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Samarium–cobalt magnet

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480:, and such may be added in small quantities to achieve better heat treatment response. By weight, the alloy will generally contain 25% of samarium. The maximum energy products of these alloys range from 20 to 32 MGOe, what is about 160-260 kJ/m. These alloys have the best reversible temperature coefficient of all rare-earth alloys, typically being -0.03%/°C. The "second generation" materials can also be used at higher temperatures. 568: 456:
fabricating, impurities may be introduced in the magnets, which form nuclei. In this case, because the impurities may have lower anisotropy or misaligned easy axes, their directions of magnetization are easier to spin, which breaks the 180° domain wall configuration. In such materials, the coercivity is controlled by nucleation. To obtain much coercivity, impurity control is critical in the fabrication process.
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desired shape, in a magnetic field to orient the magnetic field of the particles. Sintering is applied at a temperature of 1100˚C–1250˚C, followed by solution treatment at 1100˚C–1200˚C and tempering is finally performed on the magnet at about 700˚C–900˚C. It then is ground and further magnetized to increase its magnetic properties. The finished product is tested, inspected and packed.
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production. The raw materials are melted in an induction furnace filled with argon gas. The mixture is cast into a mold and cooled with water to form an ingot. The ingot is pulverized and the particles are further milled to further reduce the particle size. The resulting powder is pressed in a die of
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In the presence of a moderately strong magnetic field, unmagnetized magnets of this series will try to align their orientation axis to the magnetic field, thus becoming slightly magnetized. This can be an issue if postprocessing requires that the magnet be plated or coated. The slight field that the
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Samarium–cobalt alloys are typically machined in the unmagnetized state. Samarium–cobalt should be ground using a wet grinding process (water-based coolants) and a diamond grinding wheel. The same type of process is required if drilling holes or other features that are confined. The grinding waste
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are aligned with the easy axis direction. In this case, all of the domain walls are at 180 degrees. When there are no impurities, the reversal process of the bulk magnet is equivalent to lone-domain motes, where coherent rotation is the dominant mechanism. However, due to the imperfection of
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drifts with temperature and it is one of the important characteristics of magnet performance. Some applications, such as inertial gyroscopes and travelling wave tubes (TWTs), need to have constant field over a wide temperature range. The reversible temperature coefficient (RTC) of
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produced must not be allowed to completely dry as samarium–cobalt has a low ignition point. A small spark, such as that produced with static electricity, can easily initiate combustion. The resulting fire produced can be extremely hot and difficult to control.
472:, or SmCo Series 2:17) are age-hardened with a composition of two atoms of rare-earth samarium per 13–17 atoms of transition metals (TM). The TM content is rich in cobalt, but contains other elements such as iron and copper. Other elements like 381:
of -0.05%/°C. Saturation magnetization can be achieved with a moderate magnetizing field. This series of magnet is easier to calibrate to a specific magnetic field than the SmCo 2:17 series magnets.
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Samarium–cobalt magnets have a strong resistance to corrosion and oxidation resistance, usually do not need to be coated and can be widely used in high temperature and poor working conditions.
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The reduction/melt method and reduction/diffusion method are used to manufacture samarium–cobalt magnets. The reduction/melt method will be described since it is used for both SmCo
127:, meaning they can only be magnetized in the axis of their magnetic orientation. This is done by aligning the crystal structure of the material during the manufacturing process. 711: 750:"Toshiba : Press Release (16 Aug, 2012): Toshiba develops dysprosium-free samarium–cobalt magnet to replace heat-resistant neodymium magnet in essential applications" 377:. The energy products of these samarium–cobalt alloys range from 16 MG·Oe to 25 MG·Oe, that is, approx. 128–200 kJ/m. These samarium–cobalt magnets generally have a 605:
Samarium-cobalt (SmCo) magnets are used in aerospace and defense due to their exceptional magnetic properties. They are utilized in high-performance motors and
451:(coercive force); that is, they are not easily demagnetized. They are fabricated by packing wide-grain lone-domain magnetic powders. All of the 385:
magnet picks up can attract debris during the plating or coating process, causing coating failure or a mechanically out-of-tolerance condition.
