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<front>
<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">854892</article-id>
<article-id pub-id-type="doi">10.3389/fphy.2022.854892</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Physics</subject>
<subj-group>
<subject>Perspective</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Multidimensional Self-Propelled Motion Based on Nonlinear Science</article-title>
<alt-title alt-title-type="left-running-head">Fujita et&#x20;al.</alt-title>
<alt-title alt-title-type="right-running-head">Multidimensional Self-Propelled Motion</alt-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname>Fujita</surname>
<given-names>Risa</given-names>
</name>
<uri xlink:href="https://loop.frontiersin.org/people/1679831/overview"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Matsuo</surname>
<given-names>Muneyuki</given-names>
</name>
<uri xlink:href="https://loop.frontiersin.org/people/1678248/overview"/>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Nakata</surname>
<given-names>Satoshi</given-names>
</name>
<xref ref-type="corresp" rid="c001">&#x2a;</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1034412/overview"/>
</contrib>
</contrib-group>
<aff>
<institution>Department of Mathematical and Life Sciences</institution>, <institution>Graduate School of Integrated Sciences for Life</institution>, <institution>Hiroshima University</institution>, <addr-line>Higashihiroshima</addr-line>, <country>Japan</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/1421214/overview">Rabih Sultan</ext-link>, American University of Beirut, Lebanon</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/904797/overview">Charles Reichhardt</ext-link>, Los Alamos National Laboratory (DOE), United&#x20;States</p>
</fn>
<corresp id="c001">&#x2a;Correspondence: Satoshi Nakata, <email>nakatas@hiroshima-u.ac.jp</email>
</corresp>
<fn fn-type="other">
<p>This article was submitted to Physical Chemistry and Chemical Physics, a section of the journal Frontiers in Physics</p>
</fn>
</author-notes>
<pub-date pub-type="epub">
<day>07</day>
<month>03</month>
<year>2022</year>
</pub-date>
<pub-date pub-type="collection">
<year>2022</year>
</pub-date>
<volume>10</volume>
<elocation-id>854892</elocation-id>
<history>
<date date-type="received">
<day>14</day>
<month>01</month>
<year>2022</year>
</date>
<date date-type="accepted">
<day>04</day>
<month>02</month>
<year>2022</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2022 Fujita, Matsuo and Nakata.</copyright-statement>
<copyright-year>2022</copyright-year>
<copyright-holder>Fujita, Matsuo and Nakata</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&#x20;terms.</p>
</license>
</permissions>
<abstract>
<p>Self-propelled objects, which exhibit characteristic features of motion, are proposed based on nonlinear science. At first, a self-propelled object with length like undulatory swimming is designed, i.e.,&#x20;the phase of oscillation at several points on the object is propagated in the opposite direction of motion. Second, the vertical oscillation of a camphor disk is created at an amphiphilic molecular layer developed on water. The proposed systems suggest that nonlinearity can enhance the autonomy of self-propelled objects as multidimensional motion.</p>
</abstract>
<kwd-group>
<kwd>nonlinear</kwd>
<kwd>oscillation</kwd>
<kwd>self-propelled object</kwd>
<kwd>camphor</kwd>
<kwd>nonequilibrium</kwd>
<kwd>autonomy</kwd>
</kwd-group>
<contract-num rid="cn001">JPJSBP120204602 JPJSBP120213801 JP21H00996 JP20H01871</contract-num>
<contract-sponsor id="cn001">Japan Society for the Promotion of Science<named-content content-type="fundref-id">10.13039/501100001691</named-content>
</contract-sponsor>
</article-meta>
</front>
<body>
<sec id="s1">
<title>Introduction</title>
<p>Several types of inanimate self-propelled objects such as nano wires and Janus particles have been developed for environmental, industrial, and medical applications [<xref ref-type="bibr" rid="B1">1</xref>&#x2013;<xref ref-type="bibr" rid="B4">4</xref>]. In general, self-propelled objects exhibit random motion or unidirectional motion which is determined by their shape or the external force [<xref ref-type="bibr" rid="B1">1</xref>&#x2013;<xref ref-type="bibr" rid="B7">7</xref>]. On the other hand, animate self-propelled objects such as bacteria exhibit characteristic features of motion depending on the information of the environment. These facts suggest that the autonomy of animate self-propelled objects is significantly higher than that of the inanimate ones [<xref ref-type="bibr" rid="B5">5</xref>&#x2013;<xref ref-type="bibr" rid="B7">7</xref>].</p>
