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http://hdl.handle.net/11452/29645
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DC Field | Value | Language |
---|---|---|
dc.contributor.author | Civan, Ersin | - |
dc.date.accessioned | 2022-12-01T10:38:22Z | - |
dc.date.available | 2022-12-01T10:38:22Z | - |
dc.date.issued | 2016-08-17 | - |
dc.identifier.citation | Küçük, İ. vd. (2016). "Magnetocaloric and magnetoresistance properties in Co-based (Co0.402Fe0.201Ni0.067B0.227Si0.053Nb0.05)(100-x)Cu-x (x=0-1) glassy alloys". Philosophical Magazine, 96(30), Part A, 3120-3130. | en_US |
dc.identifier.issn | 1478-6435 | - |
dc.identifier.issn | 1478-6443 | - |
dc.identifier.uri | https://doi.org/10.1080/14786435.2016.1227485 | - |
dc.identifier.uri | https://www.tandfonline.com/doi/full/10.1080/14786435.2016.1227485 | - |
dc.identifier.uri | http://hdl.handle.net/11452/29645 | - |
dc.description.abstract | The magnetocaloric and magnetoresistance properties of amorphous Co-based (Co0.402Fe0.201Ni0.067B0.227Si0.053Nb0.05)(100-x)Cu-x (x=0, 0.5, 0.75 and 1) ribbons were investigated. Cu additions changed the crystallisation temperature (T-x) and the Curie temperature (T-C). The saturation magnetisation (M-s) and coercivity (H-c) for alloys were in the range of 65.51-38.49 emu/g and 1.99-6.84 A/m, respectively. Under an applied magnetic field change of 2.2 T, the (-S-M)(max) for (Co0.402Fe0.201Ni0.067B0.227Si0.053Nb0.05)(100-x)Cu-x with x=0, 0.5, 0.75 and 1 are 0.77, 0.71, 0.89 and 0.67 Jkg(-1)K(-1), respectively. The values of refrigeration capacity (RC) for the as-spun glassy alloys are comparable with those of previously studied Fe-based metallic glasses such as Fe80B10Zr9Cu1, (Fe0.76B0.24)(96)Nb-4 and Fe82Ni2Zr6B10. In addition, the maximum magnetoresistance (MR) values for (Co0.402Fe0.201Ni0.067B0.227Si0.053Nb0.05)(100-x)Cu-x with x=0, 0.5, 0.75 and 1 are found to be 110, 38, 23 and 1% around the Curie temperatures under an applied magnetic field change of 1 T, respectively. With good RC, negligible hysteresis due to very low coercivity values and large magnetoresistance, these Co-based amorphous alloys can be used as the high temperature magnetic refrigerants and multifunctional applications working in the temperature range of 450-600K. | en_US |
dc.language.iso | en | en_US |
dc.publisher | Taylor & Francis | en_US |
dc.rights | info:eu-repo/semantics/closedAccess | en_US |
dc.subject | Materials science | en_US |
dc.subject | Metallurgy & metallurgical engineering | en_US |
dc.subject | Physics | en_US |
dc.subject | Metallic glasses | en_US |
dc.subject | Magnetocaloric effect | en_US |
dc.subject | Magnetic entropy change | en_US |
dc.subject | Magnetoresistance | en_US |
dc.subject | Bulk metallic glasses | en_US |
dc.subject | Soft-magnetic properties | en_US |
dc.subject | Forming ability | en_US |
dc.subject | Room-temperature | en_US |
dc.subject | Amorphous-alloys | en_US |
dc.subject | Fe | en_US |
dc.subject | Ni | en_US |
dc.subject | Refrigeration | en_US |
dc.subject | Enhancement | en_US |
dc.subject | TB | en_US |
dc.subject | Amorphous alloys | en_US |
dc.subject | Amorphous silicon | en_US |
dc.subject | Coercive force | en_US |
dc.subject | Curie temperature | en_US |
dc.subject | Galvanomagnetic effects | en_US |
dc.subject | Glass | en_US |
dc.subject | High temperature applications | en_US |
dc.subject | Magnetic fields | en_US |
dc.subject | Magnetism | en_US |
dc.subject | Magnetocaloric effects | en_US |
dc.subject | Magnetoresistance | en_US |
dc.subject | Metallic glass | en_US |
dc.subject | Nickel | en_US |
dc.subject | Silicon | en_US |
dc.subject | Applied magnetic fields | en_US |
dc.subject | Co-based amorphous alloys | en_US |
dc.subject | Fe-based metallic glass | en_US |
dc.subject | Magnetic entropy change | en_US |
dc.subject | Magnetic refrigerants | en_US |
dc.subject | Magnetoresistance properties | en_US |
dc.subject | Refrigeration capacity | en_US |
dc.subject | Temperature range | en_US |
dc.subject | Iron alloys | en_US |
dc.title | Magnetocaloric and magnetoresistance properties in Co-based (Co0.402Fe0.201Ni0.067B0.227Si0.053Nb0.05)(100-x)Cu-x (x=0-1) glassy alloys | en_US |
dc.type | Article | en_US |
dc.identifier.wos | 000385367500001 | tr_TR |
dc.identifier.scopus | 2-s2.0-84984669570 | tr_TR |
dc.relation.publicationcategory | Makale - Uluslararası Hakemli Dergi | tr_TR |
dc.contributor.department | Uludağ Üniversitesi/Fen-Edebiyat Fakültesi/Fizik Bölümü. | tr_TR |
dc.relation.bap | KUAP(F)-2015/50 | en_US |
dc.relation.bap | AYP(F)-2014/6 | en_US |
dc.contributor.orcid | 0000-0002-8871-2357 | tr_TR |
dc.identifier.startpage | 3120 | tr_TR |
dc.identifier.endpage | 3130 | tr_TR |
dc.identifier.volume | 96 | tr_TR |
dc.identifier.issue | 30, Part A | en_US |
dc.relation.journal | Philosophical Magazine | en_US |
dc.contributor.buuauthor | Küçük, İlker | - |
dc.contributor.buuauthor | Şarlar, Kağan | - |
dc.contributor.buuauthor | Adam, Abdulhamit | - |
dc.contributor.researcherid | GXN-2736-2022 | tr_TR |
dc.contributor.researcherid | AAH-6293-2020 | tr_TR |
dc.contributor.researcherid | B-8159-2016 | tr_TR |
dc.relation.collaboration | Yurt içi | tr_TR |
dc.subject.wos | Materials science, multidisciplinary | en_US |
dc.subject.wos | Metallurgy & metallurgical engineering | en_US |
dc.subject.wos | Physics, applied | en_US |
dc.subject.wos | Physics, condensed matter | en_US |
dc.indexed.wos | SCIE | en_US |
dc.indexed.scopus | Scopus | en_US |
dc.wos.quartile | Q3 | en_US |
dc.wos.quartile | Q2 (Metallurgy & metallurgical engineering) | en_US |
dc.contributor.scopusid | 6602910810 | tr_TR |
dc.contributor.scopusid | 55550817200 | tr_TR |
dc.contributor.scopusid | 57215816253 | tr_TR |
dc.subject.scopus | Magnetism; Manganites; Critical Behavior | en_US |
Appears in Collections: | Scopus Web of Science |
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