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<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Phys.</journal-id>
<journal-title>Frontiers in Physics</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Phys.</abbrev-journal-title>
<issn pub-type="epub">2296-424X</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="publisher-id">1595785</article-id>
<article-id pub-id-type="doi">10.3389/fphy.2025.1595785</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Physics</subject>
<subj-group>
<subject>Original Research</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Fermentation endpoint detection of Soybean using specially designed <inline-formula id="inf1">
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<mml:mi>d</mml:mi>
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</inline-formula>-coated FBG stress sensor</article-title>
<alt-title alt-title-type="left-running-head">Mirza et al.</alt-title>
<alt-title alt-title-type="right-running-head">
<ext-link ext-link-type="uri" xlink:href="https://doi.org/10.3389/fphy.2025.1595785">10.3389/fphy.2025.1595785</ext-link>
</alt-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname>Mirza</surname>
<given-names>Jawad</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/2659397/overview"/>
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<role content-type="https://credit.niso.org/contributor-roles/writing-original-draft/"/>
<role content-type="https://credit.niso.org/contributor-roles/Writing - review &#x26; editing/"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Atieh</surname>
<given-names>Ahmad</given-names>
</name>
<xref ref-type="aff" rid="aff3">
<sup>3</sup>
</xref>
<role content-type="https://credit.niso.org/contributor-roles/methodology/"/>
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<contrib contrib-type="author">
<name>
<surname>Kanwal</surname>
<given-names>Benish</given-names>
</name>
<xref ref-type="aff" rid="aff4">
<sup>4</sup>
</xref>
<role content-type="https://credit.niso.org/contributor-roles/conceptualization/"/>
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<contrib contrib-type="author">
<name>
<surname>Kanwal</surname>
<given-names>Firdos</given-names>
</name>
<xref ref-type="aff" rid="aff4">
<sup>4</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/2722659/overview"/>
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</contrib>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Aziz</surname>
<given-names>Imran</given-names>
</name>
<xref ref-type="aff" rid="aff4">
<sup>4</sup>
</xref>
<xref ref-type="aff" rid="aff5">
<sup>5</sup>
</xref>
<xref ref-type="corresp" rid="c001">&#x2a;</xref>
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<contrib contrib-type="author" corresp="yes">
<name>
<surname>Almogren</surname>
<given-names>Ahmad</given-names>
</name>
<xref ref-type="aff" rid="aff6">
<sup>6</sup>
</xref>
<xref ref-type="corresp" rid="c001">&#x2a;</xref>
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<aff id="aff1">
<sup>1</sup>
<institution>Electrical Engineering Department</institution>, <institution>HITEC University Taxila</institution>, <addr-line>Taxila</addr-line>, <country>Pakistan</country>
</aff>
<aff id="aff2">
<sup>2</sup>
<institution>SEECS Photonics Research Group</institution>, <addr-line>Islamabad</addr-line>, <country>Pakistan</country>
</aff>
<aff id="aff3">
<sup>3</sup>
<institution>Optiwave Systems Inc.</institution>, <addr-line>Ottawa</addr-line>, <addr-line>ON</addr-line>, <country>Canada</country>
</aff>
<aff id="aff4">
<sup>4</sup>
<institution>Electrical Engineering Department</institution>, <institution>Mirpur University of Science and Technology (MUST)</institution>, <addr-line>Mirpur</addr-line>, <country>Pakistan</country>
</aff>
<aff id="aff5">
<sup>5</sup>
<institution>Department of Physics and Astronomy</institution>, <institution>Uppsala University</institution>, <addr-line>Uppsala</addr-line>, <country>Sweden</country>
</aff>
<aff id="aff6">
<sup>6</sup>
<institution>Department of Computer Science</institution>, <institution>College of Computer and Information Sciences</institution>, <institution>King Saud University</institution>, <addr-line>Riyadh</addr-line>, <country>Saudi Arabia</country>
</aff>
<author-notes>
<fn fn-type="edited-by">
<p>
<bold>Edited by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/1184687/overview">Rajib Biswas</ext-link>, Tezpur University, India</p>
</fn>
<fn fn-type="edited-by">
<p>
<bold>Reviewed by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/993057/overview">Muhammad Ijaz</ext-link>, Manchester Metropolitan University, United Kingdom</p>
<p>
<ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/2406962/overview">Xiao Sun</ext-link>, Curtin University, Australia</p>
</fn>
<corresp id="c001">&#x2a;Correspondence: Imran Aziz, <email>imran.aziz@physics.uu.se</email>; Ahmad Almogren, <email>ahalmogren@ksu.edu.sa</email>
</corresp>
</author-notes>
<pub-date pub-type="epub">
<day>18</day>
<month>06</month>
<year>2025</year>
</pub-date>
<pub-date pub-type="collection">
<year>2025</year>
</pub-date>
<volume>13</volume>
<elocation-id>1595785</elocation-id>
<history>
<date date-type="received">
<day>18</day>
<month>03</month>
<year>2025</year>
</date>
<date date-type="accepted">
<day>26</day>
<month>05</month>
<year>2025</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2025 Mirza, Atieh, Kanwal, Kanwal, Aziz and Almogren.</copyright-statement>
<copyright-year>2025</copyright-year>
<copyright-holder>Mirza, Atieh, Kanwal, Kanwal, Aziz and Almogren</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>Determining the fermentation endpoint of organic compounds is critical for optimizing yield, ensuring the product consistency, and minimizing byproducts. However, conventional detection methods are slow, labor-intensive, and lack real-time monitoring, limiting their suitability for industrial automation. We propose a novel, non-destructive method for real-time detection of fermentation endpoint of Soybean using Palladium <inline-formula id="inf2">
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</mml:mrow>
<mml:mo stretchy="false">)</mml:mo>
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</inline-formula>-coated fiber Bragg grating (FBG) stress sensor. The fermentation endpoint can be detected by monitoring the shift in Bragg wavelength caused by the stress in <inline-formula id="inf3">
<mml:math id="m3">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
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</inline-formula>-coated FBG sensor due to the volume expansion of the <inline-formula id="inf4">
<mml:math id="m4">
<mml:mrow>
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</inline-formula> coating upon the formation of Palladium Hydride <inline-formula id="inf5">
<mml:math id="m5">
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>x</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
</mml:math>
</inline-formula> after Hydrogen <inline-formula id="inf6">
<mml:math id="m6">
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mrow>
<mml:msub>
<mml:mrow>
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</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
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</mml:mrow>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
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</inline-formula> gas absorption, which is released as a byproduct during Soybean fermentation. The <inline-formula id="inf7">
<mml:math id="m7">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
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</inline-formula>-coated FBG stress sensor is analytically designed and validated using OptiSystem simulation tool, achieving a high sensitivity of 61.6 p.m./MPa. Our findings confirm that this method provides a simple, efficient, and real-time solution for monitoring the fermentation process of organic compounds that produce <inline-formula id="inf8">
<mml:math id="m8">
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<mml:msub>
<mml:mrow>
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</inline-formula> offering significant advantages over traditional techniques.</p>
</abstract>
<kwd-group>
<kwd>fermentation endpoint</kwd>
<kwd>Soybean</kwd>
<kwd>Palladium</kwd>
<kwd>Hydrogen sensing</kwd>
<kwd>fiber Bragg grating</kwd>
<kwd>wavelength sensitivity</kwd>
<kwd>induced stress</kwd>
</kwd-group>
<custom-meta-wrap>
<custom-meta>
<meta-name>section-at-acceptance</meta-name>