<p>We introduced nonlinear science into systems to enhance their autonomy, and as a result, characteristic nonlinear phenomena such as oscillation, bifurcation, synchronization, hysteresis, and pattern formation could be reproduced experimentally [<xref ref-type="bibr" rid="B5">5</xref>&#x2013;<xref ref-type="bibr" rid="B7">7</xref>]. Several types of self-propelled objects, which exhibit characteristic features of motion from the viewpoint of nonlinear science, have been reported [<xref ref-type="bibr" rid="B5">5</xref>&#x2013;<xref ref-type="bibr" rid="B18">18</xref>]. Among them, the objects composed of camphor or camphor derivatives, of which the driving force is the difference in surface tension, have been investigated as a simple experimental system [<xref ref-type="bibr" rid="B5">5</xref>&#x2013;<xref ref-type="bibr" rid="B7">7</xref>, <xref ref-type="bibr" rid="B19">19</xref>&#x2013;<xref ref-type="bibr" rid="B35">35</xref>]. For example, a camphor disk placed on a linear water channel, reciprocating motion along the channel, was observed [<xref ref-type="bibr" rid="B5">5</xref>, <xref ref-type="bibr" rid="B6">6</xref>]. When a camphor disk attached to the bottom of a larger plastic circular plate was placed on water, oscillatory motion between rest and motion was observed, and the bifurcation between the continuous and oscillatory motion was determined by the location of the camphor disk [<xref ref-type="bibr" rid="B5">5</xref>, <xref ref-type="bibr" rid="B6">6</xref>, <xref ref-type="bibr" rid="B23">23</xref>, <xref ref-type="bibr" rid="B27">27</xref>]. The period of oscillatory motion and bifurcation between continuous and oscillatory motion was observed coupled with chemical reactions [<xref ref-type="bibr" rid="B5">5</xref>&#x2013;<xref ref-type="bibr" rid="B8">8</xref>, <xref ref-type="bibr" rid="B36">36</xref>, <xref ref-type="bibr" rid="B37">37</xref>]. When two or more camphor disks or boats were placed in the same circular water channel, synchronized swimming or collective motion was observed [<xref ref-type="bibr" rid="B5">5</xref>&#x2013;<xref ref-type="bibr" rid="B7">7</xref>]. Motion with memory, i.e.,&#x20;future motion expected by previous motion, could be realized by using a camphor disk and plastic plate [<xref ref-type="bibr" rid="B22">22</xref>, <xref ref-type="bibr" rid="B28">28</xref>, <xref ref-type="bibr" rid="B35">35</xref>]. Recently, the catch and release type of chemotaxis was realized using 6-methylcoumarin as a self-propelled object and sodium phosphate as a chemical stimulus [<xref ref-type="bibr" rid="B38">38</xref>]. These characteristic features of motion could be qualitatively reproduced by numerical calculations based on reaction&#x2013;diffusion equations and the equation of motion [<xref ref-type="bibr" rid="B5">5</xref>&#x2013;<xref ref-type="bibr" rid="B7">7</xref>, <xref ref-type="bibr" rid="B28">28</xref>, <xref ref-type="bibr" rid="B31">31</xref>&#x2013;<xref ref-type="bibr" rid="B35">35</xref>,&#x20;<xref ref-type="bibr" rid="B39">39</xref>].</p>
<p>In this article, we propose novel self-propelled objects which exhibit multidimensional motion at the air&#x2013;water interface under nonequilibrium: one is a self-propelled object with length like undulatory swimming and the other exhibits vertical oscillation of a camphor disk on an amphiphilic molecular layer developed on water. The proposed systems suggest that nonlinearity can further enhance the autonomy of self-propelled objects.</p>
</sec>
<sec id="s2">
<title>Self-Propelled Filament Like Undulatory Swimming</title>
