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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Plant Sci.</journal-id>
<journal-title>Frontiers in Plant Science</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Plant Sci.</abbrev-journal-title>
<issn pub-type="epub">1664-462X</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="doi">10.3389/fpls.2017.01187</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Plant Science</subject>
<subj-group>
<subject>Original Research</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>A Model of Silicon Dynamics in Rice: An Analysis of the Investment Efficiency of Si Transporters</article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author" corresp="yes">
<name><surname>Sakurai</surname> <given-names>Gen</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<xref ref-type="author-notes" rid="fn001"><sup>&#x0002A;</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/407430/overview"/>
</contrib>
<contrib contrib-type="author">
<name><surname>Yamaji</surname> <given-names>Naoki</given-names></name>
<xref ref-type="aff" rid="aff2"><sup>2</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/39856/overview"/>
</contrib>
<contrib contrib-type="author">
<name><surname>Mitani-Ueno</surname> <given-names>Namiki</given-names></name>
<xref ref-type="aff" rid="aff2"><sup>2</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/207020/overview"/>
</contrib>
<contrib contrib-type="author">
<name><surname>Yokozawa</surname> <given-names>Masayuki</given-names></name>
<xref ref-type="aff" rid="aff3"><sup>3</sup></xref>
</contrib>
<contrib contrib-type="author">
<name><surname>Ono</surname> <given-names>Keisuke</given-names></name>
<xref ref-type="aff" rid="aff4"><sup>4</sup></xref>
</contrib>
<contrib contrib-type="author">
<name><surname>Ma</surname> <given-names>Jian Feng</given-names></name>
<xref ref-type="aff" rid="aff2"><sup>2</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/32294/overview"/>
</contrib>
</contrib-group>
<aff id="aff1"><sup>1</sup><institution>Statistical Modeling Unit, Division of Informatics and Inventory, Institute for Agro-Environmental Sciences, National Agriculture and Food Research Organization</institution> <country>Tsukuba, Japan</country></aff>
<aff id="aff2"><sup>2</sup><institution>Group of Plant Stress Physiology, Institute of Plant Science and Resources, Okayama University</institution> <country>Kurashiki, Japan</country></aff>
<aff id="aff3"><sup>3</sup><institution>Faculty of Human Sciences, Waseda University</institution> <country>Tokorozawa, Japan</country></aff>
<aff id="aff4"><sup>4</sup><institution>Crop-Climate Interaction Unit, Division of Climate Change, Institute for Agro-Environmental Sciences, National Agriculture and Food Research Organization</institution> <country>Tsukuba, Japan</country></aff>
<author-notes>
<fn fn-type="edited-by"><p>Edited by: Jan Kofod Schjoerring, University of Copenhagen, Denmark</p></fn>
<fn fn-type="edited-by"><p>Reviewed by: Miroslav T. Nikolic, University of Belgrade, Serbia; Motohide Seki, Kyushu University, Japan</p></fn>
<fn fn-type="corresp" id="fn001"><p>&#x0002A;Correspondence: Gen Sakurai <email>sakuraigen&#x00040;affrc.go.jp</email></p></fn>
<fn fn-type="other" id="fn002"><p>This article was submitted to Plant Nutrition, a section of the journal Frontiers in Plant Science</p></fn></author-notes>
<pub-date pub-type="epub">
<day>11</day>
<month>07</month>
<year>2017</year>
</pub-date>
<pub-date pub-type="collection">
<year>2017</year>
</pub-date>
<volume>8</volume>
<elocation-id>1187</elocation-id>
<history>
<date date-type="received">
<day>01</day>
<month>05</month>
<year>2017</year>
</date>
<date date-type="accepted">
<day>21</day>
<month>06</month>
<year>2017</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#x000A9; 2017 Sakurai, Yamaji, Mitani-Ueno, Yokozawa, Ono and Ma.</copyright-statement>
<copyright-year>2017</copyright-year>
<copyright-holder>Sakurai, Yamaji, Mitani-Ueno, Yokozawa, Ono and Ma</copyright-holder>
<license xlink:href="http://creativecommons.org/licenses/by/4.0/"><p>This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) or licensor are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.</p></license>
</permissions>
<abstract><p>Silicon is the second most abundant element in soils and is beneficial for plant growth. Although, the localizations and polarities of rice Si transporters have been elucidated, the mechanisms that control the expression of Si transporter genes and the functional reasons for controlling expression are not well-understood. We developed a new model that simulates the dynamics of Si in the whole plant in rice by considering Si transport in the roots, distribution at the nodes, and signaling substances controlling transporter gene expression. To investigate the functional reason for the diurnal variation of the expression level, we compared investment efficiencies (the amount of Si accumulated in the upper leaf divided by the total expression level of Si transporter genes) at different model settings. The model reproduced the gradual decrease and diurnal variation of the expression level of the transporter genes observed by previous experimental studies. The results of simulation experiments showed that a considerable reduction in the expression of Si transporter genes during the night increases investment efficiency. Our study suggests that rice has a system that maximizes the investment efficiency of Si uptake.</p></abstract>
<kwd-group>
<kwd>silicon</kwd>
<kwd>mathematical model</kwd>
<kwd>silicon transporter</kwd>
<kwd>rice</kwd>
<kwd>silicon transport</kwd>
</kwd-group>
<counts>
<fig-count count="9"/>
<table-count count="0"/>
<equation-count count="26"/>
<ref-count count="29"/>
<page-count count="11"/>
<word-count count="7624"/>
</counts>
</article-meta>
</front>
<body>
<sec sec-type="intro" id="s1">
<title>Introduction</title>
<p>Once taken up by roots, mineral elements are transported to upper part with transpiration stream, followed by distributing to different organs and tissues. Understanding of the mechanisms that control the dynamics of both water and mineral elements is an important issue in plant science. Over the past decade, many transporters for uptake of mineral elements have been identified, including those in rice for N, P, K, Mg, B, Mn, Zn, Fe, and Si (Sasaki et al., <xref ref-type="bibr" rid="B21">2016</xref>). These transporters are located in the plasma membrane. Moreover, some these transporters show polar localization. For example, Si influx transporter Lsi1 is localized to the distal side of the root exodermis and endodermis (Ma et al., <xref ref-type="bibr" rid="B16">2006</xref>), while Si efflux transporter Lsi2 is localized to the proximal side of the same cells (Ma et al., <xref ref-type="bibr" rid="B17">2007</xref>).</p>
<p>An important challenge is to develop a mathematical model that can simulate the dynamics of both water and mineral elements in the whole plant to quantitatively understand the complex mineral element transporting systems. Transporter expression depends on mineral concentrations in tissues (Sasaki et al., <xref ref-type="bibr" rid="B21">2016</xref>). To quantify the dynamics of mineral element transport, it is necessary to consider multiple factors simultaneously including transporter activities in roots and shoots, the dynamics of xylem sap and phloem sap, and the expression levels of the transporter genes.</p>
<p>For water flow in plants, the models using an analogy with an electric circuit (Landsberg and Fowkes, <xref ref-type="bibr" rid="B12">1978</xref>) is one of the most historical models. In these models, water potential (potential energy of water per unit volume relative to pure water) is treated like voltage in a circuit. Water flows according to the difference in water potentials. Because the flow of water in the phloem is strongly related to sucrose concentration, some models treat water and sucrose dynamics simultaneously (Daudet et al., <xref ref-type="bibr" rid="B2">2002</xref>; Lacointe and Minchin, <xref ref-type="bibr" rid="B11">2008</xref>; Lobet et al., <xref ref-type="bibr" rid="B13">2014</xref>; Seki et al., <xref ref-type="bibr" rid="B23">2015</xref>). For the transportation of substances in plant, several different concepts are used to model transport of mineral elements and organic pollutants from roots. In the compartment model, the plants are divided into several compartments (such as root and leaf), and substances are assumed to be transported among the compartments according to transition rates that are determined as parameter values (Fryer and Collins, <xref ref-type="bibr" rid="B7">2003</xref>; Fantke et al., <xref ref-type="bibr" rid="B5">2013</xref>; Trapp, <xref ref-type="bibr" rid="B25">2014</xref>). However, these macro-scale models do not consider not only water flow dynamics but also such micro-scale characteristics as the location and activity of the transporters. On the other hand, in models that simulate the dynamics of substances at the micro-scale (Grieneisen et al., <xref ref-type="bibr" rid="B9">2007</xref>, <xref ref-type="bibr" rid="B8">2012</xref>; Sakurai et al., <xref ref-type="bibr" rid="B20">2015</xref>; Yamaji et al., <xref ref-type="bibr" rid="B29">2015</xref>; Foster and Miklavcic, <xref ref-type="bibr" rid="B6">2016</xref>), substance flow is simulated by diffusion and convection in which the location and polarity of the transporters are considered. However, these models simulate dynamics at the cell or tissue level but not in the whole plant level.</p>
