<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">AJAC</journal-id><journal-title-group><journal-title>American Journal of Analytical Chemistry</journal-title></journal-title-group><issn pub-type="epub">2156-8251</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ajac.2018.912044</article-id><article-id pub-id-type="publisher-id">AJAC-89215</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Chemistry&amp;Materials Science</subject></subj-group></article-categories><title-group><article-title>
 
 
  Distribution and Accumulation of Major and Trace Elements in Gypsum Samples from Lignite Combustion Power Plant
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Majda</surname><given-names>Pavlin</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Radojko</surname><given-names>Jaćimović</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Andrej</surname><given-names>Stergaršek</given-names></name><xref ref-type="aff" rid="aff3"><sup>3</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Peter</surname><given-names>Frkal</given-names></name><xref ref-type="aff" rid="aff4"><sup>4</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Maja</surname><given-names>Koblar</given-names></name><xref ref-type="aff" rid="aff5"><sup>5</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Milena</surname><given-names>Horvat</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Jozef Stefan International Postgraduate School, Ljubljana, Slovenia</addr-line></aff><aff id="aff2"><addr-line>Department of Environmental Sciences, Jozef Stefan Institute, Ljubljana, Slovenia</addr-line></aff><aff id="aff4"><addr-line>Department of Inorganic Chemistry and Technology, Jozef Stefan Institute, Ljubljana, Slovenia</addr-line></aff><aff id="aff5"><addr-line>Center for Electron Microscopy and Microanalysis, Jozef Stefan Institute, Ljubljana, Slovenia</addr-line></aff><aff id="aff3"><addr-line>KEMEK d.o.o., Ljubljana, Slovenia</addr-line></aff><pub-date pub-type="epub"><day>04</day><month>12</month><year>2018</year></pub-date><volume>09</volume><issue>12</issue><fpage>602</fpage><lpage>621</lpage><history><date date-type="received"><day>24,</day>	<month>October</month>	<year>2018</year></date><date date-type="rev-recd"><day>15,</day>	<month>December</month>	<year>2018</year>	</date><date date-type="accepted"><day>18,</day>	<month>December</month>	<year>2018</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  Flue gas containing volatile elements, fine fly ash particulates not retained by particle control devices, and limestone are the most important sources of trace and major elements (TMEs) in wet flue gas desulphurization (WFGD) gypsum. In this study, samples of gypsum slurry were separated into fine and coarse fractions. Multi-elemental analysis of 45 elements in the different size fractions of gypsum, slurry waters and lignite were performed by 
  k
  <sub>0</sub>-INAA (
  k
  <sub>0</sub>-instrumental neutron activation analyses). The study found that the volatile elements (Hg, Se and halogens) in the flue gas accumulate in the fine fractions of gypsum. Moreover, the concentrations of most TMEs are considerably higher in the fine fractions compared to the coarse fractions. The exceptions are Ca and Sr that primarily originate from the limestone. Variations of TMEs in the finer fractions are dependent on the presence of CaSO
  <sub>4</sub>&#183;2H
  <sub>2</sub>O that is the main constituent of the coarse fraction. Consequently, the content of TMEs in the fine fraction is highly dependent on the efficiency of separating the fine fraction from the coarse fraction. Separation of the finer fraction, representing about 10% of the total gypsum, offers the possibility to remove effectively TMEs from WFGD slurry.
 
</p></abstract><kwd-group><kwd>Trace and Major Elements</kwd><kwd>Wet Flue Gas Desulphurization Gypsum</kwd><kwd> Particle Size Fractions</kwd><kwd> Mercury and Selenium</kwd><kwd> Sample Preparation</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Coal combustion is the major source of airborne Hg, Mo and Se, and is a significant source of As, Cr, Mn, Sb and Tl [<xref ref-type="bibr" rid="scirp.89215-ref1">1</xref>] . Not only trace elements, but also SO<sub>2</sub>, NO<sub>x</sub>, CO<sub>2</sub>, N<sub>2</sub>O, particulate matter and various gases are released into the environment by coal burning [<xref ref-type="bibr" rid="scirp.89215-ref2">2</xref>] . In general, the elements present in coal occur over a wide concentration range that varies according to the geochemical evolution of the coal deposits [<xref ref-type="bibr" rid="scirp.89215-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref7">7</xref>] . Based on their concentrations, chemical elements in coal are classified into three groups [<xref ref-type="bibr" rid="scirp.89215-ref8">8</xref>] with further division of trace elements according to their volatility [<xref ref-type="bibr" rid="scirp.89215-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref11">11</xref>] . The volatility of trace elements is the result of several factors: affinity to other elements, their physical properties, chemical reactions and transformations [<xref ref-type="bibr" rid="scirp.89215-ref11">11</xref>] , but it also depends on the combustion setup (e.g. combustion temperature, time of exposure, ash generation) [<xref ref-type="bibr" rid="scirp.89215-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref12">12</xref>] . Volatile elements are preferentially concentrated on the smallest particles due to condensation [<xref ref-type="bibr" rid="scirp.89215-ref11">11</xref>] whereas the non-volatile ones deposit on the largest ash particles [<xref ref-type="bibr" rid="scirp.89215-ref13">13</xref>] . As a result, the finest fly ash particles contain larger amounts of (trace) elements, due to their greater surface to volume ratio [<xref ref-type="bibr" rid="scirp.89215-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref14">14</xref>] .</p><p>Important sources of trace and major elements (TMEs) in the gypsum slurry are attributed to the flue gas with fly ash particles [<xref ref-type="bibr" rid="scirp.89215-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref15">15</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref16">16</xref>] not retained in the particle control devices [<xref ref-type="bibr" rid="scirp.89215-ref17">17</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref18">18</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref19">19</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref20">20</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref21">21</xref>] and limestone added to the wet flue gas desulphurisation (WFGD) system [<xref ref-type="bibr" rid="scirp.89215-ref22">22</xref>] . Small particles pass through the electrostatic precipitator (ESP), reach the WFGD device and are retained there due to adsorption, co-precipitation or other chemical reactions [<xref ref-type="bibr" rid="scirp.89215-ref23">23</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref24">24</xref>] . Although trace elements are greatly accumulated in gypsum [<xref ref-type="bibr" rid="scirp.89215-ref15">15</xref>] , a smaller amount is emitted to the atmosphere through the stack gas [<xref ref-type="bibr" rid="scirp.89215-ref13">13</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref20">20</xref>] . The control of emissions in the gaseous phase and small particulates is very important. In power plants equipped with WFGD systems, both emissions are reduced [<xref ref-type="bibr" rid="scirp.89215-ref11">11</xref>] .</p><p>Gypsum as a by-product of the WFGD process is important in terms of its disposal in landfills and/or for its further production and use [<xref ref-type="bibr" rid="scirp.89215-ref25">25</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref26">26</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref27">27</xref>] . Typically, it is mostly composed of CaSO<sub>4</sub>・2H<sub>2</sub>O [<xref ref-type="bibr" rid="scirp.89215-ref27">27</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref28">28</xref>] and minor amounts of silica, alumina, iron oxide, and other minerals [<xref ref-type="bibr" rid="scirp.89215-ref27">27</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref29">29</xref>] . Many pollutants in a gaseous form and/or as particulate matter are partitioned into solid and water streams of gypsum slurry. Under operational conditions of water recirculation from gypsum slurry, some inorganic trace pollutants are enriched in recirculated water streams by dissolution. After a number of cycles, inorganic trace pollutants may reach equilibrium and subsequent saturation in the water stream [<xref ref-type="bibr" rid="scirp.89215-ref30">30</xref>] . Distribution of TMEs during the coal combustion process has been extensively studied [<xref ref-type="bibr" rid="scirp.89215-ref17">17</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref20">20</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref31">31</xref>] - [<xref ref-type="bibr" rid="scirp.89215-ref39">39</xref>] . On the other hand, there are only a few studies describing accumulation of elements in gypsum or gypsum slurry [<xref ref-type="bibr" rid="scirp.89215-ref15">15</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref16">16</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref30">30</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref40">40</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref41">41</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref42">42</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref43">43</xref>] .</p><p>Lignite burning Šoštanj thermal power plant (Šoštanj TPP, Slovenia) is studied in this paper. We previously examined the importance of particle size regarding mercury accumulation in WFGD gypsum from a Šoštanj TPP. Grain size distribution revealed a significantly higher proportion of Hg in smaller particles where 12% of the finest fraction contains 63% of the mercury [<xref ref-type="bibr" rid="scirp.89215-ref28">28</xref>] . In the present work, in addition to mercury, the concentrations of 44 other trace and major elements (TMEs) were determined in various size fractions of gypsum. Instead of studying all water streams relating to the WFGD system, the focus was on particles in the gypsum slurry samples (gypsum). Although bulk gypsum is typically used to characterize gypsum samples, in our work all gypsum slurry samples were separated into fine (recirculated gypsum slurry) and coarse (mostly consisted of CaSO<sub>4</sub>・2H<sub>2</sub>O) fractions. Our study revealed several important findings with regards to the distribution pattern, accumulation and sources of TMEs in the different particle size fractions. We have had also emphasized the importance of proper sample preparation when separating gypsum slurry into fine and coarse fractions.</p></sec><sec id="s2"><title>2. Materials and Methods</title><sec id="s2_1"><title>2.1. Study Site</title><p>To carry out the analysis and distribution pattern of TMEs, lignite burning Šoštanj TPP Slovenia have selected for the identification of TMEs. Šoštanj TPP used to have five power blocks with combined power of 775 MW. It uses lignite from the local mine Velenje as a fuel with a heating value of 9.5 MJ・kg<sup>−1</sup>. The consumption rate is between 3.5 and 4.2 million tons per year. There are two WFGD units for removing SO<sub>2</sub>, the first covering blocks 1 through 4, while the second covers block 5 (http://www.te-sostanj.si/en/presentation/history). In this study our main concern are focused on block 5. All WFGD systems use the wet limestone process with forced oxidation and are equipped with ESP.