<p>In this section, we introduce a self-propelled filament placed on water. The filament is produced from a commercial adhesive (consisting mainly of nitrocellulose and acetone), and the energy source is acetone and the driving force of motion is the difference in the surface tension around the filament since acetone reduces the surface tension. As the shape of the filament is deformed and oscillated periodically, information of wave propagation along the filament is added as characteristic features of motion in addition to information of mass movement [<xref ref-type="bibr" rid="B40">40</xref>]. When one of the end points of the single filament is fixed on the edge of the chamber, periodic pendulum motion is produced and the phase of the filament near the fixed edge progresses faster in comparison with the phase of the free edge for the pendulum motion. When two filaments are coupled together, in-phase and out-phase synchronizations are produced depending on the distance between them and the initial floating&#x20;state.</p>
<p>We propose a self-propelled filament of which one of the end points is adhered to the free plastic film with V-shape to introduce heterogeneity. <xref ref-type="fig" rid="F1">Figure&#x20;1</xref> shows (a) snapshots of the filament and (b) outline of points a, b, c, and d on the filament. The filament moves in the direction of the plastic film while oscillating except for point a, i.e.,&#x20;the head of the filament. The phase of oscillation was propagated from b to d, i.e.,&#x20;in the opposite direction of the motion. The propagation of the phase oscillation in the animate undulatory swimming is the same as the direction of motion. Thus, the direction of the phase propagation of our inanimate meandering filament is opposite to the animate undulatory swimming like &#x201c;moon walk&#x201d; by MJ.&#x20;The opposite direction of phase propagation suggests that our inanimate filament is passive on the motion since the Marangoni flow occurs in the opposite direction of motion. The shape and size of the head of the filament should be improved to make the direction of the phase propagation the same as animate undulatory swimming.</p>
<fig id="F1" position="float">
<label>FIGURE 1</label>
<caption>
<p>
<bold>(A)</bold> Snapshots of the self-propelled filament (time interval: 0.2&#xa0;s) and <bold>(B)</bold> outline of the points a, b, c, and d on the filament from top view. The arrow around the middle of the outline denotes the direction of motion. The object around the left side of the outline denotes the schematic illustration of the filament. [See the actual movies in the supporting information as <xref ref-type="sec" rid="s10">Supplementary Movie S1</xref> (10&#xd7; speed)]. 2.2, 2.1, and 2.0&#xa0;s on the blue circles in <bold>(A)</bold> denote the time at one of the maximum values of the oscillation on the outlines of the points b, c, and d.</p>
</caption>
<graphic xlink:href="fphy-10-854892-g001.tif"/>
</fig>
</sec>
<sec id="s3">
<title>Vertical Oscillatory Motion of a Camphor Disk Placed on an Amphiphilic Molecular Layer Developed at the Air&#x2013;Water Interface</title>
<p>In this chapter, we introduce vertical oscillatory motion of a camphor disk placed on an amphiphilic molecular layer developed at the air&#x2013;water interface. Here, nervonic acid is used as an amphiphilic substance [<xref ref-type="bibr" rid="B24">24</xref>]. The surface pressure <italic>vs</italic>. area isotherm exhibits a transition point corresponding to a phase transition between the fluid and fluid/condensed phases of nervonic acid. The characteristic features of motion, i.e.,&#x20;no motion, oscillatory motion, and continuous motion, are determined by not only the value of the surface pressure but also the nature of the phase in the nervonic acid molecular layer. These results suggest that the characteristic features of motion can be designed based on the chemical structure of an amphiphilic molecule.</p>
<p>We propose vertical oscillation of a camphor disk (diameter: 3&#xa0;mm, thickness: 1&#xa0;mm) placed at the air&#x2013;water interface. Here, nervonic acid which is developed on water is in the fluid/condensed phase. <xref ref-type="fig" rid="F2">Figure&#x20;2</xref> shows (a1) snapshots of one cycle of vertical oscillation and (a2) time-variation of the lateral location of a camphor disk. The camphor disk exhibited not only lateral oscillation but also vertical oscillation even at the air&#x2013;water interface. The vertical oscillation may be generated by the following mechanism. As the surface pressure of the nervonic acid molecular layer (<italic>&#x3a0;</italic>
<sub>na</sub> &#x223c; 8&#xa0;mN&#xa0;m<sup>&#x2212;1</sup> at 293&#xa0;K and 40&#xa0;&#xc5; molecule<sup>&#x2212;1</sup>) is similar to that of the camphor (<italic>&#x3a0;</italic>
<sub>c</sub>, the saturated value of <italic>&#x3a0;</italic>
