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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Clim.</journal-id>
<journal-title>Frontiers in Climate</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Clim.</abbrev-journal-title>
<issn pub-type="epub">2624-9553</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="doi">10.3389/fclim.2025.1505472</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Climate</subject>
<subj-group>
<subject>Original Research</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Reactive transport simulation of organic and inorganic carbon cycling following carbon dioxide sorption onto soil amendments in drylands</article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author" corresp="yes">
<name><surname>Helmrich</surname> <given-names>Stefanie</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<xref ref-type="corresp" rid="c001"><sup>&#x002A;</sup></xref>
<xref ref-type="author-notes" rid="fn00001"><sup>&#x2020;</sup></xref>
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</contrib>
<contrib contrib-type="author">
<name><surname>Ringsby</surname> <given-names>Alexandra J.</given-names></name>
<xref ref-type="aff" rid="aff2"><sup>2</sup></xref>
<xref ref-type="author-notes" rid="fn00002"><sup>&#x2020;</sup></xref>
<uri xlink:href="https://loop.frontiersin.org/people/2912024/overview"/>
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</contrib>
<contrib contrib-type="author">
<name><surname>Maher</surname> <given-names>Kate</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<xref ref-type="author-notes" rid="fn00003"><sup>&#x2020;</sup></xref>
<uri xlink:href="https://loop.frontiersin.org/people/1044005/overview"/>
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<role content-type="https://credit.niso.org/contributor-roles/funding-acquisition/"/>
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<aff id="aff1"><sup>1</sup><institution>Department of Earth System Science, Stanford University</institution>, <addr-line>Stanford, CA</addr-line>, <country>United States</country></aff>
<aff id="aff2"><sup>2</sup><institution>Department of Chemical Engineering, Stanford University</institution>, <addr-line>Stanford, CA</addr-line>, <country>United States</country></aff>
<author-notes>
<fn fn-type="edited-by" id="fn0004">
<p>Edited by: Valentina Prigiobbe, University of Padua, Italy</p>
</fn>
<fn fn-type="edited-by" id="fn0005">
<p>Reviewed by: Zhang Zhihao, Xinjiang Institute of Ecology and Geography (CAS), China</p>
<p>Jiefei Mao, Xinjiang Institute of Ecology and Geography, China</p>
<p>James Amonette, Pacific Northwest National Laboratory (DOE), United States</p>
</fn>
<corresp id="c001">&#x002A;Correspondence: Stefanie Helmrich, <email>stefanie.helmrich@gmail.com</email></corresp>
<fn fn-type="other" id="fn00001"><p><sup>&#x2020;</sup>ORCID: Stefanie Helmrich, <ext-link ext-link-type="uri" xlink:href="https://orcid.org/0000-0002-7653-6720">orcid.org/0000-0002-7653-6720</ext-link></p></fn>
<fn fn-type="other" id="fn00002"><p>Alexandra J Ringsby, <ext-link ext-link-type="uri" xlink:href="https://orcid.org/0000-0002-6317-1902">orcid.org/0000-0002-6317-1902</ext-link></p></fn>
<fn fn-type="other" id="fn00003"><p>Kate Maher, <ext-link ext-link-type="uri" xlink:href="https://orcid.org/0000-0002-5982-6064">orcid.org/0000-0002-5982-6064</ext-link></p></fn>
</author-notes>
<pub-date pub-type="epub">
<day>07</day>
<month>03</month>
<year>2025</year>
</pub-date>
<pub-date pub-type="collection">
<year>2025</year>
</pub-date>
<volume>7</volume>
<elocation-id>1505472</elocation-id>
<history>
<date date-type="received">
<day>02</day>
<month>10</month>
<year>2024</year>
</date>
<date date-type="accepted">
<day>24</day>
<month>02</month>
<year>2025</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#x00A9; 2025 Helmrich, Ringsby and Maher.</copyright-statement>
<copyright-year>2025</copyright-year>
<copyright-holder>Helmrich, Ringsby and Maher</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) and the copyright owner(s) 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>Terrestrial nature-based climate solutions (NbCS) for carbon dioxide removal (CDR) are critical for mitigating climate change. However, the arid climates characteristic of drylands (aridity index &#x003C;0.65) often limit the effectiveness of many NbCS. At the same time, drylands cover approximately 45% of the global land area and are threatened by soil degradation, necessitating the deployment of CDR methods for drylands that also promote soil health. Soil amendments with high CO<sub>2</sub> sorption capacity, such as biochar, could provide CDR potential and soil health benefits in drylands provided they do not negatively impact the large inorganic carbon pools typical of dryland soils. The dynamics of soil CO<sub>2</sub> are therefore critical for assessing the response of dryland systems to sorbing amendments. To assess the soil response to CO<sub>2</sub> sorption, we developed a 1D reactive transport model of unsaturated soils in equilibrium with dissolved inorganic carbon and calcite under varying soil respiration rates and soil amendment application conditions. The simulations highlight how alteration of soil CO<sub>2</sub> due to sorption by biochar affects dissolved inorganic carbon, pH, Ca<sup>2+</sup>, and calcite. The transient conditions that emerge, including delayed emissions of respired CO<sub>2</sub>, also emphasize the need to consider response times in monitoring campaigns based on CO<sub>2</sub> measurements. In scenarios where soil respiration is low, as is typical in drylands, sorption becomes increasingly important. Although the CDR potential of CO<sub>2</sub> sorption is variable and was modest relative to the overall CDR for a biochar deployment, the impacts of altered gas dynamics on soil inorganic carbon are important to consider as dryland soil amendments are developed.</p>
</abstract>
<kwd-group>
<kwd>carbon dioxide removal (CDR)</kwd>
<kwd>gas sorption</kwd>
<kwd>soil</kwd>
<kwd>biochar</kwd>
<kwd>soil inorganic carbon</kwd>
<kwd>reactive transport model</kwd>
<kwd>CrunchFlow</kwd>
</kwd-group>
<counts>
<fig-count count="9"/>
<table-count count="0"/>
<equation-count count="14"/>
<ref-count count="121"/>
<page-count count="14"/>
<word-count count="11468"/>
</counts>
<custom-meta-wrap>
<custom-meta>
<meta-name>section-at-acceptance</meta-name>
<meta-value>Carbon Dioxide Removal</meta-value>
</custom-meta>
</custom-meta-wrap>
</article-meta>
</front>
<body>
<sec sec-type="intro" id="sec1">
<label>1</label>
<title>Introduction</title>
<p>Nature-based climate solutions (NbCS) are considered essential to limit global warming as they represent one of the most mature carbon dioxide removal (CDR) methods, complementing the need for reductions in fossil fuel emissions (<xref ref-type="bibr" rid="ref41">Griscom et al., 2017</xref>). NbCS rely on sustainable management of ecosystems to remove greenhouse gasses from the atmosphere while ideally addressing societal challenges associated with climate change (<xref ref-type="bibr" rid="ref12">Chausson et al., 2020</xref>; <xref ref-type="bibr" rid="ref96">Seddon et al., 2020</xref>). Early estimates suggest that sustainable management of forests, agricultural lands, grasslands, and wetlands could deliver over one third of the cost-effective climate mitigation needed to limit global warming to below 2&#x00B0;C above pre-industrial levels until 2030 (<xref ref-type="bibr" rid="ref41">Griscom et al., 2017</xref>).</p>
<p>Drylands (aridity index &#x003C;0.65) (<xref ref-type="bibr" rid="ref13">Cherlet et al., 2018</xref>) should be important targets for NbCS because they occupy over 45% of the global land area (<xref ref-type="bibr" rid="ref26">Dregne et al., 1991</xref>; <xref ref-type="bibr" rid="ref82">Pr&#x0103;v&#x0103;lie, 2016</xref>; <xref ref-type="bibr" rid="ref7">Berg and McColl, 2021</xref>) and play an important role in controlling atmospheric CO<sub>2</sub>. Soil inorganic carbon (SIC) accumulates in drylands. The SIC is present as pedogenic carbonate and forms at depth from Ca<sup>2+</sup> derived from a mixture of dust inputs and <italic>in situ</italic> weathering and CO<sub>2</sub> in percolating water (<xref ref-type="bibr" rid="ref11">Chadwick et al., 1999</xref>). If Ca<sup>2+</sup> is supplied by weathering of calcium silicates, this process constitutes a carbon sink (<xref ref-type="bibr" rid="ref73">Monger et al., 2015</xref>; <xref ref-type="bibr" rid="ref59">Lal et al., 2021</xref>). The SIC stock in the upper 1&#x202F;m of soil is estimated to be around 940 Pg C, which mostly occurs in drylands and is larger than the C pool in the biosphere (<xref ref-type="bibr" rid="ref58">Lal, 2020</xref>; <xref ref-type="bibr" rid="ref59">Lal et al., 2021</xref>). This SIC has turnover rates of several thousand years (<xref ref-type="bibr" rid="ref72">Monger and Gallegos, 2000</xref>). However, climate change could increase carbon sequestration via SIC or lead to SIC being a source of carbon (<xref ref-type="bibr" rid="ref55">Lal et al., 2000</xref>; <xref ref-type="bibr" rid="ref75">Naorem et al., 2022</xref>). Drylands are specifically vulnerable to changes in environmental conditions (<xref ref-type="bibr" rid="ref59">Lal et al., 2021</xref>) and it has been estimated that over 57&#x2013;70% of dryland soil is degraded or prone to degradation (<xref ref-type="bibr" rid="ref26">Dregne et al., 1991</xref>; <xref ref-type="bibr" rid="ref56">Lal, 2004</xref>; <xref ref-type="bibr" rid="ref86">Reynolds et al., 2007</xref>). Another study estimated that grazing, especially in arid and semi-arid regions might account for half of global SOC loss over the last 12,000 years (<xref ref-type="bibr" rid="ref94">Sanderman et al., 2017</xref>), which would also affect SIC storage. However, soil degradation is still difficult to quantify (<xref ref-type="bibr" rid="ref108">Verstraete et al., 2011</xref>; <xref ref-type="bibr" rid="ref84">Prince, 2016</xref>; <xref ref-type="bibr" rid="ref110">Wang et al., 2022</xref>).</p>