<p>The purpose of this study is to develop a new mathematical model that simulate silicon (Si) transport in whole plant in rice. Si is abundant in soils and is beneficial for plant growth (Ma and Takahashi, <xref ref-type="bibr" rid="B14">2002</xref>). Si deposited in plant tissues enhances tolerance to abiotic and biotic stresses via alleviation of water stress, improvement of light interception characteristics by keeping the leaf blade erect, and an increase in resistance to diseases, pests, and lodging (Epstein, <xref ref-type="bibr" rid="B4">1994</xref>; Savant et al., <xref ref-type="bibr" rid="B22">1997</xref>; Ma and Takahashi, <xref ref-type="bibr" rid="B14">2002</xref>). In rice roots, the passive transporter Lsi1 (OsLsi1) and the active transporter Lsi2 (OsLsi2) are involved in Si uptake (Ma et al., <xref ref-type="bibr" rid="B16">2006</xref>, <xref ref-type="bibr" rid="B17">2007</xref>). Both are located in the plasma membranes of the exodermal and endodermal cells, where Casparian strips are located. Lsi1 transports Si along the Si gradient between the plasma membrane, whereas Lsi2 transports Si from the symplast to the apoplast, and this transport is coupled with proton antiport (Ma et al., <xref ref-type="bibr" rid="B15">2011</xref>). In rice nodes, Lsi2, Lsi3 (OsLsi3, active), and Lsi6 (OsLsi6, passive) transport Si from enlarged vascular bundles (EVB) to diffuse vascular bundles (DVB) for preferential distribution of Si to the grains (Yamaji and Ma, <xref ref-type="bibr" rid="B28">2014</xref>; Yamaji et al., <xref ref-type="bibr" rid="B29">2015</xref>). Dehydration stress decreases the expression of Lsi1 and Lsi2 via abscisic acid (ABA) in root (Yamaji and Ma, <xref ref-type="bibr" rid="B26">2007</xref>). The expression of these transporter genes show a diurnal variation (Yamaji and Ma, <xref ref-type="bibr" rid="B26">2007</xref>). More recently, it was reported that the expression of Lsi1 and Lsi2 genes is controlled by Si accumulation in the shoots, not in the roots (Mitani-Ueno et al., <xref ref-type="bibr" rid="B18">2016</xref>). However, the mathematical models that simulate Si dynamics in whole plant have not been constructed yet.</p>
<p>In recent mathematical models of Si transport in both the root and node of rice (Sakurai et al., <xref ref-type="bibr" rid="B20">2015</xref>; Yamaji et al., <xref ref-type="bibr" rid="B29">2015</xref>), Si is assumed to be transported via diffusion and convection. In a previous study (Sakurai et al., <xref ref-type="bibr" rid="B20">2015</xref>), we modeled the dynamics of Si transport from external solution to the cortex and stele of the root using a diffusion equation in which Si diffuses along the gradient of Si concentrations on a two-dimensional grid (4 &#x000D7; 4 &#x003BC;m). Using this micro-scale diffusion model, we could explain the dynamics of the micro-scale Si transport and could account for the characteristics of the spatial location of the transporters. The parameters of the models estimated using statistical computation methods, and the simulation output match the empirical data well. However, it is difficult to extend these models to whole-plant simulation.</p>
<p>In this study, we propose a new mathematical model that simulates Si transport in the whole plant using empirical data and knowledge from previous modeling studies. Using the model, we examined the factors and mechanisms affecting the expression of Si transporter genes. We assumed three possible signaling mechanisms that control the expression of Si transporter genes in this model: accumulation control, shortage control, and water stress control. Under accumulation control, expression is reduced by excess Si concentration in leaf cells. Under shortage control, expression is increased by low Si concentration in leaf cells. Under water stress control, expression responds to water stress (indicated by transpiration rate in this model). We compared the expression levels simulated by the models with those observed. Finally, using the model, we investigated the reason for the diurnal change of transporter gene expression levels in rice from the point of view of investment efficiency.</p>
</sec>
<sec id="s2">
<title>Model and data</title>
<sec>
<title>Model structure</title>
<p>To consider the dynamics of water, sucrose, starch, Si, and the signals that control the expression level of Si transporter genes at the whole-plant level, we divided the whole plant into multiple points and connected them like in an electric circuit (Figure <xref ref-type="fig" rid="F1">1</xref>). In an electric circuit, a point of two or more elements is referred to as a &#x0201C;node,&#x0201D; but in biology the junction region of leaves and branches to the stem is also referred to as a &#x0201C;node;&#x0201D; therefore, we call a point in a circuit a &#x0201C;hydraulic node&#x0201D; (Figure <xref ref-type="fig" rid="F1">1</xref>).</p>
<fig id="F1" position="float">
<label>Figure 1</label>
<caption><p>Schematic diagram of the model structure. The model is composed of a phloem network and a xylem network. The two networks are combined at each hydraulic node.</p></caption>
<graphic xlink:href="fpls-08-01187-g0001.tif"/>
</fig>
</sec>
<sec>
<title>Water flow</title>
<p>The flow of water and sucrose in the xylem and phloem was calculated following the model proposed by Daudet et al. (<xref ref-type="bibr" rid="B2">2002</xref>). In this model, the axial water flow between hydraulic nodes conforms to the Ohm&#x00027;s law:</p>
<disp-formula id="E1"><label>(1)</label><mml:math id="M1"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mrow><mml:mtext>W</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mtext>X</mml:mtext></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mo>&#x02212;</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mi>&#x003A8;</mml:mi><mml:mrow><mml:mtext>X</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mi>j</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:msub><mml:mo>&#x02212;</mml:mo><mml:msub><mml:mi>&#x003A8;</mml:mi><mml:mrow><mml:mtext>X</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mi>i</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>r</mml:mi><mml:mrow><mml:mtext>X</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mrow></mml:math></disp-formula>
<p>where <italic>J</italic><sub>W(<italic>i,j</italic>)X</sub> is axial water flow in the xylem from the hydraulic node <italic>i</italic> to <italic>j</italic>, &#x003A8;<sub>X(<italic>i</italic>)</sub> and &#x003A8;<sub>X(<italic>j</italic>)</sub> is xylem water potential at the hydraulic node <italic>i</italic> and <italic>j</italic>, and <italic>r</italic><sub>X(<italic>i,j</italic>)</sub> is xylem flow resistance (Daudet et al., <xref ref-type="bibr" rid="B2">2002</xref>). Water moves from one area to another in accordance with the gradient of water potential in the xylem (Cosgrove, <xref ref-type="bibr" rid="B1">2010</xref>). Daudet et al. (<xref ref-type="bibr" rid="B2">2002</xref>) suggested a formula to describe the flow between the phloem and xylem and within the phloem. The lateral water flow between the xylem and phloem (<italic>J</italic><sub>W(<italic>i</italic>)Lat</sub>) is described as:</p>
<disp-formula id="E2"><label>(2)</label><mml:math id="M2"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mrow><mml:mtext>W</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mi>i</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mtext>Lat</mml:mtext></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mo>&#x02212;</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mi>&#x003A8;</mml:mi><mml:mrow><mml:mtext>P</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mi>i</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:msub><mml:mo>&#x02212;</mml:mo><mml:msub><mml:mi>&#x003A8;</mml:mi><mml:mrow><mml:mtext>X</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mi>i</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>r</mml:mi><mml:mrow><mml:mtext>Lat</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mi>i</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mrow></mml:math></disp-formula>
<p>where &#x003A8;<sub>X(<italic>i</italic>)</sub> is water potential in the xylem, &#x003A8;<sub>P(<italic>i</italic>)</sub> is water potential in the phloem, and <italic>r</italic><sub>Lat(<italic>i</italic>)</sub> is the sum of the apoplastic pathway resistance between the xylem and phloem (Daudet et al., <xref ref-type="bibr" rid="B2">2002</xref>). Axial water flow in the phloem [<italic>J</italic><sub>W(<italic>i,j</italic>)P</sub>] is described as:</p>
<disp-formula id="E3"><label>(3)</label><mml:math id="M3"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mrow><mml:mtext>W</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mtext>P</mml:mtext></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mo>&#x02212;</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:mtext>P</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mi>j</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:msub><mml:mo>&#x02212;</mml:mo><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:mtext>P</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mi>i</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>r</mml:mi><mml:mrow><mml:mtext>P</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mrow></mml:math></disp-formula>
<p>where <italic>P</italic><sub>P(<italic>i</italic>)</sub> and <italic>P</italic><sub>P(<italic>j</italic>)</sub> is hydraulic (mainly turgor) pressure in the phloem at the hydraulic node <italic>i</italic> and <italic>j</italic> and <italic>r</italic><sub>P(<italic>i,j</italic>)</sub> is phloem flow resistance. Because gravity can be ignored when calculating water flow on a small scale, the following equation holds (Daudet et al., <xref ref-type="bibr" rid="B2">2002</xref>):</p>
<disp-formula id="E4"><label>(4)</label><mml:math id="M4"><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:mtext>P</mml:mtext><mml:mo stretchy='false'>(</mml:mo><mml:mi>i</mml:mi><mml:mo stretchy='false'>)</mml:mo></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>&#x003A8;</mml:mi><mml:mrow><mml:mi>P</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>i</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:msub><mml:mo>&#x02212;</mml:mo><mml:msub><mml:mi>&#x003A0;</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></disp-formula>
<p>where &#x003A8;<sub>P(<italic>i</italic>)</sub> is water potential in the phloem and &#x003A0;<sub><italic>i</italic></sub> is osmotic potential. The latter can be described as:</p>
<disp-formula id="E5"><label>(5)</label><mml:math id="M5"><mml:mrow><mml:msub><mml:mi>&#x003A0;</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mo>&#x02212;</mml:mo><mml:mi>R</mml:mi><mml:mtext>&#x000A0;</mml:mtext><mml:mo>&#x000B7;</mml:mo><mml:mtext>&#x000A0;</mml:mtext><mml:msub><mml:mi>T</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mtext>&#x000A0;</mml:mtext><mml:mo>&#x000B7;</mml:mo><mml:mtext>&#x000A0;</mml:mtext><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mtext>S</mml:mtext><mml:mo stretchy='false'>(</mml:mo><mml:mi>i</mml:mi><mml:mo stretchy='false'>)</mml:mo></mml:mrow></mml:msub></mml:mrow></mml:math></disp-formula>