<sub>c</sub> &#x223c; 17&#xa0;mN&#xa0;m<sup>&#x2212;1</sup>), repetition between the resting and motion states is possible since no motion at <italic>&#x3a0;</italic>
<sub>na</sub> &#x2265; <italic>&#x3a0;</italic>
<sub>c</sub> and motion at <italic>&#x3a0;</italic>
<sub>na</sub> &#x2264; <italic>&#x3a0;</italic>
<sub>c</sub> occur. The periodicity and nonlinearity of the oscillation were observed as the fundamental frequency (&#x223c;0.3&#xa0;Hz) and the higher harmonics in the linear spectrum of the fast Fourier transformation (FFT) for <xref ref-type="fig" rid="F2">Figure&#x20;2A2</xref>, respectively (see <xref ref-type="fig" rid="F2">Figure&#x20;2A3</xref>). Vertical oscillation may occur due to the repetition of fluid and fluid/condensed phases since the development and sublimation of the camphor molecules at the air&#x2013;water interface induces the phase transition from the fluid/condensed to the fluid phase and <italic>vice versa</italic>, respectively. No oscillation was observed at 298&#xa0;K and 40&#xa0;&#xc5; molecule<sup>&#x2212;1</sup>, i.e.,&#x20;the fluid phase, as shown in <xref ref-type="fig" rid="F2">Figure&#x20;2B</xref>. The change in the surface pressure around the disk induces the change in the meniscus at the camphor solid/water interface including nervonic acid, and as a result, the vertical oscillation occurs.</p>
<fig id="F2" position="float">
<label>FIGURE 2</label>
<caption>
<p>
<bold>(A1)</bold> Snapshots of vertical oscillation of a camphor disk (time interval: 0.2&#xa0;s, view from an angle) and <bold>(A2)</bold> time-variation of the location of the camphor disk on the vertical axis, <bold>(A3)</bold> linear spectrum of FFT for <bold>(A2)</bold> at 293&#xa0;K and 40&#xa0;&#xc5; molecule<sup>&#x2212;1</sup> and <bold>(B)</bold> time-variation of the location of the camphor disk on the vertical axis at 298&#xa0;K and 40&#xa0;&#xc5; molecule<sup>&#x2212;1</sup>. A black circle on the camphor disk was marked to measure the vertical location using the laser displacement meter. [See the actual movies in the supporting information as <xref ref-type="sec" rid="s10">Supplementary Movie S2</xref> (10&#xd7; speed)].</p>
</caption>
<graphic xlink:href="fphy-10-854892-g002.tif"/>
</fig>
</sec>
<sec id="s4">
<title>Conclusion and Outlook</title>
<p>In this article, we proposed novel types of self-propelled objects which exhibit multidimensional motion from the viewpoint of nonlinear science. Further multidimensional motion, such as translation including rotation like drill and pattern formation coupled with motion like collective motion, will be created in the near future by enhancing autonomy.</p>
</sec>
</body>
<back>
<sec id="s5">
<title>Data Availability Statement</title>
<p>The data that support the findings of this study are available from the corresponding author, SN, upon reasonable request.</p>
</sec>
<sec id="s6">
<title>Author Contributions</title>
<p>RF performed the examination, analyzed the experimental results, and prepared the manuscript. MM analyzed the data and edited the manuscript. SN planned the experimental system and edited the manuscript.</p>
</sec>
<sec id="s7">
<title>Funding</title>
<p>This study was supported by JSPS KAKENHI (Grant Nos. JP20H02712, JP20H01871, and JP21H00996), the Cooperative Research Program of &#x201c;Network Joint Research Center for Materials and Devices&#x201d; (No. 20211061) to SN, JSPS Bilateral Joint Research Project between Japan and the Polish Academy of Sciences (JPJSBP120204602), and JSPS Japan&#x2013;Hungary Bilateral Joint Research Project (JPJSBP120213801).</p>
</sec>
<sec sec-type="COI-statement" id="s8">
<title>Conflict of Interest</title>
<p>The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.</p>
</sec>
<sec sec-type="disclaimer" id="s9">
<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>
<ack>
<p>We acknowledge Mr. Katsuhiko Kayahara for his technical support on the examination.</p>
</ack>
<sec id="s10">
<title>Supplementary Material</title>
<p>The Supplementary Material for this article can be found online at: <ext-link ext-link-type="uri" xlink:href="https://www.frontiersin.org/articles/10.3389/fphy.2022.854892/full#supplementary-material">https://www.frontiersin.org/articles/10.3389/fphy.2022.854892/full&#x23;supplementary-material</ext-link>
</p>
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