<p>Many NbCS have limited applicability in drylands due to water requirements. NbCS that are currently considered as highly promising for CDR are enhanced weathering (EW), reforestation, and biochar. EW requires leaching of alkalinity, which is inefficient in drylands (<xref ref-type="bibr" rid="ref9">Calabrese et al., 2022</xref>; <xref ref-type="bibr" rid="ref120">Zhang S. et al., 2022</xref>; <xref ref-type="bibr" rid="ref63">Lehmann et al., 2023</xref>). Similarly, net primary productivity is limited by water availability (<xref ref-type="bibr" rid="ref30">Ferguson and Veizer, 2007</xref>) therefore placing limits on restoration of organic carbon (C) stocks and discouraging biochar application that seeks to enhance primary productivity. Estimates of CDR for the aforementioned NbCS often consider only agricultural and forest lands (<xref ref-type="bibr" rid="ref89">Roe et al., 2021</xref>). However, agricultural and forest lands only constitute roughly 9 and 23% of the global land area, respectively, and thus the development of effective drylands CDR strategies presents an important avenue for increasing global CDR capacity.</p>
<p>Another challenge for CDR in drylands is that drylands are understudied (<xref ref-type="bibr" rid="ref108">Verstraete et al., 2011</xref>) and predictions from other climatic conditions might not be applicable. Eddy-covariance measurement, which works well to determine C uptake in forests, has been insufficient to identify drylands as source or sink of atmospheric CO<sub>2</sub> (<xref ref-type="bibr" rid="ref95">Schlesinger, 2017</xref>). This has been attributed partly to pressure pumping and carbonate dissolution in combination with transport to groundwater, although these abiotic processes are thought to be insufficient to explain discrepancies between analytical methods (<xref ref-type="bibr" rid="ref95">Schlesinger, 2017</xref>). Diurnal soil CO<sub>2</sub> flux behavior can be explained by diurnal changes in moisture and temperature that drive gas dissolution in soil water, however these changes do not constrain long-term changes in carbon cycling (<xref ref-type="bibr" rid="ref91">Sagi et al., 2021</xref>). Overall monitoring only soil CO<sub>2</sub> efflux does not give a complete picture of C cycling in dryland soils.</p>
<p>For water-scarce drylands, soil amendments with high CO<sub>2</sub> sorption capacity could provide CDR potential and soil health benefits. Carbon-based materials such as biochar, as well as inorganic materials such as zeolite, are suitable because of their low cost, abundance, benign nature and recalcitrance (<xref ref-type="bibr" rid="ref42">Halliday and Hatton, 2021</xref>; <xref ref-type="bibr" rid="ref37">Garbowski et al., 2023</xref>). Biochar is highly porous with variability in pore volume, pore structure, specific surface area and functional groups related to feedstock type and production conditions (<xref ref-type="bibr" rid="ref32">Francis et al., 2023</xref>). It also constitutes an important CDR strategy (<xref ref-type="bibr" rid="ref62">Lehmann et al., 2021</xref>). Minerals such as zeolites are porous materials with high sorption capacity, and they are tunable and can be functionalized (<xref ref-type="bibr" rid="ref42">Halliday and Hatton, 2021</xref>). Both materials improve soil health under a range of conditions (<xref ref-type="bibr" rid="ref71">Mondal et al., 2021</xref>; <xref ref-type="bibr" rid="ref76">Nepal et al., 2023</xref>).</p>
<p>Predicting the soil response to biochar is highly uncertain but abiotic processes involving SIC could significantly contribute to the variability of soil CO<sub>2</sub> fluxes after biochar amendment (<xref ref-type="bibr" rid="ref67">Liu et al., 2016</xref>; <xref ref-type="bibr" rid="ref74">Mosa et al., 2023</xref>). There are unfortunately relatively few field trials of biochar that completely constrain the carbon dynamics. A field study conducted in temperate and summer monsoon climate found a decrease in SIC, an increase in SOC, and depletion of water-soluble Ca<sup>2+</sup> and Mg<sup>2+</sup> in response to biochar additions (<xref ref-type="bibr" rid="ref68">Lu et al., 2021</xref>), with an accompanying study pointing toward leaching of cations (<xref ref-type="bibr" rid="ref121">Zhang et al., 2020</xref>). A biochar field study that was conducted over a range of climatic conditions found an increase in SIC with decreasing precipitation, while soil type and hydrological processes were also correlated to accumulation of SIC (<xref ref-type="bibr" rid="ref121">Zhang et al., 2020</xref>). Studies conducted under arid or semi-arid conditions generally found an increase in SIC and reasoned that there is precipitation of calcite at deeper depths (<xref ref-type="bibr" rid="ref111">Wang et al., 2015</xref>; <xref ref-type="bibr" rid="ref23">Dong et al., 2019</xref>). However, studies investigating how SIC reacts to biochar addition, especially in drylands, are still scarce.</p>
<p>In this paper we investigate CO<sub>2</sub> sorption on biochar applied as a soil amendment and explore how manipulation of soil CO<sub>2</sub> affects C cycling in dryland soils. We will briefly review sorption data and present a reactive transport model (RTM) to elucidate the coupling between geochemical reactions and gas transport. The RTM simulates gas diffusion, dissolved inorganic carbon (DIC) and weathering of calcite under different application conditions and soil respiration rates. Although the sorption of CO<sub>2</sub> is relatively low (around 2%) compared to the total C in the simulated biochar, the simulated interactions between organic and inorganic C cycling can inform application and monitoring of a range of CDR methods that affect soil C dynamics. We will discuss the limitations for application and the benefits for soil health.</p>
</sec>
<sec sec-type="methods" id="sec2">
<label>2</label>
<title>Methods</title>
<sec id="sec3">
<label>2.1</label>
<title>Sorption isotherm models</title>
<p>The model parameters for CO<sub>2</sub> sorption on soil amendments were based on sorption isotherms fitted to dry sorption data collected under soil-relevant gas conditions without the presence of soil (<xref ref-type="bibr" rid="ref88">Ringsby et al., 2024</xref>) (<xref ref-type="fig" rid="fig1">Figure 1</xref> and <xref ref-type="supplementary-material" rid="SM2">Supplementary Table S1</xref>). Dry sorption experiments with sorbent were chosen because the presence of water and soil hinders comparability between studies and makes generalization difficult. However, it should be noted that water (<xref ref-type="bibr" rid="ref19">Davidson et al., 2013</xref>) and soil (<xref ref-type="bibr" rid="ref54">Kwon and Pignatello, 2005</xref>) can reduce the specific sorption capacity.</p>
<fig position="float" id="fig1">
<label>Figure 1</label>
<caption>
<p>Langmuir CO<sub>2</sub> sorption isotherms from published data (<xref ref-type="bibr" rid="ref88">Ringsby et al., 2024</xref>). Isotherms were fitted to data from dry sorption experiments under soil relevant conditions. Langmuir constants can be found in SI.</p>
</caption>
<graphic xlink:href="fclim-07-1505472-g001.tif"/>
</fig>
<p>The sorbents were either not pre-treated before the sorption experiment (&#x201C;as received&#x201D;) or they were outgassed at 150&#x00B0;C before the sorption experiment (&#x201C;outgassed&#x201D;). This is an important distinction because pre-treatment has been identified as a major source of uncertainty (<xref ref-type="bibr" rid="ref31">Figini-Albisetti et al., 2010</xref>). No outgassing or an outgassing temperature that is too low will likely underestimate sorption capacity while elevated temperatures applied to temperature-sensitive materials might irreversibly alter the sorbent behavior (<xref ref-type="bibr" rid="ref31">Figini-Albisetti et al., 2010</xref>). However, the authors also noted that the outgassing temperature must be consistent with final application. During the large-scale application process of sorbents as soil amendment, elevated temperatures are not expected. Therefore, sorption isotherms &#x201C;as received,&#x201D; were assumed to be best in line with the intended application. The sorbent with the highest &#x201C;as received&#x201D; sorption capacity was Biochar 3 and was chosen for simulations, while the outgassed isotherm for Biochar 3 indicates the upper bounds likely for biochar sorbents (<xref ref-type="bibr" rid="ref88">Ringsby et al., 2024</xref>).</p>
<p>A sorption isotherm model that is often used to describe experimental observations such as those above is the Langmuir model (<xref ref-type="disp-formula" rid="EQ2">Equations 1</xref>&#x2013;<xref ref-type="disp-formula" rid="EQ3">3</xref>). The single site Langmuir model makes following assumptions: (1) there is a limited sorption capacity, (2) all sorption sites are equal, (3) one site sorbs one molecule of sorbent, and (4) all sites are energetically independent of the number of sorbed molecules (<xref ref-type="bibr" rid="ref66">Limousin et al., 2007</xref>). The assumed reaction is:<disp-formula id="EQ1">
<label>(1)</label>
<mml:math id="M1">
<mml:mfenced open="(" close=")">
<mml:mrow>
<mml:msub>
<mml:mi>q</mml:mi>
<mml:mi>m</mml:mi>
</mml:msub>
<mml:mo>&#x2212;</mml:mo>
<mml:mi>q</mml:mi>
</mml:mrow>
</mml:mfenced>
<mml:mo>+</mml:mo>
<mml:mi>p</mml:mi>
<mml:msub>
<mml:mrow>
<mml:mi mathvariant="normal">C</mml:mi>
<mml:mi mathvariant="normal">O</mml:mi>
</mml:mrow>
<mml:mn>2</mml:mn>
</mml:msub>
<mml:mo>&#x2194;</mml:mo>
<mml:mi>q</mml:mi>
</mml:math>
</disp-formula></p>
<p>Where <inline-formula>
<mml:math id="M2">
<mml:mi>q</mml:mi>
</mml:math>
</inline-formula> is the surface complex, <inline-formula>
<mml:math id="M3">
<mml:msub>
<mml:mi>q</mml:mi>
<mml:mi>m</mml:mi>
</mml:msub>
</mml:math>
</inline-formula> is the maximum sorption capacity, <inline-formula>
<mml:math id="M4">
<mml:msub>
<mml:mi>q</mml:mi>
<mml:mi>m</mml:mi>
</mml:msub>
<mml:mo>&#x2212;</mml:mo>
<mml:mi>q</mml:mi>
</mml:math>
</inline-formula> indicates free sites, and <italic>p</italic>CO<sub>2</sub> is partial pressure of CO<sub>2</sub>. The conditional stability constant can be written as:<disp-formula id="EQ2">
<label>(2)</label>
<mml:math id="M5">
<mml:mi>K</mml:mi>
<mml:mo>=</mml:mo>
