Loading…

Sensing strain with Ni-Mn-Ga

•Voltage amplitude in the sensing coil increases with decreasing tensile strain.•Strain sensing resolution decreases with increasing bias magnetic field.•Hysteresis in voltage occurred between loading and unloading during dynamic tests.•Static test matched the compressive portion of the dynamic test...

Full description

Saved in:
Bibliographic Details
Published in:Sensors and actuators. A. Physical. 2018-01, Vol.269, p.137-144
Main Authors: Hobza, Anthony, Patrick, Charles L., Ullakko, Kari, Rafla, Nader, Lindquist, Paul, Müllner, Peter
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-c325t-984e9c714565de2087e0e3108f64f65e2a3c11e6ce6039fd49a02c6f89015aba3
cites cdi_FETCH-LOGICAL-c325t-984e9c714565de2087e0e3108f64f65e2a3c11e6ce6039fd49a02c6f89015aba3
container_end_page 144
container_issue
container_start_page 137
container_title Sensors and actuators. A. Physical.
container_volume 269
creator Hobza, Anthony
Patrick, Charles L.
Ullakko, Kari
Rafla, Nader
Lindquist, Paul
Müllner, Peter
description •Voltage amplitude in the sensing coil increases with decreasing tensile strain.•Strain sensing resolution decreases with increasing bias magnetic field.•Hysteresis in voltage occurred between loading and unloading during dynamic tests.•Static test matched the compressive portion of the dynamic test.•Hysteresis increased with increasing strain amplitude and frequency. Deformation rearranges the crystal lattice in magnetic shape memory alloys, which changes all anisotropic properties of the material. This study investigates leveraging the deformation-induced change of magnetic permeability for a strain measurement technique. A Ni-Mn-Ga single crystal placed inside a doubly wound coil with a primary and a secondary winding was used as a strain sensor. An AC voltage excited the primary coil and the secondary voltage was measured as the sample was strained from 0 to 5.2%. This method varies from other methods that utilize complex magnetic circuits, require high magnetic fields, or other sensing methods such as Hall probes. When the sensor element was tested statically by compressing the element manually against a bias magnetic field perpendicular to the load axis, the voltage output varied from 129.7mV to 164.2mV. The dynamic performance of the sensor was tested by cycling the element between 25 and 100Hz in compression against a bias magnetic field in a displacement controlled magneto-mechanical test system. The bias magnetic field was varied from 0.2 to 0.8T (0.16 to 0.64MA/m) while the cyclic displacement was varied from 0.5 to 4.5% strain. The voltage amplitude of the signal in the secondary coil increased with decreasing tensile strain. The full scale RMS voltage at a 200 mm stroke increased from 53.0mV to 78.4mV as the bias magnetic field decreased from 0.8T to 0.2T. As the element was compressed, there was no difference in the sensor output voltage between the static and dynamic tests. When the element expanded during unloading, the voltage output of the sensor from the static test matched the voltage output during compression. For the dynamic testing, the voltage output of the sensor exhibited a hysteresis from the loading voltage output, the hysteresis increased when the strain rate increased.
doi_str_mv 10.1016/j.sna.2017.11.002
format article
fullrecord <record><control><sourceid>proquest_cross</sourceid><recordid>TN_cdi_proquest_journals_2010773249</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><els_id>S092442471731035X</els_id><sourcerecordid>2010773249</sourcerecordid><originalsourceid>FETCH-LOGICAL-c325t-984e9c714565de2087e0e3108f64f65e2a3c11e6ce6039fd49a02c6f89015aba3</originalsourceid><addsrcrecordid>eNp9kLFOwzAQhi0EEqXwAEgMlZgT7mzHjsWEKlqQCgzAbBnnAo7AKXYK4u1JVWamW_7vv7uPsVOEEgHVRVfm6EoOqEvEEoDvsQnWWhQClNlnEzBcFpJLfciOcu4AQAitJ-zskWIO8XWWh-RCnH2H4W12H4q7WCzdMTto3Xumk785Zc-L66f5TbF6WN7Or1aFF7waClNLMl6jrFTVEIdaE5BAqFslW1URd8IjkvKkQJi2kcYB96qtDWDlXpyYsvNd7zr1nxvKg-36TYrjSjt-BFoLLs2Ywl3Kpz7nRK1dp_Dh0o9FsFsJtrOjhC2iLaIdJYzM5Y6h8fyvQMlmHyh6akIiP9imD__Qv-qJYUE</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>2010773249</pqid></control><display><type>article</type><title>Sensing strain with Ni-Mn-Ga</title><source>ScienceDirect Freedom Collection</source><creator>Hobza, Anthony ; Patrick, Charles L. ; Ullakko, Kari ; Rafla, Nader ; Lindquist, Paul ; Müllner, Peter</creator><creatorcontrib>Hobza, Anthony ; Patrick, Charles L. ; Ullakko, Kari ; Rafla, Nader ; Lindquist, Paul ; Müllner, Peter</creatorcontrib><description>•Voltage amplitude in the sensing coil increases with decreasing tensile strain.