<p>where <italic>R</italic> is the universal gas constant, <italic>T</italic><sub><italic>i</italic></sub> is absolute temperature, and <italic>C</italic><sub>S(<italic>i</italic>)</sub> is sucrose concentration. The axial phloem solute flow [<italic>J</italic><sub>S(<italic>i,j</italic>)</sub>] is described as:</p>
<disp-formula id="E6"><label>(6)</label><mml:math id="M6"><mml:mrow><mml:mrow><mml:mo>{</mml:mo><mml:mtable columnalign='left'><mml:mtr><mml:mtd><mml:msub><mml:mi>J</mml:mi><mml:mrow><mml:mtext>S</mml:mtext><mml:mo stretchy='false'>(</mml:mo><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi><mml:mo stretchy='false'>)</mml:mo></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>J</mml:mi><mml:mrow><mml:mtext>W</mml:mtext><mml:mo stretchy='false'>(</mml:mo><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi><mml:mo stretchy='false'>)</mml:mo><mml:mtext>P</mml:mtext></mml:mrow></mml:msub><mml:mtext>&#x000A0;</mml:mtext><mml:mo>&#x000B7;</mml:mo><mml:mtext>&#x000A0;</mml:mtext><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mtext>S</mml:mtext><mml:mo stretchy='false'>(</mml:mo><mml:mi>i</mml:mi><mml:mo stretchy='false'>)</mml:mo></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:mo>&#x000A0;</mml:mo><mml:mtext>when</mml:mtext><mml:mo>&#x000A0;</mml:mo><mml:msub><mml:mi>J</mml:mi><mml:mrow><mml:mtext>W</mml:mtext><mml:mo stretchy='false'>(</mml:mo><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi><mml:mo stretchy='false'>)</mml:mo><mml:mtext>P</mml:mtext></mml:mrow></mml:msub><mml:mo>&#x0003E;</mml:mo><mml:mn>0</mml:mn></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:msub><mml:mi>J</mml:mi><mml:mrow><mml:mtext>S</mml:mtext><mml:mo stretchy='false'>(</mml:mo><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi><mml:mo stretchy='false'>)</mml:mo></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>J</mml:mi><mml:mrow><mml:mtext>W</mml:mtext><mml:mo stretchy='false'>(</mml:mo><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi><mml:mo stretchy='false'>)</mml:mo><mml:mtext>P</mml:mtext></mml:mrow></mml:msub><mml:mtext>&#x000A0;</mml:mtext><mml:mo>&#x000B7;</mml:mo><mml:mtext>&#x000A0;</mml:mtext><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mtext>S</mml:mtext><mml:mo stretchy='false'>(</mml:mo><mml:mi>j</mml:mi><mml:mo stretchy='false'>)</mml:mo></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:mo>&#x000A0;</mml:mo><mml:mtext>when</mml:mtext><mml:mo>&#x000A0;</mml:mo><mml:msub><mml:mi>J</mml:mi><mml:mrow><mml:mtext>W</mml:mtext><mml:mo stretchy='false'>(</mml:mo><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi><mml:mo stretchy='false'>)</mml:mo><mml:mtext>P</mml:mtext></mml:mrow></mml:msub><mml:mo>&#x0003C;</mml:mo><mml:mn>0</mml:mn></mml:mtd></mml:mtr></mml:mtable></mml:mrow></mml:mrow></mml:math></disp-formula>
<p>where <italic>J</italic><sub>W(<italic>i,j</italic>)P</sub> is the axial water flow in the phloem. Because the purpose of the model developed in this study was to estimate the dynamics of mineral transport rather than sucrose flow, we ignored lateral sucrose flow for simplicity.</p>
<p>The flow of water should be conserved at any hydraulic node in the xylem and phloem. Therefore, the following equation should hold:</p>
<disp-formula id="E7"><label>(7)</label><mml:math id="M7"><mml:mrow><mml:mstyle displaystyle='true'><mml:mo>&#x02211;</mml:mo><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mtext>W</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:mn>0</mml:mn></mml:mrow></mml:mstyle></mml:mrow></mml:math></disp-formula>
<p>where <italic>J</italic><sub>W</sub> is the water flow from the target hydraulic node to the connected nodes. As this equation should hold at any node, we can estimate water potential at each hydraulic node at any time point by solving simultaneous equations under an appropriate boundary condition.</p>
<p>To calculate osmotic potential, we need sucrose concentration. In this model, we simply input the photosynthetic and transpiration rates as the boundary condition. Following photosynthesis, starch is synthesized in the leaf. The starch is dehydrated to sucrose and gradually loaded into the phloem, which is conveyed by the flow in the phloem, which follows the hydraulic pressure. The models of the dynamics of starch and sucrose in leaves and other tissues, which are similar to that of Daudet et al. (<xref ref-type="bibr" rid="B2">2002</xref>), are explained in Supplementary Information.</p>
</sec>
<sec>
<title>Si transport</title>
<p>To understand the dynamics of Si in the whole shoot, we developed a simple two-compartment model that emulates the transport of Si in root. If we assume the compartmentation of the root cortex between the external solution (soil) and root stele, then the flow of Si from external solution (soil) to the cortex can be described as:</p>
<disp-formula id="E8"><label>(8)</label><mml:math id="M8"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mrow><mml:mtext>M</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mtext>o</mml:mtext><mml:mo>:</mml:mo><mml:mtext>c</mml:mtext></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mi>&#x003B1;</mml:mi><mml:mtext>&#x000A0;</mml:mtext><mml:mo>&#x000B7;</mml:mo><mml:mtext>&#x000A0;</mml:mtext><mml:mi>t</mml:mi><mml:msub><mml:mi>r</mml:mi><mml:mrow><mml:mtext>exo</mml:mtext></mml:mrow></mml:msub><mml:mtext>&#x000A0;</mml:mtext><mml:mo>&#x000B7;</mml:mo><mml:mtext>&#x000A0;</mml:mtext><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mtext>M</mml:mtext><mml:mo>:</mml:mo><mml:mtext>out</mml:mtext></mml:mrow></mml:msub><mml:mo>&#x02212;</mml:mo><mml:msub><mml:mi>p</mml:mi><mml:mrow><mml:mtext>cm</mml:mtext></mml:mrow></mml:msub><mml:mtext>&#x000A0;</mml:mtext><mml:mo>&#x000B7;</mml:mo><mml:mtext>&#x000A0;</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mtext>M</mml:mtext><mml:mo>:</mml:mo><mml:mtext>cor</mml:mtext></mml:mrow></mml:msub><mml:mo>&#x02212;</mml:mo><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mtext>M</mml:mtext><mml:mo>:</mml:mo><mml:mtext>out</mml:mtext></mml:mrow></mml:msub></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:math></disp-formula>
<p>where <italic>J</italic><sub>M(o:c)</sub> is the flow of Si from external solution (soil) to the cortex, &#x003B1; regulates the expression level of the transporter (from 0 to 1), <italic>tr</italic><sub>exo</sub> is the transportation capability at the maximum expression level in exodermal cells, <italic>C</italic><sub>M:out</sub> and <italic>C</italic><sub>M:cor</sub> are Si concentrations in external solution and the cortex, respectively, and <italic>p</italic><sub>cm</sub> is the permeability of the cell membrane (Sakurai et al., <xref ref-type="bibr" rid="B20">2015</xref>). Si is transported by endodermal transporters from the cortex to the stele; this flow can be described as:</p>
<disp-formula id="E9"><label>(9)</label><mml:math id="M9"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mrow><mml:mtext>M</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mtext>c</mml:mtext><mml:mo>:</mml:mo><mml:mtext>s</mml:mtext></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mi>&#x003B1;</mml:mi><mml:mtext>&#x000A0;</mml:mtext><mml:mo>&#x000B7;</mml:mo><mml:mtext>&#x000A0;</mml:mtext><mml:mi>t</mml:mi><mml:msub><mml:mi>r</mml:mi><mml:mrow><mml:mtext>end</mml:mtext></mml:mrow></mml:msub><mml:mtext>&#x000A0;</mml:mtext><mml:mo>&#x000B7;</mml:mo><mml:mtext>&#x000A0;</mml:mtext><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mtext>M</mml:mtext><mml:mo>:</mml:mo><mml:mtext>cor</mml:mtext></mml:mrow></mml:msub><mml:mo>&#x02212;</mml:mo><mml:msub><mml:mi>p</mml:mi><mml:mrow><mml:mtext>cm</mml:mtext></mml:mrow></mml:msub><mml:mtext>&#x000A0;</mml:mtext><mml:mo>&#x000B7;</mml:mo><mml:mtext>&#x000A0;</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mtext>M</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mi>n</mml:mi><mml:mi>r</mml:mi></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:msub><mml:mo>&#x02212;</mml:mo><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mtext>M</mml:mtext><mml:mo>:</mml:mo><mml:mtext>cor</mml:mtext></mml:mrow></mml:msub></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:math></disp-formula>
<p>where <italic>J</italic><sub>M(c:s)</sub> is the flow of Si from the cortex to the stele, <italic>tr</italic><sub>end</sub> is the transportation capability at the maximum expression level in the endodermis, <italic>C</italic><sub>M(<italic>nr</italic>)</sub> is the Si concentration in the stele (i.e., in the hydraulic node of the root), and <italic>nr</italic> is the sequential number of the hydraulic node of the root.</p>
<p>Note that both <italic>tr</italic><sub>exo</sub> (Equation 8) and <italic>tr</italic><sub>end</sub> (Equation 9) include the activity of both Lsi1 and Lsi2. The change of Si concentration can be described as:</p>
<disp-formula id="E10"><label>(10)</label><mml:math id="M10"><mml:mfrac><mml:mrow><mml:mi>d</mml:mi><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mtext>M</mml:mtext><mml:mo>:</mml:mo><mml:mtext>cor</mml:mtext></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mi>d</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:mfrac><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mrow><mml:mtext>M</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mtext>o</mml:mtext><mml:mo>:</mml:mo><mml:mtext>c</mml:mtext></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:msub><mml:mo>&#x02212;</mml:mo><mml:msub><mml:mi>J</mml:mi><mml:mrow><mml:mtext>M</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mtext>c</mml:mtext><mml:mo>:</mml:mo><mml:mtext>s</mml:mtext></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>V</mml:mi><mml:mrow><mml:mtext>cor</mml:mtext></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:math></disp-formula>
