.1. Descriptive Aspects

Spherical Fe0 particles are considered. Each particle has an initial diameter of d0 (t0 = 0). At t > t0, the residual diameter of the particle (non-corroded Fe0) is d. The in situ generated amount of corrosion products corresponds to Δd = d0d. The initial mass of each particle is mp = ρiron × V0 (V0 = π × d03/6) A certain Fe0 mass (m0) is made up of N0 particles, such that m0 = N0 × ρiron × π × d03/6. Assuming uniform corrosion, all N0 particles corrode with the same kinetics (kiron). At each time (t), the mass of non-corroded Fe0 can be determined and the corresponding decrease in diameter (Δd) deduced. The average corrosion rate is given by Equation (12). The best scenario is the one in which Δd is directly measured (in situ).
kiron = Δd/t
The surface area of a Fe0 particle (Ap) with a diameter d is given by Equation (13):
Ap =π × d2
The number of Fe atoms covering Ap can be deduced using Equation (14), while considering that each Fe atom (ratom = 1.24 Å or datom = 2.48 Å) covers an effective area equal to a square (datom2).
NA = Ap/datom2
This reasoning has intentionally ignored the evidence that isolated Fe0 atoms do not exist; instead, each unit cell of Fe0 (BCC) contains two (2) Fe atoms.
One major challenge for the Fe0 filtration technology has been to properly consider the contribution of (volumetric expansive nature of) iron corrosion to permeability loss [16,33,34,35,75]. That is coupling Δd to the diminution of the porosity (Challenge 1). Challenge 1 has been resolved using mass balance equations [7,8,35,76]. For example the porosity loss or the residual porosity can be evaluated for several d values, e.g., d0/2, d0/4, d0/8, d0/16, d0/32, d0/64…, d = 0 at t. The open question (Challenge 2) is how to correlate this spatial porosity loss to the service life of Fe0 filters (temporal porosity loss). Thus, determining kiron is the key to model the operation of Fe0 filters. In the context of Fe0 filters, “permeability loss” and “porosity loss” can be randomly interchanged as permeability loss is mostly mediated by the occupation of the inter-granular pore space (porosity) and, thus, to reduced interconnectivity of available pores (physical clogging). This is the reason why the entrance zone of a filter comparatively experiences increased porosity loss as a rule. This evidence alone makes the discussion of common column parameters like Reynold or Peclet numbers a complex task.

4.4.2. On the Significance of kiron Values

The kiron values used by Moraci et al. [19] as calibration parameters are expressed in mmol kg−1 d−1. According to the references cited by these authors, such expressions are common in the Fe0 literature. Each kiron value should be given in mmol particle−1 d−1. The reason being that all Fe0 particles are corroded by water (H+ or H2O) with the same kinetics. Admittedly, in the entrance zone, dissolved O2 and/or other oxidizing agents, including contaminants (e.g., CuII, CrVI, NO3) and co-solutes (e.g., Ca2+, Cl, NO3), will accelerate iron corrosion and, thus, the extent of permeability/porosity loss. However, permeability loss due to Equation (2) [7,9,33,34,35] is ideally uniform. For example, a kiron value of 30 mmol kg−1 d−1 corresponding to 1680 mg kg−1 d−1 implies a daily dissolution of 1.57 × 10−2 mmol or 0.88 mg of iron from individual spherical particles having a diameter of 1.0 mm (d value). The equations used for calculations are summarized in the previous section, and the results of all kiron values used by Moraci et al. [19] are summarized in Table 2.
Table 2 also summarizes the time to complete material depletion or Fe0 exhaustion (t) for the kiron values used by Moraci et al. [19] assuming uniform corrosion for d = 1.0 mm. It is seen that t varies from 0.2 to 69.1 years. Keeping in mind that subsurface Fe0 reactive walls (Fe0 filters) should have a service life in the range of decades, Table 2 suggests that, for d = 1.0 mm, a material exhibiting a kiron value averaging 4.0 mmol particle−1 d−1 should be used. Such a material would last for 12.22 years (t value). These calculations suggest that in a cross-disciplinary approach, a challenge for material scientists (Challenge 3) would be to manufacture a (possibly porous) spherical material with a 1.0 mm diameter exhibiting an average of 0.12 μg particle−1 d−1. The same reasoning suggests that a material exhausting within one year (t) should have a kiron value of 1.47 μg particle−1 d−1. Such a material could be useful for household water filters [77].
It is understood that solving Challenge 3 will just be the first step in designing Fe0 filters. In fact, the target kiron value (e.g., 4.0 mmol particle−1 d−1) depends on a myriad of operational parameters, including the porosity of the Fe0 materials, the Fe0 ratio in the reactive layer, the nature of the admixing aggregates (e.g., MnO2, pumice, sand, TiO2), the water flow velocity (residence time), the water chemistry (the composition of the electrolyte) and the thickness of the reactive layer. The next section proposes an approach for a systematic investigation yielding suitable materials for Fe0 filters.
Table 3 and Figure 1 summarize the trend of the expected changes in efficiency as a function of d values. It is seen that the number of particles decreases exponentially with increasing d values, while the number of atoms at the surface increases. The objective of this communication is to outline that the law of efficiency change as d0 changes to d in a Fe0 filter is not yet established.