<mml:mfrac>
<mml:mfenced open="[" close="]">
<mml:mi>q</mml:mi>
</mml:mfenced>
<mml:mrow>
<mml:mfenced open="[" close="]">
<mml:mrow>
<mml:msub>
<mml:mi>q</mml:mi>
<mml:mi>m</mml:mi>
</mml:msub>
<mml:mo>&#x2212;</mml:mo>
<mml:mi>q</mml:mi>
</mml:mrow>
</mml:mfenced>
<mml:mfenced open="[" close="]">
<mml:mrow>
<mml:mi>p</mml:mi>
<mml:mi>C</mml:mi>
<mml:msub>
<mml:mi>O</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mfrac>
</mml:math>
</disp-formula></p>
<p>Where <inline-formula>
<mml:math id="M6">
<mml:mi>K</mml:mi>
</mml:math>
</inline-formula> is the Langmuir constant. The equation can be rearranged to the typical Langmuir isotherm:<disp-formula id="EQ3">
<label>(3)</label>
<mml:math id="M7">
<mml:mi>q</mml:mi>
<mml:mo>=</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:msub>
<mml:mi>q</mml:mi>
<mml:mi>m</mml:mi>
</mml:msub>
<mml:mi>K</mml:mi>
<mml:mspace width="thickmathspace"/>
<mml:mi>p</mml:mi>
<mml:mi>C</mml:mi>
<mml:msub>
<mml:mi>O</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
</mml:mrow>
<mml:mrow>
<mml:mn>1</mml:mn>
<mml:mo>+</mml:mo>
<mml:mi>K</mml:mi>
<mml:mspace width="thickmathspace"/>
<mml:mi>p</mml:mi>
<mml:mi>C</mml:mi>
<mml:msub>
<mml:mi>O</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
</mml:mrow>
</mml:mfrac>
</mml:math>
</disp-formula></p>
<p>In many cases an improved description of experimental data can be achieved with a multisite Langmuir model (<xref ref-type="disp-formula" rid="EQ4">Equation 4</xref>):<disp-formula id="EQ4">
<label>(4)</label>
<mml:math id="M8">
<mml:mi>q</mml:mi>
<mml:mo>=</mml:mo>
<mml:munderover>
<mml:mstyle displaystyle="true">
<mml:mo stretchy="true">&#x2211;</mml:mo>
</mml:mstyle>
<mml:mrow>
<mml:mi>i</mml:mi>
<mml:mo>=</mml:mo>
<mml:mn>1</mml:mn>
</mml:mrow>
<mml:mi>p</mml:mi>
</mml:munderover>
<mml:mfrac>
<mml:mrow>
<mml:msub>
<mml:mi>q</mml:mi>
<mml:mrow>
<mml:mi>m</mml:mi>
<mml:mo>,</mml:mo>
<mml:mi>i</mml:mi>
</mml:mrow>
</mml:msub>
<mml:msub>
<mml:mi>K</mml:mi>
<mml:mi>i</mml:mi>
</mml:msub>
<mml:mi>p</mml:mi>
<mml:mi>C</mml:mi>
<mml:msub>
<mml:mi>O</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
</mml:mrow>
<mml:mrow>
<mml:mn>1</mml:mn>
<mml:mo>+</mml:mo>
<mml:msub>
<mml:mi>K</mml:mi>
<mml:mi>i</mml:mi>
</mml:msub>
<mml:mi>p</mml:mi>
<mml:mi>C</mml:mi>
<mml:msub>
<mml:mi>O</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
</mml:mrow>
</mml:mfrac>
</mml:math>
</disp-formula></p>
<p>Where <inline-formula>
<mml:math id="M9">
<mml:msub>
<mml:mi>K</mml:mi>
<mml:mi>i</mml:mi>
</mml:msub>
</mml:math>
</inline-formula> and <inline-formula>
<mml:math id="M10">
<mml:msub>
<mml:mi>q</mml:mi>
<mml:mrow>
<mml:mi>m</mml:mi>
<mml:mo>,</mml:mo>
<mml:mi>i</mml:mi>
</mml:mrow>
</mml:msub>
</mml:math>
</inline-formula> are Langmuir constant pairs <inline-formula>
<mml:math id="M11">
<mml:mi>p</mml:mi>
</mml:math>
</inline-formula> for multiple sorption sites.</p>
<p>For inclusion in the reactive transport model, a multisite competitive Langmuir sorption model was adapted (<xref ref-type="bibr" rid="ref66">Limousin et al., 2007</xref>). A reaction for a strong and a weak sorption site was implemented (<xref ref-type="disp-formula" rid="EQ5">Equations 5</xref>, <xref ref-type="disp-formula" rid="EQ6">6</xref>):<disp-formula id="EQ5">
<label>(5)</label>
<mml:math id="M12">
<mml:mo>&#x003E;</mml:mo>
<mml:msup>
<mml:msub>
<mml:mi mathvariant="normal">S</mml:mi>
<mml:mi mathvariant="normal">strong</mml:mi>
</mml:msub>
<mml:mn>0</mml:mn>
</mml:msup>
<mml:mo>+</mml:mo>
<mml:mspace width="0.5em"/>
<mml:msub>
<mml:mrow>
<mml:mi mathvariant="normal">C</mml:mi>
<mml:mi mathvariant="normal">O</mml:mi>
</mml:mrow>
<mml:mn>2</mml:mn>
</mml:msub>
<mml:mfenced open="(" close=")">
<mml:mi mathvariant="normal">g</mml:mi>
</mml:mfenced>
<mml:mo>&#x2194;</mml:mo>
<mml:mspace width="0.5em"/>
<mml:mo>&#x003E;</mml:mo>
<mml:msub>
<mml:mi mathvariant="normal">S</mml:mi>
<mml:mi mathvariant="normal">strong</mml:mi>
</mml:msub>
<mml:msubsup>
<mml:mrow>
<mml:mi mathvariant="normal">C</mml:mi>
<mml:mi mathvariant="normal">O</mml:mi>
</mml:mrow>
<mml:mn>2</mml:mn>
<mml:mn>0</mml:mn>
</mml:msubsup>
</mml:math>
</disp-formula><disp-formula id="EQ6">
<label>(6)</label>
<mml:math id="M13">
<mml:mo>&#x003E;</mml:mo>
<mml:msup>
<mml:msub>
<mml:mi mathvariant="normal">S</mml:mi>
<mml:mi mathvariant="normal">weak</mml:mi>
</mml:msub>
<mml:mn>0</mml:mn>
</mml:msup>
<mml:mo>+</mml:mo>
<mml:mspace width="0.5em"/>
<mml:msub>
<mml:mrow>
<mml:mi mathvariant="normal">C</mml:mi>
<mml:mi mathvariant="normal">O</mml:mi>
</mml:mrow>
<mml:mn>2</mml:mn>
</mml:msub>
<mml:mfenced open="(" close=")">
<mml:mi mathvariant="normal">g</mml:mi>
</mml:mfenced>
<mml:mspace width="0.5em"/>
<mml:mo>&#x2194;</mml:mo>
<mml:mspace width="0.5em"/>
<mml:mo>&#x003E;</mml:mo>
<mml:msub>
<mml:mi mathvariant="normal">S</mml:mi>
<mml:mi mathvariant="normal">weak</mml:mi>
</mml:msub>
<mml:msubsup>
<mml:mrow>
<mml:mi mathvariant="normal">C</mml:mi>
<mml:mi mathvariant="normal">O</mml:mi>
</mml:mrow>
<mml:mn>2</mml:mn>
<mml:mn>0</mml:mn>
</mml:msubsup>
</mml:math>
</disp-formula></p>
<p>Where &#x003E;S<sub>strong</sub><sup>0</sup> refers to a strong sorption site and&#x202F;&#x003E;&#x202F;S<sub>weak</sub><sup>0</sup> refers to a weak sorption site. The Langmuir constants <inline-formula>
<mml:math id="M14">
<mml:msub>
<mml:mi>K</mml:mi>
<mml:mn>1</mml:mn>
</mml:msub>
</mml:math>
</inline-formula> and <inline-formula>
<mml:math id="M15">
<mml:msub>
<mml:mi>K</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
</mml:math>
</inline-formula> were implemented as the equilibrium constants for the two reactions. The maximum adsorption capacities <inline-formula>
<mml:math id="M16">
<mml:msub>
<mml:mi>q</mml:mi>
<mml:mrow>
<mml:mi>m</mml:mi>
<mml:mo>,</mml:mo>
<mml:mn>1</mml:mn>
</mml:mrow>
</mml:msub>
</mml:math>
</inline-formula> and <inline-formula>
<mml:math id="M17">
<mml:msub>
<mml:mi>q</mml:mi>
<mml:mrow>
<mml:mi>m</mml:mi>
<mml:mo>,</mml:mo>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:math>
</inline-formula> can be directly entered in the RTM. Physical properties necessary to simulate the sorbent mass were from the same published study (<xref ref-type="supplementary-material" rid="SM2">Supplementary Table S2</xref>). The Biochar 3 sample was obtained from Atlas Olive Oils, which produces biochar from olive tree byproducts, including pulp, pits, and branches. The chemical properties that were provided by the supplier are listed in <xref ref-type="supplementary-material" rid="SM2">Supplementary Table S3</xref>.</p>
</sec>
<sec id="sec4">
<label>2.2</label>
<title>Reactive transport model</title>
<p>Simulations were conducted with the multi-component reactive transport code, CrunchFlow (<xref ref-type="bibr" rid="ref103">Steefel et al., 2015</xref>). CrunchFlow allows simulation of variably saturated conditions at steady state, including gas diffusion as well as sorption of gas species. Gas diffusion was simulated via Fick&#x2019;s law assuming a tortuosity correction via <xref ref-type="bibr" rid="ref70">Millington (1958)</xref>. A surface complexation model (SCM) capability in CrunchFlow simulates sorption. The SCM provides flexibility to simulate sorption mechanisms or empirical sorption reactions, e.g., via the Langmuir sorption model. Equilibrium between the gas and aqueous phase is governed by Henry&#x2019;s law, and gas concentrations are simulated via the ideal gas law.</p>
<sec id="sec5">
<label>2.2.1</label>
<title>Model domain and gas transport</title>
<p>To simulate gas transport and C cycling in dry soil, we implemented a 1D model with 200 vertical cells representing a 2-meter soil profile. We assumed that there was no water flow, and that gas was transported only via diffusion with a free phase gas diffusion coefficient of 0.16&#x202F;cm<sup>2</sup>/s<sup>1</sup> (<xref ref-type="bibr" rid="ref17">Currie, 1960</xref>; <xref ref-type="bibr" rid="ref90">Rolston and Moldrup, 2002</xref>). A Dirichlet boundary condition was specified at the top to ensure gas diffusion between air, fixed at atmospheric CO<sub>2</sub> levels, and soil. A no-flow or Neumann boundary condition was set at the bottom to simulate bedrock. Water saturation <italic>S<sub>w</sub></italic> was fixed to 0.4 over the whole column to simulate the presence of soil water. The value of <italic>S<sub>w</sub></italic> = 0.4 was chosen to simulate relatively dry conditions but above residual water saturation conditions (<xref ref-type="bibr" rid="ref47">Jia et al., 2021</xref>). In the model, an increase of <italic>S<sub>w</sub></italic> caused an increase in <italic>p</italic>CO<sub>2</sub> due to lower air-filled porosity at a given CO<sub>2</sub> production rate. Pre-simulations showed that the same effect was achieved by varying CO<sub>2</sub> production. Therefore, only CO<sub>2</sub> production was varied to simplify interpretation of simulation outcomes.</p>
</sec>
<sec id="sec6">
<label>2.2.2</label>
<title>Reaction network</title>
<p>The simulated reaction network with respect to C is shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>. In total, eight primary and 14 secondary aqueous species were simulated including several major cations and anions that are not shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>. Calcite was set to be in equilibrium with the aqueous phase due to its role as a pH buffer (<xref ref-type="bibr" rid="ref35">Gaillardet et al., 1999</xref>; <xref ref-type="bibr" rid="ref113">Wen et al., 2022</xref>; <xref ref-type="bibr" rid="ref80">Pfeiffer et al., 2023</xref>). To simulate soil respiration a zero-order rate law assuming no inhibition or catalysis was chosen (<xref ref-type="disp-formula" rid="EQ7">Equation 7</xref>):<disp-formula id="EQ7">
<label>(7)</label>
<mml:math id="M18">
<mml:mi>R</mml:mi>
<mml:mo>=</mml:mo>
<mml:msub>
<mml:mi>A</mml:mi>
<mml:mi>s</mml:mi>
</mml:msub>
<mml:mo>&#x22C5;</mml:mo>
<mml:msub>
<mml:mi>k</mml:mi>
<mml:mi>s</mml:mi>
</mml:msub>
</mml:math>
</disp-formula></p>
<fig position="float" id="fig2">
<label>Figure 2</label>
<caption>
<p>The simulated model domain (left) and the reaction network, including diffusive transport (right), are shown. When CO<sub>2</sub>(g) dissolves in water, it becomes aqueous: CO<sub>2</sub>(g) <inline-formula>
