High Temperature 350 °C SmCo Rod Magnets

/High Temperature 350 °C SmCo Rod Magnets
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  • High Temperature 350 °C SmCo Rod Magnets, Strong Cylinder SmCo Magnets for Sensor, Cylindrical SmCo Permanent Magnet, Rod Cobalt Samarium Magnet, Samarium Cobalt (Rare Earth) Bar Magnets

    High Temperature 350 °C SmCo Rod Magnets Item NO.  MPCO-SCC series
    Material: Samarium Cobalt
    Shape: rod, cylinder, bar
    Grade:Smco5,Sm2Co17 etc.
    Magnetic properties:Hcj,Hcb,BH,Br,BHmax,working temperature.
    Application:widely used in sensor,speakers,reed switches,motor,rotor,wind turbines/generators,AC/DC motors,drive motors,servo motors etc.
    Magnetization directions:by Axial or by radial.

    SmCo Rod Magnets are a type of magnetic material made from rare earth metal samarium and strategic metal cobalt-main elements, with iron, copper, zirconium and praseodymium, and produced by a serial of process melting, milling, pressing, sintering and aging. It has high magnetic properties (high energy product, high coercivity, high remanence), very low temperature coefficient (-0.030% / °C), high working temperature (Maximum working temperature reaches 350°C), no negative temperature limitation, and excellent corrosion resistance. At working temperature above180°C, its maximum energy product, temperature stability and chemical stability are better than NdFeB material. Therefore, According to the different components of the SmCo5 and Sm2Co17, respectively, they are the first generation and the two generation rare earth permanent magnetic material. Because of its raw materials are scarce, the price is expensive and limit the development. Samarium cobalt (SmCo) as the second generation rare earth permanent magnet, not only has a high magnetic energy product (14-28MGOe) and reliable coercivity, and exhibits excellent temperature characteristics in rare earth permanent magnet series. Compared with the NdFeB, SmCo is more suitable for working in high temperature environment. Sm2Co17 (SmCo permanent magnet) countersunk smco magnets

    Physical performance sheet of sintered SmCo

    parametersSmCo5Sm2Co17
    αBr (%/ ℃ )-0.04-0.03
    αHcj (%/ ℃ )-0.3-0.2
    Curie teperature(℃)700-750800-850
    density (g/cm3 )8.2-8.48.3-8.5
    Webster hardness (HV)450-500500-600
    Working temperature ( ℃ )250350

