<?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">AMPC</journal-id><journal-title-group><journal-title>Advances in Materials Physics and Chemistry</journal-title></journal-title-group><issn pub-type="epub">2162-531X</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ampc.2015.58032</article-id><article-id pub-id-type="publisher-id">AMPC-58955</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><subject> Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Minimum Amounts of Extracting Solvent of (A&lt;sub&gt;1&lt;/sub&gt;A&lt;sub&gt;2&lt;/sub&gt;&amp;middot;&amp;middot;&amp;middot;A&lt;sub&gt;&lt;i&gt;t&lt;/i&gt;-1&lt;/sub&gt;)/(A&lt;sub&gt;2&lt;/sub&gt;A&lt;sub&gt;3&lt;/sub&gt;&amp;middot;&amp;middot;&amp;middot;A&lt;sub&gt;&lt;i&gt;t&lt;/i&gt;&lt;/sub&gt;) Countercurrent Extraction Separation
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>u-Xiang</surname><given-names>Cheng</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>Sheng</surname><given-names>Wu</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>Song-Ling</surname><given-names>Wang</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>Bo</surname><given-names>Zhang</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>Yan</surname><given-names>Liu</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>Chun-Sheng</surname><given-names>Liao</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>Chun-Hua</surname><given-names>Yan</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>Beijing National Laboratory for Molecular Sciences, State Key Laboratory of Rare Earth Materials Chemistry and Applications, PKU-HKU Joint Lab on Rare Earth Materials and Bioinorganic Chemistry, Peking University, Beijing, China</addr-line></aff><aff id="aff1"><addr-line>China Minmetals (Beijing) Research Institute of RE Co., Ltd., Beijing, China</addr-line></aff><pub-date pub-type="epub"><day>05</day><month>08</month><year>2015</year></pub-date><volume>05</volume><issue>08</issue><fpage>325</fpage><lpage>336</lpage><history><date date-type="received"><day>20</day>	<month>July</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>18</month>	<year>August</year>	</date><date date-type="accepted"><day>21</day>	<month>August</month>	<year>2015</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>
 
 
  Minimum amounts of extracting solvent and scrubbing agent solution (denoted as 
  S
  <sub>min</sub> and 
  W
  <sub>min</sub> respectively) mean the theoretical minimal requirements for chemicals to achieve a specified separation duty, and therefore attract more concerns in the process design of countercurrent extraction separation. Over the past decade, hyperlink extraction technology has been widely used in rare earth separation industry in China with the target to decrease chemical consumption as well as pollution discharges. However, the equations of 
  S
  <sub>min</sub> and 
  W
  <sub>min</sub> derived in the earlier version of the theory of countercurrent extraction can only be correctly applied to two-component separation and become invalid for hyperlink processes. It is significant to develop new aspects of the theory for design of the hyperlink processes. The separation of (A
  <sub>1</sub>A
  <sub>2</sub>&amp;middot;&amp;middot;&amp;middot;A
  <sub>t</sub>
  <sub>－1</sub>)/(A
  <sub>2</sub>A
  <sub>3</sub>&amp;middot;&amp;middot;&amp;middot;A
  <sub>t</sub>) is the basic configuration in the hyperlink processes differently from in conventional processes, where A
  <sub>1</sub>, A
  <sub>2</sub>, &amp;middot;&amp;middot;&amp;middot;, A
  <sub>t</sub> represent different kinds of rare earth ions with the same number of valence. The separations of two and three components have been discussed and the equations of 
  S
  <sub>min</sub> and 
  W
  <sub>min</sub> are derived in our previous works. Nevertheless, it is still significant, especially for rare earth separations, to investigate the separations with more components. The present article will therefore focus on developing new expressions for 
  S
  <sub>min</sub> and 
  W
  <sub>min</sub> applied to the (A
  <sub>1</sub>A
  <sub>2</sub>&amp;middot;&amp;middot;&amp;middot;A
  <sub>t﹣</sub>
  <sub>1</sub>)/(A
  <sub>2</sub>A
  <sub>3</sub>&amp;middot;&amp;middot;&amp;middot;A
  <sub>t</sub>) separation. Also a five-component separation case is simulated according to the derived equations. This work is an essential part of the new theory to design the hyperlink extraction processes.
 
</p></abstract><kwd-group><kwd>Theory of Countercurrent Extraction</kwd><kwd> Minimum Amount of Extracting Solvent</kwd><kwd> Countercurrent Extraction</kwd><kwd> Hyperlink Process</kwd><kwd> Multi-Component Separation</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Rare earth separation processes of solvent extraction may involve as many as fifteen components. As the rare earths are all so close to each other in terms of extraction chemistry, the techniques by countercurrent extraction and scrubbing of the extract have been proved essential for the production of pure rare earth products [<xref ref-type="bibr" rid="scirp.58955-ref1">1</xref>] - [<xref ref-type="bibr" rid="scirp.58955-ref3">3</xref>] . Various methods such as McCabe-Thiele method [<xref ref-type="bibr" rid="scirp.58955-ref3">3</xref>] - [<xref ref-type="bibr" rid="scirp.58955-ref6">6</xref>] , chemical thermodynamics analysis [<xref ref-type="bibr" rid="scirp.58955-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.58955-ref8">8</xref>] , and mathematical empirical methods [<xref ref-type="bibr" rid="scirp.58955-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.58955-ref10">10</xref>] , have been developed to carry out the calculation and optimization of countercurrent extraction processes of rare earths. The remarkably rapid progress on separation processes of rare earths was created by the Theory of Countercurrent Extraction (called hereafter as “the theory” for simplicity unless otherwise specified) established by Xu et al. [<xref ref-type="bibr" rid="scirp.58955-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.58955-ref12">12</xref>] in 1970s. The theory derived a number of new algebra equations as well as flexible calculation approaches for process optimization. In particular, the theory facilitated the advent of one-step scale-up technique [<xref ref-type="bibr" rid="scirp.58955-ref13">13</xref>] , as a result of which the world rare earth industry encountered “China Impact” [<xref ref-type="bibr" rid="scirp.58955-ref14">14</xref>] .