<disp-formula id="E11"><label>(11)</label><mml:math id="M11"><mml:mfrac><mml:mrow><mml:mi>d</mml:mi><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mtext>M</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mi>n</mml:mi><mml:mi>r</mml:mi></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mi>d</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:mfrac><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mrow><mml:mtext>M</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mtext>c</mml:mtext><mml:mo>:</mml:mo><mml:mtext>s</mml:mtext></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:msub><mml:mo>&#x02212;</mml:mo><mml:msub><mml:mi>J</mml:mi><mml:mrow><mml:mtext>M</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mi>n</mml:mi><mml:mi>r</mml:mi><mml:mo>,</mml:mo><mml:mi>n</mml:mi><mml:mi>r</mml:mi><mml:mo>&#x02212;</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>V</mml:mi><mml:mrow><mml:mtext>st</mml:mtext><mml:mo stretchy='false'>(</mml:mo><mml:mi>i</mml:mi><mml:mo stretchy='false'>)</mml:mo></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:math></disp-formula>
<p>where <italic>V</italic><sub>cor</sub> is the tissue volume of the cortex (assumed to be 1 ml for simplicity), <italic>J</italic><sub>M(<italic>nr</italic>,<italic>nr</italic>&#x02212;1)</sub> is the flow of Si from the root to the hydraulic node above the root, and <italic>V</italic><sub>st(<italic>i</italic>)</sub> is the tissue volume of the sieve tube.</p>
<p>We assumed that Si absorbed in the root is transported with the flow of water only in the xylem. Therefore, the following equation holds for any node:</p>
<disp-formula id="E12"><label>(12)</label><mml:math id="M12"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mrow><mml:mtext>M</mml:mtext><mml:mo stretchy='false'>(</mml:mo><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi><mml:mo stretchy='false'>)</mml:mo></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mtext>M</mml:mtext><mml:mo stretchy='false'>(</mml:mo><mml:mi>i</mml:mi><mml:mo stretchy='false'>)</mml:mo></mml:mrow></mml:msub><mml:mtext>&#x000A0;</mml:mtext><mml:mo>&#x000B7;</mml:mo><mml:mtext>&#x000A0;</mml:mtext><mml:msub><mml:mi>J</mml:mi><mml:mrow><mml:mtext>W</mml:mtext><mml:mo stretchy='false'>(</mml:mo><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi><mml:mo stretchy='false'>)</mml:mo><mml:mtext>X</mml:mtext></mml:mrow></mml:msub></mml:mrow></mml:math></disp-formula>
<p>where <italic>J</italic><sub>M(<italic>i,j</italic>)</sub> is the axial Si flow in the xylem and <italic>C</italic><sub>M(<italic>i</italic>)</sub> is Si concentration. The model assumes only transpiration as the force driving the water in the xylem; it does not consider the case when <italic>J</italic><sub>W(<italic>i,j</italic>)X</sub> is negative.</p>
<p>Using a diffusion equation for Si transport between EVB and DVB, we previously revealed the importance of the apoplastic barrier at the bundle sheath cells and suggested that transporters generate large differences in Si concentration between DVB and EVB to enable rice to transfer sufficient Si upward (Yamaji et al., <xref ref-type="bibr" rid="B29">2015</xref>). Here, to model the dynamics of Si in the whole shoot, we simplified the model of Si distribution at the node as follows:</p>
<disp-formula id="E13"><label>(13)</label><mml:math id="M13"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mrow><mml:mtext>M</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>J</mml:mi><mml:mrow><mml:mtext>W</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:msub><mml:mtext>&#x000A0;</mml:mtext><mml:mo>&#x000B7;</mml:mo><mml:mtext>&#x000A0;</mml:mtext><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mtext>M</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mi>i</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mtext>DVB</mml:mtext></mml:mrow></mml:msub></mml:mrow></mml:math></disp-formula>
<disp-formula id="E14"><label>(14)</label><mml:math id="M14"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mrow><mml:mtext>M</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>k</mml:mi></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>J</mml:mi><mml:mrow><mml:mtext>W</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>k</mml:mi></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:msub><mml:mtext>&#x000A0;</mml:mtext><mml:mo>&#x000B7;</mml:mo><mml:mtext>&#x000A0;</mml:mtext><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mtext>M</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mi>i</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mtext>EVB</mml:mtext></mml:mrow></mml:msub></mml:mrow></mml:math></disp-formula>
<disp-formula id="E15"><label>(15)</label><mml:math id="M15"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mtext>M</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mi>i</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mtext>DVB</mml:mtext></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>&#x003C1;</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mtext>&#x000A0;</mml:mtext><mml:mo>&#x000B7;</mml:mo><mml:mtext>&#x000A0;</mml:mtext><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mtext>M</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mi>i</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mtext>EVB</mml:mtext></mml:mrow></mml:msub></mml:mrow></mml:math></disp-formula>
<disp-formula id="E16"><label>(16)</label><mml:math id="M16"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mtext>M</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mi>i</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mtext>EVB</mml:mtext></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mrow><mml:mtext>W</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>k</mml:mi></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>J</mml:mi><mml:mrow><mml:mtext>W</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>&#x003C1;</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mtext>&#x000A0;</mml:mtext><mml:mo>&#x000B7;</mml:mo><mml:mtext>&#x000A0;</mml:mtext><mml:msub><mml:mi>J</mml:mi><mml:mrow><mml:mtext>W</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>k</mml:mi></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>J</mml:mi><mml:mrow><mml:mtext>W</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mtext>&#x000A0;</mml:mtext><mml:mo>&#x000B7;</mml:mo><mml:mtext>&#x000A0;</mml:mtext><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mtext>M</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mi>i</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:msub></mml:mrow></mml:math></disp-formula>
<p>where <italic>J</italic><sub>M<italic>(i,j)</italic></sub> and <italic>J</italic><sub>M<italic>(i,k)</italic></sub> are Si flow, <italic>J</italic><sub>W<italic>(i,j)</italic></sub> and <italic>J</italic><sub>W<italic>(i,k)</italic></sub> are water flow, <italic>C</italic><sub>M</sub>(<italic>i</italic>)<sub>DVB</sub> and <italic>C</italic><sub>M(<italic>i</italic>)EVB</sub> are Si concentrations in DVB and EVB, respectively, and &#x003C1;<sub><italic>i</italic></sub> determines how Si concentration increases in DVB. We assume that hydraulic node <italic>j</italic> is connected to hydraulic node <italic>i</italic> via DVB and that <italic>k</italic> is connected to <italic>i</italic> via EVB (see also Supplementary Figure <xref ref-type="supplementary-material" rid="SM2">1</xref>). Increasing the concentration of Si in DVB can distribute a large amount of Si to upper developing tissues, to which DVB connects (Yamaji et al., <xref ref-type="bibr" rid="B29">2015</xref>). This is the function of &#x003C1;<sub><italic>i</italic></sub>.</p>
<p>We assumed that Si is unloaded in each tissue according to the following equation:</p>
<disp-formula id="E17"><label>(17)</label><mml:math id="M17"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mrow><mml:mtext>M</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mi>i</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mtext>unload</mml:mtext></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>k</mml:mi><mml:mrow><mml:mtext>M</mml:mtext><mml:mo>:</mml:mo><mml:mtext>unload</mml:mtext></mml:mrow></mml:msub><mml:mtext>&#x000A0;</mml:mtext><mml:mo>&#x000B7;</mml:mo><mml:mtext>&#x000A0;</mml:mtext><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mtext>M</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mi>i</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:msub><mml:mtext>&#x000A0;</mml:mtext><mml:mo>&#x000B7;</mml:mo><mml:mtext>&#x000A0;</mml:mtext><mml:msub><mml:mi>V</mml:mi><mml:mrow><mml:mtext>con</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mi>i</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:msub></mml:mrow></mml:math></disp-formula>
<p>where <italic>J</italic><sub>M(<italic>i</italic>)unload</sub> is Si flow from the xylem to tissue cells, <italic>k</italic><sub>M:unload</sub> is a parameter, and <italic>V</italic><sub>con(<italic>i</italic>)</sub> is the tissue volume of the conduit. The Si concentration in tissue cells, <italic>C</italic><sub>M(<italic>i</italic>)cyt</sub>, is calculated as:</p>
<disp-formula id="E18"><label>(18)</label><mml:math id="M18"><mml:mrow><mml:mfrac><mml:mrow><mml:mi>d</mml:mi><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mtext>M</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mi>i</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mtext>cyt</mml:mtext></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mi>d</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:mfrac><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mrow><mml:mtext>M</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mi>i</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mtext>unload</mml:mtext></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>V</mml:mi><mml:mrow><mml:mtext>cyt</mml:mtext><mml:mo stretchy='false'>(</mml:mo><mml:mi>i</mml:mi><mml:mo stretchy='false'>)</mml:mo></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mrow></mml:math></disp-formula>
<p>where <italic>V</italic><sub>cyt(<italic>i</italic>)</sub> is the volume of the cytoplasm in the tissue.</p>
</sec>
<sec>
<title>Transport of a signaling substances</title>