<meta-value>Optics and Photonics</meta-value>
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</article-meta>
</front>
<body>
<sec id="s1">
<title>1 Introduction</title>
<p>Fermentation of organic compounds is a vital biochemical process with significant applications in food industry, biofuel generation, and biotechnology [<xref ref-type="bibr" rid="B1">1</xref>]. It involves the microbial metabolism of organic substrates such as carbohydrates into simpler compounds like alcohols, organic acids, and gases facilitated by bacteria, yeast, and fungi [<xref ref-type="bibr" rid="B1">1</xref>]. Detecting the fermentation endpoint is essential to ensure optimal yield, quality, and process efficiency [<xref ref-type="bibr" rid="B1">1</xref>]. For example, in the fermentation of Soybean into acetic acid, the process occurs in two stages [<xref ref-type="bibr" rid="B1">1</xref>, <xref ref-type="bibr" rid="B2">2</xref>]: the first is the hydrolysis of Soybean proteins and carbohydrates into simpler sugars and amino acids, followed by the oxidation of ethanol to acetic acid by acetic acid bacteria (AAB) such as <italic>acetobacter</italic> species. Accurate endpoint detection is crucial to prevent over-oxidation which could degrade acetic acid into carbon dioxide and water, compromising both quality and yield [<xref ref-type="bibr" rid="B2">2</xref>]. Advanced analytical techniques, including pH monitoring, gas chromatography, and high-performance liquid chromatography are commonly used to determine the fermentation endpoint and maintain the desired acetic acid concentration. Research emphasizes the importance of controlling factors like temperature, oxygen levels, and microbial activity to optimize the process [<xref ref-type="bibr" rid="B2">2</xref>, <xref ref-type="bibr" rid="B3">3</xref>]. Beyond enhancing the nutritional profile of Soy-based products, Soybean fermentation for acetic acid production also yields valuable ingredients for the food industry such as vinegar and condiments, showcasing the broader economic and nutritional significance of fermentation [<xref ref-type="bibr" rid="B2">2</xref>, <xref ref-type="bibr" rid="B3">3</xref>].</p>
<p>From an economic perspective, the production of acetic acid from Soybean&#x2019;s fermentation is highly valuable due to its applications in food, pharmaceuticals, and chemicals. This process is cost-effective compared to synthetic production as it utilizes natural source, thus reducing the energy consumption and production costs. The growing demand of acetic acid produced through natural sources has further boosted its market value. The global acetic acid market, valued at over $10 billion in 2022, is projected to grow, driven by its use in food processing, textiles, and biodegradable plastics [<xref ref-type="bibr" rid="B4">4</xref>]. Fermentation supports sustainability and creates economic opportunities for agricultural communities by utilizing local raw materials.</p>
</sec>
<sec id="s2">
<title>2 Related works</title>
<p>Determining the fermentation endpoint in Soybean processing is crucial for ensuring the product quality, maximizing yield, and avoiding over-fermentation which can result in unwanted byproducts. A range of traditional analytical techniques are utilized to identify when fermentation is complete. These methods include pH monitoring [<xref ref-type="bibr" rid="B5">5</xref>], gas chromatography (GC) [<xref ref-type="bibr" rid="B6">6</xref>], high-performance liquid chromatography (HPLC) [<xref ref-type="bibr" rid="B7">7</xref>], and Fourier transform infrared (FTIR) spectroscopy [<xref ref-type="bibr" rid="B8">8</xref>]. Analytical methods for fermentation endpoint detection often suffer from limitations such as time consuming sample preparation, high operational costs, potential contamination risks, and need for specialized equipment and expertise. Non-destructive, real-time, and online techniques for fermentation endpoint detection are essential to overcome the limitations of traditional analytical methods ensuring continuous monitoring and improved process efficiency. Various real-time techniques have been proposed to monitor the fermentation endpoint in different organic compounds. For example, monitoring the fermentation in dairy products using fluorescence spectroscopy [<xref ref-type="bibr" rid="B5">5</xref>], ultrasonic sensor [<xref ref-type="bibr" rid="B9">9</xref>], infrared light backscatter sensor [<xref ref-type="bibr" rid="B10">10</xref>], near-infrared (NIR) spectroscopy [<xref ref-type="bibr" rid="B11">11</xref>], monitoring the fermentation process in ethanol using viable cell sensor [<xref ref-type="bibr" rid="B12">12</xref>], monitoring the fermentation in yeast using software controlled automatic real-time biosensor [<xref ref-type="bibr" rid="B13">13</xref>], monitoring the fermentation process in Soybean using miniature fiber NIR spectrometer [<xref ref-type="bibr" rid="B14">14</xref>], monitoring the fermentation process in wine with benchtop 1H NMR spectroscopy [<xref ref-type="bibr" rid="B15">15</xref>] and NIR spectroscopy [<xref ref-type="bibr" rid="B16">16</xref>], and monitoring the fermentation process in black tea using an electronic tongue [<xref ref-type="bibr" rid="B17">17</xref>]. The literature review has been further elaborated in <xref ref-type="table" rid="T1">Table 1</xref> by comparing the important achievements of past studies with proposed work.</p>
<table-wrap id="T1" position="float">
<label>TABLE 1</label>
<caption>
<p>Elaboration of the literature survey and comparison with proposed work.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">Study</th>
<th align="left">Organic compound</th>
<th align="left">Technique</th>
<th align="left">Sensing type</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">[<xref ref-type="bibr" rid="B5">5</xref>]</td>
<td align="left">Yogurt</td>
<td align="left">Offline and destructive</td>
<td align="left">pH monitoring</td>
</tr>
<tr>
<td align="left">[<xref ref-type="bibr" rid="B6">6</xref>]</td>
<td align="left">Milk</td>
<td align="left">Offline and destructive</td>
<td align="left">Gas chromatography</td>
</tr>
<tr>
<td align="left">[<xref ref-type="bibr" rid="B7">7</xref>]</td>
<td align="left">Grapes</td>
<td align="left">Offline and destructive</td>
<td align="left">Liquid chromatography</td>
</tr>
<tr>
<td align="left">[<xref ref-type="bibr" rid="B8">8</xref>]</td>
<td align="left">Oat and pea</td>
<td align="left">Offline and destructive</td>
<td align="left">FTIR spectroscopy</td>
</tr>
<tr>
<td align="left">[<xref ref-type="bibr" rid="B9">9</xref>]</td>
<td align="left">Yogurt</td>
<td align="left">Online and non-destructive</td>
<td align="left">Ultrasonic measurement</td>
</tr>
<tr>
<td align="left">[<xref ref-type="bibr" rid="B10">10</xref>]</td>
<td align="left">Milk</td>
<td align="left">Online and non-destructive</td>
<td align="left">Light scattering</td>
</tr>
<tr>
<td align="left">[<xref ref-type="bibr" rid="B11">11</xref>]</td>
<td align="left">Yogurt</td>
<td align="left">Online and non-destructive</td>
<td align="left">NIR spectroscopy</td>
</tr>
<tr>
<td align="left">[<xref ref-type="bibr" rid="B12">12</xref>]</td>
<td align="left">Ethanol</td>
<td align="left">Online and non-destructive</td>
<td align="left">Cell sensor</td>
</tr>
<tr>
<td align="left">[<xref ref-type="bibr" rid="B13">13</xref>]</td>
<td align="left">Yeast</td>
<td align="left">Online and non-destructive</td>
<td align="left">Biosensor</td>
</tr>
<tr>
<td align="left">[<xref ref-type="bibr" rid="B14">14</xref>]</td>
<td align="left">Soybean</td>
<td align="left">Online and non-destructive</td>
<td align="left">NIR spectroscopy</td>
</tr>
<tr>
<td align="left">[<xref ref-type="bibr" rid="B15">15</xref>]</td>
<td align="left">Wine</td>
<td align="left">Online and non-destructive</td>
<td align="left">1H NMR spectroscopy</td>
</tr>
<tr>
<td align="left">[<xref ref-type="bibr" rid="B16">16</xref>]</td>
<td align="left">Wine</td>
<td align="left">Online and non-destructive</td>
<td align="left">NIR spectroscopy</td>
</tr>
<tr>
<td align="left">[<xref ref-type="bibr" rid="B17">17</xref>]</td>
<td align="left">Black tea</td>
<td align="left">Online and non-destructive</td>
<td align="left">Electronic tongue</td>
</tr>
<tr>
<td align="left">Proposed</td>
<td align="left">Soybean</td>
<td align="left">Online and non-destructive</td>
<td align="left">FBG sensing</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>We introduce a novel non-destructive approach for real-time detection of the Soybean fermentation endpoint using a <inline-formula id="inf9">