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T. Ojima; S. Tomizawa; T. Yoneyama; T. Hori (1977). "Magnetic properties of a new type of rare-earth cobalt magnets Sm2(Co, Cu, Fe, M)17".
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To address these requirements, temperature compensated magnets were developed in the late 1970s. For conventional SmCo magnets,
575: 17: 970: 790: 613:, and satellite systems where stability and reliability are essential. They are also used in medical technologies, including 818:
K. Strnat; G. Hoffer; J. Olson; W. Ostertag; J. J. Becker (1967). "A Family of New Cobalt-Base Permanent Magnet Materials".
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In the mid-1980s some expensive headphones such as the Ross RE-278 used samarium–cobalt "Super Magnet" transducers.
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process. To increase the coercivity, impurities are intentionally added during the fabrication process.
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to 33 MG·Oe, that is approx. 112 kJ/m to 264 kJ/m; their theoretical limit is 34 MG·Oe, about 272 kJ/m.
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Research and Development of Rare Earth Transition Metal Alloys as Permanent Magnet Materials,
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They are expensive and subject to price fluctuations (cobalt is market price sensitive).
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Applications in which performance is required to be consistent with temperature change
1029: 925:, New Jersey Department of Health and Senior Services Hazardous Substance Fact Sheet. 786: 691: 688: – Strongest type of permanent magnet from an alloy of neodymium, iron and boron 544: 495:. Impurities inside the magnets impede the domain wall motion and thereby resist the 264: 211: 92: 35: 999: 870: 835: 685: 432:
increases as temperature increases within certain temperature ranges. By combining
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They are brittle, and prone to cracking and chipping. Samarium–cobalt magnets have
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per five atoms of cobalt. By weight, this magnet alloy will typically contain 36%
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Strong permanent magnet made from an alloy of a rare-earth element and cobalt
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They were developed in the early 1960s based on work done by Karl Strnat at
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Comparison of physical properties of sintered neodymium and Sm-Co magnets
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in the alloy, the temperature coefficient can be reduced to nearly zero.
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Samarium–cobalt magnets are generally ranked similarly in strength to
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Typical physical and chemical properties of some magnetic materials
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Rotary encoders where it performs the function of magnetic actuator
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Samarium–cobalt magnets are extremely resistant to demagnetization.
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decreases as temperature increases. Conversely, for GdCo magnets,
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Samarium–cobalt magnets are available in two "series", namely SmCo
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High-end electric motors used in the more competitive classes in
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These samarium–cobalt magnet alloys (generally written as SmCo
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from 700 °C (973 K) to 800 °C (1,070 K).
890:"Everything You Need to Know About Samarium Cobalt Magnets" 548: 779:
Juha Pyrhönen; Tapani Jokinen; Valéria Hrabovcová (2009).
