Loading…

Molecular dynamics model for nano-motions of FePd nanohelices

Shrinkage and relaxation motions of flexible FePd nanohelices of FePd nanorobots are simulated by a molecular dynamics (MD) model where FePd is a paramagnetic shape memory alloy that can exhibit phase transformation accompanied by softening of the nanohelix under an applied magnetic field (H-field)....

Full description

Saved in:
Bibliographic Details
Published in:Journal of applied physics 2017-04, Vol.121 (15)
Main Authors: Taya, M., Xu, C., Matsuse, T., Muraishi, S.
Format: Article
Language:English
Subjects:
Citations: Items that this one cites
Items that cite this one
Online Access:Get full text
Tags: Add Tag
No Tags, Be the first to tag this record!
cited_by cdi_FETCH-LOGICAL-c406t-c9d94b9be9a8f2704878821e961bad731ec5dffe972678b256bb872a8620c4c83
cites cdi_FETCH-LOGICAL-c406t-c9d94b9be9a8f2704878821e961bad731ec5dffe972678b256bb872a8620c4c83
container_end_page
container_issue 15
container_start_page
container_title Journal of applied physics
container_volume 121
creator Taya, M.
Xu, C.
Matsuse, T.
Muraishi, S.
description Shrinkage and relaxation motions of flexible FePd nanohelices of FePd nanorobots are simulated by a molecular dynamics (MD) model where FePd is a paramagnetic shape memory alloy that can exhibit phase transformation accompanied by softening of the nanohelix under an applied magnetic field (H-field). Two designs of FePd nanorobots are used: (i) a FePd cylindrical head connected to a FePd nanohelix tail and (ii) a FePd nanohelix alone. The geometry and dimensions of the FePd robots are taken after the as-processed FePd nanorobots. In the MD simulation, the FePd head and nanohelix are divided into a number of segmented FePd spheres, each having its magnetic moment. The results of the MD model reveal that upon the applied constant magnetic field, the initial gaps (g = 3 nm) between the adjacent turns of the FePd nanohelix are closed, resulting in the total shrinkage (Stot) of 47 nm of the FePd nanorobot. The effects of the applied H-field on Stot are examined by using the MD model and the M-H curve of FePd fitted with Langevin type, resulting in the smaller applied magnetic field leading to the smaller Stot. The results of the MD model provide us with an effective tool in the analysis and design of new nanorobots based on the paramagnetic shape memory alloy of FePd nanohelices that can exert dynamic vibrations on target cells under the oscillating magnetic field.
doi_str_mv 10.1063/1.4979474
format article
fullrecord <record><control><sourceid>proquest_scita</sourceid><recordid>TN_cdi_proquest_journals_2124502073</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>2124502073</sourcerecordid><originalsourceid>FETCH-LOGICAL-c406t-c9d94b9be9a8f2704878821e961bad731ec5dffe972678b256bb872a8620c4c83</originalsourceid><addsrcrecordid>eNqd0E1LAzEQBuAgCtbqwX-w4Elh60w2u0kOHqRYFSp60HPI5gO37G5qshX6793agndPAzMPM8xLyCXCDKEqbnHGJJeMsyMyQRAy52UJx2QCQDEX4-iUnKW0AkAUhZyQu5fQOrNpdczsttddY1LWBevazIeY9boPeReGJvQpCz5buDf72_x0bWNcOicnXrfJXRzqlHwsHt7nT_ny9fF5fr_MDYNqyI20ktWydlILTzkwwYWg6GSFtba8QGdK672TnFZc1LSs6lpwqkVFwTAjiim52u9dx_C1cWlQq7CJ_XhSUaSsBAq8GNX1XpkYUorOq3VsOh23CkHt0lGoDumM9mZvk2kGvXvwf_g7xD-o1tYXP-1xceA</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>2124502073</pqid></control><display><type>article</type><title>Molecular dynamics model for nano-motions of FePd nanohelices</title><source>American Institute of Physics:Jisc Collections:Transitional Journals Agreement 2021-23 (Reading list)</source><creator>Taya, M. ; Xu, C. ; Matsuse, T. ; Muraishi, S.</creator><creatorcontrib>Taya, M. ; Xu, C. ; Matsuse, T. ; Muraishi, S.</creatorcontrib><description>Shrinkage and relaxation motions of flexible FePd nanohelices of FePd nanorobots are simulated by a molecular dynamics (MD) model where FePd is a paramagnetic shape memory alloy that can exhibit phase transformation accompanied by softening of the nanohelix under an applied magnetic field (H-field). Two designs of FePd nanorobots are used: (i) a FePd cylindrical head connected to a FePd nanohelix tail and (ii) a FePd nanohelix alone. The geometry and dimensions of the FePd robots are taken after the as-processed FePd nanorobots. In the MD simulation, the FePd head and nanohelix are divided into a number of segmented FePd spheres, each having its magnetic moment. The results of the MD model reveal that upon the applied constant magnetic field, the initial gaps (g = 3 nm) between the adjacent turns of the FePd nanohelix are closed, resulting in the total shrinkage (Stot) of 47 nm of the FePd nanorobot. The effects of the applied H-field on Stot are examined by using the MD model and the M-H curve of FePd fitted with Langevin type, resulting in the smaller applied magnetic field leading to the smaller Stot. The results of the MD model provide us with an effective tool in the analysis and design of new nanorobots based on the paramagnetic shape memory alloy of FePd nanohelices that can exert dynamic vibrations on target cells under the oscillating magnetic field.