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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Pain Res.</journal-id>
<journal-title>Frontiers in Pain Research</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Pain Res.</abbrev-journal-title>
<issn pub-type="epub">2673-561X</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="doi">10.3389/fpain.2025.1526277</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Pain Research</subject>
<subj-group>
<subject>Original Research</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>The interplay between pulse width and activation depth in TENS: a computational study</article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author" equal-contrib="yes"><name><surname>Guillen</surname><given-names>Alexander</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<xref ref-type="author-notes" rid="an1"><sup>&#x2020;</sup></xref><uri xlink:href="https://loop.frontiersin.org/people/2215644/overview"/><role content-type="https://credit.niso.org/contributor-roles/data-curation/"/><role content-type="https://credit.niso.org/contributor-roles/formal-analysis/"/><role content-type="https://credit.niso.org/contributor-roles/investigation/"/><role content-type="https://credit.niso.org/contributor-roles/methodology/"/><role content-type="https://credit.niso.org/contributor-roles/software/"/><role content-type="https://credit.niso.org/contributor-roles/validation/"/><role content-type="https://credit.niso.org/contributor-roles/visualization/"/><role content-type="https://credit.niso.org/contributor-roles/writing-original-draft/"/><role content-type="https://credit.niso.org/contributor-roles/writing-review-editing/"/></contrib>
<contrib contrib-type="author" equal-contrib="yes"><name><surname>Truong</surname><given-names>Dennis Q.</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<xref ref-type="author-notes" rid="an1"><sup>&#x2020;</sup></xref><role content-type="https://credit.niso.org/contributor-roles/data-curation/"/><role content-type="https://credit.niso.org/contributor-roles/formal-analysis/"/><role content-type="https://credit.niso.org/contributor-roles/investigation/"/><role content-type="https://credit.niso.org/contributor-roles/methodology/"/><role content-type="https://credit.niso.org/contributor-roles/software/"/><role content-type="https://credit.niso.org/contributor-roles/supervision/"/><role content-type="https://credit.niso.org/contributor-roles/validation/"/><role content-type="https://credit.niso.org/contributor-roles/visualization/"/><role content-type="https://credit.niso.org/contributor-roles/writing-review-editing/"/></contrib>
<contrib contrib-type="author"><name><surname>Cakmak</surname><given-names>Yusuf O.</given-names></name>
<xref ref-type="aff" rid="aff2"><sup>2</sup></xref><uri xlink:href="https://loop.frontiersin.org/people/373562/overview" /><role content-type="https://credit.niso.org/contributor-roles/supervision/"/><role content-type="https://credit.niso.org/contributor-roles/validation/"/><role content-type="https://credit.niso.org/contributor-roles/writing-review-editing/"/></contrib>
<contrib contrib-type="author"><name><surname>Li</surname><given-names>Sheng</given-names></name>
<xref ref-type="aff" rid="aff3"><sup>3</sup></xref><uri xlink:href="https://loop.frontiersin.org/people/144849/overview" /><role content-type="https://credit.niso.org/contributor-roles/supervision/"/><role content-type="https://credit.niso.org/contributor-roles/validation/"/><role content-type="https://credit.niso.org/contributor-roles/writing-review-editing/"/></contrib>
<contrib contrib-type="author" corresp="yes"><name><surname>Datta</surname><given-names>Abhishek</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<xref ref-type="aff" rid="aff4"><sup>4</sup></xref>
<xref ref-type="corresp" rid="cor1">&#x002A;</xref><uri xlink:href="https://loop.frontiersin.org/people/47249/overview" /><role content-type="https://credit.niso.org/contributor-roles/conceptualization/"/><role content-type="https://credit.niso.org/contributor-roles/formal-analysis/"/><role content-type="https://credit.niso.org/contributor-roles/funding-acquisition/"/><role content-type="https://credit.niso.org/contributor-roles/investigation/"/><role content-type="https://credit.niso.org/contributor-roles/methodology/"/><role content-type="https://credit.niso.org/contributor-roles/project-administration/"/><role content-type="https://credit.niso.org/contributor-roles/resources/"/><role content-type="https://credit.niso.org/contributor-roles/software/"/><role content-type="https://credit.niso.org/contributor-roles/supervision/"/><role content-type="https://credit.niso.org/contributor-roles/validation/"/><role content-type="https://credit.niso.org/contributor-roles/visualization/"/><role content-type="https://credit.niso.org/contributor-roles/writing-original-draft/"/><role content-type="https://credit.niso.org/contributor-roles/writing-review-editing/"/></contrib>
</contrib-group>
<aff id="aff1"><label><sup>1</sup></label><institution>Research and Development, Soterix Medical</institution>, <addr-line>Woodbridge, NJ</addr-line>, <country>United States</country></aff>
<aff id="aff2"><label><sup>2</sup></label><institution>Department of Anatomy, University of Otago</institution>, <addr-line>Dunedin</addr-line>, <country>New Zealand</country></aff>
<aff id="aff3"><label><sup>3</sup></label><institution>Department of Physical Medicine and Rehabilitation, McGovern Medical School at The University of Texas Health Science Center at Houston</institution>, <addr-line>Houston, TX</addr-line>, <country>United States</country></aff>
<aff id="aff4"><label><sup>4</sup></label><institution>Biomedical Engineering, City College of New York</institution>, <addr-line>New York, NY</addr-line>, <country>United States</country></aff>
<author-notes>
<fn fn-type="edited-by"><p><bold>Edited by:</bold> Maral Tajerian, Queens College (CUNY), United States</p></fn>
<fn fn-type="edited-by"><p><bold>Reviewed by:</bold> Giovanni Berardi, The University of Iowa, United States</p>
<p>Riccardo Collu, University of Cagliari, Italy</p>
<p>Tiantian Guo, The University of Chicago, United States</p></fn>
<corresp id="cor1"><label>&#x002A;</label><bold>Correspondence:</bold> Abhishek Datta <email>adatta@soterixmedical.com</email></corresp>
<fn fn-type="equal" id="an1"><label><sup>&#x2020;</sup></label><p>These authors have contributed equally to this work</p></fn>
</author-notes>
<pub-date pub-type="epub"><day>17</day><month>04</month><year>2025</year></pub-date>
<pub-date pub-type="collection"><year>2025</year></pub-date>
<volume>6</volume><elocation-id>1526277</elocation-id>
<history>
<date date-type="received"><day>11</day><month>11</month><year>2024</year></date>
<date date-type="accepted"><day>31</day><month>03</month><year>2025</year></date>
</history>
<permissions>
<copyright-statement>&#x00A9; 2025 Guillen, Truong, Cakmak, Li and Datta.</copyright-statement>
<copyright-year>2025</copyright-year><copyright-holder>Guillen, Truong, Cakmak, Li and Datta</copyright-holder><license license-type="open-access" xlink:href="http://creativecommons.org/licenses/by/4.0/">
<p>This is an open-access article distributed under the terms of the <ext-link ext-link-type="uri" xlink:href="http://creativecommons.org/licenses/by/4.0/">Creative Commons Attribution License (CC BY)</ext-link>. 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><sec><title>Background</title>