    The Magnetic Properties of Sintered SmCo magnets

    acteristicsResidual
    Flux Br
    Coercive Force HcbIntrinsic
    Coercive Force Hcj
    Max. Enery
    Product(BH)max
    Curie
    Temp Tc
    Density ρTemp.Coefficient
    △Bd/Bd
      Thermal
    Expansion
    coefficient
    Vickers
    Hardness
    Material GradeTesal (kGs)KA/m
    (kOe)
    KA/m
    (kOe)
    kJ/m3
    (MGOe)
    (℃)g/cm3(%/℃)C⊥
    (1℃)
    C∥
    (1℃)
    Hv
    1:5  SmCo5SM~180.80~0.90
    (8.0~9.0)
    621~700
    (7.8~8.8)
    ≥1990
    (≥25.0)
    127~159
    (16.0~20.0)
    750~8008.2~8.4-0.0513×10-66×10-6450~500
    SM~200.90~0.95
    (9.0~9.5)
    676~740
    (8.5~9.3)
    ≥1432
    (≥18.0)
    151~167
    (19~21)
    750~8008.2~8.4-0.0513×10-66×10-6450~500
    SM~220.95~1.00
    (9.5~10.0)
    716~756
    (9.0~9.5)
    ≥1194
    (≥15.0)
    167~183
    (21~23)
    750~8008.2~8.4-0.0513×10-66×10-6450~500
    2:17  Sm2
    (Co,Cu,Fe,Zr) 17
    SM~18T0.85~0.95
    (8.5~9.5)
    636~716
    (8.0~9.0)
    ≥1592
    (≥20.0)
    127~159
    (16.0~20.0)
    850~9008.3~8.5-0.0111×10-68×10-6500~600
    SM~22T0.95~1.00
    (9.5~10.0)
    676~756
    (8.5~9.5)
    ≥1592
    (≥20.0)
    159~191
    (20.0~24.0)
    850~9008.3~8.5-0.0111×10-68×10-6500~600
    SM~22L0.95~1.00
    (9.5~10.0)
    477~637
    (6.0~8.0)
    493~716
    (6.2~9.0)
    159~191
    (20.0~24.0)
    800~8508.3~8.5-0.0311×10-68×10-6500~600
    SM~22H0.95~1.00
    (9.5~10.0)
    557~756
    (7.0~9.5)
    637~1194
    (8.0~15.0)
    159~191
    (20.0~24.0)
    800~8508.3~8.5-0.0311×10-68×10-6500~600
    SM~22U0.95~1.00
    (9.5~10.0)
    716~796
    (9.0~10.0)
    ≥1990
    (≥25.0)
    159~191
    (20.0~24.0)
    800~8508.3~8.5-0.0311×10-68×10-6500~600
    SM~26L1.00~1.08
    (10.0~10.8)
    477~637
    (6.0~8.0)
    493~716
    (6.2~9.0)
    191~223
    (24.0~28.0)
    800~8508.3~8.5-0.0311×10-68×10-6500~600
    SM~26H1.00~1.08
    (10.0~10.8)
    557~836
    (7.0~10.5)
    637~1194
    (8.0~15.0)
    191~223
    (24.0~28.0)
    800~8508.3~8.5-0.0311×10-68×10-6500~600
    SM~26U1.00~1.08
    (10.0~10.8)
    756~836
    (9.5~10.5)
    ≥1990
    (≥25.0)
    191~223
    (24.0~28.0)
    800~8508.3~8.5-0.0311×10-68×10-6500~600
    SM~28L1.04~1.10
    (10.4~11.0)
    477~637
    (6.0~8.0)
    493~716
    (6.2~9.0)
    207~239
    (26.0~30.0)
    800~8508.3~8.5-0.0311×10-68×10-6500~600
    SM~28H1.04~1.10
    (10.4~11.0)
    557~836
    (7.0~10.5)
    637~1194
    (8.0~15.0)
    207~239
    (26.0~30.0)
    800~8508.3~8.5-0.0311×10-68×10-6500~600
    SM~28U1.04~1.10
    (10.4~11.0)
    756~836
    (9.5~10.5)
    ≥1990
    (≥25.0)
    207~239
    (26.0~30.0)
    800~8508.3~8.5-0.0311×10-68×10-6500~600
    SM~30L1.08~1.12
    (10.8~11.2)
    477~637
    (6.0~8.0)
    493~716
    (6.2~9.0)
    223~247
    (28.0~31.0)
    800~8508.3~8.5-0.0311×10-68×10-6500~600
    SM~30H1.08~1.12
    (10.8~11.2)
    557~836
    (7.0~10.5) ~10.2).0~10.5)
    637~1194
    (8.0~15.0)
    223~247
    (28.0~31.0)
    800~8508.3~8.5-0.0311×10-68×10-6500~600
    SM~30U1.08~1.12
    (10.8~11.2)
    796~859
    (10.0~10.8)
    ≥1990
    (≥25.0)
    223~247
    (28.0~31.0)
    800~8508.3~8.5-0.0311×10-68×10-6500~600
    SM~321.10~16
    (11.0~11.6)
    (26.0~30.0)
    557~836
    (7.0~10.5)
    ≥637
    (≥8.0)
    ≥239
    (≥30.0)
    800~8508.3~8.5-0.0311×10-68×10-6500~600
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