5. Designing Long-Term, Efficient Fe0 Filters

5.1. The Problem

The main problem of the Fe0 filtration technology is the lack of appropriate standard tools to characterize the reactivity of used materials [47,48,49]. In other words, ill-defined materials have been used by various research groups and remediation companies for the past two decades. Accordingly, it is not surprising that only highly qualitative results have been presented. Considering this vacuity, the intention herein is to pave the way for the determination of kiron values useful for modeling purposes. Clearly, while determining kiron values useful for models, experiments should be designed to characterize as much parameters as possible in a systematic approach [77,78]. The major advantage of this approach is that the same set of experiments will generate data enabling the discussion of the appropriateness of current approaches, as well. For example, in a three-contaminant system employing arsenic, fluoride and uranium, the correlation of kiron values to the time-dependent extent of the removal of each contaminant can be properly discussed. In a similar way, repeating the experiments of Luo et al. [34] for the long term will enable the determination of kiron of the same sample in deionized water, groundwater and acid mine drainage (AMD).
In the absence of a reference material, an operational reference can be selected; for example, one of the materials commercialized by iPuTech mbH (Rheinfelde, Germany) and widely used in laboratory and field studies [47,79]. A material scientist solving Challenge 3 would manufacture Fe0 materials to be characterized (kiron values) and compared to the operational reference. Following this approach, available Fe0 materials could be classified according to their kiron values, which are only indirectly correlated to the intrinsic reactivity. It is understood that neither the reference nor one of the individual materials could be the material for all situations. The objective is to come out with various materials exhibiting various kiron values, such that selection to meet site-specificity would be simplified. Section 4.3 suggested for Fe0 materials with a 1.0 mm diameter, kiron = 0.12 μg particle−1 d−1 is suitable for subsurface-reactive Fe0 walls, whereas kiron = 1.47 μg particle−1 d−1 is suitable for household water filters.

5.2. Ways to Reliable kiron Values

A proven tool to determine kiron values is to allow Fe0 materials (initial diameter d0) to corrode under specific conditions and to determine the time-dependent variation of either (i) the residual diameter (d) or (ii) the amount of generated corrosion product (corresponding to Δd = d0d). The latter can be also expressed by the thickness of the oxide scale (x in Equations (7) to (9)). In essence, a good estimation can be realized by just weighing the dried materials at the start (t0) and the end (t) of the experiments (mass balance) [80]. In this approach, Δm = mm0 represents (approximately) the mass of generated corrosion products when the column is flushed by deionized water. Depending on the operational conditions (oxic/anoxic), reliable assumptions can be made on the nature of corrosion products to enable modeling porosity loss. If the system is flushed by other solutions, the mass balance of individual species must be considered. Proper assumptions on all reactions likely to occur in the system and their contribution to changes in porosity must be made.
Recent data have proven that (i) the residual diameter (d), (ii) the amount of generated corrosion products and (iii) the nature of corrosion products can be determined by in situ measurements/observations of both d and changes in the pore diameters [34]. In their excellent work using X-ray computed tomography (RX-CT), Luo et al. [34] used three different model waters: (i) distilled water, (ii) synthetic groundwater and (iii) synthetic AMD. Luo et al. [34] also investigated the impacts of three different Fe0/sand ratios (w/w): 10:90, 50:50 and 100:0. Duplicating the experiments of Luo et al. [34] for longer experimental durations and more applicable experimental set-ups (for water treatment) will certainly allow the determination of reliable kiron values for predictive models. In this effort, a pure Fe0 column (100 % Fe0) could be used just as a tool to shorten the experimental duration or as a negative reference. For long-term basic experiments, a volumetric Fe0:aggregate ratio of 25:75 should be used. Such experiments should not be stopped because contaminant breakthrough has occurred. In fact, the focus herein is on the efficiency of tested Fe0 materials [69,71,72] and possibly characterizing the time to Fe0 exhaustion (t). There is certainly an infinity of possibilities of experimental designs; the present effort will be limited to two approaches: (i) the sampling-port approach (in one column); (ii) the column-in-series approach.