</p><p>Currently due to the increasing environmental concerns, the separation techniques of solvent extraction are tending to reduce both consumption and emission of chemicals [<xref ref-type="bibr" rid="scirp.58955-ref15">15</xref>] - [<xref ref-type="bibr" rid="scirp.58955-ref17">17</xref>] . Acidic extractants are commonly used to separate rare earths [<xref ref-type="bibr" rid="scirp.58955-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.58955-ref18">18</xref>] [<xref ref-type="bibr" rid="scirp.58955-ref19">19</xref>] , and saponification by basic substances is usually necessary for the purpose of increasing and stabilizing the extraction capacity of the acidic extractants. Meanwhile, inorganic acids are demanded for both scrubbing and stripping. Thus acids and bases are the main consumed chemicals, and the resulted salts are the main pollution during rare earth separation processes. To determine the theoretical minimum requirement of the base for saponification and the acid for scrubbing, the terms of minimum amounts of extracting solvent and scrubbing agent solution (denoted hereafter as S<sub>min</sub> and W<sub>min</sub> respectively) are introduced respectively.</p><p>Hyperlink extraction technique has been developed and widely used in Chinese rare earth separation industry due to its virtue in reducing both consumptions and emissions since the early of last decades [<xref ref-type="bibr" rid="scirp.58955-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.58955-ref20">20</xref>] . By arranging two separation cascade units to offer each other with the extracting solvent or the scrubbing agent solution containing rare earths, the technique can decrease the consumption of acid or base for both of the two units. So far, the optimized parameters of a hyperlink process are determined by screening a great deal of simulation results [<xref ref-type="bibr" rid="scirp.58955-ref21">21</xref>] - [<xref ref-type="bibr" rid="scirp.58955-ref23">23</xref>] . However, the simulation cannot exactly tell the theoretical minimum values of parameters, and also the simulation task is too technical for common technicians. Therefore we are exploring to develop new aspects of the theory available for design of the hyperlink processes. Differently from the configuration of (A<sub>1</sub>A<sub>2</sub>∙∙∙A<sub>k</sub>)/(A<sub>k</sub><sub>+1</sub>A<sub>k</sub><sub>+2</sub>∙∙∙A<sub>t</sub>) (1 &lt; k &lt; t) commonly seen in conventional processes, (A<sub>1</sub>A<sub>2</sub>∙∙∙A<sub>t</sub><sub>−1</sub>)/(A<sub>2</sub>A<sub>3</sub>∙∙∙A<sub>t</sub>) is the basic separation configuration in hyperlink processes [<xref ref-type="bibr" rid="scirp.58955-ref20">20</xref>] , where t ( ≥ 3) represents the number of components. The values of S<sub>min</sub> and W<sub>min</sub> are the primary concerns for a given separation duty, and therefore in our previous works [<xref ref-type="bibr" rid="scirp.58955-ref24">24</xref>] - [<xref ref-type="bibr" rid="scirp.58955-ref27">27</xref>] , we discussed the separations with two or three components and derived the equations of S<sub>min</sub> and W<sub>min</sub>. Nevertheless, rare earth separations involve more than 3 components in most cases, and thus in this article we will derive the equations of S<sub>min</sub> and W<sub>min</sub> for multi-component separations with the (A<sub>1</sub>A<sub>2</sub>∙∙∙A<sub>t</sub><sub>−1</sub>)/ (A<sub>2</sub>A<sub>3</sub>∙∙∙A<sub>t</sub>) configuration.</p></sec><sec id="s2"><title>2. Description of the Separation System</title><p><xref ref-type="fig" rid="fig1">Figure 1</xref> displays a typical countercurrent extraction cascade unit with the separation configuration of (A<sub>1</sub>A<sub>2</sub>∙∙∙A<sub>t</sub><sub>−</sub><sub>1</sub>)/(A<sub>2</sub>A<sub>3</sub>∙∙∙A<sub>t</sub>), where t ( ≥ 3) means the number of components and A<sub>1</sub>, A<sub>2</sub>, ∙∙∙, A<sub>t</sub> represents t kinds of trivalent rare earth ions in the feed with a prior extractable sequence of A<sub>1</sub> &gt; A<sub>2</sub> &gt; ∙∙∙ &gt; A<sub>t</sub>. The feed flowrates of the t components are f<sub>1</sub>, f<sub>2</sub>,∙∙∙, and f<sub>t</sub> (hereafter in mole per unit time) respectively all the time, where f<sub>1</sub> + f<sub>2</sub> + ∙∙∙ + f<sub>t</sub> = f. The separation factor of the neighboring A<sub>i</sub>/A<sub>i</sub><sub>+1 </sub>(t &gt; i ≥ 1) pair is denoted as β<sub>i</sub><sub>/i+1</sub>; the separation factor of A<sub>i</sub>/A<sub>i</sub><sub>+j</sub> pair (t &gt; i ≥ 1; t - i ≥ j ≥ 1), β<sub>i</sub><sub>/i+j</sub>, can be calculated according to:</p><disp-formula id="scirp.58955-formula1033"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1510407x6.png"  xlink:type="simple"/></disp-formula><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Schematic diagram for the countercurrent extraction cascade of hyperlink processes</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-1510407x7.png"/></fig><p>The separation cascade couples n extraction stages and m scrubbing stages. The partly saponified barren solvent with the flowrate S and hydrochloric acid with the flowrate W enter at opposite ends of the cascade, serving as extracting solvent and scrubbing agent solution respectively. Here for brevity the term “extracting solvent” is used to include solvent mixtures. The feed stream enters either stage n or stage (n + 1) depending on its phase type, as shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>. The final raffinate and the final extract, which can behave as the feed in subsequent countercurrent units for further separation, contain no A<sub>1</sub> or no A<sub>t</sub> respectively as required.</p><p>It is assumed that the extracting solvent and the aqueous solution are immiscible and remain so at all cases of the operation. It is assumed that each stage is an equilibrium stage, and therefore all the flowrates are out of each stage in equilibrium. It is also assumed that only the saponified extractant has the extraction capacity with a single cation-exchange mechanism. The saponified extracting solvent is assumed to be always saturated with components when leaving all stages except (n + m)<sup>th</sup> stage. All the H<sup> + </sup>ion in the starting scrubbing acid is supposed to immediately exchange and migrate towards the organic phase after entering the cascade, and therefore the scrubbing agent solution has contained no acid since leaving (n + m)<sup>th</sup> stage. And also as all the components has a same number of valence, the mixed extraction factor which denotes the ratio of the total mole amount of all the components in the organic phase to that in the aqueous phase will keep constant either through extraction stages except stage 1 or through scrubbing stages except stage (n + m).</p></sec><sec id="s3"><title>3. Expressions of Adjacent Stage Impurity</title><p>To derive the equation of S<sub>min</sub> and W<sub>min</sub>, we need to introduce a term Adjacent Stage Impurity Ratio (briefly as ASIR) for the case of multi-component separation [<xref ref-type="bibr" rid="scirp.58955-ref24">24</xref>] as we did before [<xref ref-type="bibr" rid="scirp.58955-ref25">25</xref>] - [<xref ref-type="bibr" rid="scirp.58955-ref27">27</xref>] . The separation goal can be achieved by stepwise impurity removal in the countercurrent extraction cascade, and ASIR is then defined as Equation (2) which can evaluate the purification efficiency of a certain stage.