<mml:math id="M19">
<mml:mo>&#x2194;</mml:mo>
</mml:math>
</inline-formula> CO<sub>2</sub>(aq). The convention <inline-formula>
<mml:math id="M20">
<mml:msub>
<mml:mi mathvariant="normal">H</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
<mml:msubsup>
<mml:mrow>
<mml:mi mathvariant="normal">C</mml:mi>
<mml:mi mathvariant="normal">O</mml:mi>
</mml:mrow>
<mml:mn>3</mml:mn>
<mml:mo>&#x002A;</mml:mo>
</mml:msubsup>
<mml:mo>=</mml:mo>
<mml:msub>
<mml:mrow>
<mml:mi mathvariant="normal">C</mml:mi>
<mml:mi mathvariant="normal">O</mml:mi>
</mml:mrow>
<mml:mn>2</mml:mn>
</mml:msub>
<mml:mfenced open="(" close=")">
<mml:mrow>
<mml:mi mathvariant="normal">a</mml:mi>
<mml:mi mathvariant="normal">q</mml:mi>
</mml:mrow>
</mml:mfenced>
<mml:mo>+</mml:mo>
<mml:msub>
<mml:mi mathvariant="normal">H</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
<mml:msub>
<mml:mrow>
<mml:mi mathvariant="normal">C</mml:mi>
<mml:mi mathvariant="normal">O</mml:mi>
</mml:mrow>
<mml:mn>3</mml:mn>
</mml:msub>
</mml:math>
</inline-formula> has been adopted.</p>
</caption>
<graphic xlink:href="fclim-07-1505472-g002.tif"/>
</fig>
<p>Where <italic>A<sub>s</sub></italic> is the solid component surface area and <italic>k<sub>s</sub></italic> is the intrinsic rate constant. The model parameters were set such that the solid component did not decrease over the simulation time, resulting in a constant production of CO<sub>2</sub> over time, which simulates CO<sub>2</sub> emissions from the soil to the atmosphere. To reproduce observed <italic>p</italic>CO<sub>2</sub> depth profiles, the CO<sub>2</sub> production rate was simulated to be faster in the top 25&#x202F;cm compared to the remainder of the profile. This idealized representation was designed to facilitate examination of the resulting dynamics in the inorganic carbon pools.</p>
<p>Model parameterization of aqueous, and solid phases was based on literature values (<xref ref-type="bibr" rid="ref47">Jia et al., 2021</xref>; <xref ref-type="bibr" rid="ref113">Wen et al., 2022</xref>) (<xref ref-type="supplementary-material" rid="SM2">Supplementary Tables S4, S5</xref>). The calcite mineral volume fraction was set to 3 % over the entire model based on estimates for dry climates (<xref ref-type="bibr" rid="ref80">Pfeiffer et al., 2023</xref>). For simplicity a constant distribution of calcite over depth was considered sufficient because sorbent was only applied in the top centimeters and rain events were not simulated. A more accurate distribution of calcite over depth would be necessary for different conditions. Thermodynamic constants are from the EQ3/EQ6 database (<xref ref-type="bibr" rid="ref116">Wolery, 1992</xref>).</p>
</sec>
<sec id="sec7">
<label>2.2.3</label>
<title>Model approach and simulation scenarios</title>
<p>Prior to adding the sorbent, simulations were run to steady state to both create a baseline and exclude transient features that confuse the analysis. Depending on the initial scenario, steady- state profiles were obtained after 60&#x2013;100&#x202F;days. To allow all scenarios to reach steady state, the spin-up period was set to 400&#x202F;days, at which point sorbent was added, and the model was run until it reached steady state again. Simulation scenarios explored variations in (1) background CO<sub>2</sub> production rates, (2) application rates, (3) application density, (4) application depth, and (5) increased CO<sub>2</sub> production after application (<xref ref-type="supplementary-material" rid="SM2">Supplementary Table S6</xref>).</p>
<p>Three simulation scenarios with low, medium, or high CO<sub>2</sub> production over time were developed (<xref ref-type="supplementary-material" rid="SM1">Supplementary Figure S2</xref>) to simulate a range of observed <italic>p</italic>CO<sub>2</sub> profiles (<xref ref-type="bibr" rid="ref10">Cerling, 1984</xref>; <xref ref-type="bibr" rid="ref4">Amundson et al., 1998</xref>; <xref ref-type="bibr" rid="ref20">Davidson et al., 2006</xref>; <xref ref-type="bibr" rid="ref109">Wang et al., 2013</xref>; <xref ref-type="bibr" rid="ref14">Chirinda et al., 2014</xref>; <xref ref-type="bibr" rid="ref114">Winnick et al., 2020</xref>). Low CO<sub>2</sub> production resulted in low simulated <italic>p</italic>CO<sub>2</sub> and might represent soil respiration rates in drylands, although it should be noted that uncertainty of CO<sub>2</sub> production rates is high in drylands due to data scarcity (<xref ref-type="bibr" rid="ref77">Oertel et al., 2016</xref>; <xref ref-type="bibr" rid="ref112">Warner et al., 2019</xref>). Medium and high CO<sub>2</sub> production rates are more typical for temperate forests and croplands (<xref ref-type="bibr" rid="ref112">Warner et al., 2019</xref>). The medium and high rates were included because those ecosystems also occur in drylands and because soil amendments such as biochar can increase soil respiration rates (<xref ref-type="bibr" rid="ref28">El-Naggar et al., 2019</xref>).</p>
<p>Application rates were varied between 2 and 20 t/acre (<xref ref-type="bibr" rid="ref64">Lehmann and Rondon, 2006</xref>; <xref ref-type="bibr" rid="ref106">Thengane et al., 2021</xref>). The application density, which accounts for the importance of mixing and downward physical transport of biochar (<xref ref-type="bibr" rid="ref102">Spokas et al., 2014</xref>) was varied by changing the application depth while holding the application rate constant.</p>
<p>A simulated increase in CO<sub>2</sub> production after soil amendment application in addition to sorption (<xref ref-type="supplementary-material" rid="SM1">Supplementary Figure S1</xref>) was intended to replicate increased soil respiration (positive priming) that sometimes occurs after amendment of biochar, specifically in soil with initially low fertility (<xref ref-type="bibr" rid="ref28">El-Naggar et al., 2019</xref>). Although CO<sub>2</sub> sorption does not directly affect soil respiration rates, most soil amendments will fundamentally alter a range of soil properties and can change soil respiration rates. For biochar, positive and negative priming have been observed in field experiments (<xref ref-type="bibr" rid="ref74">Mosa et al., 2023</xref>). Mechanisms previously implicated in changes of CO<sub>2</sub> emissions after biochar application are transport effects introduced by altered pore structure (<xref ref-type="bibr" rid="ref29">Fan et al., 2020</xref>), increased water retention, increased SOC stock, promotion of CO<sub>2</sub>-fixing bacteria, and CO<sub>2</sub> sorption (<xref ref-type="bibr" rid="ref28">El-Naggar et al., 2019</xref>; <xref ref-type="bibr" rid="ref74">Mosa et al., 2023</xref>). Mineral soil amendments also affect soil water retention, porosity, pH, and nutrient availability (<xref ref-type="bibr" rid="ref45">Jarosz et al., 2022</xref>; <xref ref-type="bibr" rid="ref99">Sha et al., 2022</xref>) and could thereby alter bacterial communities (<xref ref-type="bibr" rid="ref45">Jarosz et al., 2022</xref>; <xref ref-type="bibr" rid="ref118">Zeng et al., 2022</xref>) and increase microbial activity (<xref ref-type="bibr" rid="ref24">Doni et al., 2021</xref>).</p>
<p>To describe the relative mobility of a chemical species, a retardation factor, <italic>R<sub>f</sub></italic>, is often used (<xref ref-type="bibr" rid="ref33">Freeze and Cherry, 1979</xref>). Various methods for calculation have been developed and critically reviewed (<xref ref-type="bibr" rid="ref83">Priddle and Jackson, 1991</xref>). The relationship between <italic>R<sub>f</sub></italic> and porosity, bulk density, and sorption coefficients is deduced from mass balance and verified with empirical data. However, transport and scale effects can lead to variations between theoretical and field measurements (<xref ref-type="bibr" rid="ref83">Priddle and Jackson, 1991</xref>). Methods based on breakthrough curves and times have been shown to give better results for gas&#x2013;solid systems and are often applied to laboratory and field data (<xref ref-type="bibr" rid="ref83">Priddle and Jackson, 1991</xref>; <xref ref-type="bibr" rid="ref25">Dou et al., 2016</xref>). Here, a simulation that mimics column experiments with a constant tracer gas injection is used to simulate the effects of sorption on migration of CO<sub>2</sub> after sorbent deposition. A simulation scenario where only sorbent was present as solid phase was compared to a scenario where only unreactive quartz was present as solid phase. To ensure comparable diffusion, the porosity was set to 0.7 for both simulations based on biochar porosity (<xref ref-type="bibr" rid="ref40">Gray et al., 2014</xref>). In both cases CO<sub>2</sub> production within the column was set to zero. However, <italic>p</italic>CO<sub>2</sub> was set to 30,000 ppm at the lower boundary. This ensures CO<sub>2</sub> diffuses through the column. When sorbent is present there will be a delay in transport. In this set up the retardation factor <italic>R<sub>f</sub></italic> is related to the ratio of breakthrough time of the sorbed CO<sub>2</sub> and the CO<sub>2</sub> in the unreactive quartz column (<xref ref-type="bibr" rid="ref25">Dou et al., 2016</xref>) (<xref ref-type="disp-formula" rid="EQ8">Equation 8</xref>):<disp-formula id="EQ8">
<label>(8)</label>
<mml:math id="M21">
<mml:msub>
<mml:mi>R</mml:mi>
<mml:mi>f</mml:mi>
</mml:msub>
<mml:mo>=</mml:mo>
<mml:mfrac>
<mml:msub>
<mml:mi>t</mml:mi>
<mml:mi>s</mml:mi>
</mml:msub>
<mml:msub>
<mml:mi>t</mml:mi>
<mml:mi>u</mml:mi>
</mml:msub>
</mml:mfrac>
</mml:math>
</disp-formula></p>
<p>Where <italic>t</italic> is the time that it takes to reach half of the initial concentration in the column filled with sorbent (subscript s) and unreactive quartz (subscript u) respectively. The retardation factors were calculated from simulated concentrations at a depth of 0.75&#x202F;cm. Breakthrough curves were constructed for <italic>p</italic>CO<sub>2</sub> at 0.5 depth.</p>
<p>A one-time reduction of CO<sub>2</sub> soil emissions was calculated as difference between simulated soil efflux without sorbent (i.e., the baseline or counterfactual) and with sorbent over the relaxation time (<xref ref-type="disp-formula" rid="EQ9">Equation 9</xref>):<disp-formula id="EQ9">
