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The Composite Materials for Localization of Volatile Radioactive Iodine Forms from Steam-Air Phase during Severe Accidents at NPPs

Written By

Sergey Kulyukhin, Lubov Mizina, Igor Rumer and Nikolai Mikheev

Submitted: 09 November 2010 Published: 20 July 2011

DOI: 10.5772/20494

From the Edited Volume

Metal, Ceramic and Polymeric Composites for Various Uses

Edited by John Cuppoletti

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1. Introduction

The safety of NPPs is currently a problem of particular concern in all industrially developed countries throughout the world. The various science and technology projects being developed in this area seek to minimize the possibility of accidents. During severe accidents the formation of large quantities of gaseous products, which leads to an abrupt increase in pressure inside the containment (protective casing) take place. Eventually, there is a risk of destroying the containment as such. Besides, such accidents may cause contamination of the nuclear power plant closed areas, such as the intercontainment area, technical and service corridors, reactor area, et cetera, due to leakage through non-airtight sectors of the containment. It was established that such a leak of the air-and-steam mix out of the containment can reach a rate of 0.3 to 1.0 % per 24 h. Today, in order to prevent environmental pollution in the event of severe accidents, the operational nuclear power plants are equipped with emergency valves that can be activated to reduce the pressure inside the containment, in which case the air-and-steam flow, carrying radioactive aerosols and volatile fission products, is forced through special decontamination systems (Asmolov, 1994; Particulate Filtration in Nuclear Facilities, 1991; Containment Systems and Components for LOCA and Severe Accident Mitigation, 1993; Rogers, 1990). The all systems, excepting sand bed and gravel filter, have a high efficiency of localization of aerosols, and some of them have a high efficiency relative to molecular form of iodine. However, these systems, excepting Germany system, including the filter based on molecular sieve, practically do not localize the organic form of iodine, such as methyl iodide.

WWER-440/V-230 NPPs are first-generation Russian NPPs that have been operated for more than 25 years now. As the engineering of the designs of these stations was realized long before severe accidents at Three Mile Island and Chernobyl NPPs, all system of localization of accidents was plotted on the concept of impossibility of severe accidents at NPPs. However now point of view varies and the concept of improvement of a protection system of Russian WWER-440/V-230 NPPs with allowance for possibilities of severe accidents is now considered. All modifications of Russian WWER-440/V-230 NPPs belong to this first generation (Kovalevich et al., 2000; Dragunov et al., 2006).

Modern designs of new generation NPPs (EPR /Framatome ANP/, SWR-1000 /Framatome ANP/, AP-1000 /Westinghouse/, ESBWR /General Electric/, APWR /Mitsubishi/, ABWR /Toshiba and Hitachi/) do not provide for pressure-drop systems, assuming that the entire peak load will be withheld by the containment (Reactor Design, 2002; Krebs, 1999; Tomorrow's reactors, 2003). Calculations show that during 122 h, pressure under the containment can raise up to 0.7 MPа, with the steam/air ratio being 2.7:1 (Dillman, 1991). This time is enough for the steam-air joint containing volatile radioactive fission products to penetrate (0.3 to 3 % per day) into the intercontainment area and then into the environment. To prevent radioactive contamination of the environment, modern designs propose using an active air decontamination system, which using high-capacity ventilators, will forward the air from the intercontainment area to filters filled with impregnated activated charcoal. This system requires regular electric power supply, which is a significant disadvantage of this technological approach.

However, in accordance with the general requirements for safety systems, alongside active ventilation systems for intercontainment space, nuclear power plants should include a passive ventilation system, which can be used during hypothetical severe accident with a complete loss of power supply.

Now a passive-mode environmental protection system for decontamination of intercontainment area, which can be used in the event of severe accidents, was developed (Bronnikov, 2004; Zeyen et al., 2006; Friesen et al., 2001; Asmolov, 1994; Kulyukhin et al., 2008; State of the art report on iodine chemistry, 2007; State of the art report on nuclear aerosols, 2009; Kulyukhin et al., 2011). The basic purpose of developed passive filtration system is creation of a rarefaction in an intercontainment space due to the organized removal of the radioactive steam-air mixture from an intercontainment space at full loss of all power sources. Steam-air mixture containing radioactive aerosols and flying fission products removal from an intercontainment space is passed through the special filtering module. Efficiency of cleaning of a radioactive steam-air mixture is determined by filtration and sorption properties of used filtering elements.

One of the nuclear fuel fission products of high environmental emergency is radioactive iodine. The International Atomic Energy Agency (IAEA) classifies accidents and other events occurring at nuclear industry enterprises in terms of the amount of radioiodine release into the environment (Bukrinskii et al., 1991). Currently we know about the existence of 14 iodine nuclides, of which only 127I is stable. Given an average nuclear fuel burn up depth of 45 GWd/t, one ton of irradiated nuclear fuel of PWR type (in Russia, WWER) contains 200 g to 300 g of iodine radionuclides or about 12 kg per the entire amount of fuel in the reactor (Radioiodine Removal in Nuclear Facilities, 1980; Ustinov et al., 2005). During a long exposure of fuel elements, all short-lived iodine radionuclides decompose, and as a result the irradiated nuclear fuel that goes to reprocessing plants includes either two (127I, 129I) or three (127I, 129I, 131I) iodine nuclides, depending on the time of storage.

On the other hand, a totally different situation may occur during accidents at nuclear power plants and especially during non-design accidents associated with nuclear fuel melting. Depending on the length of the event, the amount of radioiodine in the fuel that fully penetrates into the primary containment environment and further, possibly, into the open environment may vary from hundreds of grams to tens of kilograms. To predict the chemical forms of radioiodine and their concentrations in the containment environment during non-design accidents, the Library of Iodine Reactions in Containment (LIRIC) was created. It includes over 150 chemical reactions of iodine, including those with organic species (Evans et al., 1990). The variety of the chemical forms of radioactive iodine in gaseous media needs sophisticated protective system to localize it during irradiated nuclear fuel reprocessing, as well as in the protective systems at nuclear power plants (Particulate Filtration in Nuclear Facilities, 1991). Despite a great number of volatile forms of radioiodine, the focus of attention in modern irradiated nuclear fuel reprocessing systems in both Russia and abroad, as well as at all nuclear power plants, is the localization of CsI radioactive aerosols and gaseous I2, HI, and CH3I.

The study of the sorption of volatile compounds of radioactive iodine from a gas phase on a wide spectrum of sorbents has shown that the most effective are the sorbents containing 8-12 wt% of Ag (Kulyukhin et al., 2008; State of the art report on iodine chemistry, 2007; Kulyukhin et al., 2011). Because of high cost of Ag, which is the one of the basic components connecting radioactive iodine, there is a problem of decreasing of its quantity in sorbents by their modifying, or makes topical its replacement. Apparently, the most suitable for this purpose are d-elements whose physicochemical properties are close to those of Ag, namely, Cu, Ni and Zn.

The aim of this study was to develop new composites based on Ag-, Ni-, Zn- and Cu-containing silica gel for localization of volatile compounds of radioactive iodine from steam-air phases. These composites will be used during modernization of the environmental protection systems during severe accidents at the different types of NPPs.