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Applications that will require the system to function at
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temperatures or very hot temperatures (over 180 °C)
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1980s vintage headphones using Samarium Cobalt magnets
543:; the cobalt can be substituted by a portion of other 928: 975:The Story of the Samarium Cobalt Noiseless Pickups 527:Samarium can be substituted by a portion of other 365:, or SmCo Series 1:5) have one atom of rare-earth 767:Corrosion and oxidation resistance of SmCo magnet 72:, but have higher temperature ratings and higher 1071: 91:These magnets have good temperature stability ; 1050:"Neodymium Magnets vs. Samarium Cobalt Magnets" 676: – Trivalent metallic rare-earth elements 491:magnets, the coercivity mechanism is based on 808:, permanent magnets comparison and selection. 799: 916: 200:Temperature coefficient of coercivity (%/K) 937:, Introduction to Samarium Cobalt Magnets. 189:Temperature coefficient of remanence (%/K) 1028:. Jane's Information Group. p. 547. 948:"Fender Vintage Hot Rod '57 Stratocaster" 123:samarium–cobalt magnets exhibit magnetic 84:Some attributes of samarium-cobalts are: 1000:"Samarium Cobalt Magnets (SmCo Magnets)" 566: 887: 253:, normal to magnetizing direction (1/K) 14: 1072: 782:Design of Rotating Electrical Machines 913:Nanocomposite Sm-Co melt spun ribbons 769:, corrosion and oxidation resistance. 785:. John Wiley and Sons. p. 232. 760: 24: 379:reversible temperature coefficient 25: 1111: 968: 888:Marchio, Cathy (June 14, 2024). 739:Alden E. Ray, et al, August 1972 590:in Fender's Vintage Hot Rod '57 1042: 1024:University of Michigan (1993). 1017: 992: 962: 952:Fender Hot Rod '57 Stratocaster 940: 907: 55:Wright-Patterson Air Force Base 881: 855:IEEE Transactions on Magnetics 846: 811: 772: 742: 729: 704: 459: 13: 1: 698: 594:. These pickups were used in 502: 356: 239:, magnetizing direction (1/K) 79: 602:from 2004 until early 2010. 42:made of two basic elements: 7: 667: 464:These alloys (written as Sm 10: 1116: 820:Journal of Applied Physics 659:Benchtop NMR spectrometers 586:series of electric guitar 114:megagauss-oersteds (MG·Oe) 875:10.1109/TMAG.1977.1059703 584:Samarium Cobalt Noiseless 447:magnets have a very high 336: 977:. Fender. Archived from 954:. Fender. Archived from 609:, precision sensors and 1085:Ferromagnetic materials 562: 106:maximum energy products 1090:Loudspeaker technology 1026:Jane's Space Directory 714:. 1998. Archived from 596:American Deluxe Series 572: 497:magnetization reversal 32:samarium–cobalt (SmCo) 18:Samarium-cobalt magnet 935:Sintered SmCo Magnets 621:, and medical pumps. 578:used one of designer 570: 176:Relative permeability 112:) that range from 14 57:and Alden Ray at the 627:Other uses include: 279:Compressive strength 59:University of Dayton 867:1977ITM....13.1317O 832:1967JAP....38.1001S 643:Traveling-wave tube 529:rare-earth elements 493:domain wall pinning 414:) x (1/∆T) × 100%. 