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Original Research ARTICLE

Front. Energy Res., 01 September 2015 | https://doi.org/10.3389/fenrg.2015.00037

Radioactive Cs in the severely contaminated soils near the Fukushima Daiichi nuclear power plant

imageMakoto Kaneko1, imageHajime Iwata1, imageHiroyuki Shiotsu1, imageShota Masaki1, imageYuji Kawamoto1, imageShinya Yamasaki1, imageYuki Nakamatsu1, imageJunpei Imoto1, imageGenki Furuki1, imageAsumi Ochiai1, imageKenji Nanba2, imageToshihiko Ohnuki3, imageRodney C. Ewing4 and imageSatoshi Utsunomiya1*
  • 1Department of Chemistry, Kyushu University, Fukuoka, Japan
  • 2Department of Environmental Management, Faculty of Symbiotic System Science, Fukushima University, Fukushima, Japan
  • 3Advanced Science Research Center Japan Atomic Energy Agency, Tokai, Japan
  • 4Department of Geological Sciences, Center for International Security and Cooperation, Stanford University, Stanford, CA, USA

Radioactive Cs isotopes (137Cs, t1/2 = 30.07 years and 134Cs, t1/2 = 2.062 years) occur in severely contaminated soils within a few kilometer of the Fukushima Daiichi nuclear power plant at concentrations that range from 4 × 105 to 5 × 107 Bq/kg. In order to understand the mobility of Cs in these soils, both bulk and submicron-sized particles elutriated from four surface soils have been investigated using a variety of analytical techniques, including powder X-ray diffraction analysis, scanning electron microscopy (SEM), transmission electron microscopy (TEM), and analysis of the amount of radioactivity in sequential chemical extractions. Major minerals in bulk soil samples were quartz, feldspar, and minor clays. The submicron-sized particles elutriated from the same soil consist mainly of mica, vermiculite, and smectite and occasional gibbsite. Autoradiography in conjunction with SEM analysis confirmed the association of radioactive Cs mainly with the submicron-sized particles. Up to ~3 MBq/kg of 137Cs are associated with the colloidal size fraction (<1 μm), which accounts for ~78% of the total radioactivity. Sequential extraction of the bulk sample revealed that most Cs was retained in the residual fraction, confirming the high binding affinity of Cs to clays, aluminosilicate sheet structures. The chemistry of the fraction containing submicron-sized particles from the same bulk sample showed a similar distribution to that of the bulk sample, again confirming that the Cs is predominantly adsorbed onto submicron-sized sheet aluminosilicates, even in the bulk soil samples. Despite the very small particle size, aggregation of the particles prevents migration in the vertical direction, resulting in the retention of >98% of Cs within top ~5 cm of the soil. These results suggest that the mobility of the aggregates of submicron-sized sheet aluminosilicate in the surface environment is a key factor controlling the current Cs migration in Fukushima.

Introduction

Four years have passed since the Fukushima Daiichi nuclear power plant (FDNPP) event released ~520 PBq of radionuclides (Steinhauser et al., 2014) in the vicinity of FDNPP. An elongated area some ~27 miles in length and ~7 miles wide to the northwest of FDNPP is still contaminated with radioactivity, mainly 134Cs and 137Cs, with half-lives of 2.06 and 30.07 years, respectively. A recent study reported an ~40% decrease of radioactivity in this area (MEXT, 2013), which is greater than the decrease (~21%) that is expected from the decay constants for Cs, especially 134Cs. A number of studies have reported geochemical behavior of Cs in the contaminated area [e.g., Koarashi et al. (2012) and Yoshida and Takahashi (2012)] in order to understand the distribution and migration of radioactive Cs in the future. After the Cs release to atmosphere, most Cs aerosols were deposited by precipitation on March 15 (wet deposition), which continued through March 16th (Kinoshita et al., 2011; Kaneyasu et al., 2012; Morino et al., 2013) based on the chemical transport model, which were in good agreement with the actual Cs distribution. In the contaminated Fukushima soils, the Cs remains within the top ~5 cm of the soil profile, strongly bound to clay minerals, probably vermiculite, and illite (Tanaka et al., 2012a). On the other hand, another study reported that other mineral component were also associated with irreversibly bound radioactive Cs, based on results obtained by chemical extraction and subsequent X-ray diffraction (XRD) analysis (Kozai et al., 2012; Ohnuki and Kozai, 2013). In addition, the presence of organic matter in soils may prevent the Cs adsorption onto mineral surfaces (Matsunaga et al., 2013).