<mml:math id="m9">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula>-coated FBG stress sensor. This method detects fermentation completion by tracking the Bragg wavelength shift caused by stress in the <inline-formula id="inf10">
<mml:math id="m10">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula>-coated FBG sensor due to <inline-formula id="inf11">
<mml:math id="m11">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
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</inline-formula> coating expansion upon <inline-formula id="inf12">
<mml:math id="m12">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
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<mml:mi>x</mml:mi>
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</mml:msub>
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</inline-formula> formation after <inline-formula id="inf13">
<mml:math id="m13">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
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<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
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</inline-formula> absorption which is a key fermentation byproduct. The sensor is analytically designed and validated using OptiSystem simulation tool having a wavelength sensitivity of 61.6 p.m./MPa. This pioneering work establishes a new pathway for real-time monitoring of fermentation processes involving <inline-formula id="inf14">
<mml:math id="m14">
<mml:mrow>
<mml:msub>
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</inline-formula> production.</p>
</sec>
<sec id="s3">
<title>3 Modelling the fermentation process and working principle</title>
<p>To accurately model the fermentation process of Soybean and explain the working principle of the proposed method, it is important to estimate the total yield of <inline-formula id="inf15">
<mml:math id="m15">
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<mml:msub>
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<mml:mn>2</mml:mn>
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</mml:math>
</inline-formula> released as byproduct during fermentation process and the amount of stress induced on the <inline-formula id="inf16">
<mml:math id="m16">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula>-coated FBG sensor by volume expansion of the <inline-formula id="inf17">
<mml:math id="m17">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> coating due to the formation of <inline-formula id="inf18">
<mml:math id="m18">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>x</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> after absorption of <inline-formula id="inf19">
<mml:math id="m19">
<mml:mrow>
<mml:msub>
<mml:mi>H</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>, where <inline-formula id="inf20">
<mml:math id="m20">
<mml:mrow>
<mml:mi>x</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> is the ratio of Hydrogen to Palladium. The fermentation of Soybean involves microbial activity that degrades organic compounds, resulting in the production of <inline-formula id="inf21">
<mml:math id="m21">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> alongside other byproducts such as organic acids and carbon dioxide <inline-formula id="inf22">
<mml:math id="m22">
<mml:mrow>
<mml:mi>C</mml:mi>
<mml:msub>
<mml:mrow>
<mml:mi>O</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>. The fermentation process of soybean can be expressed by following chemical equation [<xref ref-type="bibr" rid="B18">18</xref>].<disp-formula id="e1">
<mml:math id="m23">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mtext>C</mml:mtext>
</mml:mrow>
<mml:mrow>
<mml:mn>6</mml:mn>
</mml:mrow>
</mml:msub>
<mml:msub>
<mml:mrow>
<mml:mtext>H</mml:mtext>
</mml:mrow>
<mml:mrow>
<mml:mn>12</mml:mn>
</mml:mrow>
</mml:msub>
<mml:msub>
<mml:mrow>
<mml:mtext>O</mml:mtext>
</mml:mrow>
<mml:mrow>
<mml:mn>6</mml:mn>
</mml:mrow>
</mml:msub>
<mml:mo>&#x2b;</mml:mo>
<mml:mn>2</mml:mn>
<mml:msub>
<mml:mrow>
<mml:mtext>H</mml:mtext>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
<mml:mtext>O</mml:mtext>
<mml:mo>&#x2192;</mml:mo>
<mml:mn>2</mml:mn>
<mml:msub>
<mml:mrow>
<mml:mtext>CH</mml:mtext>
</mml:mrow>
<mml:mrow>
<mml:mn>3</mml:mn>
</mml:mrow>
</mml:msub>
<mml:mtext>COOH</mml:mtext>
<mml:mo>&#x2b;</mml:mo>
<mml:mn>2</mml:mn>
<mml:msub>
<mml:mrow>
<mml:mtext>CO</mml:mtext>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
<mml:mo>&#x2b;</mml:mo>
<mml:mn>4</mml:mn>
<mml:msub>
<mml:mrow>
<mml:mtext>H</mml:mtext>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
<label>(1)</label>
</disp-formula>
</p>
<p>The <xref ref-type="disp-formula" rid="e1">Equation 1</xref> illustrates the fermentation process of Glucose <inline-formula id="inf23">
<mml:math id="m24">
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>C</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>6</mml:mn>
</mml:mrow>
</mml:msub>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>12</mml:mn>
</mml:mrow>
</mml:msub>
<mml:msub>
<mml:mrow>
<mml:mi>O</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>6</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
</mml:math>
</inline-formula> which is considered as a primary component in Soybean, into acetic acid <inline-formula id="inf24">
<mml:math id="m25">
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mrow>
<mml:mi>C</mml:mi>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>3</mml:mn>
</mml:mrow>
</mml:msub>
<mml:mi>C</mml:mi>
<mml:mi>O</mml:mi>
<mml:mi>O</mml:mi>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
</mml:math>
</inline-formula>, <inline-formula id="inf25">
<mml:math id="m26">
<mml:mrow>
<mml:mi>C</mml:mi>
<mml:msub>
<mml:mrow>
<mml:mi>O</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>, and <inline-formula id="inf26">
<mml:math id="m27">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>. From this equation, it is evident that 1 mol of <inline-formula id="inf27">
<mml:math id="m28">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>C</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>6</mml:mn>
</mml:mrow>
</mml:msub>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>12</mml:mn>
</mml:mrow>
</mml:msub>
<mml:msub>
<mml:mrow>
<mml:mi>O</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>6</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> produces 4 mol of <inline-formula id="inf28">
<mml:math id="m29">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>. Therefore, the total mass of <inline-formula id="inf29">
<mml:math id="m30">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> produced per kg of <inline-formula id="inf30">
<mml:math id="m31">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>C</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>6</mml:mn>
</mml:mrow>
</mml:msub>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>12</mml:mn>
</mml:mrow>
</mml:msub>
<mml:msub>
<mml:mrow>
<mml:mi>O</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>6</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> can be calculated by following steps.<disp-formula id="equ1">
<mml:math id="m32">
<mml:mrow>
<mml:mtable class="align-star" columnalign="left">
<mml:mtr>
<mml:mtd columnalign="right">
<mml:mtext>Molecular&#x2009;weight&#x2009;of&#x2009;</mml:mtext>
<mml:msub>
<mml:mrow>
<mml:mi>C</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>6</mml:mn>
</mml:mrow>
</mml:msub>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>12</mml:mn>
</mml:mrow>
</mml:msub>
<mml:msub>
<mml:mrow>
<mml:mi>O</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>6</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mtd>
<mml:mtd columnalign="left">
<mml:mo>&#x3d;</mml:mo>
<mml:mn>80</mml:mn>
<mml:mtext>&#x2009;&#x2009;g/mol</mml:mtext>
</mml:mtd>
</mml:mtr>
<mml:mtr>
<mml:mtd columnalign="right">
<mml:mtext>Molecular&#x2009;weight&#x2009;of&#x2009;</mml:mtext>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mtd>
<mml:mtd columnalign="left">
<mml:mo>&#x3d;</mml:mo>
<mml:mn>2</mml:mn>
<mml:mtext>&#x2009;&#x2009;g/mol</mml:mtext>
</mml:mtd>
</mml:mtr>
<mml:mtr>
<mml:mtd columnalign="right">
<mml:mtext>Mass&#x2009;of&#x2009;</mml:mtext>
<mml:mn>4</mml:mn>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mtd>
<mml:mtd columnalign="left">
<mml:mo>&#x3d;</mml:mo>
<mml:mn>4</mml:mn>
<mml:mo>&#xd7;</mml:mo>
<mml:mn>2</mml:mn>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>8</mml:mn>