•Strain sensing resolution decreases with increasing bias magnetic field.•Hysteresis in voltage occurred between loading and unloading during dynamic tests.•Static test matched the compressive portion of the dynamic test.•Hysteresis increased with increasing strain amplitude and frequency. Deformation rearranges the crystal lattice in magnetic shape memory alloys, which changes all anisotropic properties of the material. This study investigates leveraging the deformation-induced change of magnetic permeability for a strain measurement technique. A Ni-Mn-Ga single crystal placed inside a doubly wound coil with a primary and a secondary winding was used as a strain sensor. An AC voltage excited the primary coil and the secondary voltage was measured as the sample was strained from 0 to 5.2%. This method varies from other methods that utilize complex magnetic circuits, require high magnetic fields, or other sensing methods such as Hall probes. When the sensor element was tested statically by compressing the element manually against a bias magnetic field perpendicular to the load axis, the voltage output varied from 129.7mV to 164.2mV. The dynamic performance of the sensor was tested by cycling the element between 25 and 100Hz in compression against a bias magnetic field in a displacement controlled magneto-mechanical test system. The bias magnetic field was varied from 0.2 to 0.8T (0.16 to 0.64MA/m) while the cyclic displacement was varied from 0.5 to 4.5% strain. The voltage amplitude of the signal in the secondary coil increased with decreasing tensile strain. The full scale RMS voltage at a 200 mm stroke increased from 53.0mV to 78.4mV as the bias magnetic field decreased from 0.8T to 0.2T. As the element was compressed, there was no difference in the sensor output voltage between the static and dynamic tests. When the element expanded during unloading, the voltage output of the sensor from the static test matched the voltage output during compression. For the dynamic testing, the voltage output of the sensor exhibited a hysteresis from the loading voltage output, the hysteresis increased when the strain rate increased.</description><identifier>ISSN: 0924-4247</identifier><identifier>EISSN: 1873-3069</identifier><identifier>DOI: 10.1016/j.sna.2017.11.002</identifier><language>eng</language><publisher>Lausanne: Elsevier B.V</publisher><subject>Alloys ; Anisotropy ; Bias ; Coils (windings) ; Compression tests ; Crystal lattices ; Deformation ; Dynamic tests ; Electric potential ; Hall probes ; Hysteresis ; Magnetic circuits ; Magnetic fields ; Magnetic permeability ; Magnetic properties ; Magnetic shape memory ; Magnetic susceptibility ; Magneto-mechanics ; Manganese ; Mechanical tests ; Nickel ; Sensors ; Shape memory alloys ; Single crystals ; Strain measurement ; Strain rate ; Strain sensor</subject><ispartof>Sensors and actuators. A. Physical., 2018-01, Vol.269, p.137-144</ispartof><rights>2017 Elsevier B.V.</rights><rights>Copyright Elsevier BV Jan 1, 2018</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c325t-984e9c714565de2087e0e3108f64f65e2a3c11e6ce6039fd49a02c6f89015aba3</citedby><cites>FETCH-LOGICAL-c325t-984e9c714565de2087e0e3108f64f65e2a3c11e6ce6039fd49a02c6f89015aba3</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>Hobza, Anthony</creatorcontrib><creatorcontrib>Patrick, Charles L.</creatorcontrib><creatorcontrib>Ullakko, Kari</creatorcontrib><creatorcontrib>Rafla, Nader</creatorcontrib><creatorcontrib>Lindquist, Paul</creatorcontrib><creatorcontrib>Müllner, Peter</creatorcontrib><title>Sensing strain with Ni-Mn-Ga</title><title>Sensors and actuators. A. Physical.</title><description>•Voltage amplitude in the sensing coil increases with decreasing tensile strain.•Strain sensing resolution decreases with increasing bias magnetic field.•Hysteresis in voltage occurred between loading and unloading during dynamic tests.•Static test matched the compressive portion of the dynamic test.