</p><disp-formula id="scirp.58955-formula1034"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1510407x8.png"  xlink:type="simple"/></disp-formula><p>where g denotes ASIR. The subscripts i and k represent an impurity and a stage, respectively. The g<sub>i,k</sub> then means ASIR of impurity A<sub>i</sub> at stage k, and so hereafter.</p><p>In the extraction stages in <xref ref-type="fig" rid="fig1">Figure 1</xref>, the extracting solvent should withdraw component A<sub>1</sub> stage by stage to obtain the final raffinate with no A<sub>1</sub>, and therefore component A<sub>1</sub> is regarded as the impurity of the aqueous phase in the extraction section. Instead, component A<sub>t</sub> behaves as the impurity in the organic phase to be removed by scrubbing agent solution in the scrubbing stages. <xref ref-type="fig" rid="fig2">Figure 2</xref> shows the equilibrium flows of a continuous three stages, where x and y denote the flowrates of a component in the aqueous and the organic phases respectively. The subscripts i and k represent a component and a stage again, respectively. The x<sub>i</sub><sub>,k</sub> then represent the flowrates of component A<sub>i</sub> in the aqueous phase, and so hereafter. If 1 &lt; k &lt; n, which means that the three stages locate in extraction section, extraction equilibrium and mass balance in view of k<sup>th</sup> and (k + 1)<sup>th</sup> stages give the relations of Equations (3), (4) and (5).</p><disp-formula id="scirp.58955-formula1035"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1510407x9.png"  xlink:type="simple"/></disp-formula><p><img src="http://html.scirp.org/file/6-1510407x10.png" /> <img src="http://html.scirp.org/file/6-1510407x11.png" /> (4)</p><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Mass flows in a continuous three stages</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-1510407x12.png"/></fig><disp-formula id="scirp.58955-formula1036"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1510407x13.png"  xlink:type="simple"/></disp-formula><p>where x<sub>1,1</sub> means the flowrates of A<sub>1</sub> in the final raffinate, which should be approximate to zero according to the separation goal. From Equations (3) and (4), we have Equation (6).</p><disp-formula id="scirp.58955-formula1037"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1510407x14.png"  xlink:type="simple"/></disp-formula><p>Substituting the expression for y<sub>1,k</sub> as in Equation (6) into Equation (5) gives Equation (7).</p><disp-formula id="scirp.58955-formula1038"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1510407x15.png"  xlink:type="simple"/></disp-formula><p>Thus the ASIR of component A<sub>1</sub> at stage k of the extraction section, denoted by g<sub>1,k</sub>, can be expressed as the following equation:</p><disp-formula id="scirp.58955-formula1039"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1510407x16.png"  xlink:type="simple"/></disp-formula><p>As the total aqueous flowrate, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1510407x17.png" xlink:type="simple"/></inline-formula>, should have an unchanged value through the extraction stages with the</p><p>exception of stage 1 according to the constant-mixed-extraction-factor assumption mentioned before, and also the cation exchange reaction takes place always between a more extractable ion in the aqueous phase and a less extractable ion in the organic phase, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1510407x18.png" xlink:type="simple"/></inline-formula>as well as x<sub>1,k</sub> will decrease with stage from the central feed stage</p><p>towards the left end of the cascade, and consequently the ASIR of impurity A<sub>1</sub> will exhibit an increasing tendency towards this direction.</p><p>In the scrubbing stages, the same analysis can give the expression for ASIR of impurity A<sub>t</sub> as Equation (9) on the basis of extraction equilibrium and mass balance in view of (k − 1)<sup>th</sup> stage and k<sup>th</sup> stage where (n + 1) &lt; k ≤ (n + m) in <xref ref-type="fig" rid="fig2">Figure 2</xref>.</p><disp-formula id="scirp.58955-formula1040"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1510407x19.png"  xlink:type="simple"/></disp-formula><p>in which y<sub>t</sub><sub>,n+m</sub> represents the flowrate of impurity A<sub>t</sub> leaving the organic outlet in stage (n + m). From the same consideration as above, ASIR of impurity A<sub>t</sub> should also present an increasing tendency with stage from the feed stage to stage (n + m) according to Equation (9).</p><p>ASIR presents an intuitive view of the status to remove an impurity in a separation cascade. Generally ASIR should have a value larger than 1 in order to perform purification stage by stage. Nevertheless when the extracting solvent or scrubbing agent solution loses their concentration driving force to withdraw the impurity from the opposite liquid phase at a certain stage, the value of ASIR will drop to 1 there. However, ASIR is always not smaller than 1.</p></sec><sec id="s4"><title>4. Derivation of the Equations of S<sub>min</sub> and W<sub>min</sub></title><sec id="s4_1"><title>4.1. Principle Procedures of Deviation</title><p>For more accessible, the derivation procedures are outlined as the following before the details are presented.</p><p>Firstly, we need to know the conditions where both S and W have their theoretical minimum values to achieve a specified separation duty as shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>. ASIR analysis can help to find out such conditions. When an S lower than S<sub>min</sub> is given to the cascade, the two following events will occur in extraction section if this section is long enough: (i) more impurity A<sub>1</sub> than required exists in the final raffinate; (ii) ASIR at some continuous extraction stages next to scrubbing section drops to 1. In this case, adding more extraction stages cannot decrease A<sub>1</sub> in the raffinate any longer. Then if S is gradually increased, impurity A<sub>1</sub> will become less and less in the final raffinate, while the event (ii) will remain until impurity A<sub>1 </sub>completely disappears in the final raffinate. Therefore it can be addressed that S<sub>min</sub> should correspond to the S causing impurity A<sub>1</sub> in the final raffinate just removed to the required level while the lowest value of ASIR in the extraction section still remaining at 1. Similarly, W<sub>min</sub> should be the W that can just reduce impurity A<sub>t</sub> in final extract to the required level, and meanwhile there are some continuous stages with ASIR of 1 next to extraction section.