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2. Experimental

In our study we used the radionuclide 131I supplied by Izotop Joint-Stock Company in the form of carrier free Na131I solution. The radioactivity of the nuclides was determined by γ-ray spectrometry with a semiconductor Ge–Li detector on a multichannel analyzer. The radionuclide 131I was used as this study as a spike for weighable amount of inactive iodine. Therefore, designations like 131I2 and CH3 131I refer to labeled species and not to species of pure 131I radionuclide.

We used 131I2 (10-100 mg) and also CH3 131I (1-10 mg) with the specific activity from 3×102 to 3×103 Bq/mg. The 131I2 generated in a gas phase by bubbling of water solution K131I-131I2 by a steam-air flow. As a collector of CH3I labeled with 131I we used a quartz vessel into which, prior to experiment, we condensed with liquid nitrogen from a helium flow 1-100 mg of CH3 131I prepared by the reaction of dimethyl sulfate with K131I (Murata et al., 1968).

In the experiment, methyl iodide was introduced into the system by passing air at a definite rate through the quartz vessel with CH3 131I.

To prepare composites, we used macroporous silica gel with a particle size of 2.00–3.00 mm as matrices.

Nitrates of Zn2+, Cu2+, Ni2+, and Ag+, and also all the acids, alkalis and hydrazine hydrate (HH) used in the study were of chemically pure grade. Pure grade hydroxylamine sulfate (HA) was used without additional purification.

Mechanical strength of granules of developed composites was measured on MP-2C device.

Electron micrographs of developed composites were obtained on the electron microscope TEM-301 ("Philips").

X-ray electron probe microanalysis (EPМ) of developed composites was made on the scanning electron microscope JSM-U3 (Japan) with energy dispersive spectrometer "Eumex" (Germany).

Thermal gravimetric analysis of developed composites was performed with a Q-1500 derivatograph (MOM, Budapest, Hungary). Samples were heated in platinum crucibles in air at a rate of 10 deg/min.

2.1. Ag-containing composites

2.1.1. Synthesis of Ag-containing composites

The composites containing 1-8 wt% of AgNO3 were prepared by impregnation with an aqueous solution of AgNO3 with the following treatment by different N-containing compounds with the following drying on air at increasing of temperature from 20 to 300º C and next air-conditioning at 300º С.

Composites were synthesized in two stages:

  1. Impregnation of macroporous silica gel with a solution of AgNO3 with the following drying on air at 110º С;

  2. Treatment of precursors with solutions of N-containing compounds with the following drying on air at increasing of temperature from 20 to 300º C and next air-conditioning at 300º С during 4 h.

The quantity of a solution of the AgNO3, which is necessary for impregnation of silica gel, was taken in an amount ensuring 50% filling of the volume of the silica gels. The volume of silica gel was calculated from its bulk weight, which equal 0.576 kg/m3.

The quantity of AgNO3 for synthesis of composites was calculated on the basis of data about necessary Ag concentration in precursor.

The first stage of synthesis of precursors of composites on a basis of macroporous silica gel containing Ag was carried out as follows. At intensive mixing a 434 cm3 of a solution of AgNO3 with necessary concentration was added to 500 g of macroporous silica gel. The obtained mixture was mixed during 60 min for obtaining of uniformity of impregnation of total joint of silica gel with solution of AgNO3.

After obtaining of proportional impregnation of total joint of silica gel with solution of AgNO3 the wet sample was placed in BINDER drier. Precursors were dried on air at temperature 110º С to an air-dry state.

As a result of these operations there was a partial destruction of granules of precursor. Therefore before carrying out of the second stage of synthesis of composites it has been made the fractioning. As result of the fractioning of precursor granules with the size less than 1 mm has been separated. The quantity of the given fraction did not exceed 2-3% from total synthesized joint of precursor.

As a result the precursors, containing 1, 2, 4 and 8 wt% of Ag on the basis of macroporous silica gel, were synthesized.

At the second stage of synthesis of composites the precursors were treated by different N-containing compounds with the following drying on air at increasing of temperature from 20 to 300º C and next air-conditioning at 300º С during 4 h.

In our study 0.01, 0.05 and 0.1 M water solutions of HH and HA, and 0.5, 1.0 and 2.0 M water solutions of NH4OH were used as N-containing compounds.

The second stage consists on treatment of precursor by N-containing compounds for obtaining of composites with nanometric particles of different compounds of Ag, was carried out as follows. At intensive mixing the 80 cm3 of solution of N-containing compound with necessary concentration were added to 100 g air-dry precursor, containing 1, 2, 4 or 8 wt% of AgNO3. The obtained mixture was mixed during 60 min for obtaining of uniformity of impregnation of joint of precursor with solution of N-containing compounds. During impregnation the colour of precursor changed from white to grey.

After obtaining of proportionality of impregnation of total joint of precursor that proved to be true of uniformity of colour, the wet samples were placed in exiccator on 3 h. Through 3 h wet samples were placed in BINDER drier. The wet samples of composites were dried on air at increasing of temperature from 20 to 275-300º С with the following air-conditioning during 4 h at temperature 275-300º С.

As a result of these operations the composites, containing 1, 2, 4 and 8 wt% of nanometric particles of different compounds of Ag, on a basis of macroporous silica gel were obtained.

As above mentioned, during treatment of precursors by N-containing compound its colours changed. Besides, the change of precursor's colour, containing AgNO3, was observed at long-term exposure on them of sunlight. The change of colour is connected with photo reduction of ions of Ag to a metal state on the surface of material.

2.1.2. The content of Ag in synthesized composites

Percentage content of Ag in synthesized precursors and composites is specified by quantity of AgNO3, which was used for impregnation of macroporous silica gel. Whereas during synthesis of precursors and its modifying it is possible the loss of Ag with dust fraction, the final content of Ag in precursors and composites is determined by an analytical method by the following technique. The joint of precursor or composite (~1 g) carefully triturate in a porcelain mortar in the presence of 10 cm3 of water. Suspension quantitatively transfers in 30-cm3 centrifuge tube and 10 cm3 of concentrated HNO3 was added to suspension. Than centrifuge tube with suspension was heated up during 1 h on a boiling water bath. After heating centrifuge tube was cooled and a solution was separated from solid phase by centrifugation. The solid phase was washed 3 times by 25 cm3 of distilled water. The solution and all washings were merged in 100-cm3 volumetric flask for titration. The solution in volumetric flask was reduced to 100 cm3 and than the determination of Ag by titration on Volgard's method from 0.01 N solution of NH4SCN at presence of iron ammonium alum indicator was carried out (Charlout, 1961). The content of Ag was calculated by the formula:

% A g   =   ( N 1 x V 1 x M ) / ( V 2 x P ) E1

where N 1 - normality of NH4SCN solution; V 1 - volume of NH4SCN solution, which was used for titration, cm3; V 2 - aliquot of Ag solution for analysis, cm3; М - gramm-equivalent of Ag; P - joint of composite, g.