•Hysteresis increased with increasing strain amplitude and frequency. Deformation rearranges the crystal lattice in magnetic shape memory alloys, which changes all anisotropic properties of the material. This study investigates leveraging the deformation-induced change of magnetic permeability for a strain measurement technique. A Ni-Mn-Ga single crystal placed inside a doubly wound coil with a primary and a secondary winding was used as a strain sensor. An AC voltage excited the primary coil and the secondary voltage was measured as the sample was strained from 0 to 5.2%. This method varies from other methods that utilize complex magnetic circuits, require high magnetic fields, or other sensing methods such as Hall probes. When the sensor element was tested statically by compressing the element manually against a bias magnetic field perpendicular to the load axis, the voltage output varied from 129.7mV to 164.2mV. The dynamic performance of the sensor was tested by cycling the element between 25 and 100Hz in compression against a bias magnetic field in a displacement controlled magneto-mechanical test system. The bias magnetic field was varied from 0.2 to 0.8T (0.16 to 0.64MA/m) while the cyclic displacement was varied from 0.5 to 4.5% strain. The voltage amplitude of the signal in the secondary coil increased with decreasing tensile strain. The full scale RMS voltage at a 200 mm stroke increased from 53.0mV to 78.4mV as the bias magnetic field decreased from 0.8T to 0.2T. As the element was compressed, there was no difference in the sensor output voltage between the static and dynamic tests. When the element expanded during unloading, the voltage output of the sensor from the static test matched the voltage output during compression. For the dynamic testing, the voltage output of the sensor exhibited a hysteresis from the loading voltage output, the hysteresis increased when the strain rate increased.</description><subject>Alloys</subject><subject>Anisotropy</subject><subject>Bias</subject><subject>Coils (windings)</subject><subject>Compression tests</subject><subject>Crystal lattices</subject><subject>Deformation</subject><subject>Dynamic tests</subject><subject>Electric potential</subject><subject>Hall probes</subject><subject>Hysteresis</subject><subject>Magnetic circuits</subject><subject>Magnetic fields</subject><subject>Magnetic permeability</subject><subject>Magnetic properties</subject><subject>Magnetic shape memory</subject><subject>Magnetic susceptibility</subject><subject>Magneto-mechanics</subject><subject>Manganese</subject><subject>Mechanical tests</subject><subject>Nickel</subject><subject>Sensors</subject><subject>Shape memory alloys</subject><subject>Single crystals</subject><subject>Strain measurement</subject><subject>Strain rate</subject><subject>Strain sensor</subject><issn>0924-4247</issn><issn>1873-3069</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2018</creationdate><recordtype>article</recordtype><recordid>eNp9kLFOwzAQhi0EEqXwAEgMlZgT7mzHjsWEKlqQCgzAbBnnAo7AKXYK4u1JVWamW_7vv7uPsVOEEgHVRVfm6EoOqEvEEoDvsQnWWhQClNlnEzBcFpJLfciOcu4AQAitJ-zskWIO8XWWh-RCnH2H4W12H4q7WCzdMTto3Xumk785Zc-L66f5TbF6WN7Or1aFF7waClNLMl6jrFTVEIdaE5BAqFslW1URd8IjkvKkQJi2kcYB96qtDWDlXpyYsvNd7zr1nxvKg-36TYrjSjt-BFoLLs2Ywl3Kpz7nRK1dp_Dh0o9FsFsJtrOjhC2iLaIdJYzM5Y6h8fyvQMlmHyh6akIiP9imD__Qv-qJYUE</recordid><startdate>20180101</startdate><enddate>20180101</enddate><creator>Hobza, Anthony</creator><creator>Patrick, Charles L.</creator><creator>Ullakko, Kari</creator><creator>Rafla, Nader</creator><creator>Lindquist, Paul</creator><creator>Müllner, Peter</creator><general>Elsevier B.V</general><general>Elsevier BV</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7TB</scope><scope>7U5</scope><scope>8FD</scope><scope>FR3</scope><scope>L7M</scope></search><sort><creationdate>20180101</creationdate><title>Sensing strain with Ni-Mn-Ga</title><author>Hobza, Anthony ; Patrick, Charles L. ; Ullakko, Kari ; Rafla, Nader ; Lindquist, Paul ; Müllner, Peter</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c325t-984e9c714565de2087e0e3108f64f65e2a3c11e6ce6039fd49a02c6f89015aba3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2018</creationdate><topic>Alloys</topic><topic>Anisotropy</topic><topic>Bias</topic><topic>Coils (windings)</topic><topic>Compression tests</topic><topic>Crystal lattices</topic><topic>Deformation</topic><topic>Dynamic tests</topic><topic>Electric potential</topic><topic>Hall probes</topic><topic>Hysteresis</topic><topic>Magnetic circuits</topic><topic>Magnetic fields</topic><topic>Magnetic permeability</topic><topic>Magnetic properties</topic><topic>Magnetic shape memory</topic><topic>Magnetic susceptibility</topic><topic>Magneto-mechanics</topic><topic>Manganese</topic><topic>Mechanical tests</topic><topic>Nickel</topic><topic>Sensors</topic><topic>Shape memory alloys</topic><topic>Single crystals</topic><topic>Strain measurement</topic><topic>Strain rate</topic><topic>Strain sensor</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Hobza, Anthony</creatorcontrib><creatorcontrib>Patrick, Charles L.