<label>(9)</label>
<mml:math id="M22">
<mml:mo>%</mml:mo>
<mml:mi mathvariant="italic">removed</mml:mi>
<mml:mo>=</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:msubsup>
<mml:mstyle displaystyle="true">
<mml:mo stretchy="true">&#x222B;</mml:mo>
</mml:mstyle>
<mml:mrow>
<mml:mi>t</mml:mi>
<mml:mo>_</mml:mo>
<mml:mi>i</mml:mi>
</mml:mrow>
<mml:mi>t</mml:mi>
</mml:msubsup>
<mml:mi>J</mml:mi>
<mml:msub>
<mml:mfenced open="(" close=")">
<mml:mi>t</mml:mi>
</mml:mfenced>
<mml:mi>c</mml:mi>
</mml:msub>
<mml:mi>d</mml:mi>
<mml:mi>t</mml:mi>
<mml:mo>&#x2212;</mml:mo>
<mml:msubsup>
<mml:mstyle displaystyle="true">
<mml:mo stretchy="true">&#x222B;</mml:mo>
</mml:mstyle>
<mml:mrow>
<mml:mi>t</mml:mi>
<mml:mo>_</mml:mo>
<mml:mi>i</mml:mi>
</mml:mrow>
<mml:mi>t</mml:mi>
</mml:msubsup>
<mml:mi>J</mml:mi>
<mml:msub>
<mml:mfenced open="(" close=")">
<mml:mi>t</mml:mi>
</mml:mfenced>
<mml:mi>s</mml:mi>
</mml:msub>
<mml:mi>d</mml:mi>
<mml:mi>t</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:msubsup>
<mml:mstyle displaystyle="true">
<mml:mo stretchy="true">&#x222B;</mml:mo>
</mml:mstyle>
<mml:mrow>
<mml:mi>t</mml:mi>
<mml:mo>_</mml:mo>
<mml:mi>i</mml:mi>
</mml:mrow>
<mml:mi>t</mml:mi>
</mml:msubsup>
<mml:mi>J</mml:mi>
<mml:msub>
<mml:mfenced open="(" close=")">
<mml:mi>t</mml:mi>
</mml:mfenced>
<mml:mi>c</mml:mi>
</mml:msub>
<mml:mi>d</mml:mi>
<mml:mi>t</mml:mi>
</mml:mrow>
</mml:mfrac>
<mml:mo>&#x22C5;</mml:mo>
<mml:mn>100</mml:mn>
</mml:math>
</disp-formula></p>
<p>Where <italic>J</italic> is the diffusive flux between soil and air, the subscript c indicates the counterfactual scenario, and the subscript s refers to scenarios with sorbent. Because flux <italic>J</italic> equals CO<sub>2</sub> production <italic>P</italic> under steady state conditions in the baseline scenario, <xref ref-type="disp-formula" rid="EQ9">Equation (9)</xref> can be rewritten as (<xref ref-type="disp-formula" rid="EQ10">Equation 10</xref>):<disp-formula id="EQ10">
<label>(10)</label>
<mml:math id="M23">
<mml:mo>%</mml:mo>
<mml:mi mathvariant="italic">removed</mml:mi>
<mml:mo>=</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:msubsup>
<mml:mstyle displaystyle="true">
<mml:mo stretchy="true">&#x222B;</mml:mo>
</mml:mstyle>
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<mml:mo>&#x22C5;</mml:mo>
<mml:mn>100</mml:mn>
</mml:math>
</disp-formula></p>
</sec>
<sec id="sec8">
<label>2.2.4</label>
<title>Model output analysis</title>
<p>For model verification and assessment, a time- and depth-integrated mass balance was developed (<xref ref-type="disp-formula" rid="EQ11">Equation 11</xref>):<disp-formula id="EQ11">
<label>(11)</label>
<mml:math id="M24">
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<mml:mi mathvariant="italic">dCalcite</mml:mi>
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</mml:mtr>
</mml:mtable>
</mml:math>
</disp-formula></p>
<p>Where <italic>t</italic> represents time, carbon storage in the soil is calculated as the inventory of CO<sub>2</sub>(g), DIC, and calcite, while <italic>U</italic> denotes CO<sub>2</sub> sorption. A detailed description of the mass balance can be found in supplemental information. The time elapsed between sorbent addition and the return of the system to steady state is the relaxation time.</p>
</sec>
</sec>
</sec>
<sec sec-type="results" id="sec9">
<label>3</label>
<title>Results</title>
<sec id="sec10">
<label>3.1</label>
<title>Baseline conditions under varying CO<sub>2</sub> production rates</title>
<p>Under baseline conditions with no sorbent present, simulated <italic>p</italic>CO<sub>2</sub> increased with depth and was higher in scenarios with higher CO<sub>2</sub> production (<xref ref-type="fig" rid="fig3">Figure 3A</xref>). The model adequately reproduced observed CO<sub>2</sub> trends for low, medium, and high CO<sub>2</sub> production where concentrations often rapidly increase to concentrations between 5,000 and 30,000 ppm over the first 50&#x202F;cm (<xref ref-type="bibr" rid="ref10">Cerling, 1984</xref>; <xref ref-type="bibr" rid="ref4">Amundson et al., 1998</xref>; <xref ref-type="bibr" rid="ref20">Davidson et al., 2006</xref>; <xref ref-type="bibr" rid="ref109">Wang et al., 2013</xref>; <xref ref-type="bibr" rid="ref14">Chirinda et al., 2014</xref>; <xref ref-type="bibr" rid="ref114">Winnick et al., 2020</xref>). CO<sub>2</sub> gradients over depth (dCO<sub>2</sub>/d<italic>z</italic>) were positive, meaning an efflux from the soil was simulated (<xref ref-type="fig" rid="fig3">Figure 3B</xref>). Simulated DIC increased, pH decreased and Ca<sup>2+</sup> increased with depth and <italic>p</italic>CO<sub>2</sub> (<xref ref-type="fig" rid="fig3">Figures 3C</xref>&#x2013;<xref ref-type="fig" rid="fig3">E</xref>). Depletion of the calcite mineral volume fraction was higher with higher <italic>p</italic>CO<sub>2</sub> (<xref ref-type="fig" rid="fig3">Figure 3F</xref>). As noted in the methods section, the calcite distribution over depth was simplified for model interpretation and will typically vary as a function of depth depending on climate (<xref ref-type="bibr" rid="ref80">Pfeiffer et al., 2023</xref>).</p>
<fig position="float" id="fig3">
<label>Figure 3</label>
<caption>
<p>Shown are baseline conditions under constantly low, medium, and high CO<sub>2</sub> production. Simulated depth profiles of <bold>(A)</bold> <italic>p</italic>CO<sub>2</sub>, <bold>(B)</bold> concentration gradient [dCO<sub>2</sub>(g)/d<italic>z</italic>], <bold>(C)</bold> DIC, <bold>(D)</bold> pH, <bold>(E)</bold> Ca<sup><italic>2</italic>+</sup>, and <bold>(F)</bold> the calcite mineral volume fraction are presented.</p>
</caption>
<graphic xlink:href="fclim-07-1505472-g003.tif"/>
</fig>
</sec>
<sec id="sec11">
<label>3.2</label>
<title>Soil CO<sub>2</sub> response to sorbent addition</title>
<p>Sorption of CO<sub>2</sub> affected soil <italic>p</italic>CO<sub>2</sub> and soil CO<sub>2</sub> efflux (<xref ref-type="fig" rid="fig4">Figure 4</xref>). The simulated sorption capacity (sorbed CO<sub>2</sub>/g sorbent) aligned with observed data that had been used to derive sorption isotherms (<xref ref-type="fig" rid="fig4">Figure 4A</xref>). Sorption increases with <italic>p</italic>CO<sub>2</sub>, which in the simulations increased with depth and CO<sub>2</sub> production. The scenario with the highest CO<sub>2</sub> production reached almost 0.015&#x202F;bar within the application depth of 25&#x202F;cm, under which the sorption capacity was almost three times higher than at atmospheric <italic>p</italic>CO<sub>2</sub>. Over the simulation time, the addition of the sorbent to the soil is visible in a decline of <italic>p</italic>CO<sub>2</sub> (<xref ref-type="fig" rid="fig4">Figure 4B</xref>). At a depth of 20.5&#x202F;cm, the simulated <italic>p</italic>CO<sub>2</sub> was initially around 2,000&#x202F;ppm for a scenario with low CO<sub>2</sub> production. At day 400 of the simulation, sorbent was added and <italic>p</italic>CO<sub>2</sub> decreased to almost 0&#x202F;ppm. After several days the <italic>p</italic>CO<sub>2</sub> rose again and then slowly returned to steady state after around 50&#x202F;days. The return to steady state was faster with higher CO<sub>2</sub> production. Sorption behavior was transient over depth because gas diffusion and production are not instantaneous (<xref ref-type="fig" rid="fig4">Figure 4C</xref>). Immediately after application, sorbed CO<sub>2</sub> over depth followed a u-shape with high sorption at the atmosphere-soil and the shallow-deep soil interface. The shape indicates that gas from the deeper soil and the atmosphere was diffusing in (<xref ref-type="fig" rid="fig4">Figure 4D</xref>). The sorption temporarily reduced CO<sub>2</sub> efflux and even caused CO<sub>2</sub> influx from the atmosphere (<xref ref-type="fig" rid="fig4">Figure 4B</xref>). The effect on efflux lasted longer when CO<sub>2</sub> production was lower.</p>
<fig position="float" id="fig4">
<label>Figure 4</label>
<caption>
<p>Sorbed CO<sub>2</sub>, <italic>p</italic>CO<sub>2</sub> and CO<sub>2</sub> efflux after sorbent addition. <bold>(A)</bold> Sorbed CO<sub>2</sub> (mol/g sorbent) as a function of <italic>p</italic>CO<sub>2</sub> simulated under high CO<sub>2</sub> production (red line) and observed values that were used to fit the Langmuir isotherm (<xref ref-type="bibr" rid="ref88">Ringsby et al., 2024</xref>) (grey dots). Sorbent was present in model over the top 25&#x202F;cm. <bold>(B)</bold> Simulated <italic>p</italic>CO<sub>2</sub> over time at a depth of 0.205&#x202F;m for one scenario with low CO<sub>2</sub> production with sorbent addition at day 400. Simulated <italic>p</italic>CO<sub>2</sub> was at a steady state before sorbent addition and returned to steady state after roughly 50&#x202F;days. <bold>(C)</bold> Transient depth profiles of sorbed CO<sub>2</sub> over the top 0.5&#x202F;m under low CO<sub>2</sub> production. Shown are initial baseline conditions without sorbent (red), conditions at 0.1, 1, and 7&#x202F;days after sorbent application, and final sorption (green) upon which all other simulated parameters return to baseline conditions. The grey area indicates the application depth. <bold>(D)</bold> CO<sub>2</sub> efflux at soil surface with low, medium, and high CO<sub>2</sub> production. A drop below zero indicates influx to the soil.</p>
</caption>
<graphic xlink:href="fclim-07-1505472-g004.tif"/>
</fig>
<p>Total maximum sorption was higher with higher CO<sub>2</sub> production and higher total sorbent mass (<xref ref-type="fig" rid="fig5">Figure 5</xref>). Total sorption can be related to mean steady state <italic>p</italic>CO<sub>2</sub> over application depth (<xref ref-type="supplementary-material" rid="SM1">Supplementary Figure S3</xref>). A temporary reduction in efflux was related to CO<sub>2</sub> production and sorbent mass, as was expected (<xref ref-type="fig" rid="fig5">Figure 5B</xref>).</p>
<fig position="float" id="fig5">
<label>Figure 5</label>
<caption>