<mml:mtext>&#x2009;g</mml:mtext>
</mml:mtd>
</mml:mtr>
</mml:mtable>
</mml:mrow>
</mml:math>
</disp-formula>
</p>
<p>Thus, 180 g of <inline-formula id="inf31">
<mml:math id="m33">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>C</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>6</mml:mn>
</mml:mrow>
</mml:msub>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>12</mml:mn>
</mml:mrow>
</mml:msub>
<mml:msub>
<mml:mrow>
<mml:mi>O</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>6</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>(1 mol) yields 8 g of <inline-formula id="inf32">
<mml:math id="m34">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>. The mass of <inline-formula id="inf33">
<mml:math id="m35">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> produced per kg of <inline-formula id="inf34">
<mml:math id="m36">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>C</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>6</mml:mn>
</mml:mrow>
</mml:msub>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>12</mml:mn>
</mml:mrow>
</mml:msub>
<mml:msub>
<mml:mrow>
<mml:mi>O</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>6</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> is calculated as.<disp-formula id="equ2">
<mml:math id="m37">
<mml:mrow>
<mml:mfrac>
<mml:mrow>
<mml:mn>8</mml:mn>
<mml:mtext>&#x2009;g</mml:mtext>
</mml:mrow>
<mml:mrow>
<mml:mn>180</mml:mn>
<mml:mtext>&#x2009;g</mml:mtext>
</mml:mrow>
</mml:mfrac>
<mml:mo>&#xd7;</mml:mo>
<mml:mn>1000</mml:mn>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>44.49</mml:mn>
<mml:mtext>&#x2009;g</mml:mtext>
</mml:mrow>
</mml:math>
</disp-formula>
</p>
<p>Therefore, 1 kg of <inline-formula id="inf35">
<mml:math id="m38">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>C</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>6</mml:mn>
</mml:mrow>
</mml:msub>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>12</mml:mn>
</mml:mrow>
</mml:msub>
<mml:msub>
<mml:mrow>
<mml:mi>O</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>6</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> produces approximately 44.49 g of <inline-formula id="inf36">
<mml:math id="m39">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>. As we have considered 5 kg Soybean in this research, therefore 222.5 g (<inline-formula id="inf37">
<mml:math id="m40">
<mml:mrow>
<mml:mo>&#x2248;</mml:mo>
</mml:mrow>
</mml:math>
</inline-formula>2.5 <inline-formula id="inf38">
<mml:math id="m41">
<mml:mrow>
<mml:msup>
<mml:mrow>
<mml:mi>m</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>3</mml:mn>
</mml:mrow>
</mml:msup>
</mml:mrow>
</mml:math>
</inline-formula>) of <inline-formula id="inf39">
<mml:math id="m42">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> gas is produced as byproduct during the fermentation process. To calculate the volume of <inline-formula id="inf40">
<mml:math id="m43">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> generated during fermentation at STP, we use the ideal gas law. At STP, the molar volume of an ideal gas is 22 L/mol. The molar mass of <inline-formula id="inf41">
<mml:math id="m44">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> is 2 g/mol, so for 222.5 g of <inline-formula id="inf42">
<mml:math id="m45">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>, the number of moles is calculated as:<disp-formula id="equ3">
<mml:math id="m46">
<mml:mrow>
<mml:mtext>Number&#x2009;of&#x2009;moles</mml:mtext>
<mml:mo>&#x3d;</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:mtext>Mass</mml:mtext>
</mml:mrow>
<mml:mrow>
<mml:mtext>Molar&#x2009;mass</mml:mtext>
</mml:mrow>
</mml:mfrac>
<mml:mo>&#x3d;</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:mn>222.5</mml:mn>
<mml:mtext>&#x2003;</mml:mtext>
<mml:mtext>g</mml:mtext>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
<mml:mtext>&#x2003;</mml:mtext>
<mml:mtext>g/mol</mml:mtext>
</mml:mrow>
</mml:mfrac>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>111.25</mml:mn>
<mml:mtext>&#x2009;</mml:mtext>
<mml:mtext>mol</mml:mtext>
<mml:mo>.</mml:mo>
</mml:mrow>
</mml:math>
</disp-formula>
</p>
<p>Using the molar volume of an ideal gas at STP, the volume of <inline-formula id="inf43">
<mml:math id="m47">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> gas is:<disp-formula id="equ4">
<mml:math display="block" id="m48">
<mml:mrow>
<mml:mtext>Volume</mml:mtext>
<mml:mo>&#x3d;</mml:mo>
<mml:mrow>
<mml:mtext>Number</mml:mtext>
<mml:mspace width=".2em"/>
<mml:mtext>of</mml:mtext>
<mml:mspace width=".2em"/>
<mml:mtext>moles</mml:mtext>
</mml:mrow>
<mml:mo>&#xd7;</mml:mo>
<mml:mrow>
<mml:mtext>Molar</mml:mtext>
<mml:mspace width=".2em"/>
<mml:mtext>volume</mml:mtext>
</mml:mrow>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>111.25</mml:mn>
<mml:mtext>&#x2009;</mml:mtext>
<mml:mtext>mol</mml:mtext>
<mml:mo>&#xd7;</mml:mo>
<mml:mn>22.4</mml:mn>
<mml:mtext>&#x2009;</mml:mtext>
<mml:mtext>L/mol</mml:mtext>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>2492</mml:mn>
<mml:mtext>&#x2009;</mml:mtext>
<mml:mtext>L</mml:mtext>
<mml:mo>.</mml:mo>
</mml:mrow>
</mml:math>
</disp-formula>
</p>
<p>Converting liters to cubic meters (since <inline-formula id="inf44">
<mml:math id="m49">
<mml:mrow>
<mml:mn>1</mml:mn>
<mml:mtext>&#x2009;</mml:mtext>
<mml:msup>
<mml:mrow>
<mml:mtext>m</mml:mtext>
</mml:mrow>
<mml:mrow>
<mml:mn>3</mml:mn>
</mml:mrow>
</mml:msup>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>1000</mml:mn>
<mml:mtext>&#x2009;</mml:mtext>
<mml:mtext>L</mml:mtext>
</mml:mrow>
</mml:math>
</inline-formula>), the volume of <inline-formula id="inf45">
<mml:math id="m50">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> generated at STP is:<disp-formula id="equ5">
<mml:math id="m51">
<mml:mrow>
<mml:mtext>Volume</mml:mtext>
<mml:mo>&#x3d;</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:mn>2492</mml:mn>
<mml:mtext>&#x2009;</mml:mtext>
<mml:mtext>L</mml:mtext>
</mml:mrow>
<mml:mrow>
<mml:mn>1000</mml:mn>
</mml:mrow>
</mml:mfrac>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>2.492</mml:mn>
<mml:mtext>&#x2009;</mml:mtext>
<mml:msup>
<mml:mrow>
<mml:mtext>m</mml:mtext>
</mml:mrow>
<mml:mrow>
<mml:mn>3</mml:mn>
</mml:mrow>
</mml:msup>
<mml:mo>.</mml:mo>
</mml:mrow>
</mml:math>
</disp-formula>
</p>
<p>To determine the stress induced in <inline-formula id="inf46">
<mml:math id="m52">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula>-coated FBG sensor when exposed to 222.5 g of <inline-formula id="inf47">
<mml:math id="m53">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>, first we need to consider the <inline-formula id="inf48">
<mml:math id="m54">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> absorption in <inline-formula id="inf49">
<mml:math id="m55">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> coating, saturation limit of <inline-formula id="inf50">
<mml:math id="m56">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>x</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> formation, and stress-strain relationship. Then we shall be able to calculate the shift in Bragg wavelength of FBG stress sensor.</p>
<sec id="s3-1">
<title>3.1 <inline-formula id="inf51">
<mml:math id="m57">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> absorption capacity of <inline-formula id="inf52">
<mml:math id="m58">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> and saturation limit of <inline-formula id="inf53">
<mml:math id="m59">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>x</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>
</title>
<p>
<xref ref-type="fig" rid="F1">Figure 1</xref> illustrates the fabrication of <inline-formula id="inf54">
<mml:math id="m60">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula>-coated FBG sensors which involves three critical steps. First, the FBG is inscribed in the core of single-mode fiber (SMF) using a UV laser as shown in <xref ref-type="fig" rid="F1">Figure 1a</xref> to create the periodic refractive index variation. Second, the fiber cladding is selectively etched using hydrofluoric acid to reduce the diameter exposing the core as shown in <xref ref-type="fig" rid="F1">Figure 1b</xref>. Finally, a uniform <inline-formula id="inf55">
<mml:math id="m61">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> layer of 50&#x2013;200 nm thickness is deposited either through sputtering or electroless plating as illustrated in <xref ref-type="fig" rid="F1">Figure 1c</xref>.</p>