Mukai et al. (2014) recently conducted transmission electron microscopy (TEM) analysis of Fukushima soils and showed that most particles associated with radioactive Cs are aggregates of clays and other phases, such as organic matter. This aggregation makes it difficult to characterize the submicron phases associated with Cs or to estimate their contribution to the total Cs radioactivity. It is well-known that submicron-sized particles behave as colloids in surface and subsurface aquifers (McCarthy and Zachara, 1989); thus, these colloids can potentially control the migration of trace radionuclides. Hence, we have completed a detailed analysis of the colloid sized and smaller fraction of the soils. Although the previous studies reported a high affinity of Cs with clay minerals in the Fukushima surface environments (Tanaka et al., 2012a,b; Matsunaga et al., 2013; Nakao et al., 2014), the role of fine particles <1 μm has not been quantitatively determined, which is presumably the size fraction dominated by clay minerals. Finally, the severely contaminated area close to FDNPP is not easily accessible, and thus, fewer data have been reported for the soil from this area as compared with data recently reported for the samples more than several kilometers from the FDNPP. The present study investigated that the soil particles collected within a few kilometer of FDNPP utilizing a variety of analytical techniques including conventional sequential extraction methods and electron microscopy in order to describe the mineralogy, identify the Cs speciation, and determine the dose contribution from Cs sorbed onto submicron-sized particles.

Materials and Methods

Sample Description

Samples were collected on March 15–16, 2012. The localities of the sample sites are shown in Figure 1. Four soil samples were collected in the highly contaminated area in Ohkuma within 5 km of the FDNPP: two samples from the east and west zones of the Ottozawa district and the other two samples from east and west zones of the Koirino district. Hereafter, these samples are identified as OTO-E, OTO-W, KOI-E, and KOI-W, respectively. The collected samples were dried and sieved with a 2-mm polyethylene mesh filter to remove pebbles and plant material, such as grass.

FIGURE 1
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Figure 1. Map of dose at 1 m above the ground. Data from Ministry of Education, Culture, Sports, Science and Technology, Japan (MEXT, 2013). (A) Prediction of the accumulated dose during 1 year; 3/11/2011–2/11/2012. (B) Sampling location collected in March 2012.

A soil sample core (30 cm in length × 55 mm in diameter) was also collected from KOI-E, using a DAIKI core sampler, DIK-110C. The core was initially used to obtain the vertical cross-sectional autoradiography in order to image the distribution of radionuclides as a function of depth. Then, the outermost part of this cylindrical core was carefully shaved off to exclude the contamination from the core boring process. The depth profile of 134Cs and 137Cs radioactivities was made at 1 cm intervals for the core. The core sample was divided into 12 fractions by the depth: 0–1, 1–2, 2–3, 3–4, 4–5, 5–6, 6–7, 7–8, 8–9, 9–10, 10–13, and 13–16 cm.

Analytical Methods

Size Fractionation

The size-dependent 134,137Cs activity was determined for three samples: OTO-E, OTO-W, and KOI-E. The size separation was performed with a sequence of size fractions: >597, 114–597, 48–114, 1–48, and <1 μm. The soil was suspended in ultra-pure water (milli-Q) and ultrasonicated for 15 min and filtered first with a 597 μm mesh. The residue was re-suspended in pure water, ultrasonicated, and filtered using a 114-μm mesh. The size ranges, >597, 114–597 and 48–114 μm, were obtained in the same manner. The soil particles <1 μm were separated from the <48 μm fraction by a sedimentation method, in which the hydrodynamic size was calculated based on the Stokes’ law. The separated soils were air dried and weighed prior to further analysis. For the KOI-E sample, the size-fractionated samples for the >597, 114–597, and 48–114 μm fractions were subsequently ultrasonicated twice for 30 min in order to separate fine particles that were attached to large-sized particles and to quantify the actual contribution of the fine particles to the total radioactivity.