</p><p>Secondly based on the above conditions, flowrate analysis is taken on the extraction and the scrubbing sections separately. We can deduct the expressions for both the aqueous and the organic flowrates of all components leaving stage n except for impurity A<sub>1</sub>. The flowrates of each intermediate component are temporarily expressed with its flowrate in final raffinate which still remains unknown now. Similarly we will also deduct the expressions for both the aqueous and organic flowrates of each component leaving stage (n + 1) except for impurity A<sub>t</sub>, and the flowrate expressions of each intermediate component here involve its unknown flowrate in the final extract.</p><p>In the third step, we will consider the mass balance between stage n and stage (n + 1) which connect the extraction and the scrubbing sections. As a result, we can obtain the quantitative relationships between the two flowrate expressions of each intermediate component leaving stage n and stage (n + 1) as well as the ratio of the flowrates of each intermediate component leaving the two opposite ends consequently. Taking the mass balance of each component in the two ends into account, the exiting flowrates of each component in the two ends can then become known.</p><p>Finally the equations of S<sub>min</sub> and W<sub>min</sub> can be derived according to Equations (8) and (9) with the use of the flowrate expressions obtained in the steps above.</p></sec><sec id="s4_2"><title>4.2. Conditions of S<sub>min</sub> and W<sub>min</sub></title><p>Mass balance of the (A<sub>1</sub>A<sub>2</sub>∙∙∙A<sub>t</sub><sub>−1</sub>)/(A<sub>2</sub>A<sub>3</sub>∙∙∙A<sub>t</sub>) separation duty suggests the quantitative relations as the following expressions.</p><disp-formula id="scirp.58955-formula1041"><graphic  xlink:href="http://html.scirp.org/file/6-1510407x20.png"  xlink:type="simple"/></disp-formula><p>where x<sub>i</sub><sub>,1</sub> and y<sub>i</sub><sub>,n+m</sub> represent two exiting flowrates of A<sub>i</sub> (1 ≤ i ≤ t) in the aqueous and the organic streams, respectively. If stage k is an extraction stage and has the ASIR value of 1, according to the definition of ASIR, we know that</p><disp-formula id="scirp.58955-formula1042"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1510407x21.png"  xlink:type="simple"/></disp-formula><p>And taking the mass balance of A<sub>1</sub> represented by Equation (16) into account, we can obtain Equation (17).</p><disp-formula id="scirp.58955-formula1043"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1510407x22.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.58955-formula1044"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1510407x23.png"  xlink:type="simple"/></disp-formula><p>Equation (17) reveals that the aqueous and the organic flowrates of impurity A<sub>1</sub> leaving one equilibrium extraction stage with ASIR of 1 should be equal to each other. In this case the extraction equilibrium relations between A<sub>1</sub> and the other components in the k<sup>th</sup> stage can be reduced as</p><disp-formula id="scirp.58955-formula1045"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1510407x24.png"  xlink:type="simple"/></disp-formula><p>Moreover according to the constant-mixed-extraction-factor assumption, when an aqueous stream is used as feed, the overall flowrates of all components in the aqueous and the organic phases should always be (f + W) and S respectively when leaving an extraction stage with the exception of 1<sup>st</sup> stage. If it is also assumed that the extraction section of the cascade is long enough and there are at least (t − 2) continuous extraction stages including the feed stage (stage n) with the same ASIR value of 1, a series of relationships can be noted as below in view of mass balance within these stages.</p><disp-formula id="scirp.58955-formula1046"><graphic  xlink:href="http://html.scirp.org/file/6-1510407x25.png"  xlink:type="simple"/></disp-formula><p>where u = n - t + 3; expressions (20) and (21) are two collectives of (t - 2) and (t<sup>2</sup> - 4t + 3) equations respectively, and therefore expressions (19), (20) and (21) consist of a system involving (t<sup>2</sup> - 3t + 2) independent equations. Then we analyze the number of the unknowns involved in this equation system. As all of these (t - 2) stages have ASIR value of 1, the aqueous flowrates of impurity A<sub>1</sub> leaving these stages (i.e., x<sub>1,u+j</sub>) remain unvaried, and thus y<sub>1,u+j</sub> is also unvaried as it always equals x<sub>1,u+j</sub> in these (t - 2) stages. Moreover, the aqueous exiting flowrates of each component, x<sub>i,</sub><sub>1</sub> (1 ≤ i ≤ t), will not change with time as the cascade is in a steady state, and they can therefore be treated as constant terms. Thus in the equation system, only y<sub>i,u</sub><sub>+j</sub> (2 ≤ i ≤ t; 0 ≤ j ≤ t-3) are regarded as unknown quantities, with the number of (t<sup>2</sup> − 3t + 2) which is just same as that of the independent equations. Solving the equation system enables us to express all y<sub>i,u</sub><sub>+j</sub> with the involved constant terms W, S, β<sub>1/i</sub> (2 ≤ i ≤ t ), x<sub>i</sub><sub>,1</sub>(2 ≤ i ≤ t) and y<sub>1,n</sub>. Furthermore, when more continuous extraction stages than (t − 2) have ASIR of 1, any continuous (t - 2) extraction stages among them should have a same group of solutions. To satisfy this condition, it is necessary for the organic flowrate of each component to have the same value when leaving any extraction stage involved in these stages with ASIR of 1, and accordingly the aqueous flowrate of each component also remains constant when leaving these stages, which means y<sub>i,n</sub> = y<sub>i,n</sub><sub>−</sub><sub>1</sub> = ∙∙∙ = y<sub>i,u</sub><sub>−</sub><sub>1</sub> and x<sub>i,n</sub> = x<sub>i,n</sub><sub>−</sub><sub>1</sub> = ∙∙∙ = x<sub>i,u</sub><sub>−</sub><sub>1</sub> (1 ≤ i ≤ t). Working the case using an organic stream as starting feed in the same manner, we can address the same conclusion.</p></sec><sec id="s4_3"><title>4.3. Separate Analysis of Extraction and Scrubbing Sections</title><p><xref ref-type="fig" rid="fig3">Figure 3</xref> displays the material flows of four continuous stages, where the aqueous or the organic feed will flow into n<sup>th</sup> stage or (n + 1)<sup>th</sup> stage in <xref ref-type="fig" rid="fig3">Figure 3</xref>, respectively. According to the theory of countercurrent extraction [<xref ref-type="bibr" rid="scirp.58955-ref12">12</xref>] , the stage receiving an aqueous feed is generally treated as an extraction stage, whereas the stage that an organic feed enters is regarded as a scrubbing stage instead, as illustrated in <xref ref-type="fig" rid="fig1">Figure 1</xref>.