<p><bold>(A)</bold> Total sorbed CO<sub>2</sub> and <bold>(B)</bold> temporary reduction in CO<sub>2</sub> efflux, both as a function of total added sorbent mass and depending on CO<sub>2</sub> production.</p>
</caption>
<graphic xlink:href="fclim-07-1505472-g005.tif"/>
</fig>
<p>Transport occurred in simulations only via diffusion, which is slow compared to advection and results in a notably delayed breakthrough and broadened breakthrough curve (<xref ref-type="fig" rid="fig6">Figure 6</xref>) compared with sorption studies that pump gas into columns (<xref ref-type="bibr" rid="ref50">Kaur et al., 2019</xref>; <xref ref-type="bibr" rid="ref78">Pal et al., 2019</xref>; <xref ref-type="bibr" rid="ref2">Al Mesfer et al., 2020</xref>).</p>
<fig position="float" id="fig6">
<label>Figure 6</label>
<caption>
<p>Simulated breakthrough curves for <italic>p</italic>CO<sub>2</sub> at 0.5&#x202F;m depth when a 1&#x202F;m column consists of either unreactive quartz or sorbent. Gas transport occurs only through diffusion resulting in a delay to reach steady state conditions without sorption.</p>
</caption>
<graphic xlink:href="fclim-07-1505472-g006.tif"/>
</fig>
</sec>
<sec id="sec12">
<label>3.3</label>
<title>Response of soil geochemical parameters</title>
<p>Depth profiles show that changes in <italic>p</italic>CO<sub>2</sub> through sorption affected all simulated parameters (<xref ref-type="fig" rid="fig7">Figure 7</xref>). Changes are particularly visible immediately after application and where sorbent had been applied (in the top 25&#x202F;cm). Immediately after sorbent application, the <italic>p</italic>CO<sub>2</sub> reached almost zero over the application depth. The CO<sub>2</sub> gradients changed from positive to negative at the atmosphere-soil interface, indicating that there was CO<sub>2</sub> influx to the soil instead of efflux. The CO<sub>2</sub> gradients strongly increased where sorbent amended soil meets the unamended soil. Over the application depth, simulated DIC was reduced by over 90%, and pH increased from 7.5 to 8. The pH was increased because sorption of CO<sub>2</sub> that is in equilibrium with the aqueous phase removes bicarbonate ions and protons from solution via:<disp-formula id="E12">
<label>(12)</label>
<mml:math id="M26">
<mml:msub>
<mml:mrow>
<mml:mi mathvariant="normal">C</mml:mi>
<mml:mi mathvariant="normal">O</mml:mi>
</mml:mrow>
<mml:mn>2</mml:mn>
</mml:msub>
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<mml:mrow>
<mml:mi mathvariant="normal">a</mml:mi>
<mml:mi mathvariant="normal">q</mml:mi>
</mml:mrow>
</mml:mfenced>
<mml:mo>+</mml:mo>
<mml:msub>
<mml:mi mathvariant="normal">H</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
<mml:mi mathvariant="normal">O</mml:mi>
<mml:mo>&#x2194;</mml:mo>
<mml:msubsup>
<mml:mrow>
<mml:mi mathvariant="normal">H</mml:mi>
<mml:mi mathvariant="normal">C</mml:mi>
<mml:mi mathvariant="normal">O</mml:mi>
</mml:mrow>
<mml:mn>3</mml:mn>
<mml:mo>-</mml:mo>
</mml:msubsup>
<mml:mo>+</mml:mo>
<mml:msup>
<mml:mi mathvariant="normal">H</mml:mi>
<mml:mo>+</mml:mo>
</mml:msup>
</mml:math>
</disp-formula></p>
<fig position="float" id="fig7">
<label>Figure 7</label>
<caption>
<p>Simulated changes in soil geochemical parameters due to sorption on soil amendment and increased CO<sub>2</sub> production. <bold>(A)</bold> Simulated <italic>p</italic>CO<sub>2</sub> at depth 20.5&#x202F;cm and over simulation time. Heatmaps over depth and simulation time for <bold>(B)</bold> sorbed CO<sub>2</sub>, <bold>(C)</bold> <italic>p</italic>CO<sub>2</sub>, <bold>(D)</bold> dpCO<sub>2</sub>/dz., <bold>(E)</bold> DIC, <bold>(F)</bold> pH, <bold>(G)</bold> Ca<sup>2+</sup>, and <bold>(H)</bold> calcite volume fraction. Application rate of 9.86&#x202F;t/acre and 25&#x202F;cm application depth.</p>
</caption>
<graphic xlink:href="fclim-07-1505472-g007.tif"/>
</fig>
<p>The simulated Ca<sup>2+</sup> was around 50% lower and the calcite mineral volume fraction was slightly increased due to precipitation. The precipitation was temporary, and calcite redissolved. The transient change in calcite mineral volume fraction was larger with higher total sorption. Transient conditions lasted longer when CO<sub>2</sub> production was lower. Transient conditions lasted for 30&#x2013;50&#x202F;days when only sorption and no increased CO<sub>2</sub> production was simulated.</p>
<p>Assuming an increased CO<sub>2</sub> production after amendment application resulted in deviation of soil geochemical parameters after 20&#x202F;days (<xref ref-type="fig" rid="fig7">Figure 7</xref>): higher <italic>p</italic>CO<sub>2</sub>, higher dCO<sub>2</sub>/d<italic>z</italic>, higher DIC, lower pH, higher Ca<sup>2+</sup>, and lower calcite volume fraction. This indicates that changes in CO<sub>2</sub> production &#x2013; an empirical representation of soil respiration &#x2013; have the potential to persistently change soil geochemistry.</p>
<p>A high retardation factor of <inline-formula>
<mml:math id="M27">
<mml:msub>
<mml:mi>R</mml:mi>
<mml:mi>f</mml:mi>
</mml:msub>
<mml:mo>=</mml:mo>
<mml:mn>37.5</mml:mn>
</mml:math>
</inline-formula> was calculated in a simplified simulation scenario with either sorbent or unreactive quartz. The delay in diffusion due to sorption is clearly visible in <italic>p</italic>CO<sub>2</sub> heatmaps (<xref ref-type="fig" rid="fig7">Figure 7</xref>). In the column with quartz, <italic>p</italic>CO<sub>2</sub> increases rapidly in &#x003C;1 day and is then at steady state. With sorbent, there is a slow increase over 30&#x202F;days, after which steady state is reached.</p>
</sec>
</sec>
<sec sec-type="discussion" id="sec13">
<label>4</label>
<title>Discussion</title>
<p>In the following we will discuss how manipulation of soil CO<sub>2</sub> affects inorganic C cycling in unsaturated soils and the importance of transient conditions. We present implications for application and monitoring of CDR that affects the soil response. Although simulations were focused on C cycling, there are additional benefits and limitations for soil amendment application in drylands, which we will also discuss.</p>
<sec id="sec14">
<label>4.1</label>
<title>Inorganic carbon cycling in dry soils</title>
<p><xref ref-type="fig" rid="fig8">Figure 8</xref> shows how carbonate alkalinity and Ca<sup>2+</sup> concentrations are related to carbonate dissolution via acids in addition to other processes, e.g., degassing and sorption. The 1:1 line in <xref ref-type="fig" rid="fig8">Figure 8</xref> indicates carbonate dissolution through carbonic acids (<xref ref-type="bibr" rid="ref98">Semhi et al., 2000</xref>; <xref ref-type="bibr" rid="ref79">Perrin et al., 2008</xref>):<disp-formula id="E13">
<label>(13)</label>
<mml:math id="M28">
<mml:msub>
<mml:mi mathvariant="normal">CaCO</mml:mi>
<mml:mn>3</mml:mn>
</mml:msub>
<mml:mo>+</mml:mo>
<mml:msub>
<mml:mrow>
<mml:mi mathvariant="normal">C</mml:mi>
<mml:mi mathvariant="normal">O</mml:mi>
</mml:mrow>
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</mml:msub>
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<mml:mi mathvariant="normal">C</mml:mi>
<mml:mi mathvariant="normal">O</mml:mi>
</mml:mrow>
<mml:mn>3</mml:mn>
<mml:mo>-</mml:mo>
</mml:msubsup>
<mml:mo>+</mml:mo>
<mml:msup>
<mml:mrow>
<mml:mi mathvariant="normal">C</mml:mi>
<mml:mi mathvariant="normal">a</mml:mi>
</mml:mrow>
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<mml:mn>2</mml:mn>
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</mml:mrow>
</mml:msup>
</mml:math>
</disp-formula></p>
<fig position="float" id="fig8">
<label>Figure 8</label>
<caption>
<p>Carbonate alkalinity and Ca<sup>2+</sup> and Mg<sup>2+</sup> concentrations shown for steady state conditions at the soil-atmosphere interface (red square), transient conditions at the soil-atmosphere interface (blue dot), and steady state conditions at 1&#x202F;m depth. The lower line depicts the 1:1 ratio expected for carbonate dissolution exclusively from carbonic acid. The upper line depicts 2:1 stoichiometry of calcite dissolution through other acids, e.g., in fertilizer impacted sites. The area above the 2:1 line represents conversion of bicarbonate to CO<sub>2</sub> through degassing.</p>
</caption>
<graphic xlink:href="fclim-07-1505472-g008.tif"/>
</fig>
<p>And a possible reaction for the 2:1 line is (<xref ref-type="bibr" rid="ref117">Zamanian et al., 2018</xref>):<disp-formula id="E14">
<label>(14)</label>
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<mml:mrow>
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<mml:mi mathvariant="normal">H</mml:mi>
</mml:mrow>
<mml:mn>3</mml:mn>
</mml:msub>
<mml:mo>+</mml:mo>
<mml:msub>
<mml:mi mathvariant="normal">H</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
<mml:mi mathvariant="normal">O</mml:mi>
<mml:mo>+</mml:mo>
<mml:mn>2</mml:mn>
<mml:msub>
<mml:mi mathvariant="normal">O</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
<mml:mo>&#x2192;</mml:mo>
<mml:msubsup>
<mml:mrow>
<mml:mi mathvariant="normal">H</mml:mi>
<mml:mi mathvariant="normal">C</mml:mi>
<mml:mi mathvariant="normal">O</mml:mi>
</mml:mrow>
<mml:mn>3</mml:mn>
<mml:mo>-</mml:mo>
</mml:msubsup>
<mml:mo>+</mml:mo>
<mml:msup>
<mml:mrow>
<mml:mi mathvariant="normal">C</mml:mi>
<mml:mi mathvariant="normal">a</mml:mi>
</mml:mrow>
<mml:mrow>
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<mml:mo>+</mml:mo>
</mml:mrow>
</mml:msup>
<mml:mo>+</mml:mo>
<mml:msubsup>
<mml:mi mathvariant="normal">NO</mml:mi>
<mml:mn>3</mml:mn>
<mml:mo>-</mml:mo>
</mml:msubsup>
<mml:mo>+</mml:mo>
<mml:mn>2</mml:mn>
<mml:msub>
<mml:mi mathvariant="normal">H</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
<mml:mi mathvariant="normal">O</mml:mi>
</mml:math>
</disp-formula></p>
<p><xref ref-type="disp-formula" rid="E14">Equation 14</xref> describes calcite dissolution after N fertilizer application. Acidification leads to increased calcite dissolution rates and cations are balanced by nitrate anions, as opposed to only bicarbonate (<xref ref-type="bibr" rid="ref117">Zamanian et al., 2018</xref>). This reaction has been identified as a CO<sub>2</sub> source in agricultural areas that are either limed or where carbonates naturally occur (<xref ref-type="bibr" rid="ref98">Semhi et al., 2000</xref>; <xref ref-type="bibr" rid="ref79">Perrin et al., 2008</xref>; <xref ref-type="bibr" rid="ref117">Zamanian et al., 2018</xref>). Transient conditions above the 2:1 line occurred in the simulations due only to sorption and degassing&#x2014;contributing to lower bicarbonate concentrations but no cations. Some calcite precipitation occurred simultaneously resulting in a slight drop in cation concentrations.</p>