<p>Transcutaneous electrical nerve stimulation (TENS) has been a commonly used modality to relieve aches and pain for over 40 years. Commercially available devices provide multiple therapy modes involving a different combination of frequency and pulse width with intensity. While frequency sets sensation, intensity helps determine tolerability, longer pulse width is reported to induce a feeling of deeper stimulation. In fact, longer pulse width has been empirically shown to deliver current into deeper tissues, but in context of other electrical stimulation modalities. The goal of this study was to unpack the relationship between pulse width and activation depth in TENS.</p>
</sec><sec><title>Methods</title>
<p>A highly realistic, anatomically-based, 3D finite element model of the forearm was used to simulate the electric field (E-field) distribution, as the pulse width is varied. A typical titration-guided mechanism was used to obtain the strength-duration (S-D) curves of a sensory McIntyre-Richardson-Grill (MRG) axonal model simulating the pain-transmitting A-delta fibers. The pulse widths tested ranged from 30&#x2005;&#x03BC;s to 495&#x2005;&#x03BC;s.</p>
</sec><sec><title>Results</title>
<p>As expected, shorter pulse widths required more current to achieve activation, resulting in a larger E-field. The S-D curve of the target median nerve indicates a rheobase of 1.75&#x2005;mA and a chronaxie of 232&#x2005;&#x00B5;s. When the applied currents are the same, shorter pulse widths result in a smaller volume of tissue activated (VTA) compared to the longer pulse widths. A 21 fold difference in VTA was found between the longest and shortest pulse widths considered. For the conditions tested in the study, an increase in pulse width resulted in an increase in activation depth, exhibiting a linear relationship.</p>
</sec><sec><title>Conclusion</title>
<p>Our findings highlight the impact of pulse width on activation depth. While choice of a given therapy mode is usually based on an <italic>ad-hoc</italic> desirable sensation basis, medical professionals may consider advocating a certain therapy mode based on the depth of the intended target nerve.</p>
</sec>
</abstract>
<kwd-group>
<kwd>transcutaneous electrical nerve stimulation</kwd>
<kwd>TENS</kwd>
<kwd>chronic pain</kwd>
<kwd>simulation</kwd>
<kwd>arm model</kwd>
<kwd>pulse width</kwd>
<kwd>activation depth</kwd>
<kwd>penetration depth</kwd>
</kwd-group><contract-num rid="cn001">75N95020C00024</contract-num><contract-num rid="cn002">W81XWH22C0111</contract-num><contract-num rid="cn003">80NSSC22CA071</contract-num><contract-sponsor id="cn001">National Institute of Health (NIH)</contract-sponsor><contract-sponsor id="cn002">Department of Defense (DOD)</contract-sponsor><contract-sponsor id="cn003">National Aeronautics and Space Administration (NASA)</contract-sponsor><counts>
<fig-count count="6"/>
<table-count count="2"/><equation-count count="2"/><ref-count count="65"/><page-count count="13"/><word-count count="0"/></counts><custom-meta-wrap><custom-meta><meta-name>section-at-acceptance</meta-name><meta-value>Non-Pharmacological Treatment of Pain</meta-value></custom-meta></custom-meta-wrap>
</article-meta>
</front>
<body><sec id="s1" sec-type="intro"><label>1</label><title>Introduction</title>
<p>The International Association for the Study of Pain (IASP) defines pain as an unpleasant sensory and emotional experience associated with, or resembling that associated with, actual or potential tissue damage (<xref ref-type="bibr" rid="B1">1</xref>). The Centers for Disease Control and Prevention (CDC) estimates that 20.4&#x0025; (50 million) of American adults suffer from chronic pain and, of which 8&#x0025; (19.6 million) live with high-impact chronic pain (<xref ref-type="bibr" rid="B2">2</xref>). Chronic pain is further defined by IASP to be pain persisting beyond typical tissue healing time, which is generally considered to be 3 months (<xref ref-type="bibr" rid="B3">3</xref>). Common types of chronic pain include back, headache, joint, neck, hip, and osteoarthritis pain (<xref ref-type="bibr" rid="B4">4</xref>). Although treatment typically includes pharmacological approaches, one non-pharmacological and non-invasive option recommended by some clinicians for its convenience and effectiveness is Transcutaneous electrical nerve stimulation (TENS) therapy (<xref ref-type="bibr" rid="B5">5</xref>).</p>
<p>Studies suggest that TENS helps reduce pain via peripheral and central mechanisms. Conventional TENS activates large diameter afferent fibers which is then sent to the central nervous system to activate descending inhibitory systems to reduce hyperalgesia (<xref ref-type="bibr" rid="B6">6</xref>). Specifically, the potential main pathways activated by TENS include projections from the ventrolateral periaqueductal gray (PAG) sending input to the rostroventral medial medulla (RVM), which consequently, projects to the spinal cord to produce analgesia (<xref ref-type="bibr" rid="B6">6</xref>, <xref ref-type="bibr" rid="B7">7</xref>). In parallel, studies in fibromyalgia suggest that TENS can restore central pain modulation. Using small battery-powered devices, TENS typically delivers biphasic, symmetric or asymmetric, rectangular or square pulses through cutaneous electrodes positioned near the painful area (<xref ref-type="bibr" rid="B6">6</xref>). They can be applied with varying frequencies, from low (&#x003C;10&#x2005;Hz) to high (&#x003E;50&#x2005;Hz), or mixed frequencies (<xref ref-type="bibr" rid="B8">8</xref>). In general, higher-frequency stimulation is delivered at sensory intensity, and low-frequency stimulation is delivered at motor intensity (<xref ref-type="bibr" rid="B6">6</xref>). At sensory intensity, patients may experience strong but comfortable sensations without contractions, whereas at high intensity they can feel painless motor contraction (<xref ref-type="bibr" rid="B6">6</xref>).</p>
<p>The early evolution of TENS has been characterized by a faster rate of development of clinical applications rather than determining optimal parameters (<xref ref-type="bibr" rid="B9">9</xref>). This has been compounded by the fact that use for low back pain was &#x201C;grandfathered&#x201D; in the United States. As TENS for low back pain was marketed prior to the 1976 medical device regulation act (<xref ref-type="bibr" rid="B10">10</xref>), it was allowed to stay in commerce, and therefore TENS efficacy for low back pain was never &#x201C;premarket approved&#x201D;. Newer devices could thereby, obtain marketing &#x201C;clearance&#x201D; based on demonstrating equivalence to prior devices based on technology (stimulation parameter) comparison. Given no incentive for device manufacturers to develop proper clinical utility and generate high quality efficacy data, clinical evidence has continued to be debated (<xref ref-type="bibr" rid="B4">4</xref>, <xref ref-type="bibr" rid="B5">5</xref>). Newer indications such as TENS for migraine and sinus pain have however demonstrated definitive clinical utility (<xref ref-type="bibr" rid="B11">11</xref>&#x2013;<xref ref-type="bibr" rid="B13">13</xref>). TENS devices are considered medium risk (Class 2) devices and are available for both prescription and OTC use.</p>