The analysis of data on the Ag content in synthesized precursors and composites shows that the content of Ag in synthesized composites is in the range from 1.0 to 8.0 wt% that is from 95 to 99.9% from Ag quantity taken for synthesis.

2.1.3. Desorption of Ag from synthesized composites into water

During treatment of precursors by N-containing compounds the poorly soluble compounds of Ag in the composites are formed. At treatment of precursors by HH and HA the Ag0 particles can be formed. At treatment of precursors by NH4OH both Ag2O and Ag0 particles can be formed. For study of degree of conversion of AgNO3 to poorly soluble compounds studies of Ag desorption from synthesized precursors and composites into water were carried out.

The study of Ag desorption from composites into water was carried out as follows. The joint of composite (~1 g) carefully triturate in a porcelain mortar in the presence of 10 cm3 of water. Suspension quantitatively transfers in 30-cm3 centrifuge tube. The suspension was conditioned on 24 h at temperature 18-20º С. After that a solution was separated from solid phase by centrifugation. The solid phase was washed 3 times by 25 cm3 of distilled water. The solution and all washings were merged in 100-cm3 volumetric flask for titration. The solution in volumetric flask was reduced to 100 cm3 and than the determination of Ag by titration on Volgard's method from 0.01 N solution of NH4SCN at presence indicator iron ammonium alum was carried out (Charlout, 1961). The content of Ag was calculated by the formula (1).

Analysis of data on the desorption of Ag from synthesized composite into water for 24 h at temperature 18-20º С shows that the quantity of Ag which has passed into water from synthesized composites does not exceed 18% from total quantity of Ag in composites.

2.1.4. Fractional content of synthesized composites.

Determination of fractional content of synthesized composites was carried out using a nest of sieves (hole diameters were from 7.0 to 0.3 mm) by shaking of 200-400 g of composite for 15 min in according with technique, presented in (State Standard 16187-70, 1970). The resultant separated fractions were weighted. The percentage of each fraction was calculated by the formula:

% = ( m / M ) x 100 E2

where m – weight of separated fraction, g; M – total weight of composite taken for the analysis, g.

Analysis of data on the fractional content of averaged sample of synthesized composites shows that during synthesis the composites practically have not changed its initial fractional content. The changes of basis fraction of macroporous silica gel with the size of granules from 2.0 to 3.0 mm were not more than 2%.

2.1.5. Free volume of synthesized composites

The free volume, which is a sum of pore volumes of composite and intergranule space, was determined in the following way. 10 cm3 of hexane was added to 5 g of air-dry composite. Suspension carefully was mixed before full removal of air bubbles and than was conditioned during 24 h at temperature 20º С. Through 24 h summary volume of composite and hexane was measured. Knowing volume of air-dry composite, the free volume of composite Vfree was calculated by the formula:

V f r e e = { [ ( V 1 + V 2 ) V 3 ] / V 1 } x 100 % E3

where V1 - volume of a joint of air-dry composite, cm3; V2 - volume of hexane, cm3; V3 - final volume of composite and hexane through 24 h, cm3.

Analysis of data on free volume of composites shows that the free volumes for synthesized composites were in the range from 72 to 80%. The obtained data on free volume of material allow concluding that synthesized composites have large specific surface and total volume of pores. The extended surface and large porosity of composites suggests both high rate of sorption of volatile compounds, and low aerodynamic resistance to a gas flow.

2.1.6. Bulk weight of synthesized composites

Bulk weight of composites was determined as the ratio of mass of an air-dry material and the volume taken by it. Analysis of data on bulk weight of synthesized composites shows that synthesized composites have bulk weights from 0.5 to 0.7 g/cm3 or 500-700 kg/m3. The sufficiently low density of synthesized composites, as well as high values of free volume, indicates to large porosity of composites and, hence, a well developed specific surface.

2.1.7. Mechanical strength of synthesized precursors and composites

Mechanical strength of granules of precursors and composite was measured on MT-2C device which scheme is presented on Fig. 1. The device was developed and designed in Institute of Physical Chemistry and Electrochemistry of Russian Academy of Sciences. The principle of operation of this device consists in loading the sample at constant speed of a working table movement and fixing the breaking force on the indicating gage. Mechanical strength σр was calculated by the formula:

s р =   4 P / p d 2 E4

where Р - the load (kg), d - the diameter of granules of materials under study (cm).

Samples of composites were a mixture of different particles (mall, hemispherical and spherical). Only spherical granules (12 samples) with an average diameter 3.0 mm were used for measurement of mechanical strength σр. The granules were tested on squeeze in static conditions on MT-2C device at loading rate 1 mm/min. During measurements mechanical strength of granules σр (kg/cm2) and a roof-mean-square deviation S n x ¯ from arithmetical mean Sn for 36 samples were determined.

Figure 1.

The scheme of MT-2C device (1 - indicator of displacements, 2 - a flat spring of weighting device, 3 - a spring for rod weighing, 4 - guide ways, 5 - a rod, 6 - the top support, 7 - the sample, 8 - a working little table, 9 - a reduction unit, 10 - a speed gear box, 11 - electric motor, 12 - the shifter of the electric motor or handcrank to a reduction unit, 13 - a handcrank, 14 - the adaptation for test of samples for a cut, 15 - a movable support for test of samples for a bending under 3th and 4th dot scheme, 16 - a prism, 17 - a movable wedge for test of samples for a bending under 4th dot scheme, 18 - a cone with various corners for test of pastes on a method conical plastometer)

Analysis of results of tests of 36 samples of granules of composites under static loading shows that strength of granules increases with an increase in the quantity of Ag in material, i.e., the structure of the materials strengthens. On the other hand, strength of granules of composites was lower than strength of analogous precursors. Decreasing of mechanical strength occurs as a result of changing of structure of macroporous silica gel during treatment of precursors by N-containing compounds. It is known, that during treatment of silica gel by alkaline solutions dissolution of gel silica acid, which are in a pores of silica gel, takes place. The similarly process of dissolution of gel silica acid in pores of silica gel occurred during treatment of precursors by N-containing compounds. Besides, during treatment of precursors by N-containing compounds there was a change of the chemical forms of Ag in the materials under study. As a result of the various physico-chemical processes, which occurred in granules of material, there was an increasing of pore volumes of granules that leads to decrease in mechanical strength of granules. Mechanical strength of composites was more than 85 kg/cm2.

2.1.8. Electron microscopy study of synthesized composites

Figure 2 show the electron micrographs of the synthesized composites SiO2-n%Ag (n = 1, 8), obtained using a Philips TEM-301 transmission electron microscope. As shown in Fig. 2, the synthesized materials contain Ag0 nanometer particles not larger than 10 nm. The amount of the nanometer particles increases with an increase in the Ag concentration in the materials. Note that the amount of Ag0 nanometer particles depends not only on the Ag concentration in the material, but also on the nature of the nitrogen-containing compound used for the modification of the precursor.

A study of the microphotographs showed that the largest particles were formed during treatment of the precursor with ammonia solutions. The particles form aggregates (Fig. 2B). When HH or HA is used, highly dispersed particles stabilized in the matrix pores are formed (Fig. 2A). On the hand, decreasing the Ag concentration during treatment of the precursor with ammonia solutions leads to the formation of highly dispersed particles in the silica gel matrix (Fig. 2B).