Sequential Extraction of Radioactive Cs from Soils

Sequential extraction was performed for OTO-E, OTO-W, and KOI-E samples. The extraction method was based on Hou et al. (2003), which is a modified procedure after Tessier et al. (1979). Using this method, the chemical form of the Cs associated with soils is separated into six chemical categories: water soluble (F1), exchangeable (F2), bound to carbonate (F3), bound to metal oxide (F4), bound to organic matter (F5), and the residue (F6). Although the details of the extraction procedure were described in Hou et al. (2003), the procedure performed in the present study is briefly summarized as follows; first, pure water was added to 5 or 10 g soil and the suspension was continuously agitated for 24 h at room temperature. Then, the solution was centrifuged at 5000 rpm for 10 min, and the supernatant was filtered with 0.025 μm membrane filter. The filtrate was classified as water-soluble fraction (F1). The residue (residue-1) obtained by the filtering was re-suspended in 1.0M NH4OAc (pH 8.0) and agitated for 24 h at room temperature. After the treatment, the suspension was centrifuged and filtered. The residue (residue-2) was rinsed with pure water and the rinsing water was added to the leachate. The filtrate was labeled as exchangeable (F2). Subsequently, the residue-2 was re-suspended in 1.0M NH4OAc (pH 5.0) and agitated for 24 h at room temperature. The suspension was centrifuged and filtered. The residue (residue-3) was rinsed with pure water. The filtrate was labeled as the form bound to carbonate (F3). For the form bound to metal oxides (F4), 0.04M NH2OH⋅HCl in 25% (v/v) HOAc at final pH of 2.0 was added to the residue-3, and the suspension was agitated for 24 h at 95 ± 5°C. After cooling to room temperature, the suspension was centrifuged and filtered. The residue (residue-4) was rinsed with pure water. For the form bound to organic matter (F5), 30% H2O2–HNO3 at pH 2.0 was added to the residue-4, and the suspension was agitated for 2 h at 95 ± 5°C. After cooling to room temperature, the suspension was centrifuged and filtered. This extraction procedure with peroxide and nitric acid was repeated twice. Subsequently, 3.2M NH4OAc–20% HNO3 at pH of 2.0 was added to the residue (residue-5a), and the suspension was agitated for 1 h at room temperature. The suspension was centrifuged and filtered. The residue (residue-5b) was rinsed with pure water. Insoluble residue (F6) was calculated by subtracting the sum of the radioactivities of F1–F5 from the total radioactivity.

Powder X-Ray Diffraction Analysis

Major mineral phases in the soils were determined by powder XRD (Rigaku MultiFlex) with Cu target and reflected beam monochromator. Measurement was conducted for the scan range of 3°–63° with the scanning speed of 1°/min of 2θ and the step angle of 0.02° for bulk soil sample and elutriated soil sample (<1 μm). In order to obtain the detailed structural information, the elutriated samples were measured for the focused angle ranging 3°–13° at the scan rate of 0.125° or 0.25°/min of 2θ with the step angle of 0.02°. In addition, ethylene glycol treatment was also tested for the elutriated sample for the range of 3°13° at the scan rate of 0.125° or 0.25° min−1 of 2θ with the step angle of 0.02°.