132: 1100:Samarium compounds 573: 130: 93:Curie temperatures 34:magnet, a type of 840:10.1063/1.1709459 792:978-0-470-69516-6 754:www.toshiba.co.jp 692:Rare-earth magnet 545:transition metals 373:with the balance 334: 333: 265:Flexural strength 212:Curie temperature 70:neodymium magnets 36:rare-earth magnet 16:(Redirected from 1107: 1065: 1064: 1062: 1060: 1046: 1040: 1039: 1021: 1015: 1014: 1012: 1010: 1004:Stanford Magnets 996: 990: 989: 987: 986: 966: 960: 959: 944: 938: 932: 926: 920: 914: 911: 905: 904: 902: 900: 894:Stanford Magnets 885: 879: 878: 850: 844: 843: 826:(3): 1001–1002. 815: 809: 803: 797: 796: 776: 770: 764: 758: 757: 746: 740: 733: 727: 726: 724: 723: 708: 686:Neodymium magnet 453:magnetic domains 307:Vickers hardness 293:Tensile strength 133: 129: 40:permanent magnet 21: 1115: 1114: 1110: 1109: 1108: 1106: 1105: 1104: 1095:Magnetic alloys 1070: 1069: 1068: 1058: 1056: 1048: 1047: 1043: 1036: 1022: 1018: 1008: 1006: 998: 997: 993: 984: 982: 967: 963: 946: 945: 941: 933: 929: 921: 917: 912: 908: 898: 896: 886: 882: 851: 847: 816: 812: 804: 800: 793: 777: 773: 765: 761: 748: 747: 743: 734: 730: 721: 719: 710: 709: 705: 701: 670: 565: 522: 518: 514: 505: 490: 486: 471: 467: 462: 446: 430: 423: 413: 409: 400: 392: 364: 359: 352: 348: 344: 339: 136:Property (unit) 111: 82: 64: 28: 23: 22: 15: 12: 11: 5: 1113: 1103: 1102: 1097: 1092: 1087: 1082: 1067: 1066: 1041: 1034: 1016: 991: 961: 958:on 2012-12-09. 939: 927: 915: 906: 880: 845: 810: 798: 791: 771: 759: 741: 728: 702: 700: 697: 696: 695: 689: 683: 680:Magnet fishing 677: 669: 666: 665: 664: 661: 656: 653: 646: 640: 638:Turbomachinery 635: 633:slotcar racing 564: 561: 520: 516: 512: 504: 501: 488: 484: 469: 465: 461: 458: 444: 428: 421: 416: 415: 411: 407: 402:is defined as 398: 390: 362: 358: 355: 350: 346: 345:magnets and Sm 342: 338: 335: 332: 331: 328: 325: 317: 316: 313: 310: 303: 302: 299: 296: 289: 288: 285: 282: 275: 274: 271: 268: 261: 260: 257: 254: 247: 246: 243: 240: 233: 232: 229: 226: 225:Density (g/cm) 222: 221: 218: 215: 208: 207: 204: 201: 197: 196: 193: 190: 186: 185: 182: 179: 172: 171: 168: 165: 158: 157: 154: 151: 144: 143: 140: 137: 118: 117: 109: 102: 99: 96: 89: 81: 78: 62: 38:, is a strong 26: 9: 6: 4: 3: 2: 1112: 1101: 1098: 1096: 1093: 1091: 1088: 1086: 1083: 1081: 1080:Cobalt alloys 1078: 1077: 1075: 1055: 1051: 1045: 1037: 1031: 1027: 1020: 1005: 1001: 995: 981:on 2012-10-02 980: 976: 972: 965: 957: 953: 949: 943: 936: 931: 924: 919: 910: 895: 891: 884: 876: 872: 868: 864: 860: 856: 849: 841: 837: 833: 829: 825: 821: 814: 807: 802: 794: 788: 784: 783: 775: 768: 763: 755: 751: 745: 738: 732: 718:on 2013-05-27 717: 713: 707: 703: 693: 690: 687: 684: 681: 678: 675: 672: 671: 662: 660: 657: 654: 651: 647: 645:field magnets 644: 641: 639: 636: 634: 630: 629: 628: 625: 622: 620: 616: 612: 608: 603: 601: 597: 593: 589: 585: 581: 580:Bill Lawrence 577: 569: 560: 558: 554: 550: 546: 542: 538: 534: 530: 525: 509: 500: 498: 494: 481: 479: 475: 457: 454: 450: 441: 439: 435: 431: 424: 405: 404: 403: 401: 393: 386: 382: 380: 376: 372: 368: 354: 329: 326: 323: 319: 318: 314: 311: 308: 305: 304: 300: 297: 294: 291: 290: 286: 283: 280: 277: 276: 272: 269: 266: 263: 262: 258: 255: 252: 249: 248: 244: 241: 238: 235: 234: 230: 227: 224: 223: 219: 216: 213: 210: 209: 206:−0.15..