<p>Lsi2 expression is decreased by high Si accumulation in the shoot through an unknown signal from shoots to roots (Yamaji and Ma, <xref ref-type="bibr" rid="B27">2011</xref>), and the expression of Lsi1 and Lsi2 is decreased by dehydration stress (Yamaji and Ma, <xref ref-type="bibr" rid="B26">2007</xref>, <xref ref-type="bibr" rid="B27">2011</xref>); the response to dehydration stress is more rapid than the response to Si accumulation. In this study, we used the following models to investigate the dynamics of the unknown signal. We considered the following three types of models for generation of the signal:</p>
<disp-formula id="E19"><label>(19)</label><mml:math id="M19"><mml:mrow><mml:mtext>Accumulation&#x000A0;control</mml:mtext><mml:mo>:</mml:mo><mml:mi>G</mml:mi><mml:mi>R</mml:mi><mml:mo>=</mml:mo><mml:mi>s</mml:mi><mml:mi>l</mml:mi><mml:msub><mml:mi>p</mml:mi><mml:mtext>c</mml:mtext></mml:msub><mml:mtext>&#x000A0;</mml:mtext><mml:mo>&#x000B7;</mml:mo><mml:mtext>&#x000A0;</mml:mtext><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mtext>M</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mi>i</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mtext>cyt</mml:mtext></mml:mrow></mml:msub></mml:mrow></mml:math></disp-formula>
<disp-formula id="E20"><label>(20)</label><mml:math id="M20"><mml:mrow><mml:mtext>Shortage&#x000A0;control</mml:mtext><mml:mo>:</mml:mo><mml:mi>G</mml:mi><mml:mi>R</mml:mi><mml:mo>=</mml:mo><mml:mi>s</mml:mi><mml:mi>l</mml:mi><mml:msub><mml:mi>p</mml:mi><mml:mtext>r</mml:mtext></mml:msub><mml:mtext>&#x000A0;</mml:mtext><mml:mo>&#x000B7;</mml:mo><mml:mtext>&#x000A0;</mml:mtext><mml:mo stretchy='false'>(</mml:mo><mml:mn>1</mml:mn><mml:mo>&#x02212;</mml:mo><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mtext>M</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mi>i</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mtext>cyt</mml:mtext></mml:mrow></mml:msub><mml:mo stretchy='false'>)</mml:mo></mml:mrow></mml:math></disp-formula>
<disp-formula id="E21"><label>(21)</label><mml:math id="M21"><mml:mrow><mml:mtext>Water&#x000A0;stress&#x000A0;control</mml:mtext><mml:mo>:</mml:mo><mml:mi>G</mml:mi><mml:mi>R</mml:mi><mml:mo>=</mml:mo><mml:mi>s</mml:mi><mml:mi>l</mml:mi><mml:msub><mml:mi>p</mml:mi><mml:mtext>J</mml:mtext></mml:msub><mml:mtext>&#x000A0;</mml:mtext><mml:mo>&#x000B7;</mml:mo><mml:mtext>&#x000A0;</mml:mtext><mml:mi>T</mml:mi><mml:mi>r</mml:mi><mml:mi>a</mml:mi><mml:mi>n</mml:mi><mml:mi>s</mml:mi></mml:mrow></mml:math></disp-formula>
<p>where <italic>GR</italic> is the rate of signal generation, <italic>slp</italic><sub>c</sub>, <italic>slp</italic><sub>J</sub>, and <italic>slp</italic><sub>r</sub> are parameters that determine the generation rate of signal in response to the target factor, <italic>C</italic><sub>M(<italic>i</italic>)cyt</sub> is Si concentration in leaf cells, and <italic>Trans</italic> is transpiration rate in leaf. For simplicity, we assumed that the signal is generated only in the leaf. Moreover, because the signal is an unknown substance, we did not define its units. Equation (19) represents that the signal is generated according to Si concentration in leaf cells. Equation (20) represents that the signal is generated according to the transpiration rate in leaf. In this situation, we assume that the water stress is in proportion to the transpiration rate. This assumption may be rough approximation because the water stress in a plant would be affected by several factors such as soil moisture, water absorption history, and transpiration rate. However, we adopt this simple assumption because estimating exact water stress is beyond the purpose of this study. Equation (21) represents that the signal is generated according to the shortage of Si in leaf cells. In this situation, the signal transmits the information about shortage of Si. On the other hand, in Equations (19), (20), the signal transmits the information about excess of Si. The signal decays according to decay rate <italic>dec</italic>. That is,</p>
<disp-formula id="E22"><label>(22)</label><mml:math id="M22"><mml:mrow><mml:mfrac><mml:mrow><mml:mi>d</mml:mi><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mi>R</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>i</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mi>d</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:mfrac><mml:mo>=</mml:mo><mml:mo>&#x02212;</mml:mo><mml:mi>d</mml:mi><mml:mi>e</mml:mi><mml:mi>c</mml:mi><mml:mtext>&#x000A0;</mml:mtext><mml:mo>&#x000B7;</mml:mo><mml:mtext>&#x000A0;</mml:mtext><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mi>R</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>i</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:mi>G</mml:mi><mml:mi>R</mml:mi></mml:mrow></mml:math></disp-formula>
<p>where <italic>C</italic><sub>R<italic>(i</italic>)</sub> is signal concentration. We assumed that the generated signal is transferred via the phloem water flow. When the signal reaches the root, the expression level of the Si transporter is regulated according to the signal concentration as follows:</p>
<disp-formula id="E23"><label>(23)</label><mml:math id="M23"><mml:mrow><mml:mi>&#x003B1;</mml:mi><mml:mtext>&#x000A0;</mml:mtext><mml:mo>=</mml:mo><mml:mtext>&#x000A0;max</mml:mtext><mml:mo stretchy='false'>(</mml:mo><mml:mn>0</mml:mn><mml:mo>,</mml:mo><mml:mo>&#x02212;</mml:mo><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mtext>R</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mi>n</mml:mi><mml:mi>r</mml:mi><mml:mo>,</mml:mo><mml:mo>&#x000A0;</mml:mo><mml:mi>t</mml:mi><mml:mo>&#x02212;</mml:mo><mml:mi>&#x003C7;</mml:mi></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:mn>1</mml:mn><mml:mo stretchy='false'>)</mml:mo></mml:mrow></mml:math></disp-formula>
<disp-formula id="E24"><label>(24)</label><mml:math id="M24"><mml:mrow><mml:mi>&#x003B1;</mml:mi><mml:mtext>&#x000A0;</mml:mtext><mml:mo>=</mml:mo><mml:mtext>&#x000A0;min</mml:mtext><mml:mo stretchy='false'>(</mml:mo><mml:mn>1</mml:mn><mml:mo>,</mml:mo><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mtext>R</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mi>n</mml:mi><mml:mi>r</mml:mi><mml:mo>,</mml:mo><mml:mo>&#x000A0;</mml:mo><mml:mi>t</mml:mi><mml:mo>&#x02212;</mml:mo><mml:mi>&#x003C7;</mml:mi></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:msub><mml:mo stretchy='false'>)</mml:mo></mml:mrow></mml:math></disp-formula>
<p>where &#x003B1; is a factor that regulates transporter expression level, <italic>C</italic><sub>R<italic>(nr,t</italic>)</sub> is signal concentration at time <italic>t</italic> (hour), and &#x003C7; is delay of time. It is set to 0 for Accumulation control assumption and Shortage control assumptions but set to 5 for Water stress control situation because the previous study suggests that there is time lag until the decrease of the expression level by dehydration stress (Yamaji and Ma, <xref ref-type="bibr" rid="B27">2011</xref>). Equation (23) is used for Accumulation control and Water stress control assumptions. Equation (24) is used for Shortage control assumption.</p>
</sec>
<sec>
<title>Simulation settings</title>
<p>We set the values of transpiration rate, photosynthesis rate, and temperature as input data. We set the standard transpiration rate to 0.4 ml cm<sup>&#x02212;2</sup> day<sup>&#x02212;1</sup> (Kuwagata et al., <xref ref-type="bibr" rid="B10">2012</xref>) and standard photosynthesis rate to 0.0015 mol cm<sup>&#x02212;2</sup> s<sup>&#x02212;1</sup>. We assumed (i) 10-h night, (ii) 2-h peaks of photosynthesis and transpiration (Figure <xref ref-type="fig" rid="F2">2</xref>), and (iii) a transpiration rate during darkness of 10% of the standard transpiration rate. We also assumed a simplified rice plant structure: (i) the root represented by one segment; (ii) five leaves; (iii) identical internode length; (iv) identical sheath length; and (vi) constant biomass during simulation. The other structural settings are described in Supplementary Table <xref ref-type="supplementary-material" rid="SM1">1</xref>. The simulation period was 4 days.</p>
<fig id="F2" position="float">
<label>Figure 2</label>
<caption><p>Time series of transpiration rate and photosynthesis rate that was used as a boundary condition in simulation.</p></caption>
<graphic xlink:href="fpls-08-01187-g0002.tif"/>
</fig>
</sec>
<sec>
<title>Parameters for transporters in roots</title>
<p>To estimate the values of <italic>tr</italic><sub>exo</sub>, <italic>tr</italic><sub>end</sub>, and <italic>p</italic><sub>cm</sub>, we used time-series Si concentrations in xylem sap of 1-month-old seedlings exposed to 1.0 mM Si solution and measured every 5 min (Sakurai et al., <xref ref-type="bibr" rid="B20">2015</xref>). We estimated parameter distribution using Markov chain Monte Carlo methods with the following likelihood function:</p>
<disp-formula id="E25"><label>(25)</label><mml:math id="M25"><mml:mrow><mml:mi>L</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mi>&#x003B8;</mml:mi><mml:mo>&#x0007C;</mml:mo><mml:mi>D</mml:mi><mml:mi>a</mml:mi><mml:mi>t</mml:mi><mml:mi>a</mml:mi></mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mo>=</mml:mo><mml:mstyle mathsize='140%' displaystyle='true'><mml:mo>&#x0220F;</mml:mo></mml:mstyle><mml:mfrac><mml:mn>1</mml:mn><mml:mrow><mml:msqrt><mml:mrow><mml:mn>2</mml:mn><mml:mi>&#x003C0;</mml:mi><mml:msub><mml:mi>&#x003C3;</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:msqrt></mml:mrow></mml:mfrac><mml:mi>exp</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mo>&#x02212;</mml:mo><mml:mfrac><mml:mrow><mml:mo stretchy='false'>(</mml:mo><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mi>M</mml:mi><mml:mo stretchy='false'>(</mml:mo><mml:mi>n</mml:mi><mml:mi>r</mml:mi><mml:mo stretchy='false'>)</mml:mo><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub><mml:mo stretchy='false'>(</mml:mo><mml:mi>&#x003B8;</mml:mi><mml:mo stretchy='false'>)</mml:mo><mml:mo>&#x02212;</mml:mo><mml:msup><mml:mi>C</mml:mi><mml:mo>&#x02032;</mml:mo></mml:msup><mml:msub><mml:mtext>&#x000A0;</mml:mtext><mml:mrow><mml:mi>M</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mi>n</mml:mi><mml:mi>r</mml:mi></mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mo>,</mml:mo><mml:mo>&#x000A0;</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub><mml:mo stretchy='false'>)</mml:mo><mml:msup><mml:mo>&#x000A0;</mml:mo><mml:mn>2</mml:mn></mml:msup></mml:mrow><mml:mrow><mml:mn>2</mml:mn><mml:msubsup><mml:mi>&#x003C3;</mml:mi><mml:mi>t</mml:mi><mml:mn>2</mml:mn></mml:msubsup></mml:mrow></mml:mfrac></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:math></disp-formula>