<fig id="F1" position="float">
<label>FIGURE 1</label>
<caption>
<p>Important steps for <inline-formula id="inf56">
<mml:math id="m62">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> coating on FBG <bold>(a)</bold> FBG without etched cladding <bold>(b)</bold> FBG with etched cladding <bold>(c)</bold> Deposition of <inline-formula id="inf57">
<mml:math id="m63">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> coating alongwith adhesive layer.</p>
</caption>
<graphic xlink:href="fphy-13-1595785-g001.tif"/>
</fig>
<p>First of all, the reaction between <inline-formula id="inf58">
<mml:math id="m64">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> and <inline-formula id="inf59">
<mml:math id="m65">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> to form <inline-formula id="inf60">
<mml:math id="m66">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>x</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> is represented by <xref ref-type="disp-formula" rid="e2">Equation 2</xref> which is reversible equilibrium Equation 19.<disp-formula id="e2">
<mml:math id="m67">
<mml:mrow>
<mml:mtext>Pd</mml:mtext>
<mml:mo>&#x2b;</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:mi>x</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:mfrac>
<mml:msub>
<mml:mrow>
<mml:mtext>H</mml:mtext>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
<mml:mo>&#x2194;</mml:mo>
<mml:msub>
<mml:mrow>
<mml:mtext>PdH</mml:mtext>
</mml:mrow>
<mml:mrow>
<mml:mi>x</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
<label>(2)</label>
</disp-formula>
</p>
<p>The absorption of <inline-formula id="inf61">
<mml:math id="m68">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> in <inline-formula id="inf62">
<mml:math id="m69">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> occurs up to a maximum atomic ratio of <inline-formula id="inf63">
<mml:math id="m70">
<mml:mrow>
<mml:mfrac>
<mml:mrow>
<mml:mtext>H</mml:mtext>
</mml:mrow>
<mml:mrow>
<mml:mtext>Pd</mml:mtext>
</mml:mrow>
</mml:mfrac>
<mml:mo>&#x3d;</mml:mo>
<mml:mi>x</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>0.65</mml:mn>
</mml:mrow>
</mml:math>
</inline-formula> which represents the maximum saturation limit. This implies that while the total available amount of <inline-formula id="inf64">
<mml:math id="m71">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> may be around 222.5 g, <inline-formula id="inf65">
<mml:math id="m72">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> can only absorbs <inline-formula id="inf66">
<mml:math id="m73">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> up to its saturation. Consequently, stress development in <inline-formula id="inf67">
<mml:math id="m74">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> layer is confined to the period during which it becomes fully saturated with <inline-formula id="inf68">
<mml:math id="m75">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>. Once saturation is achieved, any excess <inline-formula id="inf69">
<mml:math id="m76">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> does not contribute to further stress development. It is also pertinent to mention that <inline-formula id="inf70">
<mml:math id="m77">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> absorption can be controlled to obtain the required value of <inline-formula id="inf71">
<mml:math id="m78">
<mml:mrow>
<mml:mi>x</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> either by reducing the <inline-formula id="inf72">
<mml:math id="m79">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> exposure time or using the <inline-formula id="inf73">
<mml:math id="m80">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> alloy with lower absorption capacity or using a buffer layer to limit the <inline-formula id="inf74">
<mml:math id="m81">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> expansion.</p>
</sec>
<sec id="s3-2">
<title>3.2 Calculation of stress developed in <inline-formula id="inf75">
<mml:math id="m82">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> coating</title>
<p>To calculate the stress induced in <inline-formula id="inf76">
<mml:math id="m83">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula>-coated FBG sensor, the following assumptions are crucial to consider.<list list-type="simple">
<list-item>
<p>&#x2022; Radii of the core and cladding are 4.6 <inline-formula id="inf77">
<mml:math id="m84">
<mml:mrow>
<mml:mi>&#x3bc;</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula>m and 62.5 <inline-formula id="inf78">
<mml:math id="m85">
<mml:mrow>
<mml:mi>&#x3bc;</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula>m, respectively.</p>
</list-item>
<list-item>
<p>&#x2022; Thickness of <inline-formula id="inf79">
<mml:math id="m86">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> layer over FBG sensor is 100 nm.</p>
</list-item>
<list-item>
<p>&#x2022; Thickness of adhesive layer of Titanium is 20 nm.</p>
</list-item>
<list-item>
<p>&#x2022; Saturation limit of 0.1 is considered.</p>
</list-item>
<list-item>
<p>&#x2022; The effect of temperature on Bragg wavelength shift is not considered in this research.</p>
</list-item>
</list>
</p>
<p>The strain induced in the <inline-formula id="inf80">
<mml:math id="m87">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> coating due to <inline-formula id="inf81">
<mml:math id="m88">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> absorption is given by the relation.<disp-formula id="e3">
<mml:math id="m89">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>&#x3b5;</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi mathvariant="italic">PdH</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>0.2</mml:mn>
<mml:mo>&#xd7;</mml:mo>
<mml:mi>x</mml:mi>
</mml:mrow>
</mml:math>
<label>(3)</label>
</disp-formula>In <xref ref-type="disp-formula" rid="e3">Equation 3</xref>, <inline-formula id="inf82">
<mml:math id="m90">
<mml:mrow>
<mml:mi>x</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> is the atomic ratio of <inline-formula id="inf83">
<mml:math id="m91">
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> to <inline-formula id="inf84">
<mml:math id="m92">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> and 0.2 is the empirical coefficient of expansion. At <inline-formula id="inf85">
<mml:math id="m93">
<mml:mrow>
<mml:mi>x</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>0.1</mml:mn>
</mml:mrow>
</mml:math>
</inline-formula>, the value of induced strain is <inline-formula id="inf86">
<mml:math id="m94">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>&#x3b5;</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi mathvariant="italic">PdH</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>0.2</mml:mn>
<mml:mo>&#xd7;</mml:mo>
<mml:mn>0.1</mml:mn>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>0.02</mml:mn>
</mml:mrow>
</mml:math>
</inline-formula>. Therefore, the stress in <inline-formula id="inf87">
<mml:math id="m95">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula>-coated FBG sensor due to <inline-formula id="inf88">
<mml:math id="m96">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> absorption is given by the following equation.<disp-formula id="e4">
<mml:math id="m97">
<mml:mrow>
<mml:mrow>
<mml:mi>&#x3c3;</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi mathvariant="italic">PdH</mml:mi>
</mml:mrow>
<mml:mo>&#x3d;</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>E</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
<mml:mrow>
<mml:mn>1</mml:mn>
<mml:mo>&#x2212;</mml:mo>
<mml:mrow>
<mml:mi>&#x3bd;</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:mrow>
</mml:mfrac>
<mml:mo>&#xd7;</mml:mo>
<mml:mrow>
<mml:mi>&#x3b5;</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi mathvariant="italic">PdH</mml:mi>
</mml:mrow>
</mml:mrow>
</mml:math>
<label>(4)</label>
</disp-formula>In <xref ref-type="disp-formula" rid="e4">Equation 4</xref>, <inline-formula id="inf89">
<mml:math id="m98">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>&#x3c3;</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi mathvariant="italic">PdH</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> is the stress induced in <inline-formula id="inf90">
<mml:math id="m99">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> due to <inline-formula id="inf91">
<mml:math id="m100">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> absorption, <inline-formula id="inf92">