<p>Commercially available TENS devices for peripheral pain provide multiple therapy modes with each mode delivering a different combination of frequency and pulse width with intensity. The intended use of such devices varies from symptomatic relief of chronic pain associated with sore and aching muscles in the shoulder, waist, back, neck, arm, and leg and/or adjunctive treatment in the management of post-surgical and post-traumatic acute pain. Users are asked to screen through available modes and settle on the mode that provides the &#x201C;most desirable sensation/comfort&#x201D;. While frequency selection allows to set desired sensory or motor contraction, intensity generally maps to tolerability, longer pulse width is suggested to induce a feeling of deeper stimulation.</p>
<p>Studies exploring the effects of pulse width/duration over the years, have mostly studied physiological responses and not the exact relationship to activation depth in TENS. Li and Bak 1976 (<xref ref-type="bibr" rid="B14">14</xref>) showed that isolated excitation of different nerve groups (motor, sensory, pain-conducting fibers) in adult cats may be easier with a short duration pulse. Effects on pulse width on the arm have reproduced basic relationships between pulse duration and current intensity found in prior literature (<xref ref-type="bibr" rid="B15">15</xref>, <xref ref-type="bibr" rid="B16">16</xref>). Specifically, Alon et al. (<xref ref-type="bibr" rid="B9">9</xref>) demonstrated that pain thresholds mediated by pain-conducting fibers in healthy subjects resulted in reducing thresholds (350&#x2005;mA&#x2014;30&#x2005;mA) as pulse duration was increased (5&#x2005;&#x03BC;s&#x2014;1,000&#x2005;&#x03BC;s). Further, stimulus pulse width may also be used to selectively recruit fibers of different sizes (<xref ref-type="bibr" rid="B17">17</xref>). Some efforts do however come close in context of other electrical stimulation modalities. For instance, increasing pulse width was empirically shown to improve current penetration by reaching distant muscles from surface electrodes in neuromuscular electrical stimulation (NMES) (<xref ref-type="bibr" rid="B18">18</xref>). In the context of invasive deep brain stimulation (DBS), increasing pulse width has been shown to lead to activation at greater distances from electrode center (or deeper stimulation) (<xref ref-type="bibr" rid="B19">19</xref>, <xref ref-type="bibr" rid="B20">20</xref>). Further, long pulse width stimulation has been shown to penetrate and activate deeper muscles in functional electrical stimulation (FES) (<xref ref-type="bibr" rid="B21">21</xref>, <xref ref-type="bibr" rid="B22">22</xref>).</p>
<p>The goal of this computational study was to investigate the effect of the pulse width in TENS on the arm. A high anatomically realistic finite element model was used to simulate the induced electric field (E-field) distribution. The E-field is then coupled to a sensory neuron model given TENS&#x0027;s efficacy is predicated on providing pain relief by exciting sensory nerves. We evaluated strength-duration (S-D) curve and volume of tissue activated (VTA). The VTA map was related to pulse width to provide insight on the effect of pulse width on activation depth.</p>
</sec>
<sec id="s2" sec-type="methods"><label>2</label><title>Methods</title>
<sec id="s2a"><label>2.1</label><title>Geometry setup</title>
<p>The computational study was performed using Sim4Life (V7.0.1, Zurich MedTech, Zurich, Switzerland) incorporating NEURON solver (v7.2.3.12730). Sim4Life is a simulation platform that combines human phantoms with relevant physics solvers for analyzing real-world biological problems. Important to this study, the direct integration of the NEURON simulation environment allows seamless application of E-field to neuronal dynamics. The model geometry considered corresponds to the right arm of the Yoon-sun V4-0 dataset (<xref ref-type="bibr" rid="B23">23</xref>). The model incorporates high resolution data (0.1&#x2009;&#x2009;&#x00D7;&#x2009;&#x2009;0.1&#x2009;&#x00D7;&#x2009;0.2&#x2005;mm) making it possible to resolve nerves, arteries, veins, and other small structures. Furthermore, it includes all major nerve trajectories from the cranium and spinal cord to internal organs and muscles and has been used in other peripheral nerve stimulation studies (<xref ref-type="bibr" rid="B24">24</xref>, <xref ref-type="bibr" rid="B25">25</xref>). The relevant tissue properties for this study are presented in <xref ref-type="table" rid="T1">Table&#x00A0;1</xref> and based on the IT&#x0027;IS material parameter database (<xref ref-type="bibr" rid="B26">26</xref>). Precisely, the model in <xref ref-type="fig" rid="F1">Figure&#x00A0;1A</xref> consists of a pair of stimulation electrodes placed at a separation of 2&#x2005;cm on the wrist with the goal of targeting the median nerve. The electrodes are placed along the length of the median nerve and only serves as a test placement to study the effect of pulse width. The major underlying layers that comprise the model are further indicated in <xref ref-type="fig" rid="F1">Figures&#x00A0;1B,C</xref>. The electrode and interfacing gel combination have a radius of 3&#x2005;mm with a combined total thickness of 2&#x2005;mm.</p>
<table-wrap id="T1" position="float"><label>Table 1</label>
<caption><p>Tissue electrical conductivities (S/m) used in the model.</p></caption>
<table frame="hsides" rules="groups">
<colgroup>
<col align="left"/>
<col align="center"/>
<col align="left"/>
<col align="center"/>
</colgroup>
<thead>
<tr>
<th valign="top" align="left">Tissue</th>
<th valign="top" align="center">Conductivity</th>
<th valign="top" align="left">Tissue</th>
<th valign="top" align="center">Conductivity</th>
</tr>
</thead>
<tbody>
<tr>
<td valign="top" align="left">Skin</td>
<td valign="top" align="center">0.1482</td>
<td valign="top" align="left">Tendon/ligament</td>
<td valign="top" align="center">0.3675</td>
</tr>
<tr>
<td valign="top" align="left">Bone (Cancellous)</td>
<td valign="top" align="center">0.0804</td>
<td valign="top" align="left">Muscle</td>
<td valign="top" align="center">0.4610</td>
</tr>
<tr>
<td valign="top" align="left">Bone (Marrow)</td>
<td valign="top" align="center">0.1797</td>
<td valign="top" align="left">Air</td>
<td valign="top" align="center">0</td>
</tr>
<tr>
<td valign="top" align="left">Bone (Cortical)</td>
<td valign="top" align="center">0.0063</td>
<td valign="top" align="left">Blood</td>
<td valign="top" align="center">0.6624</td>
</tr>
<tr>
<td valign="top" align="left">Fat</td>
<td valign="top" align="center">0.0776</td>
<td valign="top" align="left">Nerve</td>
<td valign="top" align="center">0.3475</td>
</tr>
<tr>
<td valign="top" align="left">Subcutaneous adipose tissue (SAT)</td>
<td valign="top" align="center">0.0776</td>
<td valign="top" align="left">Gel electrode</td>
<td valign="top" align="center">1.7</td>
</tr>
</tbody>
</table>
</table-wrap>
<fig id="F1" position="float"><label>Figure 1</label>
<caption><p>Arm geometry and tissue composition. <bold>(A)</bold> Indicates the position of the stimulation electrodes targeting the median nerve. <bold>(B)</bold> Indicates the subcutaneous adipose tissue (SAT) layer. <bold>(C)</bold> Indicates other underlying tissues such as muscle, nerves, bone, etc. Refer to <xref ref-type="table" rid="T1">Table&#x00A0;1</xref> for all tissues considered in the model and their corresponding electrical conductivities.</p></caption><alt-text>Three labeled 3D renderings of a human forearm from wrist to elbow in anatomical position. Panel A shows the external skin surface with scale bars and measurement markers. Panel B reveals the subcutaneous adipose tissue layer labeled SAT, partially transparent to show underlying vascular structures. Panel C displays internal anatomy including labeled structures such as muscle, vein, fat, artery, nerve, bone, tendon, and ligament, each color-coded for distinction.</alt-text>
<graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="fpain-06-1526277-g001.tif"/>
</fig>
</sec>
<sec id="s2b"><label>2.2</label><title>Nerve trajectories</title>
<p>The intended stimulation region and corresponding nerve anatomy is shown in <xref ref-type="fig" rid="F2">Figure&#x00A0;2A</xref>. While the regions of interest are areas in immediate proximity to the stimulation electrodes, overall visualization of anatomical details in the considered geometry is helpful, to relate to induced E-field and VTA plots. As is known, five specific nerves appear from the cords as the terminal branches of the brachial plexus: musculocutaneous, axillary, radial, median and ulnar nerves. The musculocutaneous nerve provides motor innervation to the muscles of the anterior compartment of the arm (<xref ref-type="bibr" rid="B27">27</xref>). The median nerve (comprising C6-T1 spinal roots) predominantly provides motor innervation to the flexor muscles of the forearm and hand (<xref ref-type="bibr" rid="B28">28</xref>). The radial nerve innervates most of the skin of the posterior forearm, the lateral dorsum of the hand, and the dorsal surface of the lateral three and a half digits. Lastly, the ulnar nerve carries both sensory and motor fibers and supplies sensory cutaneous innervation to the medial forearm, medial wrist, and medial one and one-half digits (<xref ref-type="bibr" rid="B27">27</xref>).</p>
<fig id="F2" position="float"><label>Figure 2</label>
<caption><p>Nerve anatomy in the arm and locations evaluated. <bold>(A)</bold> Available terminal branches of the brachial plexus nerves (musculocutaneous, radial, median, and ulnar) highlighting anatomical detail in geometry. <bold>(B)</bold> The longest nerve trajectories were subsequently considered for simulation. For instance, (C6, 6) refers to the nerve segment in the cervical section (C6) with 6 being the specific trajectory number. The ulnar nerve has 1, 2, 3, 5, 6 trajectories in the thoracic section but we consider the longest trajectory (6), or (T1, 6). <bold>(C)</bold> Point sensor locations. The nodes (520, 550, 580) indicate the exact location of simulation data collection.</p></caption><alt-text>Three anatomical renderings of a human forearm and hand skeleton with nerve pathways. Panel A displays labeled musculocutaneous, radial, median, and ulnar nerves, with numbered nerve branches extending to the fingers. Panel B illustrates dorsal and ventral paths of the radial, median, and ulnar nerves along with their corresponding spinal nerve roots. Panel C shows node-based tracking of nerve pathways, with three labeled nodes (520, 550, 580) marked by magenta dots.</alt-text>
<graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="fpain-06-1526277-g002.tif"/>
</fig>
<p>The longest trajectories of the ventral and dorsal roots of C6 and T1 were considered for analysis here (<xref ref-type="fig" rid="F2">Figure&#x00A0;2B</xref>) due to the expected direct influence on the mid-forearm&#x2014;based on electrode locations. The nerve depth from skin in contact with electrodes to the median nerve is about 5.5&#x2005;mm, the radial nerve is about 13.1&#x2005;mm, and the ulnar nerve is 14.9&#x2005;mm. The three &#x201C;point sensor&#x201D; locations along the nerve trajectory used for collecting the simulation data (i.e., nodes 520, 550, and 580) are illustrated in <xref ref-type="fig" rid="F2">Figure&#x00A0;2C</xref>. There were therefore 18 point sensors considered: 9 (ventral rami) and 9 (dorsal rami).</p>
</sec>
<sec id="s2c"><label>2.3</label><title>Injected current</title>
<p>The low-frequency electromagnetic (EM LF)&#x2014;Ohmic Quasi-Static module, a rectilinear LF solver, was used to simulate TENS on the arm at multiple pulse widths (30, 88, 146, 262, and 495&#x2005;&#x03BC;s) corresponding to the range typically available in commercial TENS stimulators. Specifically, the goal was to simulate the impact of a single pulse. Dirichlet boundary conditions were applied as 2.38&#x2005;V and &#x2212;2.38&#x2005;V at the anode and cathode corresponding to 5&#x2005;mA of current flux calculated on the electrodes. Other external boundaries were electrically insulated (i.e., normal current density&#x2009;&#x003D;&#x2009;0). The Ohmic quasi-static field as noted in <xref ref-type="disp-formula" rid="disp-formula1">Equation 2.1</xref><disp-formula id="disp-formula1"><label>(2.1)</label><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="DM1"><mml:mi mathvariant="normal">&#x2207;</mml:mi><mml:mo>&#x22C5;</mml:mo><mml:mrow><mml:mi>&#x03C3;</mml:mi></mml:mrow><mml:mi mathvariant="normal">&#x2207;</mml:mi><mml:mrow><mml:mi>&#x03D5;</mml:mi></mml:mrow><mml:mo>=</mml:mo><mml:mn>0</mml:mn></mml:math></disp-formula>was solved with the aforementioned boundary conditions for the electric potential distribution (<xref ref-type="bibr" rid="B29">29</xref>&#x2013;<xref ref-type="bibr" rid="B31">31</xref>). The injected current was then re-calculated based on the titration factor (see section on Titration mechanism) to visualize differences in the E-field between the different pulse widths.</p>
</sec>
<sec id="s2d"><label>2.4</label><title>Neuron model and additional simulation considerations</title>
<p>TENS is known to stimulate sensory nerves, suppressing the pain signals being sent to the brain to give user relief. We therefore considered the sensory McIntyre-Richardson-Grill (MRG) neuron model (<xref ref-type="bibr" rid="B32">32</xref>, <xref ref-type="bibr" rid="B33">33</xref>), with the smallest diameter setting available (5&#x2005;&#x03BC;m), to simulate the effects of pain-transmitting nerve fibers. The MRG model is based on a double-cable representation of the axon that allows separating electrical representations of the myelin and underlying internodal axolemma. The model has been used for neural predictions in a variety of applications (<xref ref-type="bibr" rid="B20">20</xref>, <xref ref-type="bibr" rid="B34">34</xref>, <xref ref-type="bibr" rid="B35">35</xref>). Specific to this study, a modified MRG model that considers electrophysiological properties of sensory fibers was considered (<xref ref-type="bibr" rid="B34">34</xref>). For simulating TENS using the titration mechanism, the modulation pulse type was set to bipolar with a unitless amplitude of 1 and an interphase interval of 0.1&#x2005;ms while varying the pulse widths. Therefore, each of the five pulse widths considered, were individually simulated. The duration and time step of the solver were set to 3.5&#x2005;ms and 0.0025&#x2005;ms respectively. The junction potential was not corrected. Running a simulation for the aforementioned nodes of interest at one pulse width took approximately 4&#x2005;h using 64 threads on a workstation with the following specifications: AMD Ryzen Threadripper 3970X 32-Core Processor, 3.70&#x2005;GHz CPU speed, and 192 GB installed RAM.</p>
</sec>
<sec id="s2e"><label>2.5</label><title>Titration mechanism</title>