</p><p>When there are (t − 1) or more extraction stages with ASIR of 1 next to scrubbing section, the mass balance on Interface I between (n − 1)<sup>th</sup> and n<sup>th</sup> stages in <xref ref-type="fig" rid="fig3">Figure 3</xref> can be expressed as the following three equations.</p><disp-formula id="scirp.58955-formula1047"><graphic  xlink:href="http://html.scirp.org/file/6-1510407x26.png"  xlink:type="simple"/></disp-formula><p>Considering that x<sub>i,n</sub> and y<sub>i,n</sub> in Equation (23) as well as x<sub>t,n</sub> and y<sub>t,n</sub> in Equation (24) should satisfy Equation (18) by letting k = n, we can obtain (t − 1) equation systems, and each of them involves two unknowns x<sub>i,n</sub> and y<sub>i,n</sub> (2 ≤ i ≤ t) as well as two independent equations. Solving these equation systems gives the expressions of the aqueous and the organic flowrates of A<sub>2</sub>, A<sub>3</sub>, ∙∙∙, A<sub>t</sub> leaving stage n as follows.</p><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Mass flows near feed stage</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-1510407x27.png"/></fig><disp-formula id="scirp.58955-formula1048"><graphic  xlink:href="http://html.scirp.org/file/6-1510407x28.png"  xlink:type="simple"/></disp-formula><p>Equations (25) and (26) specify the lowest requirement on the aqueous flowrate of each component leaving the feed stage in order to reach its exiting aqueous flowrate as required respectively by Equations (23) or (24).</p><p>To derive the equation of S<sub>min</sub> from Equation (8), we should turn to analyze the scrubbing section to obtain the expressions for the flowrates of A<sub>1</sub> as well as x<sub>i</sub><sub>,1</sub> (2 ≤ i ≤ t - 1). In scrubbing section, when there are more stages than (t - 2) involving stage (n + 1) with ASIR of 1, the analysis in exactly the same manner as in extraction section can reveal that the aqueous and the organic flowrates of each component do not vary with stage in these stages. Therefore the mass balance on interface III in <xref ref-type="fig" rid="fig3">Figure 3</xref> can provide the relations below, similarly to Equations (22)-(24).</p><disp-formula id="scirp.58955-formula1049"><graphic  xlink:href="http://html.scirp.org/file/6-1510407x29.png"  xlink:type="simple"/></disp-formula><p>The expressions of extraction equilibrium between A<sub>t</sub> and other components according to Equation (31) can be simplified to result in</p><disp-formula id="scirp.58955-formula1050"><label>(32)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1510407x30.png"  xlink:type="simple"/></disp-formula><p>Furthermore, by constructing and then solving (t − 1) equation systems involving two independent equations and two unknowns x<sub>i,n</sub><sub>+1</sub>, y<sub>i</sub><sub>,n+1</sub> (1 ≤ i ≤ t − 1) respectively according to Equations (29), (30) and (32), we can obtain the expressions for the aqueous and the organic flowrates of A<sub>1</sub>, A<sub>2</sub>, ∙∙∙, A<sub>t</sub><sub>−1</sub> leaving (n + 1)<sup>th</sup> stage as presented in Equations (33)-(36), similarly to Equations (25)-(28).</p><disp-formula id="scirp.58955-formula1051"><graphic  xlink:href="http://html.scirp.org/file/6-1510407x31.png"  xlink:type="simple"/></disp-formula></sec><sec id="s4_4"><title>4.4. Combining Analysis of Extraction and Scrubbing Sections</title><p>The relations of Equations (22)-(36) can apply to the cases of using either the aqueous feed or the organic feed. Nevertheless, the different mass balance of all components on interface II in <xref ref-type="fig" rid="fig3">Figure 3</xref> will occur if different feed is used, as expressed in Equations (37)-(39) for aqueous feed and Equations (40)-(42) for organic feed, where 2 ≤ i ≤ t − 1.</p><disp-formula id="scirp.58955-formula1052"><graphic  xlink:href="http://html.scirp.org/file/6-1510407x32.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.58955-formula1053"><graphic  xlink:href="http://html.scirp.org/file/6-1510407x33.png"  xlink:type="simple"/></disp-formula><p>In the case of using an aqueous stream as feed, the comparison of Equation (30) and Equation (38) gives</p><disp-formula id="scirp.58955-formula1054"><label>(43)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1510407x34.png"  xlink:type="simple"/></disp-formula><p>and thus by substituting Equation (27) for y<sub>i,n</sub> as well as Equation (36) for y<sub>i,n</sub><sub>+1</sub> and rearrangement, we have</p><disp-formula id="scirp.58955-formula1055"><label>(44)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1510407x35.png"  xlink:type="simple"/></disp-formula><p>Equation (44), termed by us as optimal flowrate ratio equation of intermediate components, gives the optimal ratio between its flowrates leaving two opposite outlets when both of S<sub>min</sub> and W<sub>min</sub> are applied to the (A<sub>1</sub>∙∙∙A<sub>t</sub><sub>−1</sub>)/(A<sub>2</sub>∙∙∙A<sub>t</sub>) separation system using an aqueous feed. It can be found from Equation (44) that the optimal flowrate ratio of an intermediate component, such as A<sub>i</sub>, is determined only by β<sub>1/i</sub> and β<sub>i/t</sub> (Note: β<sub>1/t</sub> = β<sub>1/I</sub> &#215; β<sub>i/t</sub>), but independent of the separation factors of other pairs as well as the composition of the initial feed.</p><p>Further, by combining Equation (14) with Equation (44) and simultaneously solving them, we can immediately obtain the optimal flowrate equations of intermediate components as expressed by Equations (45) and (46). The equations permit us to calculate the exiting flowrates of each intermediate component when both S<sub>min</sub> and W<sub>min</sub> are given to the specified separation cascade.</p><disp-formula id="scirp.58955-formula1056"><graphic  xlink:href="http://html.scirp.org/file/6-1510407x36.png"  xlink:type="simple"/></disp-formula><p>From Equations (17) and (43), the relations x<sub>1,n</sub> = y<sub>1,n</sub> = y<sub>1,n+1</sub> can be easily found when using the aqueous feed, and then taking Equation (35) into account can lead to Equation (47); introduction of the expression for x<sub>i</sub><sub>,1</sub> as in Equation (45) into Equation (25) results in Equation (48); and for the convenience of comparison, Equation (26) is listed after Equation (48) as below. It is worthwhile to notice from Equations (47), (48) and (26) that the aqueous stream leaving the feed stage has a composition exactly the same as the initial aqueous feed.</p><disp-formula id="scirp.58955-formula1057"><graphic  xlink:href="http://html.scirp.org/file/6-1510407x37.png"  xlink:type="simple"/></disp-formula><p>The analysis in the same manner will be applied when an organic feed is used. The combination of Equation (23) with Equation (41) leads to</p><disp-formula id="scirp.58955-formula1058"><label>(49)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1510407x38.png"  xlink:type="simple"/></disp-formula><p>Then the optimal flowrate ratio equation as well as the optimal flowrate equations for the separation system using organic feed can be derived respectively as Equation (50) and Equations (51), (52) respectively, and the organic flowrates of all components leaving the feed stage can be obtained and summarized as Equations (35), (53), (54).