<p>where <italic>L</italic> is the likelihood of parameter set &#x003B8; with the observed data set <italic>Data</italic>, &#x003C3;<sub><italic>t</italic></sub> is the standard deviation of the error distribution at time <italic>t, C</italic><sub><italic>M</italic>(<italic>nr</italic>),<italic>t</italic></sub>(&#x003B8;) is the Si concentration in xylem sap at time <italic>t</italic> estimated with the parameter set &#x003B8;, and <italic>C</italic>&#x02032;<sub><italic>M</italic>(<italic>nr</italic>),<italic>t</italic></sub> is the observed Si concentration. We assumed that &#x003C3;<sub><italic>t</italic></sub> is equivalent to the standard deviation of the observed data. The initial setting for <italic>C</italic><sub>M:cor</sub> (Equation 8) was 0.0 mM. The observed time-series data for xylem sap and estimated data are shown in Supplementary Figure <xref ref-type="supplementary-material" rid="SM2">2</xref>. The model adequately estimated the observed Si concentrations.</p>
</sec>
<sec>
<title>Estimation of parameters relevant to respiration</title>
<p>We estimated sucrose dynamics under several parameter settings. The estimated parameter values were 0.1, 0.15, and 0.2 for k4 and 2.0e-5, 4.0e-5, 6.0e-5, 8.0e-5, 10.0e-5, 12.0e-5, 14.0e-5, 16.0e-5, 18.0e-5, and 20.0e-5 for k1 (see Supplementary Information for k1 and k4). The parameter set where sucrose has the stable cyclic dynamics (k1 &#x0003D; 8.0e-5 and k4 &#x0003D; 0.1) was used for the simulation experiment (Supplementary Figure <xref ref-type="supplementary-material" rid="SM2">3</xref>).</p>
</sec>
<sec>
<title>Simulation of Si dynamics</title>
<p>To estimate Si dynamics, we used Equations (19), (20), or (21). In each case, we simulated Si dynamics with several parameter sets for <italic>slp</italic> and <italic>dec</italic>. For the other parameters and input data, we used the same values in all equations. The definitions of variables are described in Supplementary Table <xref ref-type="supplementary-material" rid="SM1">2</xref>. The parameter values used for the simulation are described in Supplementary Tables <xref ref-type="supplementary-material" rid="SM1">2</xref>, <xref ref-type="supplementary-material" rid="SM1">3</xref>.</p>
</sec>
<sec>
<title>Investment efficiency</title>
<p>To evaluate investment efficiency, we defined it as:</p>
<disp-formula id="E26"><label>(26)</label><mml:math id="M26"><mml:mrow><mml:mi>I</mml:mi><mml:mi>E</mml:mi><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mstyle displaystyle='true'><mml:mrow><mml:msubsup><mml:mo>&#x0222B;</mml:mo><mml:mrow><mml:mi>t</mml:mi><mml:mo>=</mml:mo><mml:mi>s</mml:mi><mml:mi>t</mml:mi><mml:mi>r</mml:mi><mml:mi>i</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi><mml:mo>=</mml:mo><mml:mi>e</mml:mi><mml:mi>n</mml:mi><mml:mi>d</mml:mi><mml:mi>i</mml:mi></mml:mrow></mml:msubsup><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mrow><mml:mtext>M</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mn>1</mml:mn><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mtext>unload</mml:mtext></mml:mrow></mml:msub><mml:mtext>&#x000A0;</mml:mtext><mml:mi>d</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:mrow></mml:mstyle><mml:mtext>&#x000A0;</mml:mtext></mml:mrow><mml:mrow><mml:mstyle displaystyle='true'><mml:mrow><mml:msubsup><mml:mo>&#x0222B;</mml:mo><mml:mrow><mml:mi>t</mml:mi><mml:mo>=</mml:mo><mml:mi>s</mml:mi><mml:mi>t</mml:mi><mml:mi>r</mml:mi><mml:mi>i</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi><mml:mo>=</mml:mo><mml:mi>e</mml:mi><mml:mi>n</mml:mi><mml:mi>d</mml:mi><mml:mi>i</mml:mi></mml:mrow></mml:msubsup><mml:mrow><mml:msub><mml:mi>&#x003B1;</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mtext>&#x000A0;</mml:mtext><mml:mi>d</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:mrow></mml:mstyle><mml:mtext>&#x000A0;</mml:mtext></mml:mrow></mml:mfrac></mml:mrow></mml:math></disp-formula>
<p>where <italic>IE</italic> is investment efficiency, <italic>t</italic> is time, <italic>stri</italic> is the starting time of the calculation, <italic>endi</italic> is the ending time of the calculation, <italic>J</italic><sub>M(<italic>i,t</italic>)unload</sub> is Si flow from the xylem to the cells of top leaf at time <italic>t</italic>, and &#x003B1;<sub><italic>t</italic></sub> is a factor that regulates transporter expression level at time <italic>t</italic>. This equation means that the investment efficiency is the amount of Si accumulated in top leaf divided by the total expression level of Si transporter genes.</p>
</sec>
<sec>
<title>Simulation under natural environment</title>
<p>Finally, we simulated Si dynamics under the natural environmental condition. In the above simulation setting, the artificial pattern of transpiration rate and photosynthesis rate were used (Figure <xref ref-type="fig" rid="F2">2</xref>). To confirm the result that is found in the above simulation experiment, we simulated the Si dynamics with the input data that was measured in the field experiment. The data were observed at the paddy site using the eddy covariance method during the growing season in 2004. The observation site was located at Mase, Tsukuba City, Ibaraki prefecture, Japan. In this observation, not only LE (Latent heat flux) and NEE (Net Ecosystem CO<sub>2</sub> Exchange) but also LAI (Leaf Area Index) were measured. We used LE and NEE for the estimation of transpiration and photosynthesis rates, respectively, assuming that the effects of evaporation from the water surface and heterotrophic respiration from the soil on the observed fluxes were negligible in our analysis. We used the data during day 33 and 35 after transplanting.</p>
</sec>
</sec>
<sec sec-type="results" id="s3">
<title>Results</title>
<sec>
<title>Si dynamics and expression of Si transporter genes under accumulation control</title>
<p>Using Equation (19), we simulated the model with several parameter sets (0.05, 0.1, and 0.2 for <italic>dec</italic> and 0.005, 0.01, and 0.02 for <italic>slp</italic><sub>c</sub>). During the day, Si concentration in the xylem of the top leaf rapidly increased and then decreased (Figure <xref ref-type="fig" rid="F3">3A</xref>) according to changes in leaf transpiration rate (Figure <xref ref-type="fig" rid="F2">2</xref>). At night, Si concentration reached zero, and then it increased again according to the increase in transpiration rate. Although Si concentration did not reach zero in the lower leaf (Supplementary Figure <xref ref-type="supplementary-material" rid="SM2">4</xref>), a similar pattern was observed. Though the pattern was similar at all parameter settings, Si concentrations during the day were low in the models with low <italic>dec</italic> values (slow decay of signaling substance) and high <italic>slp</italic><sub>c</sub> values (rapid generation of the signaling substance). Si concentration in leaf cells gradually increased, and the differences among parameter sets became apparent after 24 h (Figure <xref ref-type="fig" rid="F3">3B</xref>). Si concentration in leaf cells was the lowest at <italic>dec</italic> &#x0003D; 0.05, <italic>slp</italic><sub>c</sub> &#x0003D; 0.02, and was only about half of that at <italic>dec</italic> &#x0003D; 0.2, <italic>slp</italic><sub>c</sub> &#x0003D; 0.005. The pattern was the same in the lowest leaf (Supplementary Figure <xref ref-type="supplementary-material" rid="SM2">5</xref>). The signal level in phloem sap of the top leaf (Figure <xref ref-type="fig" rid="F3">3C</xref>) and roots (Figure <xref ref-type="fig" rid="F4">4</xref>) gradually increased with time and reached local maxima at dawn for the top leaf and at dusk for the roots. The signal level was the lowest at <italic>dec</italic> &#x0003D; 0.2, <italic>slp</italic><sub>c</sub> &#x0003D; 0.005, and was about one tenth of that at <italic>dec</italic> &#x0003D; 0.05, <italic>slp</italic><sub>c</sub> &#x0003D; 0.02) for the roots. The expression level of the transporter genes in roots gradually decreased with time (Figure <xref ref-type="fig" rid="F5">5</xref>). Two parameter sets (<italic>dec</italic> &#x0003D; 0.05, <italic>slp</italic><sub>c</sub> &#x0003D; 0.01; <italic>dec</italic> &#x0003D; 0.1, <italic>slp</italic><sub>c</sub> &#x0003D; 0.02) fit best the observed expression levels (mean mRNA levels) of Lsi1 measured using real-time RT-PCR by Yamaji and Ma (<xref ref-type="bibr" rid="B27">2011</xref>). Local maxima were reached during the day with all parameter sets.</p>
<fig id="F3" position="float">
<label>Figure 3</label>
<caption><p>Si concentration in xylem sap <bold>(A)</bold> and leaf cells <bold>(B)</bold> of the top leaf and the signal level in xylem sap <bold>(C)</bold> of the top leaf simulated with multiple parameter sets under the accumulation control assumption. Parameter <italic>dec</italic> is the decay rate of the signaling substance. Parameter <italic>slp</italic> is the generation rate of the signaling substance and corresponds to <italic>slp</italic><sub>c</sub> in Supplementary Table <xref ref-type="supplementary-material" rid="SM1">2</xref>.</p></caption>
<graphic xlink:href="fpls-08-01187-g0003.tif"/>
</fig>
<fig id="F4" position="float">
<label>Figure 4</label>
<caption><p>Signal level in xylem sap of the root simulated with multiple parameter sets. Parameter <italic>dec</italic> is the decay rate of the signaling substance. Parameter <italic>slp</italic> is the generation rate of the signaling substance and corresponds to <italic>slp</italic><sub>c</sub> in Supplementary Table <xref ref-type="supplementary-material" rid="SM1">2</xref>.</p></caption>
<graphic xlink:href="fpls-08-01187-g0004.tif"/>
</fig>
<fig id="F5" position="float">
<label>Figure 5</label>
<caption><p>Time series of the expression levels of Si transporter genes simulated with multiple parameter sets under the accumulation control assumption. Parameter <italic>dec</italic> is the decay rate of the signaling substance. Parameter <italic>slp</italic> is the generation rate of the signaling substance and corresponds to <italic>slp</italic><sub>c</sub> in Supplementary Table <xref ref-type="supplementary-material" rid="SM1">2</xref>. Blue circles indicate the observed values of the mean expression level of <italic>Lsi</italic>1 (Yamaji and Ma, <xref ref-type="bibr" rid="B27">2011</xref>).</p></caption>