5.2.1. The Sampling-Port Approach

Experiments could be performed with a single column (ID = 5.0 cm, L > 50 cm) having a reactive zone (Fe0-bearing) of 50 cm and equipped with five (5) sampling ports S1, S2, S3, S4 and S5 at 10, 20, 30, 40 and 50 cm from the inlet, respectively (Figure 2). The influent solution is pumped upwards from a reservoir and at pre-defined time intervals. Effluents from each sample port are analyzed for pH value, dissolved iron, dissolved oxygen and concentrations of contaminants and co-solutes (e.g., Ca2+, Cl, HCO3, H2PO4, SO42). In addition to aqueous analysis, time-dependent changes of the morphology of Fe0 and the pore structure should be documented by RX-CT, for example at the following distances from the inlet: 5 (S'1), 15 (S'2), 25 (S'3), 35 (S'4) and 45 cm (S'5) of the reactive zone.
This approach enables a reliable characterization of processes implying the well-documented increased porosity loss in the entrance zone of the Fe0 filters (e.g., at S1 vs. higher Si stations) and how it is influenced by the presence of oxidizing agents (e.g., CrVI, dissolved O2) in the influent solution. Moreover, by individually varying the influent O2 concentration and other oxidizing agents, while monitoring its profile in the whole column (S1 through S5), a better discussion of its impact on the porosity loss is realized. The last important feature from this experimental approach is that, before O2 breakthrough at S4, the porosity loss at S’5 is attributed solely to corrosion through water (Equation (1)) under the experimental conditions (anoxic conditions). Accordingly, by purposefully varying the composition of influent solution, the impact of relevant operational parameters (e.g., Cl, HCO3, SO42) on the extent of porosity loss through water can be characterized.
In the absence of RX-CT, or complementary to this tool, other approaches for monitoring changes of the water flow velocity at individual sample ports can be used. The reduction of the pore size is then deduced from the Darcy equation. At the end of the experiments (at least two years), the column is dismantled after the last RX-CT analysis, and the non-corroded Fe0 materials and the corrosion products are characterized by various analytical tools, including selective extraction. This effort characterizes the changes of the following parameters as a function of the distance from the inlet: (i) the extent of Fe0 depletion (e.g., in %); (ii) the average size of non-corroded Fe0; (iii) the nature, the abundance and the reactivity of individual corrosion products; and (iv) the extent of the reduction of pore sizes.

5.2.2. The Column-In-Series Approach

The sample-port approach requires some sophisticated equipment, including the column and the pump. For less equipped laboratories (e.g., in the developing world), this could be prohibitively expensive. For these situations, small research units could be made up of five shorter columns (e.g., ID = 5.0 cm; L = 30 cm) in series (Figure 3). Individual columns are mostly filled with sand and contain a 10 cm-thick reactive layer. In this embodiment, each column corresponds roughly to 10 cm of the sample-port approach (Figure 2). The larger sand mass between the reactive layers enables the characterization of the impact of in situ-coated sand on the filter’s efficiency. For Columns 1 through 4, the effluent from one column is routed to the next through a tubing system comprising a sampling station/valve (Figure 3).
The results are exploited similarly as for the sample-port approach, the main objective being to determine the long-term kinetics of iron corrosion (kiron). In this approach the system can be gravity fed. For example, it can be daily fed by 1000 mL of a model solution. For both approaches, the level of dissolved O2 in the influent solution can be regulated by pre-filters: a relevant pre-filtration system is a slow sand filter (SSF) in which O2 is consumed within a biofilm [81]. However, working with an SSF implies a low water flow velocity. Alternative approaches to decrease/lower the O2 level include using a sacrificial Fe0 column containing up to 10 vol% Fe0 possibly of a smaller particle size. In fact, Fe0 is a well-documented O2 scavenger that is used in food packaging [82,83].