</p><disp-formula id="scirp.58955-formula1059"><label>(50)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1510407x39.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.58955-formula1060"><graphic  xlink:href="http://html.scirp.org/file/6-1510407x40.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.58955-formula1061"><graphic  xlink:href="http://html.scirp.org/file/6-1510407x41.png"  xlink:type="simple"/></disp-formula><p>Equations (35), (53) and (54) clearly indicate that the composition of the organic stream leaving the feed stage is exactly the same as that of the initial organic feed.</p></sec><sec id="s4_5"><title>4.5. Derivation of S<sub>min</sub> and W<sub>min</sub> Equations</title><p>The equation of S<sub>min</sub> for the (A<sub>1</sub>A<sub>2</sub>∙∙∙A<sub>k</sub>)/(A<sub>k</sub><sub>+1</sub>A<sub>k</sub><sub>+2</sub>∙∙∙A<sub>t</sub>) separation using aqueous feed can be derived as Equation (55) by introducing Equations (47), (48), (26) into Equation (8) and using the conditions of g<sub>1,n</sub> = 1 and x<sub>1,1</sub> = 0.</p><disp-formula id="scirp.58955-formula1062"><label>(55)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1510407x42.png"  xlink:type="simple"/></disp-formula><p>Then taking the mass balance in the organic outlet as given by Equation (56) into account, we will have the expression for W<sub>min</sub> as in Equation (57) by replacing S<sub>min</sub> and y<sub>i,n</sub><sub>+m</sub> in Equation (56) with Equation (55) and Equation (46) respectively and rearranging it, if the total feed flowrate is unity, that is, f = f<sub>1</sub> + f<sub>2</sub> + ∙∙∙ + f<sub>t</sub> = 1.</p><disp-formula id="scirp.58955-formula1063"><label>(56)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1510407x43.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.58955-formula1064"><label>(57)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1510407x44.png"  xlink:type="simple"/></disp-formula><p>Also, Equation (57) can be derived by introducing the organic flowrates of all components leaving feed stage, as expressed by Equation (35), (53) and (54) into Equation (9) and making g<sub>t</sub><sub>,n+1</sub> = 1 as well as neglecting the second item. Similarly the expressions of S<sub>min</sub> and W<sub>min</sub> for organic feed system can be derived as follows:</p><disp-formula id="scirp.58955-formula1065"><label>(58)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1510407x45.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.58955-formula1066"><label>(59)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1510407x46.png"  xlink:type="simple"/></disp-formula></sec></sec><sec id="s5"><title>5. Case Study</title>Calculation of Parameters<p>The results above were used to design a separation of an aqueous solution containing Ho, Er, Tm, Yb and Lu with the (HoErTmYb)/(ErTmYbLu) separation configuration. Equal volumes of HEH(EHP) and refined kerosene, partly saponified by NaOH, consists of the starting organic phase, and 4.0 mol∙L<sup>−</sup><sup>1</sup> hydrochloric acid is used as a starting scrubbing agent solution, as the common cases in industry. The separation factors [<xref ref-type="bibr" rid="scirp.58955-ref12">12</xref>] [<xref ref-type="bibr" rid="scirp.58955-ref19">19</xref>] between the neighboring components involved in the feed together with their feeding flowrates are listed in <xref ref-type="table" rid="table1">Table 1</xref>. The exiting aqueous flowrate of Lu and organic flowrate of Ho, x<sub>Lu,1</sub> and y<sub>Ho,n+m</sub>, were determined on the basis of the total required purity (99.99%) of (HoErTmYb) in the exiting aqueous stream and that of (ErTmYbLu) in the exiting organic stream, respectively. The exiting flowrates of all intermediate components could then be calculated according to Equations (45) and (46) with the use of the data in <xref ref-type="table" rid="table1">Table 1</xref> and summarized in <xref ref-type="table" rid="table2">Table 2</xref>. Then S<sub>min</sub> and W<sub>min</sub> could be calculated as 0.2639 and 0.0176 according to Equation (55) and Equation (57), respectively.</p><p>Self-developed software [<xref ref-type="bibr" rid="scirp.58955-ref22">22</xref>] [<xref ref-type="bibr" rid="scirp.58955-ref23">23</xref>] was used to conduct static simulation of the five-component separation described above. Based on mass balance and extraction equilibrium, the calculation was started from two opposite ends stagewise towards centre simultaneously until there were enough stages where ASIR dropped to 1 for each side. <xref ref-type="fig" rid="fig4">Figure 4</xref> displays the varied compositions of the aqueous and organic streams in addition to ASIR with stage through the cascade according to the calculation results. It can be seen from <xref ref-type="fig" rid="fig4">Figure 4</xref>(c) that ASIR in some stages on both sides of the feed stage (95<sup>th</sup> stage) has approached to 1 and accordingly the flowrates of all components do not change within these stages as shown in both <xref ref-type="fig" rid="fig4">Figure 4</xref>(a) and <xref ref-type="fig" rid="fig4">Figure 4</xref>(b), which implies that the driving force of both extracting solvent and scrubbing agent solution for separation has been used up here. Moreover also from <xref ref-type="fig" rid="fig4">Figure 4</xref>(a) the rare earth composition in the aqueous stream near the feed stage is exactly same as that in the initial aqueous feed, which is also in accordance with the conclusion deducted earlier in the present article.</p></sec><sec id="s6"><title>6. Conclusions</title><p>As the basic separation configuration of hyperlink extraction process, (A<sub>1</sub>A<sub>2</sub>∙∙∙A<sub>t</sub><sub>−1</sub>)/(A<sub>2</sub>A<sub>3</sub>∙∙∙A<sub>t</sub>) separation was</p><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Variations with stage of (1) composition in aqueous phase; (2) composition in organic phase; (3) ASIR</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-1510407x47.png"/></fig><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Parameters for a five-component separation</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >f<sub>Lu</sub></th><th align="center" valign="middle"  colspan="2"  >f<sub>Yb</sub></th><th align="center" valign="middle"  colspan="2"  >f<sub>Tm</sub></th><th align="center" valign="middle"  colspan="2"  >f<sub>Er</sub></th><th align="center" valign="middle" >f<sub>Ho</sub></th></tr></thead><tr><td align="center" valign="middle" >0.045</td><td align="center" valign="middle"  colspan="2"  >0.325</td><td align="center" valign="middle"  