Figure 2.

The electron microphotograph of the composite SiO2-8%Ag obtained by treatment of the precursor with solutions of 0.1 M HH (A) and 0.5 М NH4OH (B)

As follows from Fig. 2, the amount of nanometer Ag0 particles is very small, which, as we believe, indicates the formation in the matrix of Ag particles smaller of a size smaller than the equipment resolution power, i.e., <1 nm. In addition, it is necessary to take into account a low concentration of Ag in the matrix of the composite with a strongly developed surface.

The Ag distribution in the matrix of the composites was studied using their electron probe X-ray microanalysis. Figure 3 shows a typical microphotograph of the surface of the chip of the granule of the composite, and fig. 4 shows the X-ray diffraction spectrum of the sample surface. As follows from Figure 3, particles not larger than 1 μm are evenly distributed on the granule surface and that the amount of the aggregates larger than 10 μm is relatively small. An elemental composition study of the surface showed that the composites contained O, Si, and Ag (Fig. 4).

Figure 3.

The microphotograph of the surface of the SiO2-4%Ag composite

Figure 5 shows the X-ray spectroscopy data on the Ag distribution on the surface of granules of SiO2-n%Ag (n = 1, 2, 4, 8) composites after treatment of the precursors with solutions of HH and HA. The surface of the granules was scanned at a radiation power only characteristic of Ag.

As follows from fig. 5, the Ag particles are virtually evenly distributed on the surface of the composite granules. The amount of the particles on the surface decreases with a decrease in the Ag concentration.

The obtained results are good agreement with the conclusions drawn from the microphotographs obtained using transmission electron microscopy. Actually, the well-developed surface of the synthesized composites stimulates a strong distribution of Ag in the volume of the granules of the material. As a result, when the Ag concentrations are low, the number of Ag particles per surface unit of the material proves to be very low.

Figure 4.

The X-ray diffraction spectrum of the SiO2-4%Ag composite after treatment of the precursors with solutions of HH

2.1.8. Localization of molecular iodine and methyl iodide from a steam-air flow

The efficiency of molecular iodine and methyl iodide localization by composites under analogous experimental conditions depends on many factors, the main of which are as follows: active metal concentration, preparation conditions, quantity of methyl iodide or molecular iodine, steam-air flow rate, and time of contact between the steam-air flow and the composite.

2.1.8.1. A study of the localization of molecular radioiodine from a steam-air flow

To study the localization of 131I2 from a steam-air flow, we used the procedure and installation described in (Kulyukhin et al., 2007).

Figure 5.

The distribution of Ag particles on the surface of the granule of the composite based on silica gel containing 4 wt% Ag (A) and 8 wt% Ag (b) after treatment of the precursor with a 0.1 М solution of HH and conditioning in the air at 300º С for 4 hours

It is necessary note that the efficiency of molecular iodine absorption is higher than 99% virtually in all cases. After the localization of molecular iodine, the composite changed its color from grey to lettuce green. The appearance of the lettuce green color is due to the formation of Ag131I in the composition of the composite.

Note that irrespective of the Ag concentration in the composite, the absorption efficiency is the highest in the case of using HA and is the lowest in the case of using the ammonia solution (Fig. 6). The composites obtained by treatment with HH take an intermediate position. The observed difference is most likely due to the formation of metal Ag particles in the case of HH and HA versus the formation of Ag oxide in the case of using ammonia solutions. Note that treatment of HA leads to the formation of smaller particles versus HH.

As follows from Fig. 6, when the Ag concentration in the material is increased from 1 to 8 wt%, the total molecular iodine sorption by the total layer of the sorbent remains virtually unchanged and higher than 99%. Despite the virtually equal sorption efficiencies, different distributions of molecular iodine in the layers of the column are observed. Analysis of the layer-by-layer distribution of radioactive iodine in the column as a function of the Ag concentration in the material shows that when the Ag concentration in the material is increased, the sorption front becomes steeper, i.е., the major part of molecular iodine is absorbed in the first layer of the material. The formation of the nanometer Ag particles in the case of HH and HA results in a high sorption efficiency of the synthesized materials. On the other hand, the formation of nanometer Ag oxide particles in the case of treatment of the precursors with an ammonia solution leads to a lower-angle front of the sorption curves along the columns. The difference in the slopes of the sorption curves allows us to draw conclusions regarding not only the possible Ag form in the composite, but also regarding the chemosorption speed for its different forms. For Ag oxide, the molecular iodine chemosorption rate is about 1.5 times slower than that on the metal Ag particles obtained by treatment of the precursors with HH or HA.

Figure 6.

The 131I layer-by-layer distribution on the column with the composite materials obtained by treatment of the precursor with a 0.1 М solution of HA (A) and NH4OH (B) as a function of the Ag concentration in the material (1 - wt% Ag, 2 - 2 wt% Ag, 3 - 4 wt% Ag, 4 - 8 wt% Ag)

All synthesized composites display high molecular iodine sorption efficiency. Note that the sorption efficiency of each of the studied materials is virtually independent of the nature of the N-containing compound used for treatment of the precursor.

Analysis of the layer-by-layer distribution of radioactive iodine on the column containing the SiO2-2%Ag composite obtained by treatment of the precursor by different N-containing compounds shows the layer-by-layer distribution of radioactive iodine along the column filled with the precursor of the given composite (Fig. 7). The lowest-angle molecular iodine sorption front in the layers of the column is observed for the composite obtained by treatment of the precursor with the ammonia solution; the rate of the chemosortion by Ag oxide particles is the lowest as compared with other Ag forms. The chemosorption speed for the non-modified Ag form (AgNO3) is virtually the same as that on the metal Ag particles obtained by treatment of the precursor with a 0.1 М solution of HA. The highest value is observed for the composite obtained during treatment of the precursor with a 0.1 М solution of HH. During treatment of the precursor with HH, metal Ag particles are formed in the near-to-surface layer of the granules, whereas during treatment with HA, the metal Ag particles are formed in the entire volume. As a result, gaseous molecular iodine takes a longer time to enter the chemosorption reaction with the Ag particles in the volume of the granules versus its reaction with the Ag particle in the near-to-surface layer or on the surface of the granules. Note that because of the high porosity of the material the difference in the molecular iodine sorption efficiencies in the 1st layer of the sorbents obtained by treatment of the precursor with HH and HA is very small.

Figure 8 shows the data on the molecular iodine sorption efficiency on the SiO2-2%Ag composite obtained by treatment of the precursor with a 0.01 М solution of HH as a function of the molecular iodine quantity supplied to the column. As follows from Fig. 8, when the molecular iodine quantity is increased tenfold (from 10 to 100 mg), the sorption efficiency remains virtually unchanged and is very high (higher than 99.9%). On the other hand, increasing the molecular iodine quantity leads to its redistribution in the layers of the column.

Figure 7.