5.3. The Significance of the Short-Term Kinetics of Fe0 Corrosion

The effort herein is to prepare the way for the determination of kiron values of crucial importance for modeling scenarios to design long-term, efficient Fe0 filters. Before being efficient for the long term, however, Fe0 filters have to be pre-conditioned in a “maturation” phase. Data from Kowalski and Sogaard [84] suggest that in their case, this maturation phase has lasted for six months. In the subsurface context, this means that the filtration system must contain short-term, efficient materials to assure contaminant removal in the initial service life of Fe0 filters. Examples are adsorbents or more reactive Fe0 materials, possibly with smaller particle sizes. The presentation above demonstrates that the short-term rate constants of Fe0 corrosion (k0iron) have been mistakenly used to interpret results and/or to predict the behavior of long-term experiments. According to Alamilla et al. [51], the function describing the instantaneous rate of iron corrosion is expressed as follows:
v(t) = kiron + (k0iron - kiron) × exp(−q0 × t)
where q0 is a constant, k0iron is the short-term and kiron the long-term Fe0 average corrosion rate. It can be seen that the instantaneous rate drops exponentially from k0iron to kiron (k0iron > kiron).
The real significance of k0iron values for subsurface Fe0 filters is that materials should be selected such that after the initial rapid corrosion, the permeability of the reactive zone is still superior to that of the surrounding areas. If this condition is not satisfied, preferential flow would render the filter useless before the long-term corrosion rate (kiron) is established.
While the short-term corrosion rate (k0iron value) is to be properly considered in designing subsurface Fe0 filters, it could be sufficient to design some filters for the treatment of wastewaters from various sources (agriculture, industry, mine, residential area). Here, filters may be designed to operate just for some days to weeks, and material “regeneration” consists of just letting “used” materials be “activated” by humidity and air O2 for a certain time before being re-used. k0iron values would be also sufficient to design several decontamination options using Fe0 particles in batch or fluidized column systems. In this context, the system efficiency can be purposefully enhanced by using more or less powerful oxidizing agents [10,61], because bed clogging is not an important issue. All that is needed is increased Fe0 corrosion to generate more contaminant scavengers [11,85,86]. k0iron values are also sufficient to design cementation beds for metal ion recovery.

6. Discussion

6.1. Contaminant Removal in Fe0/H2O Systems

The reliance of modelers on direct reduction by Fe0 (electrons from the core metal) is not only of concern for modeling the long-term permeability of Fe0 filters [3,87,88]. It strongly masks the real mechanisms of contaminant removal as that is a complex interplay between Fe0 particles, FeII released into solution and FeII/FeIII precipitation [89,90,91,92,93,94,95,96]. In particular, the transformation of Fe0 to Fe oxides goes through colloids and hydroxides. The transformation “colloids to hydroxides” is accompanied by contaminants enmeshment (co-precipitation). In fact, whether they are reduced or not, contaminants are removed by adsorption, co-precipitation and size exclusion. On the other hand, regarding the abundance of (partly nascent) adsorbing sites and continuous generation of FeII species, contaminant chemical reduction by so-called structural FeII (adsorbed FeII) is favored [96]. The abundance of FeII/FeIII hydroxides/oxides in Fe0/H2O systems has been experimentally demonstrated by [92]. However, the authors have suggested adsorptive removal as an important removal mechanism accompanying direct reduction, which is in contradiction to the mechanisms presented in Section 2. Accordingly, coming models for Fe0/H2O systems should be adjusted to address the main contaminant removal pathways.