Micro-Scale Analysis

Individual particle analysis of the soil samples was performed using a scanning electron microscopy (SEM, SHIMADZU SS-550) equipped with energy dispersive X-ray spectroscopy (EDX). Secondary electron (SE) imaging was conducted at 5 kV of the acceleration voltage, and the EDX point analysis and mapping were completed at 25 kV. SEM wave-length dispersive X-ray spectroscopy (SEM-WDX, Hitachi High-Technologies) was also employed for searching the Cs peak in soil samples. The operating condition was 20 kV of the acceleration voltage and 37.6 nA of the beam current. The measurement was conducted in the range of 4213–4359 eV at the scan speed of 1 or 2 eV/ch. All samples were coated with carbon using a carbon coater (SANYU SC-701C) to make conductivity.

High-resolution TEM (HRTEM), with EDX, and high-angle annular dark-field scanning electron microscopy (HAADF-STEM) were performed using JEOL ARM200F with the acceleration voltage of 200 kV. The JEOL Analysis Station software was used to control the STEM-EDX mapping. To minimize the effect of sample drift, a drift-correction mode was used in the acquisition of the elemental map. The STEM probe size was ~1.0 nm. The collection angle of the HAADF detector was ~50–110 mrad. The condenser aperture was 20 μm in diameter. TEM specimens were prepared by dispersing the sample on the holey-carbon thin film supported by a Cu mesh grid.

Cs Radioactivity Measurement

The134,137Cs radioactivities were measured using a gamma spectrometer equipped with a low background type Ge detector (EG&G ORTEC Ltd GMX, relative efficiency 55.4%) housed in the radioisotope center of Kyushu University. A spectrum analyzing software (SEIKO EG&G Ltd. Gamma Studio) was used to determine specific isotope contributions to the radioactivity.

Results and Discussion

Distribution of Cs Radioactivity in the Soil Profile

Radioactivities of 134Cs and 137Cs in the soil samples are summarized in Table 1. All samples revealed both 134Cs and 137Cs activities >100,000 Bq/kg, confirming the severe contamination. In particular, 2.66 × 107 Bq/kg of 137Cs was detected in KOI-W sample due to the Cs accumulation beneath a rainwater pipe. Radioactivities of the other soil samples are of a similar order of magnitude, for samples collected from the open fields.

TABLE 1
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Table 1. 134Cs and 137Cs radioactivities of the four bulk soils.

Figure 2A shows the cross-sectional autoradiograph image of KOI-E sample. It is evident that most of the radioactive Cs is concentrated in the top ~4 cm. Slightly elevated contrast along the outer-edge facing toward the plastic tube is a result of contamination from the surface soil during the coring process. There are some hot particles (appearing as red colored spots) near surface, indicating that some particles possesses relatively higher radioactivity among the other soil components.

FIGURE 2
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Figure 2. Vertical distribution of Cs in the KOI-E core sample. (A) Autoradigraphy image of cross section of the core sample. (B) 134Cs and 137Cs radioactivity in the soil core sample. The surface of the core along the plastic liner tube was carefully decontaminated. (C) The enlarged figure of (B). (D) The radioactivity ratio of 134Cs and 137Cs for the vertical profile.

Figures 2B–D shows the Cs radioactivities in the KOI-E core sample and the activity ratio of 134Cs/137Cs as a function of depth from the soil surface. The Cs contamination on the side surface of the core derived from the coring process was removed. A large fraction of the radioactive Cs is retained at the top of the profile (Figure 2A); 137Cs radioactivity in the 0–5 cm interval accounts for more than 98% of the total 137Cs radioactivity. These data suggest that Cs has not migrated to deeper parts of the soil profile, even 1 year after the accident. Retention of Cs in upper soil is consistent with previous studies reporting results for other Fukushima soils collected 1 month after the accident (Kato et al., 2012; Tanaka et al., 2012a). The 134Cs/137Cs activity ratios in the depth profile are almost constant, ranging 0.8–0.9 (Figure 2D), which is also consistent with the results of Kinoshita et al. (2011).