<p>Transient conditions in drylands are often driven by wetting events, which cause a complex biogeochemical soil response (<xref ref-type="bibr" rid="ref46">Jarvis et al., 2007</xref>) including increased soil respiration, desorption (<xref ref-type="bibr" rid="ref93">S&#x00E1;nchez-Garc&#x00ED;a et al., 2020</xref>), and dissolution and reprecipitation of carbonate minerals (<xref ref-type="bibr" rid="ref5">Angert et al., 2015</xref>; <xref ref-type="bibr" rid="ref36">Gallagher and Breecker, 2020</xref>). A short-term increase in CO<sub>2</sub> efflux is known as &#x201C;Birch effect&#x201D; and is mostly attributed to increased soil respiration although immediate release of CO<sub>2</sub> has been associated with desorption (<xref ref-type="bibr" rid="ref51">Kemper et al., 1985</xref>; <xref ref-type="bibr" rid="ref93">S&#x00E1;nchez-Garc&#x00ED;a et al., 2020</xref>) which strongly depends on OM content in soils (<xref ref-type="bibr" rid="ref21">De Jonge and Mittelmeijer-Hazeleger, 1996</xref>). Carbonate dissolution increases with elevated <italic>p</italic>CO<sub>2</sub>, which dampens the soil CO<sub>2</sub> efflux after wetting events and has been associated with underestimation of soil respiration rates when carbonates are present (<xref ref-type="bibr" rid="ref5">Angert et al., 2015</xref>; <xref ref-type="bibr" rid="ref36">Gallagher and Breecker, 2020</xref>). A second important source of transient conditions in drylands are daily, seasonal, and annual temperature changes. Increased temperature generally leads to increased soil respiration and desorption although concomitant changes in moisture can either amplify or reduce this response (<xref ref-type="bibr" rid="ref105">Tang et al., 2003</xref>; <xref ref-type="bibr" rid="ref100">Shen et al., 2009</xref>; <xref ref-type="bibr" rid="ref18">Darrouzet-Nardi et al., 2015</xref>; <xref ref-type="bibr" rid="ref91">Sagi et al., 2021</xref>).</p>
<p>Transient conditions lasted for varying time scales in the simulations, which has implications for monitoring (<xref ref-type="fig" rid="fig9">Figure 9</xref>). Increased calcite precipitation lasted only a few hours while the soil CO<sub>2</sub> efflux was affected over more than 10 days. Comparison to field observations shows similar variations in time scales. The Birch effect, which occurs on dryland soils, is most pronounced for a few hours or days after a wetting event (<xref ref-type="bibr" rid="ref46">Jarvis et al., 2007</xref>; <xref ref-type="bibr" rid="ref107">Unger et al., 2010</xref>). Seasonal variations in wet-dry cycles will lead to prolonged variation in carbonate dissolution and precipitation (<xref ref-type="bibr" rid="ref8">Breecker et al., 2009</xref>; <xref ref-type="bibr" rid="ref36">Gallagher and Breecker, 2020</xref>; <xref ref-type="bibr" rid="ref22">Dom&#x00ED;nguez-villar et al., 2022</xref>).</p>
<fig position="float" id="fig9">
<label>Figure 9</label>
<caption>
<p>Total concentration changes in sorbed CO<sub>2</sub>, soil CO<sub>2</sub>, DIC in porewater, and calcite over simulation time in comparison with CO<sub>2</sub> efflux from soil (right y-axis). The red area indicates the range of carbonate alkalinity flux in rivers in carbonate-dominated catchments (mol&#x202F;m<sup>&#x2212;2</sup> s<sup>&#x2212;1</sup>) (data from <xref ref-type="bibr" rid="ref120">Zhang S. et al., 2022</xref>).</p>
</caption>
<graphic xlink:href="fclim-07-1505472-g009.tif"/>
</fig>
<p>Transient conditions are also important to for managing carbon cycling in drylands. In 5 h laboratory experiments, the peak after wetting composed almost 80% of the total CO<sub>2</sub> efflux (<xref ref-type="bibr" rid="ref93">S&#x00E1;nchez-Garc&#x00ED;a et al., 2020</xref>). Transient conditions due to drying and rewetting&#x2014;even when short-lived&#x2014;were found to result in higher soil CO<sub>2</sub> emissions than constantly moist soils and gain relevance because of the spatial extent of drylands (<xref ref-type="bibr" rid="ref46">Jarvis et al., 2007</xref>; <xref ref-type="bibr" rid="ref100">Shen et al., 2009</xref>).</p>
<p>Shown as comparison to the simulated soil CO<sub>2</sub> efflux is the range of carbonate alkalinity fluxes in rivers in carbonate-dominated catchments (<xref ref-type="bibr" rid="ref120">Zhang S. et al., 2022</xref>) (<xref ref-type="fig" rid="fig9">Figure 9</xref>). Carbonate alkalinity export to rivers derived from calcite correlates with hydrological conditions and carbonate precipitation under dry conditions leads to increased CO<sub>2</sub> soil efflux (<xref ref-type="bibr" rid="ref113">Wen et al., 2022</xref>). Therein lies a potential benefit of increased gas sorption within carbonate containing soils. Sorption is reversible and desorption of CO<sub>2</sub> that occurs when water is present could aid export of carbonate alkalinity to rivers. How much of the desorbed CO<sub>2</sub> escapes to the atmosphere or is trapped in pore space depends on a myriad of environmental factors, such as water amount and soil properties (<xref ref-type="bibr" rid="ref93">S&#x00E1;nchez-Garc&#x00ED;a et al., 2020</xref>).</p>
</sec>
<sec id="sec15">
<label>4.2</label>
<title>Implications for application of soil amendments and monitoring of CDR</title>
<p>The simulated dynamics indicate both potential co-benefits and disadvantages for co-application of various soil amendments. Application of soil amendments that cause positive priming might be suitable to be combined with EW, because the increased production of CO<sub>2</sub> could drive mineral dissolution. However, soil amendments that induce negative priming associated with reduced CO<sub>2</sub> production could hinder EW. Biochar can cause positive or negative priming, but the underlying drivers are still poorly understood (<xref ref-type="bibr" rid="ref28">El-Naggar et al., 2019</xref>). Thus, sites-specific evaluation of the response to biochar may be required.</p>
<p>The simulations have further implications for monitoring established or promising soil CDR methods. CDR via biochar currently only considers C that is contained in biochar, but biochar also affects native soil C. This is why recommendations for monitoring would be relevant for biochar if native soil C is regulated in the future. This is especially important because fragile drylands soils are more vulnerable to climate change (<xref ref-type="bibr" rid="ref57">Lal, 2019</xref>). Key drivers for carbon cycling, such as temperature and precipitation, are currently changing at a regional scale, while the local response of SOC and SIC pools in drylands is uncertain (<xref ref-type="bibr" rid="ref100">Shen et al., 2009</xref>; <xref ref-type="bibr" rid="ref110">Wang et al., 2022</xref>). Depending on specific climatic and soil conditions in drylands, monitoring campaigns need to adequately capture transient conditions over different time scales. If degassing, (de)sorption, and soil gas displacement are expected to play a major role and should be investigated (<xref ref-type="bibr" rid="ref93">S&#x00E1;nchez-Garc&#x00ED;a et al., 2020</xref>), monitoring needs to capture transient conditions that might last only a few hours or days. On the other hand, climates dominated by seasonal variations need to capture these variations over longer time scales and to avoid under-or overestimation of carbon fluxes.</p>
<p>Various monitoring methods need to be applied to distinguish different processes within the carbon cycle. There are a range of parameters that can help to monitor CDR by distinguishing between organic and inorganic carbon cycling. Carbon mass balance over depths, <italic>p</italic>CO<sub>2</sub> depth profiles, O<sub>2</sub> concentrations or depth profiles, and carbon isotope composition can help to distinguish biotic and abiotic process (<xref ref-type="bibr" rid="ref5">Angert et al., 2015</xref>; <xref ref-type="bibr" rid="ref36">Gallagher and Breecker, 2020</xref>). Monitoring major cations and anions is helpful to resolve if carbonate and silicate weathering consumes CO<sub>2</sub> or is driven by other acids (<xref ref-type="bibr" rid="ref79">Perrin et al., 2008</xref>; <xref ref-type="bibr" rid="ref117">Zamanian et al., 2018</xref>).</p>
<p>Simulated carbon dynamics are specifically relevant for monitoring of EW. Monitoring of all parameters that are affected by CDR methods like EW can be expensive, which is why monitoring schemes that provide reliable CDR estimates based on as little monitoring as possible are under development and there is no consensus yet on what constitutes a reliable method. <xref ref-type="bibr" rid="ref34">Fuhr et al. (2023)</xref> also points out that highly dynamic natural background conditions need to be accounted to monitor EW fluxes reliably. Various methods to monitor or predict EW have been presented in the literature: (1) carbonate alkalinity and cation concentrations either in rivers (<xref ref-type="bibr" rid="ref53">Knapp and Tipper, 2022</xref>; <xref ref-type="bibr" rid="ref120">Zhang S. et al., 2022</xref>) or in soils (<xref ref-type="bibr" rid="ref43">Holzer et al., 2023</xref>), (2) Ca, Mg and nitrate ions and rare earth elements (<xref ref-type="bibr" rid="ref48">Kantola et al., 2023</xref>) (3) total alkalinity (<xref ref-type="bibr" rid="ref34">Fuhr et al., 2023</xref>), (4) electrical conductivity (<xref ref-type="bibr" rid="ref87">Rieder et al., 2023</xref>), and (5) simulations of varying complexity and spatial scale (<xref ref-type="bibr" rid="ref6">Beerling et al., 2020</xref>; <xref ref-type="bibr" rid="ref15">Cipolla et al., 2021</xref>; <xref ref-type="bibr" rid="ref49">Kanzaki et al., 2023</xref>). An important process that was highlighted by simulations here and should be considered when monitoring EW is degassing, which resulted in additional removal of DIC from solution as well as short-lived calcite precipitation. Most streams are oversaturated with respect to CO<sub>2</sub> and degassing is prevalent (<xref ref-type="bibr" rid="ref104">Stets et al., 2017</xref>). Estimates suggest up to 60% of CO<sub>2</sub> emissions from streams originate from DIC (<xref ref-type="bibr" rid="ref27">Duvert et al., 2019</xref>; <xref ref-type="bibr" rid="ref115">Winnick and Saccardi, 2024</xref>), and 30% of CO<sub>2</sub> originate from DOC (<xref ref-type="bibr" rid="ref52">Khadka et al., 2014</xref>). Spatial and temporal patterns of <italic>p</italic>CO<sub>2</sub>, degassing and sources of degassing depend on flow regimes, respiration, alkalinity, and groundwater inputs (<xref ref-type="bibr" rid="ref52">Khadka et al., 2014</xref>; <xref ref-type="bibr" rid="ref115">Winnick and Saccardi, 2024</xref>). A positive correlation between the pool of DIC and the contribution of DIC to degassing fluxes has been found (<xref ref-type="bibr" rid="ref115">Winnick and Saccardi, 2024</xref>). In the simulations, degassing and removal of DIC also led to calcite precipitation. However many rivers are supersaturated with respect to calcite potentially due to inhibition (<xref ref-type="bibr" rid="ref53">Knapp and Tipper, 2022</xref>).</p>