colspan="2"  >0.06</td><td align="center" valign="middle"  colspan="2"  >0.415</td><td align="center" valign="middle" >0.155</td></tr><tr><td align="center" valign="middle"  colspan="2"  >β<sub>Lu/Yb</sub></td><td align="center" valign="middle"  colspan="2"  >β<sub>Yb/Tm</sub></td><td align="center" valign="middle"  colspan="2"  >β<sub>Tm/Er</sub></td><td align="center" valign="middle"  colspan="2"  >β<sub>Er/Ho</sub></td></tr><tr><td align="center" valign="middle"  colspan="2"  >1.78</td><td align="center" valign="middle"  colspan="2"  >3.56</td><td align="center" valign="middle"  colspan="2"  >3.34</td><td align="center" valign="middle"  colspan="2"  >2.73</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></tr></tbody></table></table-wrap><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Calculated exiting flowrates of all components</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >stage 1</th><th align="center" valign="middle" >flowrates</th><th align="center" valign="middle" >stage (n + m)</th><th align="center" valign="middle" >flowrates</th></tr></thead><tr><td align="center" valign="middle" >x<sub>Lu,1</sub></td><td align="center" valign="middle" >7.537 &#215; 10<sup>−5</sup></td><td align="center" valign="middle" >y<sub>Lu,n+m</sub></td><td align="center" valign="middle" >0.0450</td></tr><tr><td align="center" valign="middle" >x<sub>Yb,1</sub></td><td align="center" valign="middle" >0.1449</td><td align="center" valign="middle" >y<sub>Yb,n+m</sub></td><td align="center" valign="middle" >0.1801</td></tr><tr><td align="center" valign="middle" >x<sub>Tm,1</sub></td><td align="center" valign="middle" >0.0514</td><td align="center" valign="middle" >y<sub>Tm,n+m</sub></td><td align="center" valign="middle" >0.0086</td></tr><tr><td align="center" valign="middle" >x<sub>Er,1</sub></td><td align="center" valign="middle" >0.4024</td><td align="center" valign="middle" >y<sub>Er,n+m</sub></td><td align="center" valign="middle" >0.0126</td></tr><tr><td align="center" valign="middle" >x<sub>Ho,1</sub></td><td align="center" valign="middle" >0.1550</td><td align="center" valign="middle" >y<sub>Ho,n+m</sub></td><td align="center" valign="middle" >2.463 &#215; 10<sup>−5</sup></td></tr><tr><td align="center" valign="middle" >W<sub>min</sub></td><td align="center" valign="middle" >0.0176</td><td align="center" valign="middle" >S<sub>min</sub></td><td align="center" valign="middle" >0.2639</td></tr></tbody></table></table-wrap><p>discussed with regard to the determination of the minimum amounts of extracting solvent and scrubbing agent solution (S<sub>min</sub> and W<sub>min</sub>), and some conclusions had been drawn as follows:</p><p>(1) Both S<sub>min</sub> in the case of using an aqueous feed and W<sub>min</sub> in the case of using an organic feed can be expressed by feed composition together with the separation factors between the components involved, whereas both W<sub>min</sub> and S<sub>min</sub> in the corresponding cases are only determined by the separation factor between the most and the least extractable components, but independent of either separation factors of other pairs or feed composition.</p><p>(2) For any intermediate component, when S<sub>min</sub> and W<sub>min</sub> are applied to the cascade with enough stages, the ratio of its flowrates leaving two opposite outlets is decided by an optimal flowrate ratio equation. This ratio can be expressed only in terms of the separation factors between the intermediate component and the two end components, and do not involve separation factors of other pairs as well as the feed composition, in spite of the different forms when different kinds of feed are used.</p><p>(3) Whichever kind of feed is used, when S<sub>min</sub> and W<sub>min</sub> are applied to a cascade with enough stages, the stream of same kind as feed should have the same composition as the initial feed when leaving the feed stage, which provides a proof for the feed-stage-composition assumption proposed in the early version of the theory of countercurrent extraction.</p></sec><sec id="s7"><title>Acknowledgements</title><p>This research was supported by the National Basic Research Program of China (973) (2012CBA01200).</p></sec><sec id="s8"><title>Cite this paper</title><p>Fu-XiangCheng,ShengWu,Song-LingWang,BoZhang,YanLiu,Chun-ShengLiao,Chun-HuaYan, (2015) Minimum Amounts of Extracting Solvent of (A<sub>1</sub>A<sub>2</sub>&amp;middot;&amp;middot;&amp;middot;A<sub>t-1</sub>)/(A<sub>2</sub>A<sub>3</sub>&amp;middot;&amp;middot;&amp;middot;A<sub>t</sub>) Countercurrent Extraction Separation. Advances in Materials Physics and Chemistry,05,325-336. doi: 10.4236/ampc.2015.58032</p></sec><sec id="s9"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.58955-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Brown, C.G. and Sherrington, L.G. (1979) Solvent Extraction Used in Industrial Separation of Rare Earths. Journal of Chemical Technology and Biotechnology, 29, 193-209. http://dx.doi.org/10.1002/jctb.503290402</mixed-citation></ref><ref id="scirp.58955-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Thakur, N.V. (2000) Separation of Rare Earths by Solvent Extraction. Mineral Processing and Extractive Metallurgy Review, 21, 277-306. http://dx.doi.org/10.1080/08827500008914171</mixed-citation></ref><ref id="scirp.58955-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Xie, F., Zhang, T.A., Dreisinger, D. and Doyle, F. (2014) A Critical Review on Solvent Extraction of Rare Earths from Aqueous Solutions. Minerals Engineering, 56, 10-28. http://dx.doi.org/10.1016/j.mineng.2013.10.021</mixed-citation></ref><ref id="scirp.58955-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">Zhu, T. (1991) Solvent Extraction in China. Hydro-metallurgy, 27, 231-245. http://dx.doi.org/10.1016/0304-386X(91)90069-X</mixed-citation></ref><ref id="scirp.58955-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">Rydberg, J., Cox, M., Musikas, C. and Choppin, G.R. (2004) Solvent Extraction Principles and Practice. 2nd Edition, CRC Press, Florida. http://dx.doi.org/10.1201/9780203021460</mixed-citation></ref><ref id="scirp.58955-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">Radhika, S., Kumar, B.N., Kantam, M.L. and Reddy, R.B. (2011) Solvent Extraction and Separation of Rare-Earths from Phosphoric Acid Solutions with TOPS 99. Hydrometallurgy, 110, 50-55. http://dx.doi.org/10.1016/j.hydromet.2011.08.004</mixed-citation></ref><ref id="scirp.58955-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">Hoh, Y.-C. and Bautista, R.G., (1979) Liquid-Liquid Extraction Equilibrium Models for Binary and Ternary Lanthanides-HDEHP Systems. Industrial and Engineering Chemistry Process Design and Development, 18, 446-453. http://dx.doi.org/10.1021/i260071a017</mixed-citation></ref><ref id="scirp.58955-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">Ryu, K.H., Lee, C.K., Lee, G.