<mml:math id="m101">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>E</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>12</mml:mn>
<mml:mo>&#xd7;</mml:mo>
<mml:mn>1</mml:mn>
<mml:msup>
<mml:mrow>
<mml:mn>0</mml:mn>
</mml:mrow>
<mml:mrow>
<mml:mn>9</mml:mn>
</mml:mrow>
</mml:msup>
</mml:mrow>
</mml:math>
</inline-formula> Pa is the Young&#x2019;s modulus of <inline-formula id="inf93">
<mml:math id="m102">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula>, and <inline-formula id="inf94">
<mml:math id="m103">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>&#x3bd;</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>0.39</mml:mn>
</mml:mrow>
</mml:math>
</inline-formula> is the Poisson&#x2019;s ratio of <inline-formula id="inf95">
<mml:math id="m104">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula>. Therefore, the value of stress at <inline-formula id="inf96">
<mml:math id="m105">
<mml:mrow>
<mml:mi>x</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>0.1</mml:mn>
</mml:mrow>
</mml:math>
</inline-formula> is around 393.44 MPa.</p>
</sec>
<sec id="s3-3">
<title>3.3 Effect of stress on Bragg wavelength shift</title>
<p>The shift in the Bragg wavelength <inline-formula id="inf97">
<mml:math id="m106">
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>&#x3bb;</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>B</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
</mml:math>
</inline-formula> of <inline-formula id="inf98">
<mml:math id="m107">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula>-coated FBG sensor due to axial strain after absorbing <inline-formula id="inf99">
<mml:math id="m108">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> is given by the equation [<xref ref-type="bibr" rid="B20">20</xref>].<disp-formula id="e5">
<mml:math id="m109">
<mml:mrow>
<mml:mi mathvariant="normal">&#x394;</mml:mi>
<mml:msub>
<mml:mrow>
<mml:mi>&#x3bb;</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>B</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:msub>
<mml:mrow>
<mml:mi>&#x3bb;</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>B</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mfenced open="(" close=")">
<mml:mrow>
<mml:mn>1</mml:mn>
<mml:mo>&#x2212;</mml:mo>
<mml:msub>
<mml:mrow>
<mml:mi>P</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>e</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:mfenced>
<mml:mo>&#x22c5;</mml:mo>
<mml:mi>&#x3b5;</mml:mi>
</mml:mrow>
</mml:math>
<label>(5)</label>
</disp-formula>where <inline-formula id="inf100">
<mml:math id="m110">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>P</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>e</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> is the effective photoelastic constant of the fiber (<inline-formula id="inf101">
<mml:math id="m111">
<mml:mrow>
<mml:mo>&#x2248;</mml:mo>
</mml:mrow>
</mml:math>
</inline-formula>0.22 for silica fibers), <inline-formula id="inf102">
<mml:math id="m112">
<mml:mrow>
<mml:mi>&#x3b5;</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> is the strain in the FBG sensor (<inline-formula id="inf103">
<mml:math id="m113">
<mml:mrow>
<mml:mo>&#x2248;</mml:mo>
</mml:mrow>
</mml:math>
</inline-formula>0.02 at saturation), and <inline-formula id="inf104">
<mml:math id="m114">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>&#x3bb;</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>B</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> is the initial Bragg wavelength (typically <inline-formula id="inf105">
<mml:math id="m115">
<mml:mrow>
<mml:mo>&#x2248;</mml:mo>
</mml:mrow>
</mml:math>
</inline-formula>1,550 nm). Applying these values in <xref ref-type="disp-formula" rid="e5">Equation 5</xref>, the shift in Bragg wavelength <inline-formula id="inf106">
<mml:math id="m116">
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mrow>
<mml:mi mathvariant="normal">&#x394;</mml:mi>
<mml:msub>
<mml:mrow>
<mml:mi>&#x3bb;</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>B</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
</mml:math>
</inline-formula> is around 24.2 nm. This is the maximum shift in the Bragg wavelength, which corresponds to a stress of 393.44 MPa induced in FBG sensor when exposed to 222.5 g of <inline-formula id="inf107">
<mml:math id="m117">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> that is released during the fermentation process.</p>
<p>The Bragg wavelength shift of 24.2 nm serves as a key indicator for detecting the fermentation endpoint in Soybean processing. This shift results from the stress-induced expansion of the <inline-formula id="inf108">
<mml:math id="m118">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> coating on the FBG sensor due to <inline-formula id="inf109">
<mml:math id="m119">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> absorption and the subsequent formation of <inline-formula id="inf110">
<mml:math id="m120">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>x</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>. Since <inline-formula id="inf111">
<mml:math id="m121">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> is a byproduct of soybean fermentation, the observed wavelength shift directly correlates with the completion of the fermentation process.</p>
</sec>
</sec>
<sec id="s4">
<title>4 Design validation of <inline-formula id="inf112">
<mml:math id="m122">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula>-coated FBG stress sensor using OptiSystem</title>
<p>The analytical model of the <inline-formula id="inf113">
<mml:math id="m123">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula>-coated FBG stress sensor that is developed in the last section produces a Bragg wavelength shift of 24.2 nm is analyzed using OptiSystem simulation tool. <xref ref-type="table" rid="T2">Table 2</xref> compares the parameters used in the analytical model with those employed in OptiSystem for design analysis. Using the parameters of the OptiSystem model, a shift of 24.5 nm in Bragg wavelength is achieved which is comparable to the analytical model making the assumption reasonable.</p>
<table-wrap id="T2" position="float">
<label>TABLE 2</label>
<caption>
<p>Comparison of parameters for the analytical model and OptiSystem analysis of the <inline-formula id="inf114">
<mml:math id="m124">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula>-coated FBG stress sensor.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">Sr. No</th>
<th align="left">Parameters</th>
<th align="left">Numerical model</th>
<th align="left">OptiSystem model</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">1</td>
<td align="left">Initial Bragg wavelength</td>
<td align="left">1,550 nm</td>
<td align="left">1,550 nm</td>
</tr>
<tr>
<td align="left">2</td>
<td align="left">Core radius</td>
<td align="left">4.6 <inline-formula id="inf115">
<mml:math id="m125">
<mml:mrow>
<mml:mi>&#x3bc;</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula>m</td>
<td align="left">4.6 <inline-formula id="inf116">
<mml:math id="m126">
<mml:mrow>
<mml:mi>&#x3bc;</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula>m</td>
</tr>
<tr>
<td align="left">3</td>
<td align="left">Cladding radius</td>
<td align="left">62.5 <inline-formula id="inf117">
<mml:math id="m127">
<mml:mrow>
<mml:mi>&#x3bc;</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula>m</td>
<td align="left">62.5 <inline-formula id="inf118">
<mml:math id="m128">
<mml:mrow>
<mml:mi>&#x3bc;</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula>m</td>
</tr>
<tr>
<td align="left">4</td>
<td align="left">Thickness of <inline-formula id="inf119">
<mml:math id="m129">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> layer</td>
<td align="left">100 nm</td>
<td align="left">100 nm</td>
</tr>
<tr>
<td align="left">5</td>
<td align="left">Young&#x2019;s modulus of <inline-formula id="inf120">
<mml:math id="m130">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula>
</td>
<td align="left">1,200 MPa</td>
<td align="left">1,200 MPa</td>
</tr>
<tr>
<td align="left">6</td>
<td align="left">Poisson&#x2019;s ratio of <inline-formula id="inf121">
<mml:math id="m131">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula>
</td>
<td align="left">0.39</td>
<td align="left">0.2</td>
</tr>
<tr>
<td align="left">7</td>
<td align="left">Photoelastic constant of the Silica fiber</td>
<td align="left">0.22</td>
<td align="left">0.9</td>
</tr>
</tbody>
</table>
</table-wrap>
</sec>