<p>Titration involves stimulating an axon with a series of modulating pulses of <italic>increasing</italic> intensity to find the threshold at which a single action potential is generated in excitable cells. This method introduces an additional scaling factor that is titrated until a response can be detected within the stimulated region (<xref ref-type="bibr" rid="B36">36</xref>, <xref ref-type="bibr" rid="B37">37</xref>). Thus, the excitability threshold (I<sub>T</sub>) as indicated in <xref ref-type="disp-formula" rid="disp-formula2">Equation 2.2</xref> is the product of the current applied to the cellular membrane of the axon, the aforementioned titration factor (T), and the modulating pulse (a(t)):<disp-formula id="disp-formula2"><label>(2.2)</label><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="DM2"><mml:msub><mml:mrow><mml:mi mathvariant="normal">I</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant="normal">T</mml:mi></mml:mrow></mml:msub><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi mathvariant="normal">t</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo><mml:mrow><mml:mspace width="thickmathspace" /></mml:mrow><mml:mo>=</mml:mo><mml:mrow><mml:mspace width="thickmathspace" /></mml:mrow><mml:mrow><mml:mi mathvariant="normal">I</mml:mi></mml:mrow><mml:mrow><mml:mo>.</mml:mo><mml:mi mathvariant="normal">T</mml:mi></mml:mrow><mml:mrow><mml:mo>.</mml:mo><mml:mi mathvariant="normal">a</mml:mi></mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi mathvariant="normal">t</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:math></disp-formula>The T parameter is considered as a scaling factor to indicate proportion or a multiple of the actual modulated current needed to generate an action potential. Potential and current can be used interchangeably here for measuring the stimulus strength.</p>
</sec>
<sec id="s2f"><label>2.6</label><title>Volume of tissue activated</title>
<p>The volume of tissue activated (VTA) was used to compare stimulation differences caused by changes in pulse width. The VTA around each electrode contact relied on the concept of activation function (AF), which was calculated from the eigenvalues of the Hessian matrix (<xref ref-type="bibr" rid="B38">38</xref>). Each eigenvalue of the Hessian matrix represents the second partial derivative of the electric potential along the respective eigenvector. A multi-step process was used to determine the VTA due to pulse width variation. This involved determining the excitability threshold (I<sub>T</sub>), using the corresponding electric potential to calculate the AF, and subsequently utilizing the AF to determine the VTA.</p>
</sec>
</sec>
<sec id="s3" sec-type="results"><label>3</label><title>Results</title>
<sec id="s3a"><label>3.1</label><title>Electric field (E-field)</title>
<p>The induced <italic>surface</italic> E-field plots due to the shortest and the longest pulse widths, calculated at their corresponding titration factors (see <xref ref-type="table" rid="T2">Table&#x00A0;2</xref>) and plotted to the same scale, are included in <xref ref-type="fig" rid="F3">Figure&#x00A0;3</xref>. As mentioned above, these simulations reflect the impact of a single pulse. The plots reveal that the smaller pulse width (30&#x2005;&#x03BC;s) induces a larger E-field (max: 456&#x2005;V/m)&#x2014;covering a larger area of the arm. On the other hand, the induced E-field due to 495&#x2005;&#x03BC;s is less diffuse, more focused, and has lower magnitude from the same pair of electrodes. However, this is intuitively expected, as the plots are generated at their respective stimulation threshold, so the 30&#x2005;&#x03BC;s E-field is the result of 19.7&#x2005;mA and the 495&#x2005;&#x03BC;s E-field is the result of injecting 1.75&#x2005;mA. The overall spatial profile resembles a stretched ellipse with the major axis along the line connecting the stimulation electrodes. The ulnar and radial nerves that are farther away from the electrode sites receive less E-field (&#x223C;0 to 132&#x2005;V/m). With longer pulse width, the induced E-field profile in the immediate vicinity of the electrode sites indicates a restricted hot-spot with dramatic fall-off (&#x223C;40 to 280&#x2005;V/m) and approximately 0&#x2013;23&#x2005;V/m for the rest of the nerves.</p>
<table-wrap id="T2" position="float"><label>Table 2</label>
<caption><p>Titration factor and corresponding excitability threshold current at chosen sensor locations. Values are noted for the shortest (30&#x2005;&#x03BC;s) and longest (495&#x2005;&#x03BC;s) pulse duration at sensor nodes (520, 550, 580). As expected, minimum titration factors and current were needed for the superficial median nerve with the highest values needed for the ulnar nerve.</p></caption>
<table frame="hsides" rules="groups">
<colgroup>
<col align="left"/>
<col align="center"/>
<col align="center"/>
<col align="center"/>
<col align="center"/>
<col align="center"/>
<col align="center"/>
<col align="center"/>
</colgroup>
<thead>
<tr>
<th valign="top" align="left" colspan="2">C6 dorsal</th>
<th valign="top" align="center" colspan="2">C6 ventral</th>
<th valign="top" align="center" colspan="2">T1 dorsal</th>
<th valign="top" align="center" colspan="2">T1 ventral</th>
</tr>
</thead>
<tbody>
<tr>
<td valign="top" align="left">Median (30&#x2005;&#x00B5;s)</td>
<td valign="top" align="center">3.93 (19.65&#x2005;mA)</td>
<td valign="top" align="center">Median (30&#x2005;&#x00B5;s)</td>
<td valign="top" align="center">3.93 (19.65&#x2005;mA)</td>
<td valign="top" align="center">Ulnar (30&#x2005;&#x00B5;s)</td>
<td valign="top" align="center">81.55 (407.75&#x2005;mA)</td>
<td valign="top" align="center">Ulnar (30&#x2005;&#x00B5;s)</td>
<td valign="top" align="center">76.57 (382.85&#x2005;mA)</td>
</tr>
<tr>
<td valign="top" align="left">Median (495&#x2005;&#x00B5;s)</td>
<td valign="top" align="center">0.34 (1.7&#x2005;mA)</td>
<td valign="top" align="center">Median (495&#x2005;&#x00B5;s)</td>
<td valign="top" align="center">0.34 (1.7&#x2005;mA)</td>
<td valign="top" align="center">Ulnar (495&#x2005;&#x00B5;s)</td>
<td valign="top" align="center">11.31 (56.55&#x2005;mA)</td>
<td valign="top" align="center">Ulnar (495&#x2005;&#x00B5;s)</td>
<td valign="top" align="center">10.87 (54.35&#x2005;mA)</td>
</tr>
<tr>
<td valign="top" align="left">Radial (30&#x2005;&#x00B5;s)</td>
<td valign="top" align="center">35.57 (177.85&#x2005;mA)</td>
<td valign="top" align="center">Radial (30&#x2005;&#x00B5;s)</td>
<td valign="top" align="center">35.57 (177.85&#x2005;mA)</td>
<td valign="top" align="center"/>
<td valign="top" align="center"/>
<td valign="top" align="center"/>
<td valign="top" align="center"/>
</tr>
<tr>
<td valign="top" align="left">Radial (495&#x2005;&#x00B5;s)</td>
<td valign="top" align="center">3.21 (16.05&#x2005;mA)</td>
<td valign="top" align="center">Radial (495&#x2005;&#x00B5;s)</td>
<td valign="top" align="center">3.21 (16.05&#x2005;mA)</td>
<td valign="top" align="center"/>
<td valign="top" align="center"/>
<td valign="top" align="center"/>
<td valign="top" align="center"/>
</tr>
</tbody>
</table>
</table-wrap>
<fig id="F3" position="float"><label>Figure 3</label>
<caption><p>Surface plot of induced E-field on the arm due to the shortest and longest pulse widths considered. The E-field was calculated based on the current due to their corresponding titration factor: for 30&#x2005;&#x03BC;s, input current was 19.7&#x2005;mA and for 495&#x2005;&#x03BC;s, 1.75&#x2005;mA.</p></caption><alt-text>Two simulated forearm models show the spatial distribution of electric fields during nerve stimulation, visualized at two time points: 30 &#x03BC;s and 495 &#x03BC;s. Each arm is overlaid with nerve pathways in red, green, and blue lines. Heatmap color gradients from blue to yellow indicate electric field strength in volts per meter, with peak intensity near the stimulation site marked by two circular electrodes. The field diffuses over time but remains centered around the electrode region. A color scale bar on the left ranges from 0 to 413 v/m.</alt-text>
<graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="fpain-06-1526277-g003.tif"/>
</fig>
</sec>
<sec id="s3b"><label>3.2</label><title>Titration factor</title>
<p>As previously stated, the titration technique was employed to find the threshold potential of membrane depolarization. <xref ref-type="table" rid="T2">Table&#x00A0;2</xref> notes the individual titration factors and the corresponding excitability threshold current needed for the roots (C6 and T1). As expected, the titration factor is substantially smaller for the 495&#x2005;&#x03BC;s pulse in comparison to the 30&#x2005;&#x03BC;s pulse. While the titration factors of dorsal and ventral sections for the C6 roots are the same, they differ somewhat for the T1 roots. Further, as anticipated, minimum titration factors and current were needed in the branches of the median nerve due to the proximity to the electrode sites.</p>
</sec>
<sec id="s3c"><label>3.3</label><title>Strength-duration curve</title>
<p>The resulting strength-duration (S-D) curve of the median nerve under electrical stimulation is shown in <xref ref-type="fig" rid="F4">Figure&#x00A0;4</xref>. For the range of 30&#x2013;495&#x2005;&#x03BC;s considered here, the rheobase was found to be &#x223C;1.75&#x2005;mA with a chronaxie of &#x223C;232&#x2005;&#x03BC;s. Consistent with the theory, the curve tends to flatten out with longer stimulus duration (or pulse width).</p>
<fig id="F4" position="float"><label>Figure 4</label>
<caption><p>Strength-duration (S-D) curve of the target median nerve. A pulse width range of 30&#x2013;495&#x2005;&#x03BC;s was considered in the study. The corresponding excitability threshold for each pulse width is noted along the curve.</p></caption><alt-text>Line graph showing the relationship between pulse duration in microseconds and excitability threshold in milliamperes. The curve decreases non-linearly, indicating that longer pulse durations require lower current to reach excitation. Red diamond markers highlight six data points, labeled with corresponding durations and thresholds: 30&#x2005;&#x00B5;s at 19.70&#x2005;mA, 88&#x2005;&#x00B5;s at 8.13&#x2005;mA, 146&#x2005;&#x00B5;s at 5.04&#x2005;mA, 262&#x2005;&#x00B5;s at 2.91&#x2005;mA, and 495&#x2005;&#x00B5;s at 1.75&#x2005;mA. Annotations indicate key physiological points: Rheobase at 1.75&#x2005;mA, 2&#x00D7; Rheobase at 3.50&#x2005;mA, and Chronaxie at approximately 232&#x2005;&#x00B5;s. Horizontal and vertical dashed lines mark Rheobase and Chronaxie thresholds.</alt-text>
<graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="fpain-06-1526277-g004.tif"/>
</fig>
</sec>
<sec id="s3d"><label>3.4</label><title>Volume of tissue activated (VTA)</title>
<p>The VTA maps illustrate isosurface plots derived from the absolute value of Hessian matrix eigenvalues of the electric potential. Since the Hessian matrix is essentially a matrix of the second partial derivative of the electric potential, it enables determination of the classic activating function in 3D (<xref ref-type="bibr" rid="B39">39</xref>, <xref ref-type="bibr" rid="B40">40</xref>). To facilitate a direct comparison across the range of pulse widths considered, we plotted the VTA maps at one common current value- i.e., the average threshold current (10.73&#x2005;mA) spanning the shortest and longest pulse widths (<xref ref-type="fig" rid="F5">Figure&#x00A0;5</xref>). As expected, the shortest pulse width requires the highest threshold to activate tissue near the input source and is approximately a factor of 11 higher with respect to the longest pulse width (8.8 e<sup>5</sup>/7.82 e<sup>4</sup>). The estimated VTA for the shortest and widest pulses were 118.72&#x2005;mm<sup>3</sup> and 2,586.24&#x2005;mm<sup>3</sup> respectively, indicating a VTA ratio of 21.2.</p>
<fig id="F5" position="float"><label>Figure 5</label>
<caption><p>Median nerve activating function (AF) and volume of tissue activated (VTA) at a fixed current amplitude (10.73&#x2005;mA). Figures show the isosurface plots of the second spatial derivative of electric potential at the AF threshold for the median nerve. Each row is the result of a simulated pulse width in ascending order (30, 88, 146, 262, 495&#x2005;&#x03BC;s). Electrode 2 is the electrode closer to the wrist.</p></caption><alt-text>Five rows of 3D visualizations showing the volume of tissue activated (VTA) at increasing pulse durations: 30, 88, 146, 262, and 495 &#x03BC;s. Each row includes three views labeled .1, .2, and .3, depicting spatial distributions of stimulated tissue in blue surrounding two circular electrodes (green and orange). Activation thresholds decrease as pulse duration increases, while VTA values expand from 118.72 mm&#x00B3; to 2586.24 mm&#x00B3;. The images illustrate a clear growth in stimulated region with longer pulses. A legend identifies electrodes and activated tissue.</alt-text>
<graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="fpain-06-1526277-g005.tif"/>
</fig>
<p>The value of this study is exemplified by observing the shape and pattern of the VTA maps. While VTA investigation in invasive applications such as DBS reveal uniform &#x201C;blobs&#x201D; around the electrode contacts reflecting <italic>one</italic> brain region (<xref ref-type="bibr" rid="B19">19</xref>, <xref ref-type="bibr" rid="B41">41</xref>), the maps here are scattered and irregular, due to varying complex anatomy. This is only captured due to the realistic arm geometry considered here. The VTA maps also help visualize the influence of pulse width on activation depth. The plots in the first column indicate that for pulse widths up to 146&#x2005;&#x03BC;s, it is not possible to recruit the deeper radial and the ulnar nerves. At the longest pulse width, there is some activation at the levels of the deeper nerves of the arm.</p>
</sec>
<sec id="s3e"><label>3.5</label><title>Influence of the pulse width with respect to activation depth</title>
<p>To understand the influence of pulse width on activation depth, we plotted predicted VTA with respect to the varying pulse widths considered (<xref ref-type="fig" rid="F6">Figure&#x00A0;6</xref>). We note a linear relationship for the range of pulse widths considered here.</p>
<fig id="F6" position="float"><label>Figure 6</label>
<caption><p>Volume of tissue activated (VTA) vs. pulse width at a fixed current amplitude (10.73&#x2005;mA). VTA is used as a surrogate for activation depth. For the range of pulse widths and conditions considered here, the relationship is linear.</p></caption><alt-text>Line graph showing a positive linear relationship between pulse width in microseconds and volume of tissue activated (VTA) in cubic millimeters. Five red diamond markers represent VTA values at pulse widths of 30, 88, 146, 262, and 495 &#x03BC;s, with corre- sponding volumes labeled as 118.72 mm&#x00B3;, 401.64 mm&#x00B3;, 717.34 mm&#x00B3;, 1,311.43 mm&#x00B3;, and 2,586.24 mm&#x00B3;. The increasing trend indicates that longer pulse durations lead to greater activation volumes.</alt-text>
<graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="fpain-06-1526277-g006.tif"/>