6.2. The Shortcomings of Current Modeling Efforts

An overview of the Fe0 filtration literature reveals conflicting information regarding the causes of permeability loss [7,75]. There is always a discrepancy between the observed and the predicted porosity loss; the actual porosity loss being higher than that predicted [75]. Two examples for illustration: (i) Mackenzie et al. [82] measured a 5 to 10% porosity loss using tracer tests, while calculations based on mineral precipitation predicted only 1 %; and (ii) Kamolpornwijit and Liang [97] measured porosity losses of 25 to 30% based on tracer tests and attributed 1.3% to trapped gas. Mackenzie et al. [82] attributed the remaining porosity loss (up to 9%) to H2 gas production. Henderson and Demond [75] realized that available models for Fe0 filters [98,99,100] do not account for the effects of H2 on permeability loss. In a series of carefully-designed experiments, Henderson and Demond [75] could validate their working hypothesis that the majority of porosity loss is not attributable to precipitates, but to gas.
The problem with the data of Henderson and Demond [75] is that they have not considered that each individual Fe0 atom corrodes and produces both volumetric expansive precipitates and H2 gas [35]. Moreover, the pore filling by Fe precipitates was evaluated using tabulated molar volume values (ν = 7.6 cm3 mol−1 for Fe0), which are not necessarily relevant for Fe0 particles confined in a packed bed (Fe0 filter). For example, the coefficient of volumetric expansion (η = Voxide/Viron) for magnetite (Fe3O4; ν = 45.0 cm3 mol−1) using ν values is 5.0, while the η value for confined system is close to 2.2 [60]. This combined with the lack of appropriate kiron values has diminished the value of the models presented.

6.3. The True Value of Mathematical Modeling

Mathematical modeling constitutes the third pillar of science and engineering, achieving the fulfilment of the two more traditional disciplines: (i) theoretical analysis; and (ii) experimentation [101]. Mathematical models explore new solutions in a very short time period. This increases the speed of innovation cycles. However, this is only possible when theoretical analysis and experimentation are perfectly performed. The presentation herein has recalled that for Fe0 filters, both theoretical analysis [102,103] and experimentation [104] have been unsatisfactory. This suggests that there is a huge gap between calculations and understanding [105]. Admittedly, all modelers are not chemists nor electrochemists, but even in the absence of a real cross-disciplinary approach, self-critical scientists should have realized that something fundamental is missing. Moreover, consultations with material and corrosion engineers would have been necessary in the fitness of things to save millions of money (mostly from tax payer) spent in intensive research on a biased basis. The damage is huge, as the credibility of modeling could be questioned [105]. This communication advocates for saving the credibility of mathematical modeling through the generation of credible data for Fe0 filters.
The true value of mathematical models was recalled by Grauer [106] by the following wording: “theory and models cannot be validated in the strict sense but only refuted“. The presentation herein has collectively refuted all modeling efforts regarding the design and operation of Fe0 filters for the past two decades. The reason is the very poor theoretical analysis. The equation currently used for kiron (corresponding to Equation (1)) is simply wrong, and the reductive transformation of contaminants is at best a side process (Equations (3) and (4)) (Section 2).
Better models are possible, they should be based on a systematic analysis of the Fe0/H2O system. A sound analysis [102,103] has demonstrated that contaminants are removed by adsorption, co-precipitation and size exclusion. Accordingly, chemical reduction when it occurs is not responsible for (quantitative) contaminant removal and is rather a side reaction occurring within the oxide scale in the vicinity of Fe0 and not at its surface. The evidence that the surface of Fe0 and oxides changes with time and the Fe0 surface is not accessible to the contaminant question of the normalization of rate constants to the surface area [107]. Lastly, kiron values are the pillar for modeling the temporal realization of permeability loss. These values are yet to be determined in well-designed long-term experiments.

6.4. Messages to Anonymous Collaborators

There is evidence in the Fe0 literature that the aspects challenged herein are difficult to accept [108,109,110,111,112]. However, this argumentation corresponds to mainstream science (chemical thermodynamics). The first message to an anonymous collaborator (a reader) is “no single reference is a quality guarantee”. Accordingly, sound scientific arguments should justify each reference. Moreover, the rationale for preferring a work to another should be known and named, if applicable.
The second message is for a reviewer either for a submitted manuscript or a grant proposal. An author/applicant is a colleague and needs collegial remarks to improve his/her manuscript/proposal. A minimal requirement is that reviewer comments focus on points that need improvements or are unacceptable [113,114,115].
The third message is to the attention of funding agencies. Each applicant should have the opportunity to write some comments on the reviewer's evaluation before the final decision is made. This is of particular importance when the majority of available comments is negative. Admittedly, this could/would lengthen the review process, but this is the way to greater fairness. This procedure is already adopted by some agencies, but should be universally adopted. The reason is that the best evaluator could not recognize an innovation at first glance.
The fourth and last message is for everyone. Research on water treatment and environmental remediation has been wrongly directed from the beginning onward. Warnings from chemists [116,117,118,119] were simply ignored. Whenever a mistake is identified, starting on a new basis is always a good decision. Individual researchers already went down this path [10,119]. As an example, the author of this communication has published on reductive precipitation of UVI by Fe0 [120], then on reduction as a removal mechanism, until 2010 [14], only with [121] and hints from anonymous reviewers did he realize that at concentrations relevant for safe drinking water, reduction cannot be a stand-alone removal mechanism for any contaminant [78,122]. For environmental remediation, chemical reduction (degradation) may be sufficient when reaction products are readily degradable, for instance when nitrobenzene is quantitatively reduced to aniline. For safe drinking water provision, even reduction products (here, aniline) must be removed [123,124,125,126].