The 131I layer-by-layer distribution on the column containing the SiO2-2%Ag composite material as a function of the nature of the N-containing compound used for treatment of the precursor (1 - without modification, 2 - 0.1 М hydrazine hydrate, 3 - 0.1 М hydroxylamine, 4 - 0.5 М NH4OH)

Figure 8.

The 131I layer-by-layer distribution on the column containing the SiO2-2%Ag composite material obtained by treatment of the precursor with 0.01 M solution of HH as a function of the 131I2 quantity (1 - 10 mg, 2 - 50 mg, 3 - 100 mg)

One of the major factors influencing the degree of the molecular iodine sorption from the gas flow is the time of contact between the composites and the gas flow. The time of the contact is determined by the linear gas flow rate and the height of the sorbent in the column.

Figure 9 shows the data on the molecular iodine sorption from the gas flow as a function of the time of contact between the steam-air flow and the SiO2-2%Ag composite obtained by treatment of the precursor with a 2.0 М ammonia solution. As follows from Fig. 9, when the time of the contact between gas phase and composite is decreased from 4.5 to 1.1 s, the molecular iodine sorption remains virtually unchanged and is higher than 99%. An increase the linear gas flow rate and hence, a decreases in the time of contact between the gas flow and the composite lowers the sorption front angle. Note that it takes two or three layers of the composite to localize radioactive iodine.

Another factor influencing the sorption efficiency is the composition of steam-air phase. The presence of water molecules in the gas phase has a competitive influence during the interaction of molecular iodine with active centers of the sorbent.

Figure 10 show the data on the molecular iodine sorption on the SiO2-8%Ag composite obtained by treatment of precursors with 0.1 M solution of HH from steam-air flows with different steam quantities. As follows from Fig. 10, when the steam content in the gas phase is increased about twofold, the total degree of the molecular iodine sorption remains virtually unchanged and equal to more than 99%. On the other hand, it is necessary note that an increase in the steam quantity in the gas phase causes the radioactive iodine to move along the column. Thus, even a small change in the steam quantity impacts the sorption capacity of the composites.

In conclusion note that all synthesized composites have high sorption efficiency for molecular iodine in the gas flow.

Figure 9.

The 131I layer-by-layer distribution on the column containing the SiO2-2%Ag composite material obtained by treatment of the precursor with 2.0 M solution of NH4OH as a function of the time of contact between the steam-air flow and composite (1 - 4.53 s, 2 - 2.06 s, 3 - 1.11 s)

Figure 10.

The 131I layer-by-layer distribution on the column containing the SiO2-8%Ag composite material obtained by treatment of the precursor with 0.1 M solution of HH as a function of the steam quantity in the steam-air flow (1 - 5-6 vol%, 2 -10-11 vol%)

2.1.8.2. A study of the CH3 131I sorption from the steam-air phase by the synthesized composites

To study the localization of CH3 131I from a steam-air flow, we used the procedure and installation described in (Kulyukhin et al., 2007).

In contrast to the molecular iodine sorption, for which the sorption degree was higher than 99% in all cases, the CH3 131I sorption efficiencies of the synthesized composites differ a lot. An increase in the Ag quantity increases the total CH3 131I localization degree. Thus, increasing the Ag quantity from 1 to 8 wt% for the composites prepared by treatment of the precursor with a 0.1 М solution of HH, the localization degree increases from ~1.8% to ~60.2% (Fig. 11A). An analogous picture is also observed for the composites obtained as a result of treatment of the precursors with solutions of HA or ammonia (Fig. 11B).

Analysis of the data on the total CH3 131I sorption on the composites obtained by treatment with 0.1 М solutions of HH and HA, as well as with a 0.5 М solutions of ammonia as a function of the Ag content in the material shows that increasing the Ag concentration in the material increases its sorption capacity. The highest CH3 131I sorption capacity of the composites is observed for the materials obtained by treatment of the precursors with a 0.1 М solution of HA, and the lowest sorption capacity is observed for the samples treated with a 0.5 М solution of ammonia.

For the composites containing 1, 2 and 4 wt% of Ag, the sorption capacity of the precursor is higher (Fig. 12A). For the composite containing 8 wt% of Ag the sorption efficiency of the material obtained by treatment of the precursor with a 0.1 М solution of HA is higher than that of the precursor (Fig. 12B).

Note that for all composites containing 1, 2, and 4 wt.% of Ag, the quantity of the sorbed CH3 131I increases from layer to layer (Fig. 13). The only exception are composites containing 8 wt% of Ag, which display standard dependences; i.e., a decrease in the sorbed CH3 131I along the column length (Fig. 13). The observed picture is likely to be due to a drop in the flow rate in the composite layer because of a rise in its turbulence, which leads to an increase in the time of contact between the gas phase and the composite.

Figure 11.

The efficiency of CH3 131I sorption on the composite materials obtained by treatment of the precursor with a 0.1 М solution of HH (A) and 0.5 M solution of NH4OH (B) as a function of the Ag concentration in the material

Figure 12.

The efficiency of the CH3 131I sorption on the SiO2-2%Ag (A) and SiO2-8%Ag (B) composite materials as a function of the nature of the N-containing compound used for treatment of the precursor (1 - without the modification, 2 - 0.1 М HH, 3 - 0.1 М HA, and 4 - 0.5 М NH4OH)

The obtained data on the CH3 131I sorption are very curious. Ag0 is known not to react with CH3 131I, whereas Ag2O can react with the compound in the presence of water steam by the reaction:

2 C H 3 131 I   + A g 2 O   +   H 2 O Þ 2 A g 131 I   +   2 C H 3 O H E5

Treatment of the precursors with HH and HA solutions leads to the formation of nanometer Ag0 particles in the material, and treatment with NH4OH yields nanometer Ag2O particles, which should suggest that the highest sorption efficiency for CH3 131I would be characteristic of the composites obtained by treatment of the precursors with solutions NH4OH. However in reality, the sorption efficiency of these composites proved to be the lowest. The nanometer Ag0 particles are likely to act as catalysts of the CH3 131I decomposition into CH3 and 131I radicals. In this case, the CH3 can react with the components of the gas phase (oxygen and water steam) to form various volatile organic compounds. In turn, the 131I can form 131I2 in the gas phase, which will be absorbed at a high speed by the silver compounds in the composition of the composites. The smaller the Ag0 particles are the higher their catalytic activity is.

Figure 13.

The 131I layer-by-layer distribution on the column with the composite materials obtained by treatment of the precursor with a 0.1 М solution of HA as a function of the Ag concentration in the material (1 - 1 wt% Ag, 2 - 2 wt% Ag, 3 - 4 wt% Ag, 4 - 8 wt% Ag)

Increasing the concentration of the HH or HA should lead to both an increase in the quantity of nanometer Ag0 or Ag2O particles and their further aggregation. The aggregation will result in the formation of larger particles with a smaller specific surface. In this case, the catalytic activity of the composites should decrease, which can influence their sorption capacity.