<sec id="s5">
<title>5 Simulation setup</title>
<p>
<xref ref-type="fig" rid="F2">Figure 2</xref> shows the block diagram of the simulation setup designed in OptiSystem to detect the fermentation endpoint of Soybean. A white light source (WLS) with a power spectral density (PSD) and center wavelength of &#x2212;60 dBm/Hz and 1,551 nm, respectively is used to illuminate the FBG stress sensor. <xref ref-type="fig" rid="F3">Figure 3</xref> illustrates the spectrum of WLS. The WLS model used in OptiSystem generates noise bins or sampled signals at the output according to the following mathematical expression.<disp-formula id="e6">
<mml:math id="m132">
<mml:mrow>
<mml:mfenced open="[" close="]">
<mml:mrow>
<mml:mtable class="matrix">
<mml:mtr>
<mml:mtd columnalign="center">
<mml:msub>
<mml:mrow>
<mml:mi>E</mml:mi>
</mml:mrow>
<mml:mrow>
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</mml:mrow>
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<mml:mrow>
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</mml:mrow>
</mml:mfenced>
</mml:mtd>
</mml:mtr>
<mml:mtr>
<mml:mtd columnalign="center">
<mml:msub>
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<mml:mi>E</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>y</mml:mi>
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</mml:msub>
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</mml:mfenced>
</mml:mtd>
</mml:mtr>
</mml:mtable>
</mml:mrow>
</mml:mfenced>
<mml:mo>&#x3d;</mml:mo>
<mml:mfenced open="[" close="]">
<mml:mrow>
<mml:mtable class="matrix">
<mml:mtr>
<mml:mtd columnalign="center">
<mml:msub>
<mml:mrow>
<mml:mi>x</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>x</mml:mi>
</mml:mrow>
</mml:msub>
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<mml:mrow>
<mml:mi>t</mml:mi>
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</mml:mfenced>
<mml:mo>&#x2b;</mml:mo>
<mml:mi>j</mml:mi>
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<mml:mrow>
<mml:mi>y</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>x</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mfenced open="(" close=")">
<mml:mrow>
<mml:mi>t</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mtd>
</mml:mtr>
<mml:mtr>
<mml:mtd columnalign="center">
<mml:msub>
<mml:mrow>
<mml:mi>x</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>y</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mfenced open="(" close=")">
<mml:mrow>
<mml:mi>t</mml:mi>
</mml:mrow>
</mml:mfenced>
<mml:mo>&#x2b;</mml:mo>
<mml:mi>j</mml:mi>
<mml:msub>
<mml:mrow>
<mml:mi>y</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>y</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mfenced open="(" close=")">
<mml:mrow>
<mml:mi>t</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mtd>
</mml:mtr>
</mml:mtable>
</mml:mrow>
</mml:mfenced>
<mml:mo>&#x22c5;</mml:mo>
<mml:msqrt>
<mml:mrow>
<mml:mfrac>
<mml:mrow>
<mml:mi>P</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>4</mml:mn>
</mml:mrow>
</mml:mfrac>
</mml:mrow>
</mml:msqrt>
</mml:mrow>
</mml:math>
<label>(6)</label>
</disp-formula>In <xref ref-type="disp-formula" rid="e6">Equation 6</xref>, <inline-formula id="inf122">
<mml:math id="m133">
<mml:mrow>
<mml:mi>E</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> is the optical field and <inline-formula id="inf123">
<mml:math id="m134">
<mml:mrow>
<mml:mi>P</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> is average power. In the above equation, a Gaussian distribution has been assumed to describe the probability density function (PDF) for the real and imaginary parts of the optical field components <inline-formula id="inf124">
<mml:math id="m135">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>E</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>x</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> and <inline-formula id="inf125">
<mml:math id="m136">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>E</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>y</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>. A broadband light source is essential for FBG sensors because it provides a wide spectral range to accurately track the shifts in Bragg wavelength caused by external perturbations [<xref ref-type="bibr" rid="B21">21</xref>]. Unlike narrowband lasers that require fast scanning to avoid missing signal detection, WLS enables high-resolution detection of small wavelength changes which are critical for real-time monitoring in applications like <inline-formula id="inf126">
<mml:math id="m137">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula>-coated FBG stress sensor [<xref ref-type="bibr" rid="B21">21</xref>]. Additionally, broadband light sources support multiplexing of multiple FBGs on a single fiber, making it ideal for scalable industrial systems. Its stable and noise-resistant output ensures reliable measurement of stress-induced shifts which are vital for precise fermentation endpoint detection [<xref ref-type="bibr" rid="B21">21</xref>]. In practical scenario, the <inline-formula id="inf127">
<mml:math id="m138">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula>-coated FBG stress sensor will be placed inside the fermentation container holding 5 kg of Soybean with a suitable microbial culture to initiate the fermentation process. The temperature, humidity, and pressure inside the container is controlled to ensure optimal fermentation conditions. The <inline-formula id="inf128">
<mml:math id="m139">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> layer serves as the active sensing material, absorbing <inline-formula id="inf129">
<mml:math id="m140">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> molecules released during fermentation. Upon absorption, <inline-formula id="inf130">
<mml:math id="m141">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> undergoes a phase transition to <inline-formula id="inf131">
<mml:math id="m142">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>x</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>, leading to volumetric expansion which induces mechanical strain inside the FBG sensor. This strain modifies the grating period of the FBG, causing a Bragg wavelength shift which serves as an indicator of the fermentation endpoint. In OptiSystem, this process is realized using the numerical values of stress calculated in <xref ref-type="sec" rid="s3">Section 3</xref> to create the corresponding shift in Bragg wavelength of stress sensor. The optical signal reflected from the FBG stress sensor at a shifted Bragg wavelength corresponding to the applied stress, is split into two parts using a 20:80 power splitter (PS) attached to the sensor&#x2019;s reflection port (RP). The 20% output of the PS is sent to an optical spectrum analyzer (OSA) for analysis of the results while the 80% output is connected to the alarm system (AS) for annunciation of the fermentation endpoint. Similarly, the transmitted spectrum is directed to another OSA via the transmission port (TP) for analysis. The important simulation parameters used in this work are described in <xref ref-type="table" rid="T3">Table 3</xref>.</p>
<fig id="F2" position="float">
<label>FIGURE 2</label>
<caption>
<p>Block diagram of the sensor setup designed in Optisystem. WLS: White light source, FBG: Fiber Bragg grating stress sensor, PS: Power splitter, OSA: Optical spectrum analyzer, AS: Alam system.</p>
</caption>
<graphic xlink:href="fphy-13-1595785-g002.tif"/>
</fig>
<fig id="F3" position="float">
<label>FIGURE 3</label>
<caption>
<p>Spectral plot of WLS centered at 1551 nm.</p>
</caption>
<graphic xlink:href="fphy-13-1595785-g003.tif"/>
</fig>
<table-wrap id="T3" position="float">
<label>TABLE 3</label>
<caption>
<p>List of simulation parameters.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">Sr. No</th>
<th align="left">Parameters</th>
<th align="left">Values</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">1</td>
<td align="left">Operating wavelength of WLS</td>
<td align="left">1,551 nm</td>
</tr>
<tr>
<td align="left">2</td>
<td align="left">Initial Bragg wavelength of FBG</td>
<td align="left">1,550 nm</td>
</tr>
<tr>
<td align="left">3</td>
<td align="left">Power spectral density of WLS</td>
<td align="left">&#x2212;60 dBm/Hz</td>
</tr>
<tr>
<td align="left">4</td>
<td align="left">Effective index of FBG</td>
<td align="left">1.45</td>
</tr>
<tr>
<td align="left">5</td>
<td align="left">Grating length</td>
<td align="left">10 mm</td>
</tr>
<tr>
<td align="left">6</td>