</creatorcontrib><creatorcontrib>Ullakko, Kari</creatorcontrib><creatorcontrib>Rafla, Nader</creatorcontrib><creatorcontrib>Lindquist, Paul</creatorcontrib><creatorcontrib>Müllner, Peter</creatorcontrib><collection>CrossRef</collection><collection>Mechanical &amp; Transportation Engineering Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Engineering Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Sensors and actuators. A. Physical.</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Hobza, Anthony</au><au>Patrick, Charles L.</au><au>Ullakko, Kari</au><au>Rafla, Nader</au><au>Lindquist, Paul</au><au>Müllner, Peter</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Sensing strain with Ni-Mn-Ga</atitle><jtitle>Sensors and actuators. A. Physical.</jtitle><date>2018-01-01</date><risdate>2018</risdate><volume>269</volume><spage>137</spage><epage>144</epage><pages>137-144</pages><issn>0924-4247</issn><eissn>1873-3069</eissn><abstract>•Voltage amplitude in the sensing coil increases with decreasing tensile strain.•Strain sensing resolution decreases with increasing bias magnetic field.•Hysteresis in voltage occurred between loading and unloading during dynamic tests.•Static test matched the compressive portion of the dynamic test.•Hysteresis increased with increasing strain amplitude and frequency. Deformation rearranges the crystal lattice in magnetic shape memory alloys, which changes all anisotropic properties of the material. This study investigates leveraging the deformation-induced change of magnetic permeability for a strain measurement technique. A Ni-Mn-Ga single crystal placed inside a doubly wound coil with a primary and a secondary winding was used as a strain sensor. An AC voltage excited the primary coil and the secondary voltage was measured as the sample was strained from 0 to 5.2%. This method varies from other methods that utilize complex magnetic circuits, require high magnetic fields, or other sensing methods such as Hall probes. When the sensor element was tested statically by compressing the element manually against a bias magnetic field perpendicular to the load axis, the voltage output varied from 129.7mV to 164.2mV. The dynamic performance of the sensor was tested by cycling the element between 25 and 100Hz in compression against a bias magnetic field in a displacement controlled magneto-mechanical test system. The bias magnetic field was varied from 0.2 to 0.8T (0.16 to 0.64MA/m) while the cyclic displacement was varied from 0.5 to 4.5% strain. The voltage amplitude of the signal in the secondary coil increased with decreasing tensile strain. The full scale RMS voltage at a 200 mm stroke increased from 53.0mV to 78.4mV as the bias magnetic field decreased from 0.8T to 0.2T. As the element was compressed, there was no difference in the sensor output voltage between the static and dynamic tests. When the element expanded during unloading, the voltage output of the sensor from the static test matched the voltage output during compression. For the dynamic testing, the voltage output of the sensor exhibited a hysteresis from the loading voltage output, the hysteresis increased when the strain rate increased.</abstract><cop>Lausanne</cop><pub>Elsevier B.V</pub><doi>10.1016/j.sna.2017.11.002</doi><tpages>8</tpages></addata></record>
fulltext fulltext
identifier ISSN: 0924-4247
ispartof Sensors and actuators. A. Physical., 2018-01, Vol.269, p.137-144
issn 0924-4247
1873-3069
language eng
recordid cdi_proquest_journals_2010773249
source ScienceDirect Freedom Collection
subjects Alloys
Anisotropy
Bias
Coils (windings)
Compression tests
Crystal lattices
Deformation
Dynamic tests
Electric potential
Hall probes
Hysteresis
Magnetic circuits
Magnetic fields
Magnetic permeability
Magnetic properties
Magnetic shape memory
Magnetic susceptibility
Magneto-mechanics
Manganese
Mechanical tests
Nickel
Sensors
Shape memory alloys
Single crystals
Strain measurement
Strain rate
Strain sensor
title Sensing strain with Ni-Mn-Ga
url http://sfxeu10.hosted.exlibrisgroup.com/loughborough?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2024-12-27T12%3A12%3A31IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest_cross&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Sensing%20strain%20with%20Ni-Mn-Ga&rft.jtitle=Sensors%20and%20actuators.%20A.%20Physical.&rft.au=Hobza,%20Anthony&rft.date=2018-01-01&rft.volume=269&rft.spage=137&rft.epage=144&rft.pages=137-144&rft.issn=0924-4247&rft.eissn=1873-3069&rft_id=info:doi/10.1016/j.sna.2017.11.002&rft_dat=%3Cproquest_cross%3E2010773249%3C/proquest_cross%3E%3Cgrp_id%3Ecdi_FETCH-LOGICAL-c325t-984e9c714565de2087e0e3108f64f65e2a3c11e6ce6039fd49a02c6f89015aba3%3C/grp_id%3E%3Coa%3E%3C/oa%3E%3Curl%3E%3C/url%3E&rft_id=info:oai/&rft_pqid=2010773249&rft_id=info:pmid/&rfr_iscdi=true