Figure 14 shows the data on the total sorption degree for the synthesized composite materials as a function of the concentration of the N-containing compounds and used for treatment of the precursor. As was expected for the SiO2-8%Ag composite obtained by treatment of the precursor with solutions of HH and HA, the sorption degree decreased with an increase in the concentration of the N-containing compound (Fig. 14A). On the other hand, the sorption degree of these materials is higher than that of the precursor. In the case of using NH4OH solutions, the sorption efficiency also decreases with an increase in the concentration of the N-containing compound; however, it is not higher than the sorption capacity of the precursor (Fig. 14B).

Figure 15 shows the data on the 131I layer-by-layer distribution in the columns containing the SiO2-8%Ag composite obtained by treatment of the precursor with solutions of N-containing compounds of different concentrations. Figure 15A shows that increasing the HA (or HH) concentration leads to a noticeable decrease in the CH3 131I sorption in the 1st layer of the materials. Simultaneously, the angle of the sorption front becomes lower. In the case of NH4OH (Fig. 15B), 131I is virtually evenly distributed over the layers, and as in the case of HH and HA, the highest sorption is observed for the lowest NH4OH concentration. Note that in the case of the composites obtained by treatment of the precursor with 1.0 and 2.0 М solutions of NH4OH, the sorption degree increases from layer to layer. The effect is again likely to be due to an increase in the turbulence of the gas flow as it passes through the column, which leads to an increase in the time of contact between the gas phase and the composite.

Figure 14.

The efficiency of the CH3 131I sorption on the SiO2-8%Ag composite, obtained by treatment of the precursor with a solution of HA (A) and NH4OH (B) as a function of the N-containing compounds concentration

Figure 15.

The 131I layer-by-layer distribution on the column with the SiO2-8%Ag composite obtained by treatment of the precursor with a solution of HA (A, 1 - 0.01 M, 2 - 0.05 M, 3 - 0.1 M) and NH4OH (B, 1 - 0.5 M, 2 - 1.0 M, 3 - 2.0 M) as a function of N-containing compound concentration

As established earlier, the degree of the CH3 131I and 131I2 sorption depends on the quantity of radioactive compound supplied to the column.

Figure 16 shows the data on the CH3 131I sorption from the steam-air flow on the mixture (1:1) of composites SiO2-8%Ag obtained by treatment of the precursor with a 0.01 M solution of HH and HA as a function of CH3 131I quantity. As follows from Fig. 16, a tenfold increase in the CH3 131I quantity leads to a decrease in its sorption degree from 99.3% to 95.6%. On the other hand, increasing the CH3 131I quantity from 5 to 10 mg has hardly any effect on the degree of its sorption on the composites. The 131I distribution in the layers changes accordingly. Increasing the CH3 131I quantity lowers the angle of the sorption front. On the other hand, increasing the CH3 131I quantity from 5 to 10 mg gives us virtually identical 131I distribution patterns in the layers of the composites in the column.

Figure 16.

The CH3 131I layer-by-layer distribution on the column with the mixture (1:1) of composites SiO2-8%Ag obtained by treatment of the precursor with a 0.01 M solution of HH and HA as a function of CH3 131I quantity supplied to the column ( 1 - 1 mg, 2 - 5 mg, 3 - 10 mg)

The linear gas flow rate and the related time of contact between the gas phase and the composite also impact the sorption degree. Increasing the linear gas flow rate decreases the time of contact of CH3 131I present in the gas phase with the elements of the composites responsible for its chemosorption (in the synthesized materials, these are nanometer Ag particles).

Figure 17 shows the data on the CH3 131I sorption from the air flow on the composite SiO2-8%Ag obtained by treatment of the precursor with a 0.01 M solution of HA as a function of the linear gas flow rate. A threefold increase in the linear gas flow rate decreases the

Figure 17.

The CH3 131I sorption efficiency on the composite SiO2-8%Ag obtained by treatment of the precursor with a 0.01 M solution of HA as a function of the linear gas flow rate (1 - 4.4 cm/s, 2 - 8.1 cm/s, 3 - 14.8 cm/s)

sorption degree of CH3 131I from 99.9% to 96.5%. The 131I distribution in the layers of the composites in the columns also changed. As follows from Fig. 17, decreasing the linear gas flow rate increases the angle of the CH3 131I sorption front. Thus, increasing the linear gas flow rate from 4.4 to 14.8 cm/s decreases the quantity of 131I in the 1st layer of the composite in the column from ~78 to ~48%. At the same time, the 131I quantity in the 4th layer increased from ~0.2% to ~6.1%.

The findings of the investigations allow us to conclude that the most suitable composite material for CH3 131I localization from the gas flow is SiO2-8%Ag obtained by treatment of the precursor with a 0.01 М solution of HA.

2.2. Composites, containing Ag, Ni, Cu, and Zn

Presently, there is carrying out investigations aiming to produce a new granulated sorbent based on macroporous silica gel containing simultaneously nanometric particles of Ag and Ni (or Zn, or/and Cu) compounds for use in the filtering units of the emergency filters at WWER-1000 nuclear power plants (NPP-2006 project).

2.2.1. Synthesis of composites

The sorbents containing 10 wt% of AgNO3 and Ni(NO3)2 [or Zn(NO3)2, or/and Cu(NO3)2] were prepared by impregnation with an aqueous solution of d-element nitrates with the following treatment by ammonia with the following drying on air at increasing of temperature from 20 to 300º C and next air-conditioning at 300º С.

Composites were synthesized in two stages:

  1. Impregnation of macroporous silica gel with a solution of d-element nitrates in different ratio with the following drying on air at 110º С;

  2. Treatment of precursors with solutions of ammonia with the following drying on air at increasing of temperature from 20 to 300º C and next air-conditioning at 300º С during 4 h.

The quantity of a solution of d-element nitrates, which is necessary for impregnation of silica gel, was taken in an amount ensuring 50% filling of the volume of the silica gels. The volume of silica gel was calculated from its bulk weight, which equal 0.576 kg/m3.

The quantity of d-elements nitrates for synthesis of composites was calculated on the basis of data about necessary d-element concentration in precursor.

The first stage of synthesis of precursors of composites on a basis of macroporous silica gel containing Ag and Ni (or Zn, or/and Cu) was carried out as follows. At intensive mixing a 434 cm3 of a solution of d-element nitrates with necessary concentration was added to 500 g of macroporous silica gel. The obtained mixture was mixed during 60 min for obtaining of uniformity of impregnation of total joint of silica gel with solution of d-element nitrates.

After obtaining of proportional impregnation of total joint of silica gel with solution of d-element nitrates the wet sample was placed in BINDER drier. Precursors were dried on air at temperature 110º С to an air-dry state.

As a result of these operations there was a partial destruction of granules of precursor. Therefore before carrying out of the second stage of synthesis of composites it has been made the fractioning. As result of the fractioning of precursor granules with the size less than 1 mm has been separated. The quantity of the given fraction did not exceed 2-3% from total synthesized joint of precursor.

As a result the precursors, containing 10 wt% of Ag and Ni (or Zn, or/and Cu), on the basis of macroporous silica gel were synthesized.

At the second stage of synthesis of composites the precursors were treated by solution of NH4OH with the following drying on air at increasing of temperature from 20 to 300º C and next air-conditioning at 300º С during 4 h.