7. Concluding Remarks

Iron corrosion is a stochastic, probabilistic phenomenon that requires interdisciplinary concepts, including chemistry, electrochemistry, hydrodynamics, materials science, metallurgy, physics and surface science. From a pure chemical perspective, the thermodynamics and kinetics of the involved processes must be understood in order to effectively design and fabricate materials to be used for optimal (efficient and affordable) applications. This communication has recalled that the chemistry of the Fe0/H2O system is being incompletely considered while using Fe0 as a remediation material. It is particularly disappointing/frustrating that the principles of corrosion as already understood and largely disseminated in the broad scientific literature have been simply ignored. The net result is that a fictive reaction (Equation (1)) has been used for dimensioning Fe0 filters for more than two decades (25 years).
This communication has also recalled that mathematical modeling is the third and only the third pillar of science and technology. The two first pillars are theoretical analysis (system analysis) and experimentation. The best model will not correct mistakes in system analysis or experimentation. It is clear that Fe0 filtration technology requires more accurate models that take into account the various mechanisms that underpin the process. The year-long experimentation on iron corrosion (prior to the advent of Fe0 filters) has demonstrated that uniform corrosion assumed by almost all models is an over-simplification. In other words, even considering reliable values of kiron will only describe how Fe0 filters would behave considering the assumptions made (without biotic processes). This evidence confirms/suggests that (independent, where necessary) monitoring of the performance of Fe0 filters is mandatory.
To conclude, Rolf Grauer will be paraphrased as follows: It would make more sense to devote more time and energy to determine kiron values than to develop sophisticated, but unreliable numerical models. It is clearly understood that no particular Fe0 material is a universal solution for all contaminations. Each and every case has to be considered in its totality before a decision is made on the proper material, characterized by its kiron value. Therefore, a sort of database for kiron values is needed. Establishing such a database is a scientific challenge and not just laborious work.

Acknowledgments

Arnaud Igor Ndé-Tchoupé (Faculty of Sciences, University of Douala/Cameroon), Günther Meinrath (RER Consultants, Passau/Germany), Hans Rupprt (Department of Sedimentology & Environmental Geology, University of Göttingen), Hezron T. Mwakabona (Department of Physical Sciences, Sokoine University of Agriculture, Morogoro/Tanzania) and Mohammad Azizur Rahman (ISU, Leibniz University, Hannover/Germany) are thanked for their valuable advice. The manuscript was further improved by the insightful comments of anonymous reviewers from Water. The author acknowledges support by the German Research Foundation and the Open Access Publication Funds of the Göttingen University.

Conflicts of Interest

The author declares no conflict of interest.

Abbreviations

The following abbreviations are used in this manuscript:
AMD
acid mine drainage
ID
internal diameter
L
length (of the column)
MAR
monitored aquifer recharge
RX-CT
X-ray computed tomography
SSF
slow sand filter