</p></sec><sec id="s2_2"><title>2.2. Sample Description</title><p>Lignite samples (LIG) and three different gypsum slurries were taken from the batch of block 5, Šoštanj TPP. All samples were separately recorded, labelled and collected. The preparation procedures for those samples are described below (Section 2.2.1). The data of multi-elemental analyses for bulk gypsum (a mixture of finer and coarse fraction) and limestone were taken from previous work [<xref ref-type="bibr" rid="scirp.89215-ref28">28</xref>] .</p><sec id="s2_2_1"><title>2.2.1. Preparation of Lignite Sample</title><p>LIG was sampled in 2012 from a conveyer belt during a normal working day to ensure representative sample. The combined mass of the obtained samples was ~3 kg. The samples were dried and maintained a fixed weight at 38˚C for one week in an electric drier/oven (MEMMERT UFE 500). After the drying process, they were ground with a ball mill and sieved with a Fritsch Pulverisette 0 Vibratory Micro Mill to a particle size of less than ~250 &#181;m.</p></sec><sec id="s2_2_2"><title>2.2.2. Preparation of Gypsum Samples</title><p>Three samples of gypsum slurry were drawn from the agitated tank of the WFGD absorber (main scrubber, block 5). Representative samples were taken, when the process in the desulphurisation scrubber was in a steady state. In this paper, the terms gypsum slurry, gypsum and slurry water are used. Gypsum slurry represents total slurry (liquid together with solids) while gypsum consists only of moist solid fraction (a mixture of coarse and finer fraction). The solid fraction in gypsum slurry is settled and slurry water represents the liquid above the solid fraction that contains dissolved pollutants together with small particles, typically not seen or only seen as an opaque solution. Each slurry was separated using size selective fraction into fine and coarse fractions. Two different separation techniques were adopted for this procedure:</p><p>1) In the first approach, separation of gypsum slurry particles with the help of a hydrocyclone (pilot version, laboratory set-up, <xref ref-type="fig" rid="fig1">Figure 1</xref>) into a fine fraction (FF) and coarse fraction (CF) labelled as TEŠ5-FF and TEŠ5-CF. Using centrifugal force, fractions were separated such that denser CF settles at the bottom (underflow, TEŠ5-CF) and a lighter FF at the top (overflow, TEŠ5-FF), of which the latter in actual WFGD hydrocyclone systems is recirculated back into the agitated tank as recirculated slurry. In addition, slurry water was also subjected for elemental analysis (TEŠ5-W<sub>1</sub>, TEŠ5-W<sub>2</sub>). Samples of the above process were carefully collected and stored in May 2013.</p><p>2) The second separation involved two samples. Gypsum slurries were homogenised by shaking, and left 72 hours to settle until two well-defined layers were formed. While the bottom layer consolidated rather quickly, it took several hours for the upper layer to separate particulates from clear water phases. After decantation, the water layer was extracted with a pipette yielding a creamy brown material. Using this approach, two particulate fractions were obtained, labelled as TEŠ5-FF1 and TEŠ5-CF1 for the first sample and TEŠ5-FF2 and TEŠ5-CF2 for the second sample. Samples were collected in December 2013 and January 2014. In this case, slurry water was not obtained for further analysis.</p></sec><sec id="s2_2_3"><title>2.2.3. Characterisation of Gypsum Samples</title><p>1) Grain size distribution</p><p>Grain size distribution of samples was done using Microtrac PSA FRA 9200 which is based on Fraunhofer laser diffraction method. All fractions were subjected to air-dry and maintained constant weight at 38˚C in an electric drier/oven (MEMMERT UFE 500). After drying, samples were homogenised in agate containers of a planetary mill (Fritsch planetary mill Pulverisette 7).</p><p>2) Morphological characteristic study using scanning electron microscopy (SEM)</p><p>Structure and morphological signature characteristics of samples (FF and CF of gypsum) were detailed studies with SEM (JEOL JSM-7600F) equipped with an energy dispersive spectrometer (EDS) (Oxford INCA 350). The samples were mounted and fixed using carbon tape and coated with amorphous carbon using an evaporation device (Balzers CED) before their size, morphology and chemical</p><p>characterisation were analysed. The images were obtained with 5 kV accelerating voltage and 0.1 pA electron beam currents, and measured with an inside column Faraday cup.</p><p>3) Multi-elemental Analysis of Lignite, Process Water and Gypsum Samples Using k<sub>0</sub>-INAA</p><p>Determination of major, minor and trace elements was carried out with k<sub>0</sub>-standardisation method of instrumental neutron activation analysis (k<sub>0</sub>-INAA). For k<sub>0</sub>-INAA purposes, homogenised samples (~150 - 200 mg) were sealed into pure polyethylene ampoules (SPRONK system, Netherland ), stacked together in sandwich form with standard Al-0.1%Au alloy (IRMM-530R alloy) and irradiated in the 250 kW TRIGA Mark II reactor of the Jožef Stefan Institute (JSI) in Ljubljana, Slovenia. In the k<sub>0</sub>-INAA, the standard for all elements is Au. All relevant nuclear data for the method are summarized in the form of Excel file, which is available at http://www.kayzero.com/k0naa/k0naaorg/Nuclear_Data_SC/Entries/2016/1/11_New_k0-data_Library_2015.html. Data are regularly updated and recommended to use by the k<sub>0</sub>-NDSC (k<sub>0</sub>-Nuclear Data Subcommittee) as it is presented in Ref [<xref ref-type="bibr" rid="scirp.89215-ref44">44</xref>] . Depending on the purpose of the analysis, typically two irradiations were performed in the carousel facility of the TRIGA reactor at a thermal neutron flux of 1.1 &#215; 10<sup>12</sup> cm<sup>−2</sup>・s<sup>−1</sup>: short irradiation (up to a few minutes) to determine elements via their corresponding short half-life radionuclides, and second irradiation (up to 12 hours) to determine elements via their corresponding medium/long half-life radionuclides. For QA/QC purposes, the certified reference material BCR-320R Channel Sediment was used. Our results we presented graphically on <xref ref-type="fig" rid="fig2">Figure 2</xref>, where good agreement between k<sub>0</sub>-INAA data and certified values can be seen.</p><p>After irradiation and appropriate cooling time, the samples were measured on absolutely calibrated HPGe detectors (40% and 45% relative efficiency). For peak area evaluation, the HyperLab program was used. For elemental content determinations and effective solid angle calculations, the software package Kayzero for Windows was used [<xref ref-type="bibr" rid="scirp.89215-ref45">45</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref46">46</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref47">47</xref>] .</p><p>The k<sub>0</sub>-INAA at the Department of Environment Sciences of the JSI is accredited according ISO/IEC 17025:2005 since 2009 under accreditation certificate LP-090 awarded by Slovenian Accreditation (SA). The Annex to the accreditation certificate LP-090 dated on 21. March 2018 is available at http://www.slo-akreditacija.si/acreditation/institut-jozef-stefan/. Under the scope of accreditation, the k<sub>0</sub>-INAA is accredited for 31 elements in different matrices as follows: soil, sediment, ores, sewage sludge, biological samples, foodstuffs and fuels.</p></sec></sec></sec><sec id="s3"><title>3. Results and Discussion</title><p>The data obtained for total elemental concentrations and corresponding uncertainties in LIG sample, limestone, slurry waters, bulk and various CF and FF of gypsum are presented in <xref ref-type="table" rid="table1">Table 1</xref> and <xref ref-type="table" rid="table2">Table 2</xref>. In most papers, data are available for a limited number of elements, while the present study provides information for 45 elements, including some strategically important rare earth elements (REEs) that are rarely discussed. The results are concentrated and discussed based on 1) the properties of FF and CF of gypsum samples, 2) enrichment of elements in FF with respect to the CF of gypsum, 3) input of elements with limestone as a source of TMEs into the system, and 4) a comparison between FF and CF versus LIG, and evaluation among the different preparation procedures.</p><table-wrap-group id="1"><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Elemental content with combined standard uncertainty (mg・kg<sup>−1</sup>) in coal (LIG), limestone, slurry waters (FGD-W<sub>1</sub> and FGD-W<sub>2</sub>) and in bulk gypsum obtained by k<sub>0</sub>-instrumental neutron activation analyses (k<sub>0</sub>-INAA). Multi-elemental analysis was done for 45 elements where Hg in limestone and bulk gypsum were measured by CVAAS</title></caption><table-wrap id="1_1"><table><tbody><thead><tr><th align="center" valign="middle"  colspan="11"  >Concentration of elements in different fractions and their uncertainties</th></tr></thead><tr><td align="center" valign="middle" ></td><td align="center" valign="middle"  colspan="2"  >Lignite (LIG)</td><td align="center" valign="middle"  colspan="2"  >Limestone</td><td align="center" valign="middle"  colspan="2"  >FGD-W<sub>1</sub></td><td align="center" valign="middle"  colspan="2"  >FGD-W<sub>2</sub></td><td align="center" valign="middle"  colspan="2"  >Bulk gypsum</td></tr><tr><td align="center" valign="middle" >Ag</td><td align="center" valign="middle" ><sup>a</sup>0.12</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>0.02</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>0.003</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>0.003</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>0.1</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >Al</td><td align="center" valign="middle" >22,200</td><td align="center" valign="middle" >800</td><td align="center" valign="middle" ><sup>a</sup>2430</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>3.00</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>2.50</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >7650</td><td align="center" valign="middle" >280</td></tr><tr><td align="center" valign="middle" >As</td><td align="center" valign="middle" >8.19</td><td align="center" valign="middle" >0.30</td><td align="center" valign="middle" >1.32</td><td align="center" valign="middle" >0.05</td><td align="center" valign="middle" ><sup>a</sup>0.03</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>0.04</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >7.52</td><td align="center" valign="middle" >0.27</td></tr><tr><td align="center" valign="middle" >Au</td><td align="center" valign="middle" ><sup>a</sup>0.0008</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>0.0003</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>0.0002</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>0.0001</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>0.001</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >Ba</td><td