<graphic xlink:href="fpls-08-01187-g0005.tif"/>
</fig>
</sec>
<sec>
<title>Expression of Si transporter genes under shortage control</title>
<p>Using Equation (20) and the same parameter sets, we simulated the expression level of the transporter genes in roots (Figure <xref ref-type="fig" rid="F6">6</xref>). As with accumulation control, the expression level gradually decreased with time, but local maxima were reached at dusk and local minima were reached at dawn with all parameter sets.</p>
<fig id="F6" position="float">
<label>Figure 6</label>
<caption><p>Time series of the expression levels of Si transporter genes simulated with multiple parameter sets under the shortage control assumption. Parameter <italic>dec</italic> is the decay rate of the signaling substance. Parameter <italic>slp</italic> is the generation rate of the signaling substance and corresponds to <italic>slp</italic><sub>r</sub> in Supplementary Table <xref ref-type="supplementary-material" rid="SM1">2</xref>. Blue circles indicate the observed values of the mean expression level of <italic>Lsi</italic>1 (Yamaji and Ma, <xref ref-type="bibr" rid="B27">2011</xref>).</p></caption>
<graphic xlink:href="fpls-08-01187-g0006.tif"/>
</fig>
</sec>
<sec>
<title>Si dynamics under water stress control</title>
<p>Using Equation (21) and the same parameter sets, we simulated the dynamics of Si concentration in the xylem (Supplementary Figure <xref ref-type="supplementary-material" rid="SM2">6A</xref>) and in top-leaf cells (Supplementary Figure <xref ref-type="supplementary-material" rid="SM2">6B</xref>). The patterns were similar to those under accumulation control. However, the pattern of the signal level in xylem sap differed: the local maxima were reached at dusk, but the signal level did not increase with time (Supplementary Figure <xref ref-type="supplementary-material" rid="SM2">6C</xref>). A diurnal expression pattern in roots was found with some parameter sets (Figure <xref ref-type="fig" rid="F7">7</xref>); local maxima were reached during the day and local minima at night. This pattern is similar to that observed by Yamaji and Ma (<xref ref-type="bibr" rid="B26">2007</xref>) for the <italic>Lsi1</italic> expression level in the root.</p>
<fig id="F7" position="float">
<label>Figure 7</label>
<caption><p>Time series of the expression level of Si transporter genes simulated with multiple parameter sets under the water stress control assumption. Parameter <italic>dec</italic> is the decay rate of the signaling substance. Parameter <italic>slp</italic> is the generation rate of the signaling substance and corresponds to <italic>slp</italic><sub>J</sub> in Supplementary Table <xref ref-type="supplementary-material" rid="SM1">2</xref>.</p></caption>
<graphic xlink:href="fpls-08-01187-g0007.tif"/>
</fig>
</sec>
<sec>
<title>Investment efficiency</title>
<p>We investigated the reason why the expression level of the transporter genes shows diurnal variation in the point of view of investment efficiency. We used <italic>dec</italic> &#x0003D; 0.2 with <italic>slp</italic><sub>J</sub> &#x0003D; 0.05 (low sensitivity of Si transporter expression to water stress), 0.1 (intermediate), or 0.2 (high) under the water stress control assumption (see Figure <xref ref-type="fig" rid="F7">7</xref>). Under &#x0201C;constant&#x0201D; setting (which means that the expression level of the transporter does not change in response to water stress), the investment during the night was 71.4% of that during the day. The nighttime investment decreased with increasing sensitivity (Figure <xref ref-type="fig" rid="F8">8A</xref>). As the results, the investment efficiency increased with increasing sensitivity: it was 5.8% at low sensitivity, 13.0% at intermediate sensitivity, and 34.9% at high sensitivity (Figure <xref ref-type="fig" rid="F8">8B</xref>).</p>
<fig id="F8" position="float">
<label>Figure 8</label>
<caption><p>Ratio of the investment during the night to that during the day for each parameter set <bold>(A)</bold> and the change rate of the investment efficiency relative to that under the constant expression of the transporter genes <bold>(B)</bold>. The parameter sets were constant (no sensitivity of Si transporter expression to water stress; <italic>dec</italic> &#x0003D; 0.0, <italic>slp</italic><sub>J</sub> &#x0003D; 0.0), low sensitivity (<italic>dec</italic> &#x0003D; 0.2, <italic>slp</italic><sub>J</sub> &#x0003D; 0.05), intermediate sensitivity (<italic>dec</italic> &#x0003D; 0.2, <italic>slp</italic><sub>J</sub> &#x0003D; 0.1), and high sensitivity (<italic>dec</italic> &#x0003D; 0.2, <italic>slp</italic><sub>J</sub> &#x0003D; 0.2) under the water stress control assumption (see Figure <xref ref-type="fig" rid="F7">7</xref>).</p></caption>
<graphic xlink:href="fpls-08-01187-g0008.tif"/>
</fig>
</sec>
<sec>
<title>Simulation under natural environment</title>
<p>Patterns of photosynthesis and transpiration rates were similar between the artificial input data and empirical data (compare Figures <xref ref-type="fig" rid="F2">2</xref>, <xref ref-type="fig" rid="F9">9A</xref>). As the results, the simulated patterns of the expression levels of the transporter genes were similar between them (compare Figures <xref ref-type="fig" rid="F7">7</xref>, <xref ref-type="fig" rid="F9">9B</xref>), with local maxima during the day and local minima during the night. The investment efficiency increased by 4.2% at low sensitivity, 10.3% at intermediate sensitivity, and 27.4% at high sensitivity in comparison with that at &#x0201C;constant&#x0201D; setting.</p>
<fig id="F9" position="float">
<label>Figure 9</label>
<caption><p>Time-series of measured transpiration and photosynthesis rates <bold>(A)</bold> and of the transporter expression level at low, intermediate, and high sensitivity simulated under the water stress control assumption <bold>(B)</bold>.</p></caption>
<graphic xlink:href="fpls-08-01187-g0009.tif"/>
</fig>
</sec>
</sec>
<sec sec-type="discussion" id="s4">
<title>Discussion</title>
<p>In this study, we proposed a new mathematical model that simulate the Si dynamics in whole plant in rice and investigated the possible mechanisms underlying diurnal variation of the expression level of the transporter genes. To simulate the dynamics of mineral nutrients in rice, we have to simulate not only water flows in the xylem and phloem but also the transport and distribution of mineral nutrients via transporters. Models have been developed that simulate water flows in the xylem and phloem (Daudet et al., <xref ref-type="bibr" rid="B2">2002</xref>; Lacointe and Minchin, <xref ref-type="bibr" rid="B11">2008</xref>; Lobet et al., <xref ref-type="bibr" rid="B13">2014</xref>; Seki et al., <xref ref-type="bibr" rid="B23">2015</xref>) and transport of mineral nutrients from roots or mineral distribution at nodes (Sakurai et al., <xref ref-type="bibr" rid="B20">2015</xref>; Yamaji et al., <xref ref-type="bibr" rid="B29">2015</xref>). However, no study has been conducted on modeling the dynamics of mineral nutrients by considering both water flow and transporter expression level.</p>
<p>The conceptual characteristics of the model proposed here are as follows: (1) it can simulate the dynamics of a mineral nutrient in a whole rice plant while considering plant morphology (multiple leaves, nodes, and stems); (2) the model can simulate mineral transport from roots and its distribution at nodes; and (3) the model can simulate the control of the expression level of the transporter genes in roots. This concept can also be applied to other mineral nutrients and crops if the experimental data on the absorption and distribution of the target mineral nutrients can be obtained.</p>
<p>In the present study, we assumed that three mechanisms control transporter expression levels. The first mechanism is accumulation control, in which a signaling substance is generated in response to Si concentration in leaf cells and is then transported to roots through phloem sap flow. The model based on this mechanism reproduces the experimental data to some extent: the <italic>Lsi1</italic> expression level gradually decreases after root exposure to Si solution of sufficient concentration (Figure <xref ref-type="fig" rid="F5">5</xref>). The best parameter sets that agree with the empirical data were <italic>dec</italic> &#x0003D; 0.05, <italic>slp</italic><sub>c</sub> &#x0003D; 0.01 and <italic>dec</italic> &#x0003D; 0.1, <italic>slp</italic><sub>c</sub> &#x0003D; 0.02 (Figure <xref ref-type="fig" rid="F5">5</xref>). For all parameter sets, the estimated Si concentration in xylem sap was nearly zero during the night because a low transpiration rate at night decreases the differences between water potentials of hydraulic nodes. Interestingly, the concentration of the signaling substance in the leaf xylem showed diurnal variation (Figure <xref ref-type="fig" rid="F3">3C</xref>) despite the steady increase in the generation rate of the signaling substance in response to the Si concentration in leaf cells (Figure <xref ref-type="fig" rid="F3">3B</xref>). This phenomenon may be related to the dynamics of phloem sap. At dawn, the difference in the potential between hydraulic nodes in phloem became small (Supplementary Figure <xref ref-type="supplementary-material" rid="SM2">7</xref>) because of the depletion of starch in leaves by this time. Therefore, the flow of phloem sap from top to bottom decreased and the signaling substance remained in the leaves. In the root, the concentration of the signaling substance decreased at dawn (Figure <xref ref-type="fig" rid="F4">4</xref>). The diurnal variation in the transport rate of the signaling substance generated the diurnal variation in the expression level of the transporter genes (Figure <xref ref-type="fig" rid="F5">5</xref>).</p>