</sec>
<sec id="sec16">
<label>4.3</label>
<title>Carbon sequestration potential</title>
<p>The simulations show that abiotic C-sinks such as CO<sub>2</sub> sorption gain importance as a C sink in soils when biological activity is low, which is the case in many dryland ecosystems (<xref ref-type="bibr" rid="ref112">Warner et al., 2019</xref>; <xref ref-type="bibr" rid="ref91">Sagi et al., 2021</xref>). The relative reduction in CO<sub>2</sub> efflux over relaxation time was higher with lower CO<sub>2</sub> production (<xref ref-type="fig" rid="fig5">Figure 5</xref>). Moreover, dryland soils with low organic matter content have the lowest sorption capacity of all naturally occurring soils and around 10 times lower sorption capacity than the simulated sorbents (<xref ref-type="bibr" rid="ref21">De Jonge and Mittelmeijer-Hazeleger, 1996</xref>; <xref ref-type="bibr" rid="ref85">Ravikovitch et al., 2005</xref>; <xref ref-type="bibr" rid="ref19">Davidson et al., 2013</xref>). Although CDR through sorption is estimated to be relatively low for a single application (around 2% of total C for the simulated biochar as detailed in SI), soil amendments could be relevant for drylands due to the limitations of other methods and through provision of soil health benefits.</p>
</sec>
<sec id="sec17">
<label>4.4</label>
<title>Additional considerations for soil amendments in drylands</title>
<p>Soil amendments have the co-benefit of alleviating soil degradation, specifically salinization. Soil salinity is a worldwide concern, with drylands, irrigated lands, and agricultural lands most at risk (<xref ref-type="bibr" rid="ref26">Dregne et al., 1991</xref>; <xref ref-type="bibr" rid="ref44">Ivushkin et al., 2019</xref>). Mechanisms that have been implicated in salinity amelioration with biochar are: release of Ca<sup>2+</sup> and Mg<sup>2+</sup>, adsorption of Na<sup>+</sup>, proton release that promotes Na<sup>+</sup> uptake in certain plant species, increased salt leaching through increased porosity (<xref ref-type="bibr" rid="ref1">Akhtar et al., 2015</xref>; <xref ref-type="bibr" rid="ref3">Amini et al., 2016</xref>), reduced EC (<xref ref-type="bibr" rid="ref60">Lashari et al., 2015</xref>), and changes in evaporation dynamics (<xref ref-type="bibr" rid="ref65">Liang et al., 2021</xref>; <xref ref-type="bibr" rid="ref61">Lee et al., 2022</xref>). However, depending on biochar characteristics biochar could release Na<sup>+</sup> (<xref ref-type="bibr" rid="ref92">Saifullah Dahlawi et al., 2018</xref>) and some biochar studies have been criticized because salt stress was induced with NaCl (<xref ref-type="bibr" rid="ref1">Akhtar et al., 2015</xref>).</p>
<p>Challenges for soil amendment application are health risks, transport emission and albedo changes. Although biochar feedstock can contain heavy metals and organic contaminants, the fraction that is bioavailable after pyrolysis tends to be small (<xref ref-type="bibr" rid="ref39">Godlewska et al., 2021</xref>). Sorbent materials generally immobilize contaminants if the sorbent is immobile (<xref ref-type="bibr" rid="ref39">Godlewska et al., 2021</xref>) suggesting positive health effects. Soil amendments can lead to reduced wind erosion long-term, which could be an important benefit for drylands (<xref ref-type="bibr" rid="ref97">&#x015E;eker and Manirakiza, 2020</xref>; <xref ref-type="bibr" rid="ref81">Pi et al., 2021</xref>).</p>
<p>Emissions from implementation, e.g., material preparation and transport will reduce the CDR potential. Transport emissions are a particular concern, because there is typically little infrastructure in drylands. Sources for biochar are scarce in drylands due to relatively lower above ground biomass (<xref ref-type="bibr" rid="ref16">Cook-Patton et al., 2020</xref>), however, most of the global irrigated lands are situated on drylands (<xref ref-type="bibr" rid="ref26">Dregne et al., 1991</xref>; <xref ref-type="bibr" rid="ref101">Siebert et al., 2015</xref>) and could provide biomass sources, as could other organic wastes.</p>
<p>Albedo refers to surface albedo, which varies by land cover type, color, wetness and surface irregularities (<xref ref-type="bibr" rid="ref119">Zhang X. et al., 2022</xref>). Albedo is highest in deserts (0.2&#x2013;0.45) and dry soils (0.15&#x2013;0.36) while increased water content (0.06&#x2013;0.19) and vegetation cover reduce albedo (grasses 0.2, savannah 0.15&#x2013;0.2) (<xref ref-type="bibr" rid="ref38">Garratt, 1993</xref>). Biochar application was found to lead to albedo reduction of 0.05 on agricultural soil, which lowered the predicted climate change mitigation benefit by 13&#x2013;22% (<xref ref-type="bibr" rid="ref69">Meyer et al., 2012</xref>). The changes in soil albedo are less of a concern for vegetated grasslands and shrublands, which make up around two thirds of global drylands. Future work should assess albedo changes in field trials.</p>
</sec>
</sec>
<sec id="sec18">
<label>5</label>
<title>Summary</title>
<p>Reactive transport simulations were performed to investigate dynamics between organic and inorganic C pools in dryland soils and to predict CDR via CO<sub>2</sub> sorption on soil amendments. In the simulations, CDR via sorption gained importance when biological activity was low &#x2013;transient conditions lasted longer and a larger percentage of CO<sub>2</sub> was prevented from efflux during those transient conditions. Simulations highlighted that CO<sub>2</sub> removal via sorption causes transient conditions affecting CO<sub>2</sub> efflux, <italic>p</italic>CO<sub>2</sub>, DIC, pH, major cations and calcite. The simulated dynamics have implications for the application of a range of CDR methods, e.g., if the combined application of biochar and minerals for enhanced rock weathering will benefit CDR depends on soil priming effects. The transient conditions have implications for monitoring: the presence of carbonates, degassing, and desorption can affect the timing and magnitude of the soil CO<sub>2</sub> response, which needs to be considered in sampling schedules or sampling parameters. Future work should include evaluation of different sorbent designs, transport modes, and albedo changes. Considering that a high percentage of dryland soils are degraded and that other methods are limited by water availability, soil amendments with high sorption potential and soil health benefits could provide valuable CDR potential and aid restoration of dryland soils.</p>
</sec>
</body>
<back>
<sec sec-type="data-availability" id="sec19">
<title>Data availability statement</title>
<p>The original contributions presented in the study are included in the article/<xref ref-type="supplementary-material" rid="SM1">Supplementary material</xref>, further inquiries can be directed to the corresponding author.</p>
</sec>
<sec sec-type="author-contributions" id="sec20">
<title>Author contributions</title>
<p>SH: Conceptualization, Formal analysis, Methodology, Visualization, Writing &#x2013; original draft, Writing &#x2013; review &#x0026; editing. AR: Data curation, Writing &#x2013; review &#x0026; editing. KM: Conceptualization, Funding acquisition, Methodology, Supervision, Writing &#x2013; review &#x0026; editing.</p>
</sec>
<sec sec-type="funding-information" id="sec21">
<title>Funding</title>
<p>The author(s) declare that financial support was received for the research, authorship, and/or publication of this article. The authors gratefully acknowledge support from the Stanford Doerr School of Sustainability Accelerator Program. AJR acknowledges support from the National Science Foundation Graduate Research Fellowship Program under Award DGE-1656518.</p>
</sec>
<sec sec-type="COI-statement" id="sec22">
<title>Conflict of interest</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 sec-type="ai-statement" id="sec23">
<title>Generative AI statement</title>
<p>The authors declare that no Generative AI was used in the creation of this manuscript.</p>
</sec>
<sec sec-type="disclaimer" id="sec24">
<title>Publisher&#x2019;s note</title>
<p>All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.</p>
</sec>
<sec sec-type="supplementary-material" id="sec25">
<title>Supplementary material</title>
<p>The Supplementary material for this article can be found online at: <ext-link xlink:href="https://www.frontiersin.org/articles/10.3389/fclim.2025.1505472/full#supplementary-material" ext-link-type="uri">https://www.frontiersin.org/articles/10.3389/fclim.2025.1505472/full#supplementary-material</ext-link></p>
<supplementary-material xlink:href="Data_Sheet_1.ZIP" id="SM1" mimetype="application/zip" xmlns:xlink="http://www.w3.org/1999/xlink"/>
<supplementary-material xlink:href="Data_Sheet_2.PDF" id="SM2" mimetype="application/pdf" xmlns:xlink="http://www.w3.org/1999/xlink"/>
</sec>
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