align="center" valign="middle" >122</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >19.9</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" ><sup>a</sup>0.20</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>0.15</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >48.8</td><td align="center" valign="middle" >2.1</td></tr></tbody></table></table-wrap><table-wrap id="1_2"><table><tbody><thead><tr><th align="center" valign="middle" >Br</th><th align="center" valign="middle" >6.19</th><th align="center" valign="middle" >0.23</th><th align="center" valign="middle" >0.29</th><th align="center" valign="middle" >0.01</th><th align="center" valign="middle" >55.8</th><th align="center" valign="middle" >2.0</th><th align="center" valign="middle" >60.3</th><th align="center" valign="middle" >2.1</th><th align="center" valign="middle" >18.8</th><th align="center" valign="middle" >0.7</th></tr></thead><tr><td align="center" valign="middle" >Ca</td><td align="center" valign="middle" >19,400</td><td align="center" valign="middle" >700</td><td align="center" valign="middle" >365,000</td><td align="center" valign="middle" >13,000</td><td align="center" valign="middle" >519</td><td align="center" valign="middle" >25</td><td align="center" valign="middle" >544</td><td align="center" valign="middle" >25</td><td align="center" valign="middle" >200,000</td><td align="center" valign="middle" >7000</td></tr><tr><td align="center" valign="middle" >Cd</td><td align="center" valign="middle" ><sup>a</sup>0.50</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>0.33</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>0.07</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>0.14</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>0.85</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >Ce</td><td align="center" valign="middle" >14.5</td><td align="center" valign="middle" >0.5</td><td align="center" valign="middle" >2.03</td><td align="center" valign="middle" >0.08</td><td align="center" valign="middle" ><sup>a</sup>0.01</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>0.01</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >4.61</td><td align="center" valign="middle" >0.17</td></tr><tr><td align="center" valign="middle" >Cl</td><td align="center" valign="middle" >69.9</td><td align="center" valign="middle" >7.4</td><td align="center" valign="middle" ><sup>a</sup>6.20</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >962</td><td align="center" valign="middle" >35</td><td align="center" valign="middle" >958</td><td align="center" valign="middle" >34</td><td align="center" valign="middle" >409</td><td align="center" valign="middle" >16</td></tr><tr><td align="center" valign="middle" >Co</td><td align="center" valign="middle" >3.07</td><td align="center" valign="middle" >0.11</td><td align="center" valign="middle" >0.37</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.082</td><td align="center" valign="middle" >0.003</td><td align="center" valign="middle" >0.066</td><td align="center" valign="middle" >0.003</td><td align="center" valign="middle" >1.04</td><td align="center" valign="middle" >0.04</td></tr><tr><td align="center" valign="middle" >Cr</td><td align="center" valign="middle" >20.8</td><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >6.94</td><td align="center" valign="middle" >0.27</td><td align="center" valign="middle" ><sup>a</sup>0.01</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>0.005</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >24.3</td><td align="center" valign="middle" >0.90</td></tr><tr><td align="center" valign="middle" >Cs</td><td align="center" valign="middle" >3.26</td><td align="center" valign="middle" >0.11</td><td align="center" valign="middle" >0.34</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.0008</td><td align="center" valign="middle" >0.0002</td><td align="center" valign="middle" >0.0011</td><td align="center" valign="middle" >0.0002</td><td align="center" valign="middle" >1.38</td><td align="center" valign="middle" >0.05</td></tr><tr><td align="center" valign="middle" >Dy</td><td align="center" valign="middle" ><sup>a</sup>0.35</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >0.35</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" ><sup>a</sup>0.02</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>0.02</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >0.56</td><td align="center" valign="middle" >0.02</td></tr><tr><td align="center" valign="middle" >Eu</td><td align="center" valign="middle" >0.31</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.06</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" ><sup>a</sup>0.0002</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>0.0002</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >0.11</td><td align="center" valign="middle" >0.01</td></tr><tr><td align="center" valign="middle" >Fe</td><td align="center" valign="middle" >15,600</td><td align="center" valign="middle" >500</td><td align="center" valign="middle" >1060</td><td align="center" valign="middle" >40</td><td align="center" valign="middle" ><sup>a</sup>0.55</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>0.40</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >5320</td><td align="center" valign="middle" >190</td></tr><tr><td align="center" valign="middle" >Ga</td><td align="center" valign="middle" ><sup>a</sup>0.80</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >0.45</td><td align="center" valign="middle" >0.03</td><td align="center" valign="middle" ><sup>a</sup>0.50</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>0.50</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >2.91</td><td align="center" valign="middle" >0.12</td></tr><tr><td align="center" valign="middle" >Hf</td><td align="center" valign="middle" >0.66</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >0.14</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" ><sup>a</sup>0.0005</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>0.0001</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >0.24</td><td align="center" valign="middle" >0.01</td></tr><tr><td align="center" valign="middle" >Hg</td><td align="center" valign="middle" >0.119</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" ><sup>b</sup>0.0054</td><td align="center" valign="middle" >0.0005</td><td align="center" valign="middle" ><sup>a</sup>0.02</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>0.02</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >0.95</td><td align="center" valign="middle" >0.09</td></tr><tr><td align="center" valign="middle" >I</td><td align="center" valign="middle" ><sup>a</sup>5.00</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>0.95</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >24.6</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >24.3</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >7.17</td><td align="center" valign="middle" >0.45</td></tr><tr><td align="center" valign="middle" >In</td><td align="center" valign="middle" >/</td><td align="center" valign="middle" >/</td><td align="center" valign="middle" ><sup>a</sup>0.005</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>0.001</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >0.002</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>0.01</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >K</td><td align="center" valign="middle" >2890</td><td align="center" valign="middle" >110</td><td align="center" valign="middle" >383</td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >53.4</td><td align="center" valign="middle" >8.5</td><td align="center" valign="middle" >57.1</td><td align="center" valign="middle" >9.1</td><td align="center" valign="middle" >1920</td><td align="center" valign="middle" >70</td></tr><tr><td align="center" valign="middle" >La</td><td align="center" valign="middle" >7.34</td><td align="center" valign="middle" >0.27</td><td align="center" valign="middle" >1.49</td><td align="center" valign="middle" >0.06</td><td align="center" valign="middle" ><sup>a</sup>0.002</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>0.002</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >3.18</td><td align="center" valign="middle" >0.12</td></tr><tr><td align="center" valign="middle" >Mg</td><td align="center" valign="middle" >4160</td><td align="center" valign="middle" >240</td><td align="center" valign="middle" ><sup>a</sup>1380</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >2600</td><td align="center" valign="middle" >90</td><td align="center" valign="middle" >2590</td><td align="center" valign="middle" >90</td><td align="center" valign="middle" >4450</td><td align="center" valign="middle" >180</td></tr><tr><td align="center" valign="middle" >Mn</td><td align="center" valign="middle" >600</td><td align="center" valign="middle" >20</td><td align="center" valign="middle" >37.6</td><td align="center" valign="middle" >1.4</td><td align="center" valign="middle" >15.3</td><td align="center" valign="middle" >0.5</td><td align="center" valign="middle" >14.8</td><td align="center" valign="middle" >0.5</td><td align="center" valign="middle" >46.5</td><td align="center" valign="middle" >1.6</td></tr><tr><td align="center" valign="middle" >Mo</td><td align="center" valign="middle" >11.3</td><td align="center" valign="middle" >0.5</td><td align="center" valign="middle" ><sup>a</sup>0.19</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >0.40</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >0.41</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >2.61</td><td align="center" valign="middle" >0.23</td></tr><tr><td align="center" valign="middle" >Na</td><td align="center" valign="middle" >1370</td><td align="center" valign="middle" >50</td><td align="center" valign="middle" >90.9</td><td align="center" valign="middle" >3.2</td><td align="center" valign="middle" >140</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >149</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >431</td><td align="center" valign="middle" >15</td></tr><tr><td align="center" valign="middle" >Nd</td><td align="center" valign="middle" >6.92</td><td align="center" valign="middle" >0.32</td><td align="center" valign="middle" >2.30</td><td align="center" valign="middle" >0.17</td><td align="center" valign="middle" ><sup>a</sup>0.02</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>0.02</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >3.72</td><td align="center" valign="middle" >0.35</td></tr><tr><td align="center" valign="middle" >Rb</td><td align="center" valign="middle" >25.5</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >2.84</td><td align="center" valign="middle" >0.18</td><td align="center" valign="middle" >0.12</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.16</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >13.6</td><td align="center" valign="middle" >0.5</td></tr><tr><td align="center" valign="middle" >S</td><td align="center" valign="middle" ><sup>a</sup>2450</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>6030</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >3300</td><td align="center" valign="middle" >478</td><td align="center" valign="middle" >2980</td><td align="center" valign="middle" >479</td><td align="center" valign="middle" >143,000</td><td align="center" valign="middle" >14,600</td></tr><tr><td align="center" valign="middle" >Sb</td><td align="center" valign="middle" >2.07</td><td align="center" valign="middle" >0.07</td><td align="center" valign="middle" >0.21</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.0060</td><td