–0.30 205: 202: 199: 198: 195:−0.03..–0.05 194: 191: 188: 187: 183: 180: 177: 174: 173: 169: 166: 163: 160: 159: 155: 152: 149: 146: 145: 141: 138: 135: 134: 128: 126: 122: 115: 107: 103: 100: 97: 94: 90: 87: 86: 85: 77: 75: 71: 66: 60: 56: 51: 49: 45: 41: 37: 33: 19: 1057:. Retrieved 1053: 1044: 1025: 1019: 1007:. Retrieved 1003: 994: 983:. Retrieved 979:the original 974: 969:Smith, Dan. 964: 956:the original 951: 942: 930: 918: 909: 897:. Retrieved 893: 883: 858: 854: 848: 823: 819: 813: 801: 781: 774: 762: 753: 744: 736: 731: 720:. Retrieved 716:the original 706: 626: 623: 604: 598:Guitars and 592:Stratocaster 574: 533:praseodymium 526: 510: 506: 482: 463: 442: 426: 419: 417: 396: 388: 387: 383: 360: 340: 327:(110–170)×10 203:−0.40..–0.65 192:–0.09..–0.12 119: 83: 67: 52: 31: 29: 923:Cobalt HSFS 861:(5): 1317. 460:Series 2:17 330:(50–90)×10 322:resistivity 320:Electrical 259:(10–13)×10 170:0.493–2.79 1074:Categories 1054:JDA Magnet 1035:0710610750 985:2012-08-16 737:AD-750 746 722:2017-01-10 699:References 674:Lanthanide 619:pacemakers 617:machines, 611:gyroscopes 547:including 541:gadolinium 531:including 503:Production 449:coercivity 438:gadolinium 357:Series 1:5 167:0.875–2.79 162:Coercivity 125:anisotropy 80:Attributes 74:coercivity 650:cryogenic 607:actuators 557:zirconium 474:zirconium 353:magnets. 287:800–1000 284:1000–1100 245:(5–9)×10 184:1.05–1.1 156:0.8–1.16 148:Remanence 139:Neodymium 668:See also 434:samarium 371:samarium 367:samarium 315:400–650 273:150–180 256:(1–3)×10 242:(3–4)×10 231:8.2–8.5 220:700–850 121:Sintered 44:samarium 1059:Aug 10, 1009:Aug 10, 899:Aug 29, 863:Bibcode 828:Bibcode 588:pickups 478:hafnium 312:500–650 270:200–400 228:7.3–7.7 217:310–370 1032:  789:  600:Basses 576:Fender 555:, and 553:copper 539:, and 537:cerium 515:and Sm 375:cobalt 337:Series 324:(Ω·cm) 301:35–40 295:(N/mm) 281:(N/mm) 267:(N/mm) 164:(MA/m) 142:Sm-Co 48:cobalt 483:In Sm 298:80–90 153:1–1.5 1061:2024 1030:ISBN 1011:2024 901:2024 787:ISBN 563:Uses 549:iron 443:SmCo 436:and 309:(HV) 214:(°C) 181:1.05 46:and 871:doi 836:doi 615:MRI 582:'s 406:(∆B 251:CTE 237:CTE 178:(–) 150:(T) 110:max 108:(BH 1076:: 1052:. 1002:. 973:. 950:. 892:. 869:. 859:13 857:. 834:. 824:38 822:. 752:. 559:. 551:, 535:, 521:17 519:Co 489:17 487:Co 476:, 470:17 468:Co 410:/B 351:17 349:Co 76:. 65:. 50:. 30:A 1063:. 1038:. 1013:. 988:. 903:. 877:. 873:: 865:: 842:. 838:: 830:: 795:. 756:. 725:. 517:2 513:5 485:2 466:2 445:5 429:r 427:B 422:r 420:B 412:r 408:r 399:r 397:B 391:r 389:B 363:5 347:2 343:5 63:5 20:)

Index

Samarium-cobalt magnet
rare-earth magnet
permanent magnet
samarium
cobalt
Wright-Patterson Air Force Base
University of Dayton
neodymium magnets
coercivity
Curie temperatures
maximum energy products
megagauss-oersteds (MG·Oe)
Sintered
anisotropy
Remanence
Coercivity
Relative permeability
Curie temperature
CTE
CTE
Flexural strength
Compressive strength
Tensile strength
Vickers hardness
resistivity
samarium
samarium
cobalt
reversible temperature coefficient
samarium

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