</fig>
</sec>
</sec>
<sec id="s4" sec-type="discussion"><label>4</label><title>Discussion</title>
<p>The central aim of this study was to unpack the relationship between pulse width and activation depth during TENS on the arm. Prior electrical stimulation studies using other modalities have empirically shown that wider pulses can recruit deeper targets. Using a highly detailed 3D model, we provide enhanced visualization of available geometry, induced E-field profile, VTA maps, and relationship to activation depth, for the first time.</p>
<p>The S-D curves for nerve stimulation have clearly established its shape over numerous investigations dating back to the 30&#x0027;s (<xref ref-type="bibr" rid="B42">42</xref>&#x2013;<xref ref-type="bibr" rid="B45">45</xref>). Given the dominant electrical capacitance of the neural membrane, S-D curves expectedly follow a capacitor discharge curve. A TENS practitioner can therefore readily use the inverse relationship between intensity and pulse width to make an informed stimulation strategy choice. Now longer pulse widths at the same current would lead to more charge delivered across the membrane- presumably translating to deeper stimulation. However, the exact relationship has not been explored previously in TENS. Further for non-invasive electrical nerve stimulation applications, lowering pulse width in order to deliver higher current intensity is limited to the intensity at which the user can comfortably receive stimulation (<xref ref-type="bibr" rid="B46">46</xref>). This restriction is however not applicable for invasive delivery (<xref ref-type="bibr" rid="B20">20</xref>) as stimulation does not have to navigate superficial cutaneous sensation.</p>
<p>The linear relationship between VTA and pulse width observed in our simulations indicates that longer widths would lead to deeper activation. We note that our observations are restricted to only the pulse widths and the concomitant geometry (forearm) considered here. We expected the relationship to asymptote at higher pulse widths as the excitability threshold reaches rheobase. While the excitability threshold in the S-D curve (<xref ref-type="fig" rid="F4">Figure&#x00A0;4</xref>) follows a hyperbolic or exponential decay similar to classical equations [Weiss-Lapique and Lapique-Blair (<xref ref-type="bibr" rid="B44">44</xref>, <xref ref-type="bibr" rid="B45">45</xref>)], the VTA expands with a similar convexity resulting in a <italic>net</italic> linear VTA&#x2014;pulse width relationship. We suspect this is due to (1) volume being cubic and (2) the Hessian of voltage dropping exponentially away from the electrodes. There are several limiting assumptions to the plot. We are considering only the magnitude of the Hessian, which does not account for orientation/alignment with any possible axon. The AF thresholds were calibrated for the median nerve A-delta fiber running along the length of the arm; other nerve orientations and fiber types would be expected to respond differently. Further, heterogeneous tissues cause spikes in E-field and AF at material boundaries. Additionally, the MRG model is a simplification of real nerves (i.e., devoid of complex morpho-electric properties) and does not incorporate all ion channel sub-types. It is therefore possible that the lack of model complexity masks non-linearities.</p>
<p>TENS efficacy is likely predicated upon a net effect of stimulating multiple underlying nerves of various types including discharge frequencies. We note that we simply used the median nerve in this study as a test nerve to explore relationships between E-field, strength, duration, activation depth, etc. However, the choice of A-delta fiber is rational as nociceptors generally transmit noxious stimuli through A-delta and C-fiber nerves (<xref ref-type="bibr" rid="B47">47</xref>). Further, it is known that the C-fiber afferents carry slow sensations associated with aches, whereas the A-delta afferents are associated with fast sensations such as sharp pain. Given the type of pain felt and if one were to know underlying nerve depth (<xref ref-type="bibr" rid="B47">47</xref>), one could potentially start with a suitable pulse width. In reality however, pre-programmed therapy modes (combination of pre-set frequency and pulse width) are provided in TENS devices for pain relief, limiting full flexibility to the user in parameter selection. Therefore, the best approach continues to be to try all modes first, and in each case, titrating intensity to the strongest possible but at a level that is comfortable. If deeper pain relief is desired, patients may consider picking the next mode with longer pulse width while maintaining the frequency and intensity from the prior mode. The caveat however, is that overall pain relief is contingent not only on pulse width parameter of TENS but other factors including discharge frequency, temporal and spatial summation of signals, segmental and central pain mechanisms should also be accounted.</p>
<p>The strength of our modeling process in simulating TENS on the arm is the usage of a highly realistic model. Previous 3-D FEM approaches have either used <italic>idealized</italic> geometries such as a cylindrical arm (<xref ref-type="bibr" rid="B48">48</xref>&#x2013;<xref ref-type="bibr" rid="B50">50</xref>) or derived from 2-D anatomical images by extruding geometry (<xref ref-type="bibr" rid="B37">37</xref>) and limiting to certain cross sections (<xref ref-type="bibr" rid="B34">34</xref>). The modeling methodology applied here, from the geometry, applying EM simulations into a dynamic Neuron solver, using the modified MRG model, and subsequently using titration analysis, mimics the one employed in the context of magnetic stimulation (MS) (<xref ref-type="bibr" rid="B24">24</xref>). The simulation setup used in the aforementioned MS study has been further validated using clinical experiments. Specifically, numerically estimated latencies and waveforms were in agreement with the empirical measurements on subjects undergoing MS on the arm (<xref ref-type="bibr" rid="B25">25</xref>). The only difference to our simulation is the application of electrical stimulation and thereby, related governing equation. However, the governing equation is a standard equation used to predict induced current in volumetric media and has been validated in other applications (<xref ref-type="bibr" rid="B51">51</xref>, <xref ref-type="bibr" rid="B52">52</xref>). Further, the MRG model has been shown to generate accurate predictions for TENS specifically, compared to active cable and mammalian nerve models (<xref ref-type="bibr" rid="B29">29</xref>, <xref ref-type="bibr" rid="B37">37</xref>). Taken together, we expect the main conclusions of this study to be robust.</p>
<p>We specifically isolated the effects due to pulse width given the main aim of our study. In reality, pulse widths are associated with pulse repetition frequency and it is well known that frequency also allows for selective nerve activation. However, this isolation was needed to unpack the relationship of pulse width to activation depth.</p>