</description><identifier>ISSN: 0021-8979</identifier><identifier>EISSN: 1089-7550</identifier><identifier>DOI: 10.1063/1.4979474</identifier><identifier>CODEN: JAPIAU</identifier><language>eng</language><publisher>Melville: American Institute of Physics</publisher><subject>Applied physics ; Computer simulation ; Ferrous alloys ; Intermetallic compounds ; Iron compounds ; Magnetic fields ; Magnetic moments ; Magnetism ; Martensitic transformations ; Molecular dynamics ; Palladium compounds ; Phase transitions ; Shape memory alloys ; Shrinkage</subject><ispartof>Journal of applied physics, 2017-04, Vol.121 (15)</ispartof><rights>Author(s)</rights><rights>2017 Author(s). Published by AIP Publishing.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c406t-c9d94b9be9a8f2704878821e961bad731ec5dffe972678b256bb872a8620c4c83</citedby><cites>FETCH-LOGICAL-c406t-c9d94b9be9a8f2704878821e961bad731ec5dffe972678b256bb872a8620c4c83</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids></links><search><creatorcontrib>Taya, M.</creatorcontrib><creatorcontrib>Xu, C.</creatorcontrib><creatorcontrib>Matsuse, T.</creatorcontrib><creatorcontrib>Muraishi, S.</creatorcontrib><title>Molecular dynamics model for nano-motions of FePd nanohelices</title><title>Journal of applied physics</title><description>Shrinkage and relaxation motions of flexible FePd nanohelices of FePd nanorobots are simulated by a molecular dynamics (MD) model where FePd is a paramagnetic shape memory alloy that can exhibit phase transformation accompanied by softening of the nanohelix under an applied magnetic field (H-field). Two designs of FePd nanorobots are used: (i) a FePd cylindrical head connected to a FePd nanohelix tail and (ii) a FePd nanohelix alone. The geometry and dimensions of the FePd robots are taken after the as-processed FePd nanorobots. In the MD simulation, the FePd head and nanohelix are divided into a number of segmented FePd spheres, each having its magnetic moment. The results of the MD model reveal that upon the applied constant magnetic field, the initial gaps (g = 3 nm) between the adjacent turns of the FePd nanohelix are closed, resulting in the total shrinkage (Stot) of 47 nm of the FePd nanorobot. The effects of the applied H-field on Stot are examined by using the MD model and the M-H curve of FePd fitted with Langevin type, resulting in the smaller applied magnetic field leading to the smaller Stot. The results of the MD model provide us with an effective tool in the analysis and design of new nanorobots based on the paramagnetic shape memory alloy of FePd nanohelices that can exert dynamic vibrations on target cells under the oscillating magnetic field.</description><subject>Applied physics</subject><subject>Computer simulation</subject><subject>Ferrous alloys</subject><subject>Intermetallic compounds</subject><subject>Iron compounds</subject><subject>Magnetic fields</subject><subject>Magnetic moments</subject><subject>Magnetism</subject><subject>Martensitic transformations</subject><subject>Molecular dynamics</subject><subject>Palladium compounds</subject><subject>Phase transitions</subject><subject>Shape memory alloys</subject><subject>Shrinkage</subject><issn>0021-8979</issn><issn>1089-7550</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2017</creationdate><recordtype>article</recordtype><recordid>eNqd0E1LAzEQBuAgCtbqwX-w4Elh60w2u0kOHqRYFSp60HPI5gO37G5qshX6793agndPAzMPM8xLyCXCDKEqbnHGJJeMsyMyQRAy52UJx2QCQDEX4-iUnKW0AkAUhZyQu5fQOrNpdczsttddY1LWBevazIeY9boPeReGJvQpCz5buDf72_x0bWNcOicnXrfJXRzqlHwsHt7nT_ny9fF5fr_MDYNqyI20ktWydlILTzkwwYWg6GSFtba8QGdK672TnFZc1LSs6lpwqkVFwTAjiim52u9dx_C1cWlQq7CJ_XhSUaSsBAq8GNX1XpkYUorOq3VsOh23CkHt0lGoDumM9mZvk2kGvXvwf_g7xD-o1tYXP-1xceA</recordid><startdate>20170421</startdate><enddate>20170421</enddate><creator>Taya, M.</creator><creator>Xu, C.</creator><creator>Matsuse, T.</creator><creator>Muraishi, S.