align="center" valign="middle" >0.0003</td><td align="center" valign="middle" >0.0064</td><td align="center" valign="middle" >0.0003</td><td align="center" valign="middle" >0.75</td><td align="center" valign="middle" >0.03</td></tr><tr><td align="center" valign="middle" >Sc</td><td align="center" valign="middle" >4.74</td><td align="center" valign="middle" >0.13</td><td align="center" valign="middle" >0.42</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" ><sup>a</sup>0.00004</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>0.00001</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >1.57</td><td align="center" valign="middle" >0.06</td></tr><tr><td align="center" valign="middle" >Se</td><td align="center" valign="middle" >0.79</td><td align="center" valign="middle" >0.03</td><td align="center" valign="middle" ><sup>a</sup>0.04</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >0.23</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.23</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >8.37</td><td align="center" valign="middle" >0.30</td></tr><tr><td align="center" valign="middle" >Sm</td><td align="center" valign="middle" >1.40</td><td align="center" valign="middle" >0.05</td><td align="center" valign="middle" >0.33</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" ><sup>a</sup>0.004</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>0.004</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >0.60</td><td align="center" valign="middle" >0.02</td></tr><tr><td align="center" valign="middle" >Sr</td><td align="center" valign="middle" >103</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >366</td><td align="center" valign="middle" >13</td><td align="center" valign="middle" >2.20</td><td align="center" valign="middle" >0.13</td><td align="center" valign="middle" >2.71</td><td align="center" valign="middle" >0.13</td><td align="center" valign="middle" >168</td><td align="center" valign="middle" >7</td></tr><tr><td align="center" valign="middle" >Ta</td><td align="center" valign="middle" >0.21</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.020</td><td align="center" valign="middle" >0.002</td><td align="center" valign="middle" ><sup>a</sup>0.0005</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>0.0005</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >0.08</td><td align="center" valign="middle" >0.003</td></tr><tr><td align="center" valign="middle" >Tb</td><td align="center" valign="middle" >0.19</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.052</td><td align="center" valign="middle" >0.002</td><td align="center" valign="middle" ><sup>a</sup>0.0005</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>0.0003</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >0.087</td><td align="center" valign="middle" >0.003</td></tr><tr><td align="center" valign="middle" >Th</td><td align="center" valign="middle" >2.88</td><td align="center" valign="middle" >0.10</td><td align="center" valign="middle" >0.32</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" ><sup>a</sup>0.0005</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>0.0005</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >0.99</td><td align="center" valign="middle" >0.04</td></tr><tr><td align="center" valign="middle" >Ti</td><td align="center" valign="middle" >815</td><td align="center" valign="middle" >73</td><td align="center" valign="middle" ><sup>a</sup>250</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>14.0</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>13.0</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >282</td><td align="center" valign="middle" >31</td></tr><tr><td align="center" valign="middle" >U</td><td align="center" valign="middle" >8.94</td><td align="center" valign="middle" >0.32</td><td align="center" valign="middle" >4.55</td><td align="center" valign="middle" >0.16</td><td align="center" valign="middle" >0.13</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.103</td><td align="center" valign="middle" >0.004</td><td align="center" valign="middle" >5.11</td><td align="center" valign="middle" >0.18</td></tr><tr><td align="center" valign="middle" >V</td><td align="center" valign="middle" >34.2</td><td align="center" valign="middle" >1.40</td><td align="center" valign="middle" >13.5</td><td align="center" valign="middle" >1.4</td><td align="center" valign="middle" >0.18</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >0.23</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >29.0</td><td align="center" valign="middle" >1.2</td></tr><tr><td align="center" valign="middle" >W</td><td align="center" valign="middle" >0.80</td><td align="center" valign="middle" >0.08</td><td align="center" valign="middle" >0.04</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" ><sup>a</sup>0.05</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>0.07</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >0.29</td><td align="center" valign="middle" >0.02</td></tr><tr><td align="center" valign="middle" >Yb</td><td align="center" valign="middle" >0.57</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >0.18</td><td align="center" valign="middle" >0.001</td><td align="center" valign="middle" ><sup>a</sup>0.001</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>0.001</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >0.33</td><td align="center" valign="middle" >0.01</td></tr><tr><td align="center" valign="middle" >Zn</td><td align="center" valign="middle" >49.0</td><td align="center" valign="middle" >1.70</td><td align="center" valign="middle" >4.74</td><td align="center" valign="middle" >0.21</td><td align="center" valign="middle" >0.22</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.08</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >30.9</td><td align="center" valign="middle" >1.1</td></tr><tr><td align="center" valign="middle" >Zr</td><td align="center" valign="middle" ><sup>a</sup>14.5</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>5.06</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>0.35</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>0.25</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>9.5</td><td align="center" valign="middle" >-</td></tr></tbody></table></table-wrap></table-wrap-group><p><sup>a</sup> bresults obtained by CVAAS (Stergaršek et al., 2008).</p><table-wrap-group id="2"><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Elemental content with combined standard uncertainty (mg・kg<sup>−1</sup>) in gypsum samples (TEŠ5-FF, TEŠ5-CF, TEŠ5-FF1, TEŠ5-CF1, TEŠ5-FF2 and TEŠ5-CF2) obtained by k<sub>0</sub>-instrumental neutron activation analyses. Multi-elemental analysis was done for 45 elements</title></caption><table-wrap id="2_1"><table><tbody><thead><tr><th align="center" valign="middle" ></th><th align="center" valign="middle"  colspan="3"  >TEŠ5-CF</th><th align="center" valign="middle"  colspan="4"  >TEŠ5-FF</th><th align="center" valign="middle"  colspan="4"  >TEŠ5-CF1</th><th align="center" valign="middle"  colspan="4"  >TEŠ5-FF1</th><th align="center" valign="middle"  colspan="4"  >TEŠ5-CF2</th><th align="center" valign="middle"  colspan="4"  >TEŠ5-FF2</th><th align="center" valign="middle" ></th></tr></thead><tr><td align="center" valign="middle" >Ag</td><td align="center" valign="middle" ><sup>a</sup>0.07</td><td align="center" valign="middle"  colspan="2"  >-</td><td align="center" valign="middle"  colspan="2"  ><sup>a</sup>0.21</td><td align="center" valign="middle"  colspan="2"  >-</td><td align="center" valign="middle"  colspan="2"  ><sup>a</sup>0.04</td><td align="center" valign="middle"  colspan="2"  >-</td><td align="center" valign="middle"  colspan="2"  ><sup>a</sup>0.27</td><td align="center" valign="middle"  colspan="2"  >-</td><td align="center" valign="middle"  colspan="2"  ><sup>a</sup>0.04</td><td align="center" valign="middle"  colspan="2"  >-</td><td align="center" valign="middle"  colspan="2"  ><sup>a</sup>0.33</td><td align="center" valign="middle"  colspan="2"  >-</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >Al</td><td align="center" valign="middle" >1000</td><td align="center" valign="middle"  colspan="2"  >40</td><td align="center" valign="middle"  colspan="2"  >52,100</td><td align="center" valign="middle"  colspan="2"  >1800</td><td align="center" valign="middle"  colspan="2"  >544</td><td align="center" valign="middle"  colspan="2"  >20</td><td align="center" valign="middle"  colspan="2"  >42,200</td><td align="center" valign="middle"  colspan="2"  >1500</td><td align="center" valign="middle"  colspan="2"  >650</td><td align="center" valign="middle"  colspan="2"  >23</td><td align="center" valign="middle"  colspan="2"  >67,500</td><td align="center" valign="middle"  colspan="2"  >2400</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >As</td><td align="center" valign="middle" >0.93</td><td align="center" valign="middle"  colspan="2"  >0.04</td><td align="center" valign="middle"  colspan="2"  >39.4</td><td align="center" valign="middle"  colspan="2"  >1.4</td><td align="center" valign="middle"  colspan="2"  >0.74</td><td align="center" valign="middle"  colspan="2"  >0.03</td><td align="center" valign="middle"  colspan="2"  >42.5</td><td align="center" valign="middle"  colspan="2"  >1.5</td><td align="center" valign="middle"  colspan="2"  >0.60</td><td align="center" valign="middle"  colspan="2"  >0.02</td><td align="center" valign="middle"  colspan="2"  >52.6</td><td align="center" valign="middle"  colspan="2"  >1.9</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >Au</td><td align="center" valign="middle" ><sup>a</sup>0.0003</td><td align="center" valign="middle"  colspan="2"  >-</td><td align="center" valign="middle"  colspan="2"  ><sup>a</sup>0.001</td><td align="center" valign="middle"  colspan="2"  >-</td><td align="center" valign="middle"  colspan="2"  ><sup>a</sup>0.0005</td><td align="center" valign="middle"  colspan="2"  >-</td><td align="center" valign="middle"  colspan="2"  >0.0056</td><td align="center" valign="middle"  colspan="2"  >0.0006</td><td align="center" valign="middle"  colspan="2"  ><sup>a</sup>0.0003</td><td align="center" valign="middle"  colspan="2"  >-</td><td align="center" valign="middle"  colspan="2"  >0.0073</td><td align="center" valign="middle"  colspan="2"  >0.0007</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >Ba</td><td align="center" valign="middle" >11.0</td><td align="center" valign="middle"  colspan="2"  >0.9</td><td align="center" valign="middle"  colspan="2"  >262</td><td align="center" valign="middle"  colspan="2"  >11</td><td align="center" valign="middle"  colspan="2"  ><sup>a</sup>2.28</td><td align="center" valign="middle"  colspan="2"  >-</td><td align="center" valign="middle"  colspan="2"  >177</td><td align="center" valign="middle"  colspan="2"  >10</td><td align="center" valign="middle"  colspan="2"  ><sup>a</sup>1.86</td><td align="center" valign="middle"  colspan="2"  >-</td><td align="center" valign="middle"  colspan="2"  >294</td><td align="center" valign="middle"  colspan="2"  >16</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >Br</td><td align="center" valign="middle" >8.01</td><td align="center" valign="middle"  colspan="2"  >0.28</td><td align="center" valign="middle"  colspan="2"  >35.1</td><td align="center" valign="middle"  colspan="2"  >1.2</td><td align="center" valign="middle"  colspan="2"  >14.6</td><td align="center" valign="middle"  colspan="2"  >0.5</td><td align="center" valign="middle"  colspan="2"  >249</td><td align="center" valign="middle"  colspan="2"  >9</td><td align="center" valign="middle"  colspan="2"  >13.2</td><td align="center" valign="middle"  colspan="2"  >0.5</td><td align="center" valign="middle"  colspan="2"  >408</td><td align="center" valign="middle"  colspan="2"  >14</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >Ca</td><td align="center" valign="middle" >223,000</td><td align="center" valign="middle"  colspan="2"  >8000</td><td align="center" valign="middle"  colspan="2"  >144,000</td><td align="center" valign="middle"  colspan="2"  >5000</td><td align="center" valign="middle"  colspan="2"  >232,000</td><td align="center" valign="middle"  colspan="2"  >8200</td><td align="center" valign="middle"  colspan="2"  >118,000</td><td align="center" valign="middle"  colspan="2"  >4000</td><td align="center" valign="middle"  colspan="2"  >232,000</td><td align="center" valign="middle"  colspan="2"  >8000</td><td align="center" valign="middle"  colspan="2"  >43,100</td><td align="center" valign="middle"  colspan="2"  >1630</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >Cd</td><td align="center" valign="middle" ><sup>a</sup>0.20</td><td align="center" valign="middle"  colspan="2"  >-</td><td align="center" valign="middle"  colspan="2"  >9.58</td><td align="center" valign="middle"  colspan="2"  >0.51</td><td align="center" valign="middle"  colspan="2"  ><sup>a</sup>0.60</td><td align="center" valign="middle"  colspan="2"  >-</td><td align="center" valign="middle"  colspan="2"  >8.27</td><td align="center" valign="middle"  colspan="2"  >1.44</td><td align="center" valign="middle"  colspan="2"  ><sup>a</sup>0.39</td><td align="center" valign="middle"  colspan="2"  >-</td><td align="center" valign="middle"  colspan="2"  >11.7</td><td align="center" valign="middle"  colspan="2"  >1.5</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >Ce</td><td align="center" valign="middle" >0.95</td><td align="center" valign="middle"  colspan="2"  >0.05</td><td align="center" valign="middle"  colspan="2"  >40.6</td><td align="center" valign="middle"  colspan="2"  >1.5</td><td align="center" valign="middle"  colspan="2"  >0.77</td><td align="center" valign="middle"  colspan="2"  >0.04</td><td align="center" valign="middle"  colspan="2"  >27.1</td><td align="center" valign="middle"  colspan="2"  >1.0</td><td align="center" valign="middle"  colspan="2"  >0.88</td><td align="center" valign="middle"  colspan="2"  >0.05</td><td align="center" valign="middle"  colspan="2"  >40.1</td><td align="center" valign="middle"  colspan="2"  >1.5</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >Cl</td><td align="center" valign="middle" >147</td><td align="center" valign="middle"  colspan="2"  >6</td><td align="center" valign="middle"  colspan="2"  >568</td><td align="center" valign="middle"  colspan="2"  >22</td><td align="center" valign="middle"  colspan="2"  >266</td><td align="center" valign="middle"  colspan="2"  >10</td><td align="center" valign="middle"  colspan="2"  >4150</td><td align="center" valign="middle"  colspan="2"  >150</td><td align="center" valign="middle"  colspan="2"  >254</td><td align="center" valign="middle"  colspan="2"  >10</td><td align="center" valign="middle"  colspan="2"  >7760</td><td align="center" valign="middle"  colspan="2"  >280</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >Co</td><td align="center" valign="middle" >0.16</td><td align="center" valign="middle"  colspan="2"  >0.01</td><td align="center" valign="middle"  colspan="2"  >8.39</td><td align="center" valign="middle"  colspan="2"  >0.30</td><td align="center" valign="middle"  colspan="2"  >0.13</td><td align="center" valign="middle"  colspan="2"  >0.01</td><td align="center" valign="middle"  colspan="2"  >7.07</td><td align="center" valign="middle"  colspan="2"  >0.25</td><td align="center" valign="middle"  colspan="2"  >0.13</td><td align="center" valign="middle"  colspan="2"  >0.01</td><td align="center" valign="middle"  colspan="2"  >10.7</td><td align="center" valign="middle"  colspan="2"  >0.4</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >Cr</td><td align="center" valign="middle" >2.58</td><td align="center" valign="middle"  colspan="2"  >0.15</td><td align="center" valign="middle"  colspan="2"  >178</td><td align="center" valign="middle"  colspan="2"  >6</td><td align="center" valign="middle"  colspan="2"  >2.14</td><td align="center" valign="middle"  colspan="2"  >0.10</td><td align="center" valign="middle"  colspan="2"  >149</td><td align="center" valign="middle"  colspan="2"  >5</td><td align="center" valign="middle"  colspan="2"  >2.24</td><td align="center" valign="middle"  colspan="2"  >0.19</td><td align="center" valign="middle"  colspan="2"  >227</td><td align="center" valign="middle"  colspan="2"  >8</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >Cs</td><td align="center" valign="middle" >0.18</td><td align="center" valign="middle"  colspan="2"  >0.01</td><td align="center" valign="middle"  colspan="2"  >10.4</td><td align="center" valign="middle"  colspan="2"  >0.4</td><td align="center" valign="middle"  colspan="2"  >0.108</td><td align="center" valign="middle"  colspan="2"  >0.004</td><td align="center" valign="middle"  colspan="2"  >8.51</td><td align="center" valign="middle"  colspan="2"  >0.30</td><td align="center" valign="middle"  colspan="2"  >0.13</td><td align="center" valign="middle"  colspan="2"  >0.01</td><td align="center" valign="middle"  colspan="2"  >13.5</td><td align="center" valign="middle"  colspan="2"  >0.5</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >Dy</td><td align="center" valign="middle" >0.15</td><td align="center" valign="middle"  colspan="2"  >0.01</td><td align="center" valign="middle"  colspan="2"  >5.82</td><td align="center" valign="middle"  colspan="2"  >0.21</td><td align="center" valign="middle"  colspan="2"  >0.125</td><td align="center" valign="middle"  colspan="2"  >0.006</td><td align="center" valign="middle"  colspan="2"  >2.35</td><td align="center" valign="middle"  colspan="2"  >0.10</td><td align="center" valign="middle"  colspan="2"  >0.13</td><td align="center" valign="middle"  colspan="2"  >0.01</td><td align="center" valign="middle"  colspan="2"  >3.32</td><td align="center" valign="middle"  colspan="2"  >0.17</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >Eu</td><td align="center" valign="middle"  colspan="2"  ><sup>a</sup>0.005</td><td align="center" valign="middle"  colspan="2"  >-</td><td align="center" valign="middle"  colspan="2"  >1.20</td><td align="center" valign="middle"  colspan="2"  >0.05</td><td align="center" valign="middle"  colspan="2"  ><sup>a</sup>0.03</td><td align="center" valign="middle"  colspan="2"  >-</td><td align="center" valign="middle"  colspan="2"  >0.63</td><td align="center" valign="middle"  colspan="2"  >0.03</td><td align="center" valign="middle"  colspan="2"  ><sup>a</sup>0.03</td><td align="center" valign="middle"  colspan="2"  >-</td><td align="center" valign="middle"  colspan="2"  >0.91</td><td align="center" valign="middle"  colspan="2"  >0.06</td></tr><tr><td align="center" valign="middle" >Fe</td><td align="center" valign="middle"  colspan="2"  >726</td><td align="center" valign="middle"  colspan="2"  >26</td><td align="center" valign="middle"  colspan="2"  >33,700</td><td align="center" valign="middle"  colspan="2"  >1200</td><td align="center" valign="middle"  colspan="2"  >482</td><td align="center" valign="middle"  colspan="2"  >17</td><td align="center" valign="middle"  colspan="2"  >34,100</td><td align="center" valign="middle"  colspan="2"  >1200</td><td align="center" valign="middle"  colspan="2"  >452</td><td align="center" valign="middle"  colspan="2"  >16</td><td align="center" valign="middle"  colspan="2"  >46,800</td><td align="center" valign="middle"  colspan="2"  >1700</td></tr><tr><td align="center" valign="middle" >Ga</td><td align="center" valign="middle"  colspan="2"  ><sup>a</sup>0.33</td><td align="center" valign="middle"  colspan="2"  >-</td><td align="center" valign="middle"  colspan="2"  >25.1</td><td align="center" valign="middle"  colspan="2"  >1.1</td><td align="center" valign="middle"  colspan="2"  ><sup>a</sup>0.17</td><td align="center" valign="middle"  colspan="2"  >-</td><td align="center" valign="middle"  colspan="2"  ><sup>a</sup>3.26</td><td align="center" valign="middle"  colspan="2"  >-</td><td align="center" valign="middle"  colspan="2"  ><sup>a</sup>0.15</td><td align="center" valign="middle"  colspan="2"  >-</td><td align="center" valign="middle"  colspan="2"  >28.6</td><td align="center" valign="middle"  colspan="2"  >4.2</td></tr><tr><td align="center" valign="middle" >Hf</td><td align="center" valign="middle"  colspan="2"  >0.043</td><td align="center" valign="middle"  colspan="2"  >0.003</td><td align="center" valign="middle"  colspan="2"  >1.50</td><td align="center" valign="middle"  colspan="2"  >0.06</td><td align="center" valign="middle"  colspan="2"  >0.036</td><td align="center" valign="middle"  colspan="2"  >0.003</td><td align="center" valign="middle"  colspan="2"  >1.44</td><td align="center" valign="middle"  colspan="2"  >0.05</td><td align="center" valign="middle"  colspan="2"  >0.050</td><td align="center" valign="middle"  colspan="2"  >0.002</td><td align="center" valign="middle"  colspan="2"  >2.33</td><td align="center" valign="middle"  colspan="2"  >0.08</td></tr><tr><td align="center" valign="middle" >Hg</td><td align="center" valign="middle"  colspan="2"  >0.22</td><td align="center" valign="middle"  colspan="2"  >0.01</td><td align="center" valign="middle"  colspan="2"  >10.6</td><td align="center" valign="middle"  colspan="2"  >0.4</td><td align="center" valign="middle"  colspan="2"  >0.12</td><td align="center" valign="middle"  colspan="2"  >0.02</td><td align="center" valign="middle"  colspan="2"  >8.62</td><td align="center" valign="middle"  colspan="2"  >0.31</td><td align="center" valign="middle"  colspan="2"  >0.15</td><td align="center" valign="middle"  colspan="2"  >0.01</td><td align="center" valign="middle"  colspan="2"  >11.9</td><td align="center" valign="middle"  colspan="2"  >0.4</td></tr><tr><td align="center" valign="middle" >I</td><td align="center" valign="middle"  colspan="2"  >3.14</td><td align="center" valign="middle"  colspan="2"  >0.13</td><td align="center" valign="middle"  colspan="2"  >22.5</td><td align="center" valign="middle"  colspan="2"  >0.9</td><td align="center" valign="middle"  colspan="2"  >1.40</td><td align="center" valign="middle"  colspan="2"  >0.09</td><td align="center" valign="middle"  colspan="2"  >42.5</td><td align="center" valign="middle"  colspan="2"  >2.0</td><td align="center" valign="middle"  colspan="2"  >1.22</td><td align="center" valign="middle"  colspan="2"  >0.09</td><td align="center" valign="middle"  colspan="2"  >112</td><td align="center" valign="middle"  colspan="2"  >4</td></tr><tr><td align="center" valign="middle" >In</td><td align="center" valign="middle"  colspan="2"  ><sup>a</sup>0.002</td><td align="center" valign="middle"  colspan="2"  >-</td><td align="center" valign="middle"  colspan="2"  >0.09</td><td align="center" valign="middle"  colspan="2"  >0.01</td><td align="center" valign="middle"  colspan="2"  ><sup>a</sup>0.005</td><td align="center" valign="middle"  colspan="2"  >-</td><td align="center" valign="middle"  