<p>Under the assumption of shortage control, the expression level of the transporter genes gradually decreased, as under the assumption of accumulation control, but local minima were reached at dawn (Figure <xref ref-type="fig" rid="F6">6</xref>). The downward convex curve of the expression level under shortage control may be attributable to the mechanisms that determine how fast the expression is suppressed. Under accumulation control, the decrease in the suppression rate depends mainly on the rate of generation of the signaling substance in leaves, whereas under shortage control, it depends mainly on the rate of decay of the signaling substance. The convex curve of the expression level under shortage control appears to fit the data reported by Yamaji and Ma (<xref ref-type="bibr" rid="B27">2011</xref>). Therefore, shortage control may be a more likely mechanism for the control of Si dynamics than accumulation control from the aspect of the shape of the curve (but see below).</p>
<p>Simulation under the assumption of water stress control shows diurnal variation of the expression level of the transporter genes (Figure <xref ref-type="fig" rid="F7">7</xref>). Local minima were reached around midnight. All parameter sets produced similar expression cycles, but the amplitudes differed depending on <italic>slp</italic> parameter values. The parameter set of <italic>dec</italic> &#x0003D; 0.2, <italic>slp</italic> &#x0003D; 0.2 fit well the experimental data of Yamaji and Ma (<xref ref-type="bibr" rid="B26">2007</xref>), which show a decrease in the <italic>Lsi1</italic> expression level at midnight to one-third of that at daytime.</p>
<p>Why does rice have a control system that generates the diurnal pattern of the expression level of the transporter genes? To answer this question, we compared the investment efficiency at different parameter values. A decrease in the transporter expression level during the night decreased the relative investment into the expression of the transporter genes (Figure <xref ref-type="fig" rid="F8">8A</xref>). As a result, the investment efficiency was highest in the simulation that had the largest amplitude of the diurnal variation of expression (Figure <xref ref-type="fig" rid="F8">8B</xref>) because of the difference in the transpiration rates between day and night. During the day, the transpiration rate is high, xylem sap flow is large, and Si absorbed in the root is efficiently transported to the upper tissues. During the night, the transpiration rate is low, xylem sap flow is small, and Si is not efficiently transported. In other words, when a conveyor belt is moving rapidly, many pieces of baggage can be loaded, but loading many pieces of baggage on a slow conveyor belt is not a good strategy. Interestingly, the increasing rate of the Si concentrations in the tissue cells of the roots during the night were higher than during the day (Supplementary Figure <xref ref-type="supplementary-material" rid="SM2">8</xref>). It is because &#x0201C;many pieces of baggage&#x0201D; fell from the slow conveyor. As the results, the average Si concentration of all hydraulic nodes constantly increased even during the night to some extent (Supplementary Figure <xref ref-type="supplementary-material" rid="SM2">9</xref>). This result is consistent with the previous experimental studies in which the rate of Si uptake did not slow down during the night (Ma and Takahashi, <xref ref-type="bibr" rid="B14">2002</xref>).</p>
<p>We also investigated the investment efficiencies of accumulation control and shortage control. Under accumulation control, the investment efficiencies do not change greatly among parameter sets (Supplementary Figure <xref ref-type="supplementary-material" rid="SM2">10A</xref>). Under shortage control, on the other hand, they were greatly decreased at all settings (Supplementary Figure <xref ref-type="supplementary-material" rid="SM2">10B</xref>), perhaps because the level of expression of the transporters decreased during daytime rather than nighttime. Therefore, accumulation control may be preferable for rice from the aspect of investment efficiency. Although, it was reported that dehydration stress decreases the expression of Lsi1 and Lsi2 via ABA in root (Yamaji and Ma, <xref ref-type="bibr" rid="B26">2007</xref>), the mechanism that gradually decreases the expression of transporter genes is not well-understood. Evaluating whether accumulation control or shortage control is the actual mechanism in rice is a task for future study.</p>
<p>The transpiration rate during the night used for the present simulation setting (10% of the daytime transpiration rate) may be large from the actual night-time transpiration rate. However, if the actual transpiration rate during the night is lower than 10% (e.g., Nakano et al., <xref ref-type="bibr" rid="B19">2010</xref>), the conclusion discussed above would not change. It is because lower transpiration rate during the night should slow the xylem sap flow.</p>
<p>To confirm the result, we simulated the model with field data and found a similar diurnal pattern of transporter expression (Figure <xref ref-type="fig" rid="F9">9</xref>). The investment efficiency was highest when the model was simulated with the most sensitive (large-amplitude) parameters (<italic>dec</italic> &#x0003D; 0.2, <italic>slp</italic> &#x0003D; 0.2).</p>
<p>A previous study suggested that the localization and polarity of transporters observed in rice roots provide highest investment efficiency among all possible patterns evaluated (Sakurai et al., <xref ref-type="bibr" rid="B20">2015</xref>). The present study suggests that rice maximizes the investment efficiency in terms of not only the spatial pattern but also the temporal pattern. A gradual decrease in the expression level of Si transporter genes in response to Si concentration in leaf cells might be the mechanism that increases investment efficiency. In rice, many positive effects of Si have been reported with no detectable negative effects of excess Si intake (Ma and Takahashi, <xref ref-type="bibr" rid="B14">2002</xref>). However, the control of the transporter expression level in response to Si concentration in shoot should improve the efficiency of resource allocation.</p>
<p>In the current model, the processes of Si transport in roots and distribution in nodes are simplified. Including more detailed processes will be needed if the aim is to focus on the dynamics of Si at finer scales, such as the dynamics inside and outside of the cell membrane or the localization and polarity of transporters. However, as the current model was designed to describe the dynamics of Si at the whole-plant scale, its degree of simplicity is appropriate. Moreover, the photosynthate dynamics modeled in this study would be a general pattern of plants and does not include characteristic partitioning processes of carbohydrates found in grasses. Grasses store carbohydrates in mainly stem tissue when carbohydrates from the source is greater than whole plant demand (Slewinski, <xref ref-type="bibr" rid="B24">2012</xref>). However, the non-structural carbohydrates in the stem is mainly expended during reproductive growth period (Slewinski, <xref ref-type="bibr" rid="B24">2012</xref>) and leaves would be the main source of carbohydrates during daytime and nighttime in rice (Eom et al., <xref ref-type="bibr" rid="B3">2012</xref>). Therefore, it could be assumed that the downward transport of sucrose is predominant during nighttime at least in the early vegetative period. This was the case of our simulation in the present study. If the model is applied for the Si dynamics during the reproductive period, it might have to be modified so as to include the effect of the storage.</p>
<p>In the current study, the model structure and values of resistance may be oversimplified. The purpose of this study was to propose a new model to investigate qualitatively why rice controls the expression of Si transporter genes. For quantitative understanding of mineral transport, more realistic structure and resistance of water flow values should be reflected in the model, which would be require a large amount of additional experimental data.</p>
</sec>
<sec sec-type="conclusions" id="s5">
<title>Conclusion</title>
<p>We developed a new model that simulates the dynamics of Si in a whole rice plant by considering Si transport in the roots, its distribution at the nodes, and the control of the expression level of Si transporter genes by a signaling substances. The model reproduced a gradual decrease and diurnal variation of the expression level of the transporter genes observed by Yamaji and Ma (<xref ref-type="bibr" rid="B26">2007</xref>, <xref ref-type="bibr" rid="B27">2011</xref>). Our modeling suggests that a considerable reduction in the expression level of Si transporter genes during the night increases investment efficiency (the amount of Si accumulated in top leaf divided by the total expression level of Si transporter genes). Our study suggests that rice has a system that maximizes the investment efficiency for Si uptake in terms of not only the spatial pattern (Sakurai et al., <xref ref-type="bibr" rid="B20">2015</xref>) but also the temporal pattern.</p>
</sec>
<sec id="s6">
<title>Author contributions</title>
<p>GS, NY, NM, MY, and JFM designed the study. GS performed the simulations. KO measured field data. All authors contributed to drafting the paper.</p>
<sec>
<title>Conflict of interest statement</title>
<p>The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.</p></sec>
</sec>
</body>
<back>
<sec sec-type="supplementary-material" id="s7">
<title>Supplementary material</title>
<p>The Supplementary Material for this article can be found online at: <ext-link ext-link-type="uri" xlink:href="http://journal.frontiersin.org/article/10.3389/fpls.2017.01187/full#supplementary-material">http://journal.frontiersin.org/article/10.3389/fpls.2017.01187/full#supplementary-material</ext-link></p>
<supplementary-material xlink:href="Table1.pdf" id="SM1" mimetype="application/pdf" xmlns:xlink="http://www.w3.org/1999/xlink"/>
<supplementary-material xlink:href="Image1.PDF" id="SM2" mimetype="application/pdf" xmlns:xlink="http://www.w3.org/1999/xlink"/>
</sec>
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<fn fn-type="financial-disclosure"><p><bold>Funding.</bold> This project is supported by Grant-in-Aid for Specially Promoted Research to JFM (16H06296).</p>
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