<p>It is further meaningful to compare our simulation results to previous experimental attempts. When Kuhn et al., (<xref ref-type="bibr" rid="B48">48</xref>) tested three volunteers using 5&#x2009;&#x00D7;&#x2009;5&#x2005;cm electrodes placed on Flexor Digitorum Superficialis and on the wrist, the S-D curve at 0.5&#x2005;ms indicated a corresponding intensity of &#x223C;5&#x2005;mA. Goffredo and colleagues tested direct stimulation of the median nerve at the biceps brachii level using a pair of round electrodes (1.5&#x2005;cm diameter) on six subjects (<xref ref-type="bibr" rid="B49">49</xref>). The S-D curve based on experiments indicated intensities of &#x223C;16&#x2005;mA and &#x223C;9&#x2005;mA at pulse widths of 200&#x2005;&#x03BC;s and 500&#x2005;&#x03BC;s respectively. When considering smaller diameter A-beta fibers to study tactile sensation and 9&#x2005;mm diameter electrodes on forearm (separation&#x2009;&#x003D;&#x2009;12&#x2005;mm) on six subjects, S-D curve indicated a &#x223C;1.7&#x2005;mA multiples of rheobase at 200&#x2005;&#x03BC;s pulse width (<xref ref-type="bibr" rid="B50">50</xref>). Finally, Gaines and colleagues report good agreement with historical experimental data with multiples of rheobase of &#x223C;6&#x2005;V and a chronaxie of 230&#x2005;&#x03BC;s for a sensory axon (10&#x2005;&#x03BC;m diameter) (<xref ref-type="bibr" rid="B34">34</xref>). The region of interest was the arm near the elbow. We note that a one-to-one comparison across aforementioned efforts and our simulations is non-trivial due to several differences&#x2014;from geometry (3D forearm is different to 3D upper arm), specific stimulation electrode montage (size and separation)/induced E-field distribution, nerve fiber/related properties considered, etc. Notwithstanding, our predictions of 1.75&#x2005;mA (rheobase) and 232&#x2005;&#x03BC;s (chronoaxie) considering the median nerve in the forearm are in the range of experimentally shown values. For similar reasons, extrapolating our predictions to other body parts is not possible due to geometrical, electrode placement, and nerve fiber differences.</p>
<p>There are practical limitations to increasing the pulse width at the same current intensity to increase activation depth, namely battery life. The chronaxie is usually considered the most efficient pulse width choice for conserving the pulse generator&#x0027;s battery life and is naturally a key factor in invasive applications (<xref ref-type="bibr" rid="B53">53</xref>). With modern day TENS devices powered by high capacity small rechargeable batteries, this is not much of a concern. However, as mentioned above, we expect the linear relationship to ultimately change and plateau. Promising solutions such as coupling TENS with a nerve cuff to facilitate activation of deeper nerves has been proposed (<xref ref-type="bibr" rid="B37">37</xref>). However, nerve cuff involves surgery and moreover, such solutions are still being developed and not currently available to the practitioner or the patient.</p>
<p>Computational modeling and simulation such as the one reported here is now increasingly used across a range of stimulation modalities, from optimizing delivery, performing safety analysis, to supporting device design/development (<xref ref-type="bibr" rid="B31">31</xref>, <xref ref-type="bibr" rid="B41">41</xref>, <xref ref-type="bibr" rid="B54">54</xref>&#x2013;<xref ref-type="bibr" rid="B57">57</xref>). Furthermore, these predictions have helped in elucidating stimulation parameter choices, understanding mechanism of action, explaining stimulation outcome, and thereby advancing stimulation administration in general (<xref ref-type="bibr" rid="B13">13</xref>, <xref ref-type="bibr" rid="B58">58</xref>&#x2013;<xref ref-type="bibr" rid="B62">62</xref>). We expect this study on the arm to guide researchers in performing future explorations on other body parts, determine ideal pulse width range for target nerve of interest, attempt validation using TENS like the one performed in MS (<xref ref-type="bibr" rid="B25">25</xref>), and investigate new TENS delivery approaches (<xref ref-type="bibr" rid="B63">63</xref>). One could screen across different electrode montages (i.e., electrode separation, size, and shape) to optimally deliver stimulation to a desired target. Modalities such as interferential (IF)/temporal interference stimulation is now being studied in brain using high resolution anatomical models (<xref ref-type="bibr" rid="B64">64</xref>), but it has existed in peripheral stimulation since the 50s (<xref ref-type="bibr" rid="B65">65</xref>). Our simulations could be further expanded to study IF stimulation for specific peripheral targets.</p>
</sec>
<sec id="s5" sec-type="conclusions"><label>5</label><title>Conclusions</title>
<p>Stimulation parameter selection during TENS programming for pain relief is typically based on an ad-hoc sensation basis. Using a highly detailed and realistic 3D arm model, we demonstrate a linear relationship between commonly available pulse width settings and activation depth for TENS on the forearm. While multiple factors impact overall pain relief, once frequency and intensity are set, medical professionals may consider choosing a certain pulse width setting based on the depth of pain relief desired. One can expect a 21 fold difference in volume of tissue activated across the range of pulse width settings available in commercially available devices.</p>
</sec>
</body>
<back>
<sec id="s6" sec-type="data-availability"><title>Data availability statement</title>
<p>The original contributions presented in the study are included in the article/Supplementary Material, further inquiries can be directed to the corresponding author.</p>
</sec>
<sec id="s7" sec-type="author-contributions"><title>Author contributions</title>
<p>AG: Data curation, Formal analysis, Investigation, Methodology, Software, Validation, Visualization, Writing &#x2013; original draft, Writing &#x2013; review &#x0026; editing. DT: Data curation, Formal analysis, Investigation, Methodology, Software, Supervision, Validation, Visualization, Writing &#x2013; review &#x0026; editing. YC: Supervision, Validation, Writing &#x2013; review &#x0026; editing. SL: Supervision, Validation, Writing &#x2013; review &#x0026; editing. AD: Conceptualization, Formal analysis, Funding acquisition, Investigation, Methodology, Project administration, Resources, Software, Supervision, Validation, Visualization, Writing &#x2013; original draft, Writing &#x2013; review &#x0026; editing.</p>
</sec>
<sec id="s8" sec-type="funding-information"><title>Funding</title>
<p>The author(s) declare that financial support was received for the research and/or publication of this article. AD is supported by grants from the National Institute of Health (NIH): 75N95020C00024, Department of Defense (DOD): W81XWH22C0111, and National Aeronautics and Space Administration (NASA): 80NSSC22CA071.</p>
</sec>
<ack><title>Acknowledgments</title>
<p>This research was sponsored by the Department of Defense (DOD) under contract &#x0023; W81XWH22C0111 awarded to Soterix Medical, Inc. The opinions expressed herein are those of the authors and do not reflect those of the United States government. The U.S. government is authorized to reproduce and distribute reprints for Government purposes notwithstanding any copyright notation herein.</p>
</ack>
<sec id="s9" sec-type="COI-statement"><title>Conflict of interest</title>
<p>AG, DT, and AD are employees of Soterix Medical, 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 id="s10" sec-type="ai-statement"><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 id="s11" sec-type="disclaimer"><title>Publisher&#x0027;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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