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Figure 1. Changes of the number of particles (N0) making up 1 kg of Fe0 and the corresponding number of atoms at the surface (NA) as a function of the d values. While the N0 values exponentially decrease with increasing d, the NA values increase.
Figure 1. Changes of the number of particles (N0) making up 1 kg of Fe0 and the corresponding number of atoms at the surface (NA) as a function of the d values. While the N0 values exponentially decrease with increasing d, the NA values increase.
Water 08 00162 g001
Figure 2. Side view of a single Fe0/sand water filter comprising five sampling ports. To optimize the efficiency of the filtration unit, the effluent should be clarified and deaerated before being introduced into the first column. A simple device for clarification and deaeration is a slow sand filter [78].
Figure 2. Side view of a single Fe0/sand water filter comprising five sampling ports. To optimize the efficiency of the filtration unit, the effluent should be clarified and deaerated before being introduced into the first column. A simple device for clarification and deaeration is a slow sand filter [78].
Water 08 00162 g002
Figure 3. Side view of a series of the Fe0/sand water filter comprising five individual columns and sampling valves. To optimize the efficiency of the filtration unit, the effluent should be clarified and deaerated before being introduced into the first column. A simple device for clarification and deaeration is a slow sand filter [78].
Figure 3. Side view of a series of the Fe0/sand water filter comprising five individual columns and sampling valves. To optimize the efficiency of the filtration unit, the effluent should be clarified and deaerated before being introduced into the first column. A simple device for clarification and deaeration is a slow sand filter [78].
Water 08 00162 g003
Table 1. Theoretical ratios (η values) between the volume of expansive corrosion products (Voxide) and the volume of iron consumed during the corrosion process (VFe). η values are compiled by Caré et al. [60]. The ratios of ρ values (densities) indicate that corrosion products are 1.5 to 2.2 times larger in volume than the parent Fe0.
Table 1. Theoretical ratios (η values) between the volume of expansive corrosion products (Voxide) and the volume of iron consumed during the corrosion process (VFe). η values are compiled by Caré et al. [60]. The ratios of ρ values (densities) indicate that corrosion products are 1.5 to 2.2 times larger in volume than the parent Fe0.
SpeciesFormulaρ (kg m−3)ρiron/ρoxideVoxide/Viron
IronFe7800
HematiteFe2O352601.52.12
MagnetiteFe3O451801.52.08
Goethiteα-FeOOH42601.82.91
Akageneiteβ-FeOOH35602.23.48
Lepidocrociteγ-FeOOH40901.93.03
Table 2. Values of kiron used by Moraci et al. [19] and the corresponding t values. Calculations are made for d = 1.0 mm and m = 1 kg.
Table 2. Values of kiron used by Moraci et al. [19] and the corresponding t values. Calculations are made for d = 1.0 mm and m = 1 kg.
kiron (mmol kg−1 d−1)kiron (mg kg−1 d−1)kiron (μg particle−1 d−1)t (years)
0.7390.0269.8
1.2670.0440.7
1.5840.0432.6
4.02240.1212.2
7.03920.217.0
10.05600.294.9
12.06720.354.1
15.08400.443.3
21.011760.622.3
30.016800.881.6
170.095204.990.3
200.011,2005.870.2
242.013,5527.100.2
300.016,8008.800.2
Table 3. Values of the number of particles (N0) making up 1 kg of Fe0 as a function of the d values. The corresponding particle area (Ap) and the number of atoms at the surface (NA) are specified.
Table 3. Values of the number of particles (N0) making up 1 kg of Fe0 as a function of the d values. The corresponding particle area (Ap) and the number of atoms at the surface (NA) are specified.
d (mm)N0Ap (m²)NANA (μmol)
0.051.53 × 10107.86 × 1075.1 × 10138.48 × 10−5
0.084.53 × 1091.77 × 10−61.1 × 10141.91 × 10−4
0.139.77 × 1084.91 × 10−63.2 × 10145.30 × 10−4
0.251.22 × 1081.96 × 10−51.3 × 10152.12 × 10−3
0.501.53 × 1077.86 × 10−55.1 × 10158.48 × 10−3
0.754.53 × 1061.77 × 10−41.1 × 10161.91 × 10−2
1.001.91 × 1063.14 × 10−42.0 × 10153.39 × 10−2
1.259.77 × 1054.91 × 10−43.2 × 10155.30 × 10−2
1.505.66 × 1057.07 × 10−44.6 × 10157.64 × 10−2
1.753.56 × 1059.63 × 10−46.3 × 10151.04 × 10−1
2.002.39 × 1051.26 × 10−38.2 × 10151.36 × 10−1
2.251.68 × 1051.59 × 10−31.0 × 10151.72 × 10−1
2.501.22 × 1051.96 × 10−31.3 × 10152.12 × 10−1
2.759.18 × 1042.38 × 10−31.5 × 10152.57 × 10−1
3.007.07 × 1042.83 × 10−31.8 × 10153.05 × 10−1

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Noubactep, C. Predicting the Hydraulic Conductivity of Metallic Iron Filters: Modeling Gone Astray. Water 2016, 8, 162. https://doi.org/10.3390/w8040162

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