Size Fraction of Cs Radioactivity in the Soils

In order to investigate the particle size dependence of Cs radioactivity, three soils (OTO-E, OTO-W, and KOI-E) were separated into five fractions, 597 μm–2 mm, 114–597, 48–114, 1–48, and <1 μm by a filtering or sedimentation method. The size-fractionated 137Cs radioactivity revealed that relatively high 137Cs is present in the smaller size fraction; <1 and <48 μm, while about 105 Bq/kg of 137Cs still exist in the large particle fractions: 114–597 μm and 597 μm–2 mm (Figure 3A). The highest radioactivity was detected in the <1 μm fraction in OTO-E and KOI-E (Figure 3B). Specifically, the more than 3.0 × 106 Bq/kg of 137Cs in this fraction from KOI-E accounts for 58% of the total radioactivity, confirming that the greatest proportion of the radioactivity is to be found in the submicron-sized particles. Because small particles bearing 137Cs can aggregate and form a larger particle, a certain portion of radioactivity derived from submicron-sized particles must also occur in the large size fractions. In order to quantify the actual Cs radioactivity of the large size fractions, the same specimen of KOI-E was sieved for the size fraction, 597 μm–2 mm, 114–597, and 48–114 μm in Figure 3 was ultrasonicated, and the radioactivities were measured again. As shown in Figure 3C, the Cs radioactivity of the three larger size fractions decreased dramatically by an order of magnitude. This significant decrease of radioactivity by the ultrasonication confirms of the extensive aggregation and attachment of submicron-sized Cs particles to larger particles. The specific surface area, which is typically proportional to the number of surface adsorption site for ions, increases as the particle size decreases. However, in this case, the preferential distribution of Cs in the submicron-sized particle cannot be simply explained by the increased number of adsorption site for Cs. The cation exchange capacity, as determined for Fukushima soils is on the order of 1 ~ 5 cmol/kg (Iwata et al., 2012), which is eight orders of magnitude greater than the Cs concentrations. If 106 Bq/kg of 137Cs occur in a soil, this corresponds to only 3 × 10−2 ppb. Thus, despite the great abundance of adsorption sites in the small particle fraction, only a small number of these sites are occupied by Cs. In the case of OTO-W, the 137Cs radioactivities in the bulk and submicron fraction are 1.11 × 106 and 1.53 × 106 Bq/kg, respectively. This difference is not consistent with the difference in the surface areas that are simply estimated based on the particle size. Thus, it appears that the very high-surface area of the small particle fraction is not entirely responsible for the high level of radioactivity in very small particle size fractions.

FIGURE 3
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Figure 3. (A) The 137Cs radioactivity of the three samples separated to the five size fractions; <1, 1–48, 48–114, 114–597 μm, and 597 μm–2 mm. (B) A pie diagram of (A) showing the percentage of radioactivity in each size fraction. (C) A pie diagram of the size-dependent radioactivity of the KOI-E sample ultrasonicated twice after obtaining (B).

Characterization of Soil Minerals

Major mineral phases in the three soils, OTO-E, OTO-W, and KOI-E, were determined by XRD analysis (Figures 4A–C). Quartz was dominant in the three samples. Other mineral phases vary depending on the soils; possible akaganeite in OTO-E, kaolinite, cristobalite, and albite in OTO-W, kaolinite, gibbsite, cristobalite, and albite in KOI-E. The XRD patterns of the elutriated samples containing only submicron-sized particles in OTO-W and KOI-E revealed that the intensity of the diffraction peaks of quartz and albite decreased, while gibbsite and 7 Å peaks were enhanced (Figures 4D,E). Slow-scan analysis of the elutriated sample of KOI-E at the low angles showed the characteristic diffraction peaks of clay minerals corresponding to 14, 10, and 7 Å (Figure 4F). The possible phases based on these diffraction maxima are vermiculite, smectite, and chlorite for 14 Å, micas for 10 Å, and kaolinite for 7 Å.

FIGURE 4
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Figure 4. X-ray diffraction spectrum of three soil samples: OTO-E, OTO-W, and KOI-E. (A–C) The patterns obtained from the bulk samples. (D–F) The patterns obtained from submicron-sized particle after elutriation of the samples (A–C), respectively. Qtz, quartz; Kln, kaolinite; Crs, cristobalite; Ab, albite; Ilt, mica and illite; Gbs, gibbsite; Crs, cristobalite; Ab, albite; Ver, vermiculite; Chl, chlorite.