</creator><general>American Institute of Physics</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope></search><sort><creationdate>20170421</creationdate><title>Molecular dynamics model for nano-motions of FePd nanohelices</title><author>Taya, M. ; Xu, C. ; Matsuse, T. ; Muraishi, S.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c406t-c9d94b9be9a8f2704878821e961bad731ec5dffe972678b256bb872a8620c4c83</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2017</creationdate><topic>Applied physics</topic><topic>Computer simulation</topic><topic>Ferrous alloys</topic><topic>Intermetallic compounds</topic><topic>Iron compounds</topic><topic>Magnetic fields</topic><topic>Magnetic moments</topic><topic>Magnetism</topic><topic>Martensitic transformations</topic><topic>Molecular dynamics</topic><topic>Palladium compounds</topic><topic>Phase transitions</topic><topic>Shape memory alloys</topic><topic>Shrinkage</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Taya, M.</creatorcontrib><creatorcontrib>Xu, C.</creatorcontrib><creatorcontrib>Matsuse, T.</creatorcontrib><creatorcontrib>Muraishi, S.</creatorcontrib><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of applied physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Taya, M.</au><au>Xu, C.</au><au>Matsuse, T.</au><au>Muraishi, S.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Molecular dynamics model for nano-motions of FePd nanohelices</atitle><jtitle>Journal of applied physics</jtitle><date>2017-04-21</date><risdate>2017</risdate><volume>121</volume><issue>15</issue><issn>0021-8979</issn><eissn>1089-7550</eissn><coden>JAPIAU</coden><abstract>Shrinkage and relaxation motions of flexible FePd nanohelices of FePd nanorobots are simulated by a molecular dynamics (MD) model where FePd is a paramagnetic shape memory alloy that can exhibit phase transformation accompanied by softening of the nanohelix under an applied magnetic field (H-field). Two designs of FePd nanorobots are used: (i) a FePd cylindrical head connected to a FePd nanohelix tail and (ii) a FePd nanohelix alone. The geometry and dimensions of the FePd robots are taken after the as-processed FePd nanorobots. In the MD simulation, the FePd head and nanohelix are divided into a number of segmented FePd spheres, each having its magnetic moment. The results of the MD model reveal that upon the applied constant magnetic field, the initial gaps (g = 3 nm) between the adjacent turns of the FePd nanohelix are closed, resulting in the total shrinkage (Stot) of 47 nm of the FePd nanorobot. The effects of the applied H-field on Stot are examined by using the MD model and the M-H curve of FePd fitted with Langevin type, resulting in the smaller applied magnetic field leading to the smaller Stot. The results of the MD model provide us with an effective tool in the analysis and design of new nanorobots based on the paramagnetic shape memory alloy of FePd nanohelices that can exert dynamic vibrations on target cells under the oscillating magnetic field.</abstract><cop>Melville</cop><pub>American Institute of Physics</pub><doi>10.1063/1.4979474</doi><tpages>11</tpages><oa>free_for_read</oa></addata></record>
fulltext fulltext
identifier ISSN: 0021-8979
ispartof Journal of applied physics, 2017-04, Vol.121 (15)
issn 0021-8979
1089-7550
language eng
recordid cdi_proquest_journals_2124502073
source American Institute of Physics:Jisc Collections:Transitional Journals Agreement 2021-23 (Reading list)
subjects Applied physics
Computer simulation
Ferrous alloys
Intermetallic compounds
Iron compounds
Magnetic fields
Magnetic moments
Magnetism
Martensitic transformations
Molecular dynamics
Palladium compounds
Phase transitions
Shape memory alloys
Shrinkage
title Molecular dynamics model for nano-motions of FePd nanohelices
url http://sfxeu10.hosted.exlibrisgroup.com/loughborough?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-07T16%3A39%3A06IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest_scita&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Molecular%20dynamics%20model%20for%20nano-motions%20of%20FePd%20nanohelices&rft.jtitle=Journal%20of%20applied%20physics&rft.au=Taya,%20M.&rft.date=2017-04-21&rft.volume=121&rft.issue=15&rft.issn=0021-8979&rft.eissn=1089-7550&rft.coden=JAPIAU&rft_id=info:doi/10.1063/1.4979474&rft_dat=%3Cproquest_scita%3E2124502073%3C/proquest_scita%3E%3Cgrp_id%3Ecdi_FETCH-LOGICAL-c406t-c9d94b9be9a8f2704878821e961bad731ec5dffe972678b256bb872a8620c4c83%3C/grp_id%3E%3Coa%3E%3C/oa%3E%3Curl%3E%3C/url%3E&rft_id=info:oai/&rft_pqid=2124502073&rft_id=info:pmid/&rfr_iscdi=true