-G., Jo, S.K. and Sung, S.W. (2013) Modeling and Simulation of Solvent Extraction Processes for Purifying Rare Earth Metals with PC88A. Korean Journal of Chemical Engineering, 30, 1946-1953. http://dx.doi.org/10.1007/s11814-013-0135-3</mixed-citation></ref><ref id="scirp.58955-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">Giles, A.E., Aldrich, C. and Van Deventer, J.S.J. (1996) Modeling of Rare Earth Solvent Extraction with Artificial Neural Nets. Hydrometallurgy, 43, 241-255. http://dx.doi.org/10.1016/0304-386X(95)00098-2</mixed-citation></ref><ref id="scirp.58955-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">Anitha, M. and Singh, H. (2008) Artificial Neural Network Simulation of Rare Earths Solvent Extraction Equilibrium Data. Desalination, 232, 59-70. http://dx.doi.org/10.1016/j.desal.2007.10.037</mixed-citation></ref><ref id="scirp.58955-ref11"><label>11</label><mixed-citation publication-type="book" xlink:type="simple">Xu, G.X., Li, B.G., Yan, C.H., Zhang, L.P. and Hao, H.M. (1985) Theory of Countercurrent Extraction and Its Applications in Rare Earth Extraction Industry. In: Xu, G.X., Ed., New Frontiers in Rare Earth Science and Applications, Science Press, Beijing, 429-437.</mixed-citation></ref><ref id="scirp.58955-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">Xu, G.X. (1995) Chapter 8: Rare Earths. Metallurgical Industry Press, Beijing. (In Chinese)</mixed-citation></ref><ref id="scirp.58955-ref13"><label>13</label><mixed-citation publication-type="other" xlink:type="simple">Yan, C.H. (1988) One-Step Scale-Up of Rare Earth Extraction Separation Process. Doctoral Dissertation, Peking University, Beijing. (In Chinese)</mixed-citation></ref><ref id="scirp.58955-ref14"><label>14</label><mixed-citation publication-type="other" xlink:type="simple">Yan, C.H., Jia, J.J., Liao, C.S., Wu, S. and Xu, G.X. (2006) Rare Earth Separation in China. Tsinghua Science &amp; Technology, 11, 241-247. http://dx.doi.org/10.1016/S1007-0214(06)70183-3</mixed-citation></ref><ref id="scirp.58955-ref15"><label>15</label><mixed-citation publication-type="other" xlink:type="simple">Feng, Z.Y., Huang, X.W., Liu, H.J., Wang, M., Long, Z.Q., Yu, Y. and Wang, C.M. (2012) Study on Preparation and Application of Novel Saponification Agent for Organic Phase of Rare Earths Extraction. Journal of Rare Earths, 30, 903-908. http://dx.doi.org/10.1016/S1002-0721(12)60152-5</mixed-citation></ref><ref id="scirp.58955-ref16"><label>16</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>Han</surname><given-names> Q.Y. </given-names></name>,<etal>et al</etal>. (<year>2013</year>)<article-title>Technical and Economical Evaluation on Separation Process of Light Rare Earth</article-title><source> Journal of the Chinese Society of Rare Earths</source><volume> 31</volume>,<fpage> 399</fpage>-<lpage>404</lpage>.<pub-id pub-id-type="doi"></pub-id></mixed-citation></ref><ref id="scirp.58955-ref17"><label>17</label><mixed-citation publication-type="other" xlink:type="simple">Xiao, Y.F., Long, Z.Q., Huang, X.W., Feng, Z.Y., Cui, D.L. and Wang, L.S. (2013) Study on Non-Saponification Extraction Process for Rare Earth Separation. Journal of Rare Earths, 31, 512-516.http://dx.doi.org/10.1016/S1002-0721(12)60311-1</mixed-citation></ref><ref id="scirp.58955-ref18"><label>18</label><mixed-citation publication-type="other" xlink:type="simple">Moeller, T., Martin, D.F., Thompson, L.C., Ferrus, R., Feistel, G.R. and Randall, W.J. (1965) The Coordination Chemistry of Yttrium and the Rare Earth Metal Ions. Chemical Reviews, 65, 1-50. http://dx.doi.org/10.1021/cr60233a001</mixed-citation></ref><ref id="scirp.58955-ref19"><label>19</label><mixed-citation publication-type="other" xlink:type="simple">Sato, T. (1989) Liquid-Liquid Extraction of Rare-Earth Elements from Aqueous Acid Solutions by Acid Organophosphorus Compounds. Hydrometallurgy, 22, 121-140. http://dx.doi.org/10.1016/0304-386X(89)90045-5</mixed-citation></ref><ref id="scirp.58955-ref20"><label>20</label><mixed-citation publication-type="other" xlink:type="simple">Liao, C.S., Wu, S., Cheng, F.X., Wang, S.L., Liu, Y., Zhang, B. and Yan, C.H. (2013) Clean Separation Technologies of Rare Earth Resources in China. Journal of Rare Earths, 31, 331-336.http://dx.doi.org/10.1016/S1002-0721(12)60281-6</mixed-citation></ref><ref id="scirp.58955-ref21"><label>21</label><mixed-citation publication-type="other" xlink:type="simple">Wu, S., Liao, C.S. and Jia, J.T. (2003) Chinese Software Registration. Register No. 2003SR4279.</mixed-citation></ref><ref id="scirp.58955-ref22"><label>22</label><mixed-citation publication-type="other" xlink:type="simple">Wu, S., Liao, C.S., Jia, J.T. and Yan, C.H. (2004) Static Design for Multiple Components and Multiple Outlets Rare Earth Countercurrent Extraction (I): Algorithm of Static Design. Journal of the Chinese Society of Rare Earths, 22, 17-21. (In Chinese)</mixed-citation></ref><ref id="scirp.58955-ref23"><label>23</label><mixed-citation publication-type="other" xlink:type="simple">Wu, S., Liao, C.S., Jia, J.T. and Yan, C.H. (2004) Static Design for Multi-Component and Multi-Outlet Rare Earth Countercurrent Extraction (II): Static Design and Its Verification. Journal of the Chinese Society of Rare Earths, 22, 171-176. (In Chinese)</mixed-citation></ref><ref id="scirp.58955-ref24"><label>24</label><mixed-citation publication-type="other" xlink:type="simple">Cheng, F.X., Wu, S., Liao, C.S. and Yan, C.H. (2013) Adjacent Stage Impurity Ratio in Rare Earth Countercurrent Extraction Process. Journal of Rare Earths, 31, 169-173. http://dx.doi.org/10.1016/S1002-0721(12)60253-1</mixed-citation></ref><ref id="scirp.58955-ref25"><label>25</label><mixed-citation publication-type="other" xlink:type="simple">Cheng, F.X., Wu, S., Liu, Y., Wang, S.L., Zhang, B., Liao, C.S. and Yan, C.H. (2014) Minimum Amount of Extracting Solvent for AB/BC Countercurrent Separation Using Aqueous Feed. Separation and Purification Technology, 131, 8-13. http://dx.doi.org/10.1016/j.seppur.2014.04.031</mixed-citation></ref><ref id="scirp.58955-ref26"><label>26</label><mixed-citation publication-type="other" xlink:type="simple">Cheng, F.X., Wu, S., Zhang, B., Liu, Y., Wang, S.L., Liao, C.S. and Yan, C.H. (2014) Minimum Amount of Extracting Solvent of AB/BC Countercurrent Extraction Separation Using Organic Feed. Journal of Rare Earths, 32, 439-444.http://dx.doi.org/10.1016/S1002-0721(14)60091-0</mixed-citation></ref><ref id="scirp.58955-ref27"><label>27</label><mixed-citation publication-type="other" xlink:type="simple">Cheng, F.X., Wu, S., Liu, Y., Wang, S.L., Zhang, B., Liao, C.S. and Yan, C.H. (2014) Minimum Amount of Extracting Solvent of a Separation of Two Rare Earth Components. Advances in Materials Physics and Chemistry, 4, 275-283.http://dx.doi.org/10.4236/ampc.2014.412030</mixed-citation></ref></ref-list></back></article>