A SEM–EDX elemental map of OTO-W sample revealed that the presence of various minerals, such as quartz, feldspar, Fe-oxide, and aluminosilicate (Figure 5A). It was difficult to detect Cs peak because the low concentration adsorbed on the soil minerals was below the detection limit of EDX, ~0.1 wt%. Aluminosilicates were further analyzed for their composition (Figures 5B,C). The particle of edx1 may be kaolinite or zeolite. The edx2 represents biotite composition. The edx 3 and 4 likely indicate a mixture of biotite–vermiculite and possible Ca-carbonate. Wave-length dispersive X-ray analysis was also attempted on the sheet silicate minerals; however, Cs was not detected (data not shown).

FIGURE 5
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Figure 5. Representative results of SEM analyses. (A) A secondary electron image of OTO-W sample with EDX elemental maps of the same area. (B) A secondary electron image of KOI-E sample with EDX spectra of the point analysis collected from the red circles. (C) A secondary electron image of KOI-W sample with EDX spectra of the point analysis collected from the red circles.

A droplet of the elutriated suspension of OTO-W that contains submicron-sized particle was dried on a silicon wafer (Figure 6). The particles concentrated at the edge of droplet while drying due to the surface tension and arrayed as ring shape on the substrate. The autoradiograph of this sample revealed that the radioactive Cs is also distributed in the same manner as the submicron-sized particles that were confirmed in the SEM image (Figures 6A,B). The average chemical composition of these particles was Si, Al, Fe, and little K (Figure 6C). The SEM analysis in conjunction with the autoradiography indicates that radioactive Cs was mainly associated with the submicron-sized aluminosilicates.

FIGURE 6
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Figure 6. (A) Autoradiography of a droplet of the suspended submicron-sized particles elutriated from OTO-W sample, which was dried on a smooth Si-metal plate. (B) A secondary electron image of a part of the area indicated by the red square in (A). (C) A SEM–EDX elemental map obtained from the area indicated by the red square in (A).

The submicron-sized particles elutriated from OTO-E were further characterized by TEM. Figures 7A–C show HAADF–STEM images of an aggregate of the submicron-sized particles. A wide area view (Figure 7A) shows numerous flaky-shaped particles in the aggregate, which correspond to the texture of clay minerals like vermiculite. The flaky-shape particle appears to consist of a few domains of layered particles with different contrast (Figure 7B). Single layered particles were analyzed by EDX point analysis (edx1 and 2), revealing that the major composition is consistent with that of vermiculite (Figure 7C). Unfortunately, the Cs concentration was too low to detect by EDX. Figure 7D is the elemental maps of Figure 7A revealing the dominant occurrence of aluminosilicate with some Fe and occasional little K. The Fe-rich and Ti-rich particles are likely Fe-oxide and Ti-oxides, respectively. Bright-field TEM image of the clay particles clearly shows the shape of the clay aggregates as large as a few hundred nanometer in length and several 10 nm in width (Figure 7E). A HRTEM image of individual particles revealed that tetrahedral–octahedral–tetrahedral layers continue only <10 layers with spacing of ~1.0 nm Figure 7F. These clays are most likely anhydrated vermiculite in conjunction with EDX analysis.

FIGURE 7
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Figure 7. Results of TEM analyses of the submicron-sized particles elutriated from OTO-E. (A–C) HAADF-STEM images of an aggregate of the submicron-sized particles. (A) A wide view, (B) an enlarged image of (A) showing flaky-shaped particles, and (C) a further enlarged image indicating the position of EDX point analyses. (D) Elemental maps of the area imaged in (A). (E) Bright-field TEM image of the clay particles. (F) A HRTEM image of individual particles showing the lattice spacing of ~1.0 nm.