<td align="left">Resolution bandwidth of OSA</td>
<td align="left">0.1 nm</td>
</tr>
<tr>
<td align="left">7</td>
<td align="left">Sequence length</td>
<td align="left">1,024 bits</td>
</tr>
<tr>
<td align="left">8</td>
<td align="left">Samples per bit</td>
<td align="left">512</td>
</tr>
</tbody>
</table>
</table-wrap>
</sec>
<sec sec-type="results|discussion" id="s6">
<title>6 Results and discussion</title>
<p>
<xref ref-type="fig" rid="F4">Figure 4</xref> illustrates the induced stress due to formation of <inline-formula id="inf132">
<mml:math id="m143">
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</inline-formula> by <inline-formula id="inf134">
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<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula>-coated FBG sensor versus wavelength shift. It is clear that wavelength sensitivity of 61.6 p.m./MPa has been achieved. A linear relationship between the wavelength shift and induced stress can be observed. The reason of linear relationship between the wavelength shift and the stress shown in <xref ref-type="fig" rid="F4">Figure 4</xref> is attributed to the fundamental principle of opto-mechanical coupling as expressed in <xref ref-type="disp-formula" rid="e5">Equation 5</xref>. We acknowledge that practical scenarios may introduce noise and nonlinearities due to thermal fluctuations, mechanical vibrations, material hysteresis, and deformations in the <inline-formula id="inf135">
<mml:math id="m146">
<mml:mrow>
<mml:mi>P</mml:mi>
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</inline-formula> coating which can affect wavelength shift and resolution. However, the reported sensitivity threshold of 61.6 p.m./MPa sets a floor for the FBG interrogators. <xref ref-type="fig" rid="F5">Figure 5a</xref> shows the transmission spectra of the FBG sensor for stress values of 0 MPa and 393.44 MPa obtained by connecting the OSA to TP of FBG stress sensor as illustrated in <xref ref-type="fig" rid="F2">Figure 2</xref>. Similarly, <xref ref-type="fig" rid="F5">Figure 5b</xref> shows the reflection spectra of FBG the sensor for stress values of 0 MPa and 393.44 MPa indicating the onset and endpoint of fermentation process, respectively. Reflection spectra is obtained by connecting the OSA with 20% output of the PS, that is connected with RP of the FBG stress sensor as shown in <xref ref-type="fig" rid="F2">Figure 2</xref>. Assuming the fermentation starts at time <inline-formula id="inf136">
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</mml:msub>
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</inline-formula>, the transmission dip and the reflection peak of the transmitted and reflected optical signals, respectively equal to the initial Bragg wavelength of <inline-formula id="inf137">
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<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula>-coated FBG sensor which is 1,550 nm, as shown in <xref ref-type="fig" rid="F5">Figure 5</xref> corresponding to the absence of detectable <inline-formula id="inf138">
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</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>. As fermentation process progresses, microbial activity produces <inline-formula id="inf139">
<mml:math id="m150">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> which is absorbed by the <inline-formula id="inf140">
<mml:math id="m151">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> coating forming <inline-formula id="inf141">
<mml:math id="m152">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>x</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>. This induces stress in the <inline-formula id="inf142">
<mml:math id="m153">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula>-coated FBG stress sensor, linearly shifting the Bragg wavelength of reflected optical signal. Similarly, the fermentation endpoint is achieved at time <inline-formula id="inf143">
<mml:math id="m154">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>t</mml:mi>
</mml:mrow>
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<mml:mi>e</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>. Consequently, the absorption of <inline-formula id="inf144">
<mml:math id="m155">
<mml:mrow>
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<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> in <inline-formula id="inf145">
<mml:math id="m156">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> coating saturates and any excess <inline-formula id="inf146">
<mml:math id="m157">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> will not contribute to further stress development. The transmission dip and reflection peak of transmitted and reflected optical signals equal to 1,574.5 nm. A maximum shift of 24.5 nm in Bragg wavelength corresponding to a stress of 393.44 MPa is induced in FBG sensor indicating the fermentation endpoint.</p>
<fig id="F4" position="float">
<label>FIGURE 4</label>
<caption>
<p>Induced stress versus wavelength shift plot.</p>
</caption>
<graphic xlink:href="fphy-13-1595785-g004.tif"/>
</fig>
<fig id="F5" position="float">
<label>FIGURE 5</label>
<caption>
<p>
<bold>(a)</bold> Transmission spectra of FBG stress sensor <bold>(b)</bold> Reflection spectra of FBG stress sensor.</p>
</caption>
<graphic xlink:href="fphy-13-1595785-g005.tif"/>
</fig>
</sec>
<sec sec-type="conclusion" id="s7">
<title>7 Conclusion</title>
<p>In this study, we demonstrated a non-destructive and real-time method for detecting the fermentation endpoint of Soybeans using a <inline-formula id="inf147">
<mml:math id="m158">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula>-coated fiber Bragg grating stress sensor. The method relies on monitoring the shift in the Bragg wavelength, which is caused by the stress induced in the <inline-formula id="inf148">
<mml:math id="m159">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula>-coated FBG sensor due to the volume expansion of the Palladium layer upon the formation of Palladium Hydride after absorbing Hydrogen gas released as a byproduct during the fermentation of Soybeans. The <inline-formula id="inf149">
<mml:math id="m160">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula>-coated fiber Bragg grating sensor was analytically designed and its performance was analyzed using the OptiSystem simulation tool, achieving a wavelength sensitivity of 61.6 p.m./MPa. The results demonstrate that the proposed method provides a reliable, straightforward, and efficient solution for real-time monitoring and detection of the fermentation endpoint of various organic compounds that release Hydrogen gas as a byproduct. This approach holds significant potential for applications in food processing, biotechnology, and industrial fermentation processes.</p>
</sec>
</body>
<back>
<sec sec-type="data-availability" id="s8">
<title>Data availability statement</title>
<p>The raw data supporting the conclusions of this article will be made available by the authors, without undue reservation.</p>
</sec>
<sec sec-type="author-contributions" id="s9">
<title>Author contributions</title>
<p>JM: Conceptualization, Project administration, Software, Validation, Writing &#x2013; original draft, Writing &#x2013; review and editing. AA: Methodology, Writing &#x2013; review and editing. BK: Conceptualization, Investigation, Writing &#x2013; original draft. FK: Investigation, Methodology, Software, Writing &#x2013; original draft. IA: Funding acquisition, Resources, Software, Writing &#x2013; original draft, Writing &#x2013; review and editing. AA: Resources, Software, Writing &#x2013; original draft. </p>
</sec>
<sec sec-type="funding-information" id="s10">
<title>Funding</title>
<p>The author(s) declare that financial support was received for the research and/or publication of this article.</p>
</sec>
<ack>
<p>This work was supported by King Saud University, Riyadh, Saudi Arabia, through ongoing research funding program (ORF-2025-184).</p>
</ack>
<sec sec-type="COI-statement" id="s11">
<title>Conflict of interest</title>
<p>Author AA was employed by Optiwave Systems Inc.</p>
<p>The remaining 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="s12">
<title>Generative AI statement</title>
<p>The author(s) declare that no Generative AI was used in the creation of this manuscript.</p>
</sec>
<sec sec-type="disclaimer" id="s13">
<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>
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