colspan="2"  ><sup>a</sup>0.03</td><td align="center" valign="middle"  colspan="2"  >-</td><td align="center" valign="middle"  colspan="2"  ><sup>a</sup>0.005</td><td align="center" valign="middle"  colspan="2"  >-</td><td align="center" valign="middle"  colspan="2"  >0.13</td><td align="center" valign="middle"  colspan="2"  >0.02</td></tr><tr><td align="center" valign="middle" >K</td><td align="center" valign="middle"  colspan="2"  >300</td><td align="center" valign="middle"  colspan="2"  >20</td><td align="center" valign="middle"  colspan="2"  >14,500</td><td align="center" valign="middle"  colspan="2"  >500</td><td align="center" valign="middle"  colspan="2"  >179</td><td align="center" valign="middle"  colspan="2"  >9</td><td align="center" valign="middle"  colspan="2"  >10,500</td><td align="center" valign="middle"  colspan="2"  >400</td><td align="center" valign="middle"  colspan="2"  >176</td><td align="center" valign="middle"  colspan="2"  >9</td><td align="center" valign="middle"  colspan="2"  >17,600</td><td align="center" valign="middle"  colspan="2"  >600</td></tr><tr><td align="center" valign="middle" >La</td><td align="center" valign="middle"  colspan="2"  >0.75</td><td align="center" valign="middle"  colspan="2"  >0.03</td><td align="center" valign="middle"  colspan="2"  >29.1</td><td align="center" valign="middle"  colspan="2"  >1.1</td><td align="center" valign="middle"  colspan="2"  >0.61</td><td align="center" valign="middle"  colspan="2"  >0.02</td><td align="center" valign="middle"  colspan="2"  >15.2</td><td align="center" valign="middle"  colspan="2"  >0.6</td><td align="center" valign="middle"  colspan="2"  >0.66</td><td align="center" valign="middle"  colspan="2"  >0.02</td><td align="center" valign="middle"  colspan="2"  >21.8</td><td align="center" valign="middle"  colspan="2"  >0.9</td></tr><tr><td align="center" valign="middle" >Mg</td><td align="center" valign="middle"  colspan="2"  >1920</td><td align="center" valign="middle"  colspan="2"  >90</td><td align="center" valign="middle"  colspan="2"  >36,500</td><td align="center" valign="middle"  colspan="2"  >1400</td><td align="center" valign="middle"  colspan="2"  >1900</td><td align="center" valign="middle"  colspan="2"  >85</td><td align="center" valign="middle"  colspan="2"  >36,300</td><td align="center" valign="middle"  colspan="2"  >1300</td><td align="center" valign="middle"  colspan="2"  >1370</td><td align="center" valign="middle"  colspan="2"  >70</td><td align="center" valign="middle"  colspan="2"  >50,900</td><td align="center" valign="middle"  colspan="2"  >1900</td></tr><tr><td align="center" valign="middle" >Mn</td><td align="center" valign="middle"  colspan="2"  >7.68</td><td align="center" valign="middle"  colspan="2"  >0.27</td><td align="center" valign="middle"  colspan="2"  >207</td><td align="center" valign="middle"  colspan="2"  >7</td><td align="center" valign="middle"  colspan="2"  >7.12</td><td align="center" valign="middle"  colspan="2"  >0.25</td><td align="center" valign="middle"  colspan="2"  >237</td><td align="center" valign="middle"  colspan="2"  >8</td><td align="center" valign="middle"  colspan="2"  >6.21</td><td align="center" valign="middle"  colspan="2"  >0.22</td><td align="center" valign="middle"  colspan="2"  >322</td><td align="center" valign="middle"  colspan="2"  >11</td></tr><tr><td align="center" valign="middle" >Mo</td><td align="center" valign="middle"  colspan="2"  ><sup>a</sup>0.26</td><td align="center" valign="middle"  colspan="2"  >-</td><td align="center" valign="middle"  colspan="2"  >3.87</td><td align="center" valign="middle"  colspan="2"  >1.17</td><td align="center" valign="middle"  colspan="2"  ><sup>a</sup>0.50</td><td align="center" valign="middle"  colspan="2"  >-</td><td align="center" valign="middle"  colspan="2"  >26.5</td><td align="center" valign="middle"  colspan="2"  >1.6</td><td align="center" valign="middle"  colspan="2"  ><sup>a</sup>0.36</td><td align="center" valign="middle"  colspan="2"  >-</td><td align="center" valign="middle"  colspan="2"  >43.2</td><td align="center" valign="middle"  colspan="2"  >2.4</td></tr><tr><td align="center" valign="middle" >Na</td><td align="center" valign="middle"  colspan="2"  >58.9</td><td align="center" valign="middle"  colspan="2"  >2.1</td><td align="center" valign="middle"  colspan="2"  >1570</td><td align="center" valign="middle"  colspan="2"  >60</td><td align="center" valign="middle"  colspan="2"  >96.5</td><td align="center" valign="middle"  colspan="2"  >3.4</td><td align="center" valign="middle"  colspan="2"  >3500</td><td align="center" valign="middle"  colspan="2"  >100</td><td align="center" valign="middle"  colspan="2"  >109</td><td align="center" valign="middle"  colspan="2"  >4</td><td align="center" valign="middle"  colspan="2"  >4900</td><td align="center" valign="middle"  colspan="2"  >200</td></tr><tr><td align="center" valign="middle" >Nd</td><td align="center" valign="middle"  colspan="2"  ><sup>a</sup>0.27</td><td align="center" valign="middle"  colspan="2"  >-</td><td align="center" valign="middle"  colspan="2"  >25.2</td><td align="center" valign="middle"  colspan="2"  >1.1</td><td align="center" valign="middle"  colspan="2"  >1.18</td><td align="center" valign="middle"  colspan="2"  >0.15</td><td align="center" valign="middle"  colspan="2"  >10.6</td><td align="center" valign="middle"  colspan="2"  >0.8</td><td align="center" valign="middle"  colspan="2"  ><sup>a</sup>0.36</td><td align="center" valign="middle"  colspan="2"  >-</td><td align="center" valign="middle"  colspan="2"  >15.7</td><td align="center" valign="middle"  colspan="2"  >1.4</td></tr><tr><td align="center" valign="middle" >Rb</td><td align="center" valign="middle"  colspan="2"  >1.73</td><td align="center" valign="middle"  colspan="2"  >0.12</td><td align="center" valign="middle"  colspan="2"  >97.9</td><td align="center" valign="middle"  colspan="2"  >3.6</td><td align="center" valign="middle"  colspan="2"  >1.46</td><td align="center" valign="middle"  colspan="2"  >0.14</td><td align="center" valign="middle"  colspan="2"  >77.8</td><td align="center" valign="middle"  colspan="2"  >3.7</td><td align="center" valign="middle"  colspan="2"  >1.37</td><td align="center" valign="middle"  colspan="2"  >0.09</td><td align="center" valign="middle"  colspan="2"  >126</td><td align="center" valign="middle"  colspan="2"  >5</td></tr><tr><td align="center" valign="middle" >S</td><td align="center" valign="middle"  colspan="2"  >-</td><td align="center" valign="middle"  colspan="2"  >-</td><td align="center" valign="middle"  colspan="2"  >-</td><td align="center" valign="middle"  colspan="2"  >-</td><td align="center" valign="middle"  colspan="2"  >188,000</td><td align="center" valign="middle"  colspan="2"  >11,000</td><td align="center" valign="middle"  colspan="2"  >110,000</td><td align="center" valign="middle"  colspan="2"  >13,000</td><td align="center" valign="middle"  colspan="2"  >178,000</td><td align="center" valign="middle"  colspan="2"  >11,000</td><td align="center" valign="middle"  colspan="2"  >86,600</td><td align="center" valign="middle"  colspan="2"  >11,900</td></tr><tr><td align="center" valign="middle" >Sb</td><td align="center" valign="middle"  colspan="2"  >0.120</td><td align="center" valign="middle"  colspan="2"  >0.005</td><td align="center" valign="middle"  colspan="2"  >4.68</td><td align="center" valign="middle"  colspan="2"  >0.17</td><td align="center" valign="middle"  colspan="2"  >0.097</td><td align="center" valign="middle"  colspan="2"  >0.004</td><td align="center" valign="middle"  colspan="2"  >5.68</td><td align="center" valign="middle"  colspan="2"  >0.22</td><td align="center" valign="middle"  colspan="2"  >0.108</td><td align="center" valign="middle"  colspan="2"  >0.005</td><td align="center" valign="middle"  colspan="2"  >8.69</td><td align="center" valign="middle"  colspan="2"  >0.31</td></tr><tr><td align="center" valign="middle" >Sc</td><td align="center" valign="middle"  colspan="2"  >0.25</td><td align="center" valign="middle"  colspan="2"  >0.01</td><td align="center" valign="middle"  colspan="2"  >11.1</td><td align="center" valign="middle"  colspan="2"  >0.4</td><td align="center" valign="middle"  colspan="2"  >0.146</td><td align="center" valign="middle"  colspan="2"  >0.005</td><td align="center" valign="middle"  colspan="2"  >9.33</td><td align="center" valign="middle"  colspan="2"  >0.33</td><td align="center" valign="middle"  colspan="2"  >0.20</td><td align="center" valign="middle"  colspan="2"  >0.01</td><td align="center" valign="middle"  colspan="2"  >14.6</td><td align="center" valign="middle"  colspan="2"  >0.5</td></tr><tr><td align="center" valign="middle" >Se</td><td align="center" valign="middle"  colspan="2"  >2.35</td><td align="center" valign="middle"  colspan="2"  >0.09</td><td align="center" valign="middle"  colspan="2"  >87.0</td><td align="center" valign="middle"  colspan="2"  >3.1</td><td align="center" valign="middle"  colspan="2"  >1.31</td><td align="center" valign="middle"  colspan="2"  >0.05</td><td align="center" valign="middle"  colspan="2"  >54.7</td><td align="center" valign="middle"  colspan="2"  >1.9</td><td align="center" valign="middle"  colspan="2"  >1.08</td><td align="center" valign="middle"  colspan="2"  >0.05</td><td align="center" valign="middle"  colspan="2"  >72.7</td><td align="center" valign="middle"  colspan="2"  >2.6</td></tr><tr><td align="center" valign="middle" >Sm</td><td align="center" valign="middle"  colspan="2"  >0.15</td><td align="center" valign="middle"  colspan="2"  >0.01</td><td align="center" valign="middle"  colspan="2"  >5.90</td><td align="center" valign="middle"  colspan="2"  >0.22</td><td align="center" valign="middle"  colspan="2"  >0.131</td><td align="center" valign="middle"  colspan="2"  >0.006</td><td align="center" valign="middle"  colspan="2"  >2.76</td><td align="center" valign="middle"  colspan="2"  >0.18</td><td align="center" valign="middle"  colspan="2"  >0.14</td><td align="center" valign="middle"  colspan="2"  >0.01</td><td align="center" valign="middle"  colspan="2"  >4.55</td><td align="center" valign="middle"  colspan="2"  >0.38</td></tr><tr><td align="center" valign="middle" >Sr</td><td align="center" valign="middle"  colspan="2"  >180</td><td align="center" valign="middle"  colspan="2"  >7</td><td align="center" valign="middle"  colspan="2"  >271</td><td align="center" valign="middle"  colspan="2"  >16</td><td align="center" valign="middle"  colspan="2"  >235</td><td align="center" valign="middle"  colspan="2"  >9</td><td align="center" valign="middle"  colspan="2"  >224</td><td align="center" valign="middle"  colspan="2"  >19</td><td align="center" valign="middle"  colspan="2"  >204</td><td align="center" valign="middle"  colspan="2"  >7</td><td align="center" valign="middle"  colspan="2"  >196</td><td align="center" valign="middle"  colspan="2"  >14</td></tr><tr><td align="center" valign="middle" >Ta</td><td align="center" valign="middle"  colspan="2"  ><sup>a</sup>0.01</td><td align="center" valign="middle"  colspan="2"  >-</td><td align="center" valign="middle"  colspan="2"  >0.50</td><td align="center" valign="middle"  colspan="2"  >0.02</td><td align="center" valign="middle"  colspan="2"  ><sup>a</sup>0.01</td><td align="center" valign="middle"  colspan="2"  >-</td><td align="center" valign="middle"  colspan="2"  >0.48</td><td align="center" valign="middle"  colspan="2"  >0.02</td><td