In our study 2.0 M water solutions of ammonia were used for treatment of precursors.

The second stage consist on treatment of precursor by solution of 2.0 M solution of NH4OH for obtaining of composites with nanometric particles of different compounds of d-element, was carried out as follows. At intensive mixing the 80 cm3 of 2.0 M solution of NH4OH were added to 100 g air-dry precursor, containing 10 wt% of d-element nitrates. The obtained mixture was mixed during 60 min for obtaining of uniformity of impregnation of joint of precursor with solution of ammonia. During impregnation the colour of precursor changed from green to black for composites containing Ag, Ni or/and Cu, and from light grey to grey for composites containing Ag and Zn.

After obtaining of proportionality of impregnation of total joint of precursor that proved to be true of uniformity of colour, the wet samples were placed in exiccator on 3 h. Through 3 h wet samples were placed in BINDER drier. The wet samples of composites were dried on air at increasing of temperature from 20 to 275-300º С with the following air-conditioning during 4 h at temperature 275-300º С.

As a result of these operations the composites, containing 10 wt% of nanometric particles of different compounds of Ag and Ni (or Zn, or/and Cu), on a basis of macroporous silica gel were obtained (Table 1). The figure in the brackets shows the molar ratio of the metal.

Composites Precursor Composite
wet dried wet dried
SiO2-10%AgNi (1 : 4) green light green black black
SiO2-10%AgCuNi (1.6 : 0.4 : 4) green light green black black
SiO2-10%AgCuNi (1 : 1 : 4) green light green black black
SiO2-10%AgCuNi (0.4 : 1.6 : 4) green light green black black
SiO2-10%AgCu (1 : 4) green light green black black
SiO2-10%AgZn (1 : 4) white light grey grey grey

Table 1.

The colour parameters of the synthesized composites

2.2.2. Analysis of synthesized composites

To determine the total metal content, the composite was treated with concentrated nitric acid for 2 hours. The mother solution was separated from it. The composite was washed with water, and the metal content was then determined. The Ag content in the solutions was measured by titration by the Volgard method. The nickel, copper and zinc contents were determined by direct titration with murexide (Schwarzenbach, 1958).

The amount of the metals in the form of nitrates in the composites was determined by the above methods in the solution which was obtained as a result of treatment of the composite with distilled water for 24 hours. The amount of d-elements in poorly soluble forms in the composite was calculated as the difference between the total concentrations of each metal in the composite and the amounts of the metals in nitrate form.

As a result, we obtained a granulated composites with a Ag content of 0.4÷2.0 wt% and a d-element (Ni, Zn, Cu) content equal to its molar ratio to Ag from 14:1 to 4:1 (Table 1).

2.2.3. Electron microscopy study of synthesized composites

Figure 18 shows the electron micrographs of the composite SiO2-10%AgNi(1:4), obtained using a Philips TEM-301 transmission electron microscope. As shown in Fig. 18, the synthesized materials contain nanometer particles of Ag0 and possibly NiO not larger than 10 nm. As follows from Fig. 18, the amount of nanometer Ag0 and NiO particles is very high. In addition, it is necessary to take into account a low concentration of Ag in the matrix of the composite with a strongly developed surface.

The Ag distribution in the matrix of the composites was studied using their electron probe X-ray microanalysis.

Figure 19 shows a typical microphotograph of the surface of the chip of the granule of the composite, and figure 20 shows the X-ray diffraction spectrum of the sample surface.

Figure 18.

The electron microphotograph of the SiO2-10%AgNi(1:4) composite

Figure 19.

The microphotograph of the surface of the SiO2-10%AgNi(1:4) composite

As follows from Fig. 19, particles not larger than 1 μm are evenly distributed on the granule surface and that the amount of the aggregates larger than 10 μm is relatively small.

An elemental composition study of the surface showed that the composites contained O, Si, Ni, Ag and trace quantity of Na (Fig. 20).

Figure 21 shows the X-ray spectroscopy data on the Ag (A) and Ni (B) distribution on the surface of granules of SiO2-10%AgNi(1:4) composite. The surface of the granules was scanned separately at a radiation power characteristic of Ag or Ni. As follows from Fig. 21, the Ag and Ni are virtually evenly distributed on the surface of the composite granules.

Figure 20.

The X-ray diffraction spectrum of the SiO2-10%AgNi(1:4) composite

Figure 21.

The distribution of Ag (A) and Ni (B) particles on the surface of the granule of the SiO2-10%AgNi(1:4) composite

2.2.4. Thermal gravimetric analysis of synthesized composite

The results of thermal gravimetric analysis of SiO2-10%AgNi(1:4) and SiO2-10%AgCu(1:4) composites are shown in Figs. 22-23. It can be seen that thermal decomposition of the composites is a multistep process accompanied by both evolution and absorption of heat.

As seen from Fig. 22, the patterns of thermal decomposition in air in a platinum crucible of SiO2-10%AgNi(1:4) composite without conditioning during 4 h at 300º C and with it differ essentially. The composite obtained without conditioning during 4 h at 300º C (Fig. 22A) decomposes in two steps, the first of which is apparently associated with endothermic loss of water (65-175º С). The second step is apparently related to partial exothermic decomposition of d-elements and ammonium nitrate (265º С). The total loss of mass was about 30 wt%. At the same time, as follows from Fig. 22B, the composite obtained with conditioning during 4 h at 300º C decomposes without thermal effects. The total loss of mass was about 11 wt%.

As follows from Fig. 23, the character of decomposition of SiO2-10%AgCu(1:4) composite is similar to that for SiO2-10%AgNi(1:4) composite. The SiO2-10%AgCu(1:4) composite also decomposes without thermal effects. The total loss of mass was about 9 wt%.

Figure 22.

Results of thermal gravimetric analysis of SiO2-10%AgNi(1:4) composite without conditioning during 4 h at 300º C (A, sample weight 102.4 mg) and with it (B, sample weight 115.7 mg)

Figure 23.

Results of thermal gravimetric analysis of SiO2-10%AgCu(1:4) composite (sample weight 89.9 mg)

2.2.5. Localization of molecular iodine and methyl iodide from a steam-air flow

To study the localization of CH3 131I and 131I2 from a steam-air flow, we used the procedure and installation described in (Kulyukhin et al., 2007).

Results of the studies of the sorption of CH3 131I and 131I2 from a steam-air flow on developed composites are presented in Table 2. As follows from the Table 2, all composites have high sorption efficiency for CH3 131I and 131I2 in the gas flow. The highest CH3 131I sorption capacity is observed for the SiO2-10AgNi(1:4) composites, and the lowest sorption capacity is observed for the SiO2-10AgCuNi(0.4:1.6:4) composites.

It is necessary note that with increasing of time of the contact between gas flow and composite the sorption efficiency appreciably increases. For example, at increasing of time of the contact between gas flow and SiO2-10%AgNi(1:4) composite from 1 to 5 s the CH3 131I adsorption degree increases from 88.74% to 99.99%.

In conclusion note that synthesized composites containing 10 wt% of Ag and Ni have high sorption efficiency for 131I2 and CH3 131I in the gas flow.