Irreversible Sorption of Cs on the Surface Soils

Figure 8A shows the results of sequential extraction for three samples: OTO-E, OTO-W, and KOI-E revealing that 3.95–21.4% of 137Cs was leached by 1M NH4OAc (pH 8) solution and more than 63% of Cs was retained in the insoluble fraction. This result is consistent with the previous studies reporting that a small fraction of radiocesium in the interlayer of phyllosilicate minerals is exchangeable with NH4+ and a large fraction is fixed in the structure, probably along frayed edges (Evans et al., 1983; Cremer et al., 1988; McKinley et al., 2004). Because the Cs in the aerosols emitted just after the accident were predominantly water soluble, 50–90% (Tanaka et al., 2012b), the soluble Cs was delivered by rain water and fixed in the structure of phyllosilicate minerals. Comans and Hockley (1992) studied the irreversibility of Cs sorbed onto the clay minerals and concluded that the highly selective Cs sorption site was at frayed edge sites (FES) that develop along the weathered edges of micas. Their immediate weathering products are hydrous-mica and illite. At the FES, wedge zones form, and the 1.0 nm mica sheet opens to 1.4 nm vermiculite, providing a stereoselective environment for Cs+ sorption (Jackson, 1963). The selectivity coefficients of Cs relative to the other cations (Na+, K+, and Ca2+) expressed as logKc, (Kc = [Au+][ECsX]u/[Cs+]u[EAXu], where ECsX and EAXu represent adsorption density divided by CEC for Cs and cation A) estimated to be up to ~6.76 based on the ion exchange models (Bradbury and Baeyens, 2000; Zachara et al., 2002), stating the high affinity of Cs with sheet aluminosilicate. Hence, in the soils at Fukushima, similar Cs-binding mechanisms may play a role in fixing Cs onto aluminosilicate sheet structures; hence, the release of radioactive Cs from soil minerals should be minimal. A limited amount of Cs can be released by an ion exchange process, but it is expected that the released soluble Cs will be immediately adsorbed onto aluminosilicate minerals with a sheet structure, that is clays.

FIGURE 8
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Figure 8. (A) Fraction of the Cs chemical form in three soil samples determined by a sequential extraction. (B) Fraction of Cs chemical form in the submicron-sized particle elutriated from OTO-W as compared to that in the bulk OTO-W soil.

Sequential extraction was also conducted for the submicron-sized particle elutriated from OTO-W sample (Figure 8B). The chemical form of Cs in the submicron-sized particle fraction is similar to that in the bulk, although the major mineral constituents were different from that of the bulk. Quartz and feldspar were major minerals in bulk; whereas, clays and mica-like minerals were dominant in the submicron-sized fraction. The results of sequential extraction indicate that Cs is predominantly adsorbed onto the clays in the bulk sample, as well as in the submicron-sized fraction, because the number of adsorption site on the sheet structure of the aluminosilicate clays is much greater than the amount of Cs available. The sequential extraction for Cs in Fukushima soils probably represents the chemical form of Cs adsorbed on the submicron-sized sheet alumino silicate.