align="center" valign="middle"  colspan="2"  ><sup>a</sup>0.005</td><td align="center" valign="middle"  colspan="2"  >-</td><td align="center" valign="middle"  colspan="2"  >0.74</td><td align="center" valign="middle"  colspan="2"  >0.03</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr></tbody></table></table-wrap><table-wrap id="2_2"><table><tbody><thead><tr><th align="center" valign="middle" >Tb</th><th align="center" valign="middle" >0.021</th><th align="center" valign="middle" >0.002</th><th align="center" valign="middle" >0.88</th><th align="center" valign="middle" >0.03</th><th align="center" valign="middle" >0.022</th><th align="center" valign="middle" >0.001</th><th align="center" valign="middle" >0.41</th><th align="center" valign="middle" >0.01</th><th align="center" valign="middle" >0.020</th><th align="center" valign="middle" >0.001</th><th align="center" valign="middle" >0.57</th><th align="center" valign="middle" >0.02</th></tr></thead><tr><td align="center" valign="middle" >Th</td><td align="center" valign="middle" >0.16</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >6.43</td><td align="center" valign="middle" >0.23</td><td align="center" valign="middle" >0.124</td><td align="center" valign="middle" >0.005</td><td align="center" valign="middle" >6.49</td><td align="center" valign="middle" >0.23</td><td align="center" valign="middle" >0.11</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >9.36</td><td align="center" valign="middle" >0.33</td></tr><tr><td align="center" valign="middle" >Ti</td><td align="center" valign="middle" ><sup>a</sup>53.1</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >1910</td><td align="center" valign="middle" >130</td><td align="center" valign="middle" ><sup>a</sup>50.3</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >1630</td><td align="center" valign="middle" >110</td><td align="center" valign="middle" ><sup>a</sup>48.5</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >2630</td><td align="center" valign="middle" >150</td></tr><tr><td align="center" valign="middle" >U</td><td align="center" valign="middle" >1.03</td><td align="center" valign="middle" >0.04</td><td align="center" valign="middle" >46.9</td><td align="center" valign="middle" >1.7</td><td align="center" valign="middle" >0.81</td><td align="center" valign="middle" >0.03</td><td align="center" valign="middle" >39.2</td><td align="center" valign="middle" >1.4</td><td align="center" valign="middle" >0.58</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >65.9</td><td align="center" valign="middle" >2.4</td></tr><tr><td align="center" valign="middle" >V</td><td align="center" valign="middle" >4.65</td><td align="center" valign="middle" >0.20</td><td align="center" valign="middle" >227</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >3.16</td><td align="center" valign="middle" >0.15</td><td align="center" valign="middle" >199</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >3.27</td><td align="center" valign="middle" >0.16</td><td align="center" valign="middle" >352</td><td align="center" valign="middle" >13</td></tr><tr><td align="center" valign="middle" >W</td><td align="center" valign="middle" ><sup>a</sup>0.06</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >1.65</td><td align="center" valign="middle" >0.22</td><td align="center" valign="middle" ><sup>a</sup>0.05</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>0.80</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>0.05</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>1.04</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >Yb</td><td align="center" valign="middle" >0.074</td><td align="center" valign="middle" >0.004</td><td align="center" valign="middle" >3.19</td><td align="center" valign="middle" >0.12</td><td align="center" valign="middle" >0.073</td><td align="center" valign="middle" >0.004</td><td align="center" valign="middle" >1.71</td><td align="center" valign="middle" >0.07</td><td align="center" valign="middle" >0.073</td><td align="center" valign="middle" >0.003</td><td align="center" valign="middle" >2.46</td><td align="center" valign="middle" >0.10</td></tr><tr><td align="center" valign="middle" >Zn</td><td align="center" valign="middle" >3.69</td><td align="center" valign="middle" >0.26</td><td align="center" valign="middle" >227</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >2.88</td><td align="center" valign="middle" >0.20</td><td align="center" valign="middle" >183</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >2.65</td><td align="center" valign="middle" >0.12</td><td align="center" valign="middle" >241</td><td align="center" valign="middle" >9</td></tr><tr><td align="center" valign="middle" >Zr</td><td align="center" valign="middle" ><sup>a</sup>5.60</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>34.9</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>5.01</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>31.0</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ><sup>a</sup>4.41</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >120</td><td align="center" valign="middle" >11</td></tr></tbody></table></table-wrap></table-wrap-group><sec id="s3_1"><title>3.1. Properties of Finer and Coarse Fractions</title><p>Determination of particle sizes by grain size distribution analyses are detailed in <xref ref-type="fig" rid="fig3">Figure 3</xref>. The differences in gypsum samples are most likely caused by mainly sample preparation procedures as well as different sampling time, sample locations and conditions within the WFGD system. The differences are more pronounced in the composition of the FF (<xref ref-type="fig" rid="fig3">Figure 3</xref>). FF of TEŠ5-FF contains a relatively high amount of CF (<xref ref-type="fig" rid="fig3">Figure 3</xref>(a)). This indicates that sedimentation technique provides better separation of FF and CF with respect to hydrocyclone separation. CF slightly differ among subsamples where TEŠ5-CF2 contains a bigger proportion of particles smaller than 50 &#181;m (<xref ref-type="fig" rid="fig3">Figure 3</xref>(c)).</p><p>SEM technique gives insight into the structure of fine and coarse particles (<xref ref-type="fig" rid="fig4">Figure 4</xref>). Differences between the two fractions are clearly marked and highlighted. Mainly, CaSO<sub>4</sub>・2H<sub>2</sub>O crystals represent the mainstream in CF (<xref ref-type="fig" rid="fig4">Figure 4</xref>(b)). Non-uniform size distribution of FF illustrates different structure, presumably consisting of unburned particles and different minerals originating from fly ash, agglomerates and precipitates (<xref ref-type="fig" rid="fig4">Figure 4</xref>(a) and <xref ref-type="fig" rid="fig4">Figure 4</xref>(c)). Bigger agglomerates are typically found in FF (<xref ref-type="fig" rid="fig4">Figure 4</xref>(d)). However, FF may also contain some bigger crystals of gypsum (<xref ref-type="fig" rid="fig4">Figure 4</xref>(a) and <xref ref-type="fig" rid="fig4">Figure 4</xref>(c)) that could be present as a consequence of the incomplete separation of the original gypsum slurry sample.</p><p>The bulk gypsum sample represents an average between CF and FF containing a lower amount of CaSO<sub>4</sub>・2H<sub>2</sub>O with respect to the CF. According to the previous study, FF represents only about 12% of the whole gypsum, while the majority of the sample is CF [<xref ref-type="bibr" rid="scirp.89215-ref28">28</xref>] . CF is predominantly in the form of CaSO<sub>4</sub>・2H<sub>2</sub>O while in FF its proportion is much lower. The fine fraction TEŠ5-FF differs from TEŠ5-FF1 and TEŠ-FF2 according to a higher proportion of CaSO<sub>4</sub>・2H<sub>2</sub>O due to the incomplete gypsum slurry separation into TEŠ5-FF and TEŠ5-CF as observed in <xref ref-type="fig" rid="fig3">Figure 3</xref>(a). The possible explanation of this can be a lower amount of CaSO<sub>4</sub>・2H<sub>2</sub>O in CF as compared with FF. Hence, <xref ref-type="table" rid="table3">Table 3</xref> indicates far less CaSO<sub>4</sub>・2H<sub>2</sub>O in TEŠ5-FF2 than in TEŠ5-FF and TEŠ5-FF1. However, less amount of CaSO<sub>4</sub>・2H<sub>2</sub>O present in FF is consistent with lower particle size and increasing proportion of other species (elements) comprising in the sample. A small proportion of Ca could also be present as unconsumed CaCO<sub>3</sub>.</p><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> Percentage of Ca and adequate proportion of CaSO<sub>4</sub>・2H<sub>2</sub>O crystals in gypsum samples</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Sample</th><th align="center" valign="middle" >Percentage of calcium in finer/coarse fraction (%)<sup>a</sup></th><th align="center" valign="middle" >Proportion of CaSO<sub>4</sub>・2H<sub>2</sub>O in gypsum (%)</th></tr></thead><tr><td align="center" valign="middle" >Bulk gypsum</td><td align="center" valign="middle" >20.4</td><td align="center" valign="middle" >87.6</td></tr><tr><td align="center" valign="middle" >TEŠ5-CF</td><td align="center" valign="middle" >22.3</td><td align="center" valign="middle" >95.6</td></tr><tr><td align="center" valign="middle" >TEŠ5-FF</td><td align="center" valign="middle" >14.4</td><td align="center" valign="middle" >61.9</td></tr><tr><td align="center" valign="middle" >TEŠ5-CF1</td><td align="center" valign="middle" >23.2</td><td align="center" valign="middle" >99.6</td></tr><tr><td align="center" valign="middle" >TEŠ5-FF1</td><td align="center" valign="middle" >11.8</td><td align="center" valign="middle" >50.5</td></tr><tr><td align="center" valign="middle" >TEŠ5-CF2</td><td align="center" valign="middle" >23.2</td><td align="center" valign="middle" >99.6</td></tr><tr><td align="center" valign="middle" >TEŠ5-FF2</td><td align="center" valign="middle" >4.31</td><td align="center" valign="middle" >18.5</td></tr></tbody></table></table-wrap><p><sup>a</sup>Theoretical molar proportion of Ca in CaSO<sub>4</sub>・2H<sub>2</sub>O is 23.3%.</p></sec><sec id="s3_2"><title>3.2. Enrichment of Elements in Finer Fraction</title><p>Accumulation of TMEs in gypsum samples mainly depends on particle sizes. The elements are partitioned between FF and CF respectively (<xref ref-type="fig" rid="fig5">Figure 5</xref>). Most of the elements are considerably enriched in the FF, with some exceptions (Ca, Sr and S) that constitute the bulk of gypsum. Strontium is usually introduced in the system with limestone, and typically occurs as SrCO<sub>3</sub> [<xref ref-type="bibr" rid="scirp.89215-ref22">22</xref>] . In general, the enrichment of elements in TEŠ5-FF is smaller with respect to TEŠ5-FF1 and TEŠ5-FF2. A larger proportion of bigger particles in the fine fraction TEŠ5-FF causing a “dilution” effect (<xref ref-type="fig" rid="fig3">Figure 3</xref>(a)). However, much higher enrichment was observed for most TMEs in TEŠ5-FF2 with respect to TEŠ5-FF1 and TEŠ5-FF fraction of gypsum, suggesting the importance of sampling and preparation procedures. Higher enrichment of most TMEs in TEŠ5-FF2 is consistent with <xref ref-type="table" rid="table3">Table 3</xref>, where the proportion of CaSO<sub>4</sub>・2H<sub>2</sub>O is significantly lower as a consequence of other particles present in the sample.