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3. Conclusion

The developed composites do not have analogs in the world and can compete with other sorption materials designed to prevent the release of volatile radioiodine compounds into the environment. In addition, the developed composites can be used for effective localization of volatile chlorine, bromine, and arsenic, as well as polonium radionuclide into the environment.

Composites 131I2, % CH3 131I, %
20oC 20oC 110oC 170oC
SiO2-10%AgNi (1 : 4) 99.95 88.74 97.00 98.28
SiO2-10%AgCuNi (1.6 : 0.4 : 4) 99.98 74.28 96.67 98.58
SiO2-10%AgCuNi (1 : 1 : 4) 99.98 69.04 95.69 96.02
SiO2-10%AgCuNi (0.4 : 1.6 : 4) 99.99 33.71 86.30 86.34
SiO2-10%AgCu (1 : 4) 99.99 64.89 95.38 97.15
SiO2-10%AgZn (1 : 4) 99.97 52.34 90.52 95.32

Table 2.

The sorption of 131I2 (100 mg) and CH3 131I (20 mg) from the air flow on the developed composites containing 10 wt% of d-elements (the surface area of the cross-section of the column - 3.3 cm2; the time of the experiment, including the time of the 131I2 or CH3 131I supply - 4.0 h; the composite particle size - 3.0-6.0 mm, the linear steam-air flow speed in the column - 4-6 cm/s, the time of contact between gas phase and composite - 1 s).

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Acknowledgments

Authors thank Department of Chemistry and Material Science of Russian Academy of Sciences (program of fundamental research № 8 /academician A.Yu.Tsivadze/) for financial support.

References

  1. 1. Asmolov V. G. 1994 Test data of severe accidents at WWER, Atomnaya Energiya (Russia), 76 4 (April 1994), 282 302 , 0004-7163
  2. 2. Bronnikov V. A. 2004 Eksperimentalnye Issledovaniya Protsessov Razrusheniya Aktivnoi Zony Reaktorov LWR Pri Tyazheloi Avarii (Proekt LACOMERA), Atomnaya Tekhnika za Rubezhom (Russia), 11 (November 2004), 16 20 , 0320-9326
  3. 3. Bukrinskii A. M. Fedulov A. F. 1991 International scale of estimation of event risk at NPPs, Atomnaya Energiya (Russia), 70 1 (January 1991), 3 8 , 0004-7163
  4. 4. Charlot G. 1961 Les methods de la chimie analytique. Analyse quantitative minerale, Paris: Masson, 1961, 4th ed. Translated under the title: Metody analiticheskoi khimii. Kolichestvennyi analiz neorganicheskikh soedinenii, 2 1108, Khimiya, Moscow, Russia.
  5. 5. Containment Systems and Components for LOCA and Severe Accident Mitigation 1993 Promotion Materials from "Siemens AG. Power Generation Group (KWU)".
  6. 6. Dillman y. G. Bunz H. 1991 Design of a Filter System for PWR Containment Venting, Journal of Aerosol Science, 22 Supplement 1, S701 S704 , 0021-8502
  7. 7. Dragunov Yu. G. Denisov V. P. 2006 Support of safe operation of WWER unit at NPPs, Atomnaya Energiya (Russia), 101 2 (August 2006), 87 93 , 0004-7163
  8. 8. Evans G. J. Melnyk A. et al. 1990 The LIRIC database/model, Proceeding of 2nd International Conference on Containment Design and Operation, 7.1 7 .20, Toronto, Canada, October 1990.
  9. 9. Friesen E. Meseth J. et al. 2001 Containment behaviour in the event of core melt with gaseous and aerosol releases (CONGA), Nuclear Engineering and Design, 209 1-3 , (November 2001), 253 262 , 0029-5493
  10. 10. Kovalevich O. 2000 What is preferentially: reconstruction or construction?, Journal of Russian Nuclear Society, 1 (March 2000), 34 38 .
  11. 11. Krebs W.-D. 1999 The new generation, Siemens Power Journal, 4 (April 1999), 10 13
  12. 12. Kulyukhin S. A. Mizina L. V. et al. 2007 Sorption of 131I2 and CH3 131I from steam-air phase on porous inorganic sorbents containing d-elements, Radiokhimiya (Russia), 49 2 (April 2007), 156 158 , 0033-8311
  13. 13. Kulyukhin S. A. Kamenskaya A. N. et al. 2008 Chemistry of radioactive iodine in gas phase: fundamental and applied aspects, Radiokhimiya (Russia), 50 1 (January 2008), 3 21 , 0033-8311
  14. 14. Kulyukhin S. A. Kamenskaya A. N. Konovalova N. A. 2011 Chemistry of radioactive iodine in aqueous phases: fundamental and applied aspects, Radiokhimiya (Russia), 53 2 (April 2011), 107 123 , 0033-8311
  15. 15. Particulate Filtration in Nuclear Facilities 1991 Technical Report Series, 241 101, 9-20125-491-1 Vienna, Austria.
  16. 16. Radioiodine Removal in Nuclear Facilities. Methods and Techniques for Normal and Emergencies Situations 1980 Technical Report Series, 201 98, 9-20125-280-3 Vienna, Austria.
  17. 17. Reactor Design 2002 Nuclear Engineering International, Advert. Supplement.
  18. 18. Rogers J. T. 1990 Fission Product Transport Processes in Reactor Accidents, 978-0-89116-876-8 Himespere Publishing, New York, USA.
  19. 19. Schwarzenbach H. 1958 Complexometric titration, In: Complexonometry, N.I. Stupnikova, (Ed.), 104, Goskhimizdat, Moscow, Russia.
  20. 20. State of the art report on iodine chemistry 2007 Report NEA/CSNI. R1
  21. 21. State of the art report on nuclear aerosols 2009 Report NEA/CSNI. R5
  22. 22. State Standard. 16187 7 Sorbents A. method of. determination of. fractional composition. 1970 Committee of standards, measures and measuring devices at Ministerial council of the USSR, Moscow, Russia.
  23. 23. Tomorrow’s reactors 2003 Alternatives, 2 (March 2003), 4 5
  24. 24. Murata T. Kamiya K. 1968 Removal of iodine and methyl iodide by a full-sized charcoal filter, Proceedings of a symposium on operating and developmental experience in the treatment of airborne radioactive wastes, 451 463 , New York, USA, August 26-30, 1968.
  25. 25. Ustinov O. A. Sukhanov L. P. et al. 2005 Incidents at nuclear power plants, ways of their prevention and the localization of the incidents consequences, Russian Chemical Journal, 49 4 (August 2005), 54 60 , 0373-0247
  26. 26. Zeyen R. Clement B. 2006 The PHEBUS Fission Product And Source Term International Programmes, Proceedings of Annual Meeting on Nuclear Technology "AMNT 2006", 234 239 , Aachen, Germany, May 16-18, 2006.

Written By

Sergey Kulyukhin, Lubov Mizina, Igor Rumer and Nikolai Mikheev

Submitted: 09 November 2010 Published: 20 July 2011