Role of Submicron-Sized Particles as Cs Carrier

In general, submicron-sized particles in aquifer behave as colloids, which have unique properties in the subsurface. Colloid-facilitated transport of toxic elements is typically ascribed to hydrodynamic chromatographic effects (McCarthy and Zachara, 1989; Kim, 1991). In the heavily contaminated soils of the present study, the 137Cs radioactivity was ~3,000,000 Bq/kg on the colloids and these submicron-sized particles can potentially contribute to the migration of radioactive Cs as pseudo-colloids. Short range migration of Cs particles might occur only within top of the profile as reported in Ohnuki and Tanaka (1989) and Tanaka and Ohnuki (1996). However, the particles that have sorbed the radioactive Cs remain within the top ~5 cm of vertical profile (Figure 2), and the amount of radioactivity in groundwater collected from a well at Iitate village was below the detection limit (data not shown). This suggests that Cs migration through vadose zone to groundwater did not occur for the period from March 2011 to March 2012. As shown in the results above, a large fraction of Cs was adsorbed onto the submicron-sized aluminosilicates with sheet structures, that is clays, and although they are potentially mobile, their movement has been limited because the small particles have aggregated due to the fact that the pH of the ground water is near neutral and the point of zero charge (PZC) of sheet aluminosilicate is ~6–7 [based on the PZC of biotite as reported in Goldberg et al. (2012)]. Formation of aggregates has prevented the Cs particles from being transported vertically through the soils due to a filtering effect. Rather, the aggregates of small Cs particles currently migrate through surface water. Indeed, 90–98% of the radioactive Cs is transported as suspended fine particle from hydrographic basin to rivers, which is supposed to be a major dose contributor of the Cs flux to the ocean: 200–500 GBq/year for 5 years after the accident (JAEA, 2013). As a consequence, transport of Cs particle aggregates through surface water should have been responsible for the removal of Cs radioactivity of surface environment to the lower level than that simply calculated by radioactive decay of 134Cs.

Conclusion

The submicron-sized particles in the contaminated soils near Fukushima are mainly composed of aluminosilicates with sheet structures, clays. These clays, mica, vermiculite, chlorite, and smectite, are responsible for adsorbing more than 70% of the total Cs in the soil profile. The adsorbed Cs does not desorb easily, probably because of strong binding at FES of the clays (Iwata et al., 2012). Aggregation of the very small clay particles into larger particles has further limited their migration downward through the soil profile; hence, most of the radioactivity remains within the top 5 cm of the soil profile. Currently, the mobility of the aggregates of submicron-sized sheet aluminosilicate in the surface environment is a key factor controlling the Cs migration in Fukushima. Still, the aggregates can be potentially transported as suspended colloids in case of deflocculation in a specific geochemical condition of ground water, and this should be considered in transport models that predict future migration of Cs in these highly contaminated regions.

Conflict of Interest Statement

The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.

Acknowledgments

This study is partially supported by JST Initiatives for Atomic Energy Basic and Generic Strategic Research and by the Science Grant of the Ministry of Education, Science and Culture. SU is also supported by ESPEC Foundation for Global Environment Research and Technology (Charitable Trust) (ESPEC Prize for the Encouragement of Environmental Studies). SU is also grateful to Dr. Watanabe for her assistance on SEM and XRD analyses at the Center of Advanced Instrumental Analysis, Kyushu University.

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Keywords: cesium, colloid, electron microscopy, Fukushima Daiichi nuclear disaster, clay minerals

Citation: Kaneko M, Iwata H, Shiotsu H, Masaki S, Kawamoto Y, Yamasaki S, Nakamatsu Y, Imoto J, Furuki G, Ochiai A, Nanba K, Ohnuki T, Ewing RC and Utsunomiya S (2015) Radioactive Cs in the severely contaminated soils near the Fukushima Daiichi nuclear power plant. Front. Energy Res. 3:37. doi: 10.3389/fenrg.2015.00037

Received: 22 June 2015; Accepted: 06 August 2015;
Published: 01 September 2015

Edited by:

Muhammad Zubair, University of Engineering and Technology Taxila, Pakistan

Reviewed by:

Anca Melintescu, Horia Hulubei National Institute of Physics and Nuclear Engineering, Romania
Giuseppe Vella, University of Palermo, Italy
Qazi Muhammad Nouman Amjad, University of Engineering and Technology Taxila, Pakistan

Copyright: © 2015 Kaneko, Iwata, Shiotsu, Masaki, Kawamoto, Yamasaki, Nakamatsu, Imoto, Furuki, Ochiai, Nanba, Ohnuki, Ewing and Utsunomiya. This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) or licensor are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.

*Correspondence: Satoshi Utsunomiya, Department of Chemistry, Kyushu University, Hakozaki 6-10-1, Higashi-ku, Fukuoka, Japan, utsunomiya.satoshi.998@m.kyushu-u.ac.jp