</p><p>Alkali elements show similar enrichment with the exception of Na, while earth-alkaline elements show enrichment for Mg and Ba, but not for Ca and Sr (<xref ref-type="fig" rid="fig5">Figure 5</xref>). In addition, Ba is highly enriched in FF of TEŠ5-FF2. Since the salts of alkali and earth alkali elements have solubility several orders of magnitude higher then salts of the transition elements, the precipitation reactions alone cannot explain these findings. This enrichment is mainly supported by adsorption. Aluminium is enriched in all FFs and is one of the most enriched elements. A small part is supplied with limestone, while most enters with fly ash that escapes the ESP and could be present as small aluminosilicate cenospheres with high specific surface for adsorption/condensation. On the other hand, it could</p><p>enter as sulphate (oxide) aluminium species, where some are well soluble and therefore TMEs can be released [<xref ref-type="bibr" rid="scirp.89215-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref43">43</xref>] . Al can be introduced by different insoluble, saturated species as well [<xref ref-type="bibr" rid="scirp.89215-ref43">43</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref48">48</xref>] . As, Sb and Se show similar enrichment in all fractions. Enrichment of transition elements is comparable, except for La, Hf and Mn. Mn, as a non-volatile element, is typically retained in bottom ash and therefore its presence in gypsum is mostly the consequence of limestone addition [<xref ref-type="bibr" rid="scirp.89215-ref22">22</xref>] and only minor amounts could enter with the smallest particles. In addition, Mn can form precipitates such as MnO<sub>2</sub> in a WFGD slurry tank [<xref ref-type="bibr" rid="scirp.89215-ref24">24</xref>] . Lanthanides in TEŠ5-FF are slightly enriched compared to other FFs. Actinides, namely Th and U, are similar in both blocks with the exception of finer fraction TEŠ5-FF2, where strong enrichment of both elements was observed.</p><p>The data of TMEs in slurry water are shown in <xref ref-type="table" rid="table1">Table 1</xref>. The concentration of elements (TEŠ5-W<sub>1</sub> and TEŠ5-W<sub>2</sub>) decreases within the following order: Cl, Mg, Ca ≫ Na, Br, K &gt; I, Mn, Ti &gt; other elements. Different soluble complexes with halogens, SO 4 2 − and OH- anions can form in a WFGD scrubber [<xref ref-type="bibr" rid="scirp.89215-ref43">43</xref>] . Some soluble elements (species) tend to concentrate through the recirculation process, where they could reach equilibrium, and possibly saturate, precipitate, or accumulate in FF afterwards. However, enrichment of halogens in FF with respect to CF is not significant, except for iodine in TEŠ5-FF2 (<xref ref-type="fig" rid="fig5">Figure 5</xref>). High concentrations of those elements in slurry water and in gypsum afterwards indicate their accumulation followed by formation of different insoluble species and/or adsorption process. Halogens that are well soluble with higher concentrations in slurry water enter in the system as volatile compounds, while other elements are mostly in the form of particulate matter and become mobile (released) in water media.</p></sec><sec id="s3_3"><title>3.3. Limestone as a Source of Elements</title><p>As seen in <xref ref-type="fig" rid="fig5">Figure 5</xref>, most elements in FF are enriched relative to the CF. The composition of CF is similar to limestone, which is an important source of elements in the system. In the present study, CF of TEŠ5-CF1 was chosen for comparison with limestone (<xref ref-type="fig" rid="fig6">Figure 6</xref>) since it contains almost 100% of CaSO<sub>4</sub>・2H<sub>2</sub>O according to calculations (<xref ref-type="table" rid="table3">Table 3</xref>). Most elements show higher concentrations in limestone with respect to CF. Halogens, Hg and Se show the opposite trend since they are not originating from limestone (<xref ref-type="fig" rid="fig6">Figure 6</xref>). During the desulphurisation process in a WFGD scrubber, elements present in limestone and those that enter with fly ash are included in different reactions, like the formation of different soluble/insoluble species, adsorption to particles and other oxidation/reduction processes. Elements entering with small particles alongside flue gases are of minor importance in CF where bigger crystals of CaSO<sub>4</sub>・2H<sub>2</sub>O are a predominant matrix. However, the particle size is a very important parameter in determining the reactivity of limestones [<xref ref-type="bibr" rid="scirp.89215-ref22">22</xref>] and has an effect on the adsorption properties in CF and FF.</p></sec><sec id="s3_4"><title>3.4. Comparison of Finer and Coarser Fractions versus Lignite</title><p>In order to compare trend lines and concentration of elements that are enriched/depleted in all fractions of finer and coarser gypsum, concentrations of elements in different samples are shown in the same graph (<xref ref-type="fig" rid="fig7">Figure 7</xref>). Similar behaviour for most of the elements is observed; however some distinct differences related to Br, Cl, and I are seen. Concentrations of Cl, Br and I in the FF of TEŠ5-FF are close to the trend line itself, following the predicted concentration ratios between FF and lignite samples (<xref ref-type="fig" rid="fig7">Figure 7</xref>). On the other hand, much higher concentrations of these elements are present in the other FF of block 5. Similarly, all CFs (TEŠ5-CF, TEŠ5-CF1 and TEŠ5-CF2) show that Br, Cl and I are located significantly higher with respect to the concentrations in coal and according to the other elements present in CF. CFs with a majority of CaSO<sub>4</sub>・2H<sub>2</sub>O seem to be a relatively efficient matrix for removal of halogens, whereas high retention is even more apparent in FFs, indicating greater accumulation with possible binding and/or reactions with other elements, and adsorption onto the minerals or to smaller crystals of gypsum. With respect to the position of trend lines, it is obvious that TEŠ5-FF2 contains higher concentrations of most TMEs, while within CFs there are no such differences between.</p><p>Among the most interesting features is high accumulation/retention of Hg and Se in all gypsum fractions regarding coal. Se mainly condenses on fly ash particles, while Hg is found as volatile species in flue gas [<xref ref-type="bibr" rid="scirp.89215-ref20">20</xref>] . Concentrations of Se and Hg in the particles leaving the ESP are higher in medium to fine fraction. In the gypsum, Se is suggested to be in oxidation state Se(IV) [<xref ref-type="bibr" rid="scirp.89215-ref49">49</xref>] . SeO<sub>2</sub> is a</p><p>predominant species in flue gas that combines with lime in the scrubber to form CaSeO<sub>3</sub> [<xref ref-type="bibr" rid="scirp.89215-ref50">50</xref>] . Another explanation for Se accumulation is attributed to its presence in gypsum as calcium selenatedihydrate (CaSeO<sub>4</sub>・2H<sub>2</sub>O), which has similar properties as CaSO<sub>4</sub>・2H<sub>2</sub>O [<xref ref-type="bibr" rid="scirp.89215-ref51">51</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref52">52</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref53">53</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref54">54</xref>] . In the case of Hg, various mercury compounds have been suggested to be present in gypsum, such as Hg-Cl compounds, HgS, HgO, Hg-SO<sub>4</sub>, etc. [<xref ref-type="bibr" rid="scirp.89215-ref25">25</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref42">42</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref48">48</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref55">55</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref56">56</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref57">57</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref58">58</xref>] . Although Hg and Se form stable Hg-Se compounds, e.g. in biological systems [<xref ref-type="bibr" rid="scirp.89215-ref59">59</xref>] , this has not been proven in WFGD gypsum so far [<xref ref-type="bibr" rid="scirp.89215-ref60">60</xref>] . Fe and Al may also have an important role in the adsorption of Hg to Fe/Al (oxides/hydroxides) in the WFGD system [<xref ref-type="bibr" rid="scirp.89215-ref27">27</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref29">29</xref>] [<xref ref-type="bibr" rid="scirp.89215-ref48">48</xref>] .</p><p>In general, conditions are expected to be constant during the coal combustion process and the partitioning of elements in air pollution control devices (APCDs). However, sampling procedure itself and separation of gypsum into different fractions are important factors affecting partitioning in finer and coarser fractions of gypsum samples. Improved separation procedures and further investigations are needed to understand better the species formed, and to explain reactions present in a WFGD boiler. Identification of different species there would help in understanding the chemistry and enrichment/depletion process of elements.</p></sec></sec><sec id="s4"><title>4. Conclusion</title><p>The presence of TMEs in gypsum is primarily related to 1) small size fraction of fly ash not retained by the particle control devices, 2) volatile elements (e.g. Hg, Se and halogens) that are highly accumulated in the WFGD with respect to coal 3) introduction of limestone as an additional source of TMEs (e.g. Mg, Ca, Sr) associated mostly with CF, 4) and the conditions present in a WFGD scrubber (e.g. oxidation-reduction, temperature, pH, etc.). In general, the concentrations of TMEs in the CF and FF of gypsum varied, demonstrating the importance of particle size. Small particles retain much higher concentrations of most elements, especially Hg and Se, which are highly enriched relative to their occurrence in coal. FF represents a small mass portion in the gypsum as a whole (about 10%), but contains a large proportion of TMEs. Removal of fine gypsum fraction in the process of recirculation of gypsum slurry therefore represents one of the possible cost-effective remediation technologies. Thus, the appropriate approach based on the removal of the smallest size fraction of gypsum could eliminate most TMEs. Finally, the study also showed that the methodologies for sampling and separation of gypsum particle sizes need to be standardized in order to assure comparability of the results. Moreover, concentrations of TMEs in coal (lignite), limestone, fly ash and various size fractions of gypsum could provide a good indication of the removal efficiency of APCDs.</p></sec><sec id="s5"><title>Acknowledgements</title><p>This work was funded by the Slovenian Research Agency program P1-0143 and project L1-5446 and the young researchers program. The study was also supported by the EMPIR MercOx project (16ENV01). We thank the Šoštanj thermal power plant for permitting us to obtain samples.</p></sec><sec id="s6"><title>Conflicts of Interest</title><p>The authors declare no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s7"><title>Cite this paper</title><p>Pavlin, M., Jaćimović, R., Stergaršek, A., Frkal, P., Koblar, M. and Horvat, M. (2018) Distribution and Accumulation of Major and Trace Elements in Gypsum Samples from Lignite Combustion Power Plant. American Journal of Analytical Chemistry, 9, 602-621. https://doi.org/10.4236/ajac.2018.912044</p></sec></body><back><ref-list><title>References</title><ref id="scirp.89215-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Nriagu, J.O. and Pacyna, J.M. (1988) Quantitative Assessment of Worldwide Contamination of Air, Water and Soils by Trace Metals. 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