Description-Ferrite Ring magnet
Ferrite Ring Magnet is a ring magnet whose basic construction consists of a ferrite material and a coil. Ferrite is a magnetic ceramic material with good magnetic permeability and magnetic saturation strength, so it is often used to make magnets. The coil is a magnetic field generator wound with a conductor wire, which can generate a magnetic field after being energized.
Ferrite Ring Magnet are characterized by uniform magnetic field strength, and the direction of the magnetic field is perpendicular to the cross section of the magnet. It is widely used in research in the fields of biomedicine, materials science, and physics, such as magnetic resonance imaging (MRI), magnetic fluid separation, magnetic probes, etc.
Hard Ferrite magnets, made by molding powder mixture of about 80% Fe2O3 and about 20% either BaCo3 or SrO3, is also called ceramic magnet. Along with deepening of research, some additives such as cobalt (Co) and lanthanum (La) are mixed together to improve the magnetic performance. The molded powder metallic green is sintered inside a temperature controlled furnace what is heated with electricity or coal. Though Hard Ferrite magnet is with low magnetic property, it is still a preferable choice to engineer in their design due to several factors: abundantly available raw material,the cheapest cost among permanent magnet family, low density, excellent stability of chemistry, high maximum working temperature and Curie temperature.
Ferrite Ring Magnet for acoustic application is the primarily marketed product and acts as an important business pillar to our company at the beginning phase. With realization of increasing demand for electric motion application, we have been concentrating our works on promotion of Hard Ferrite segment magnet and have accumulated rich experience on properly producing magnet to minimize noise, maximize performance and optimize other intention of application. Also we have achieved success of developing Hard Ferrite magnet with irregular structure ( super-small, super-big, super-thin ), complicated geometry and super precision made by wet molding process. Limited by processing difficulty, such kinds of magnet were usually made by dry process and bonded process with shortage of low property and or expensive cost. Now our marketed Hard Ferrite magnets are extensively assembled inside motor, generator, sensor, loudspeaker, meter, relay, separator and many other applications for defense, automotive, robot, household electric appliance, wireless communication base station and mineral plant …
Dimension range-Ferrite Ring magnet
Outer Diameter: 30-330mm
Inner Diameter: 10-170mm
Thickness: 30mm
Standard property: Y30, Y30H-1, Y30BH
Typical Magnetic Performance for Hard Ferrite magnet
Grade | Remanence | Coercive Force | Intrinsic Coercive | Max Energy | Density | ||||
Br | Hcb | Hcj | (BH)max | ||||||
mT | Gs | KA/m | Oe | KA/m | Oe | KJ/m³ | MGOe | g/cm³ | |
Y8T | 200-235 | ≧2000 | 125-160 | ≧1570 | 210-280 | ≧2610 | 6.5-9.5 | ≧0.8 | 4.8 |
Y22H | 310-360 | ≧3100 | 220-250 | ≧2770 | 280-320 | ≧3520 | 20.0-24.0 | ≧2.5 | 4.9 |
Y25 | 360-400 | ≧3600 | 135-170 | ≧1700 | 140-200 | ≧1760 | 22.5-28.0 | ≧2.8 | 4.9 |
Y26H-1 | 360-390 | ≧3600 | 200-250 | ≧2512 | 225-255 | ≧2830 | 23.0-28.0 | ≧2.9 | 4.9 |
Y26H-2 | 360-380 | ≧3600 | 263-288 | ≧3300 | 318-350 | ≧4000 | 24.0-28.0 | ≧3 | 4.9 |
Y27H | 350-380 | ≧3500 | 225-240 | ≧2830 | 235-260 | ≧2950 | 25.0-29.0 | ≧3.1 | 4.9 |
Y28 | 370-400 | ≧3700 | 175-210 | ≧2200 | 180-220 | ≧2260 | 26.0-30.0 | ≧3.3 | 4.9 |
Y28H-1 | 380-400 | ≧3800 | 240-260 | ≧3020 | 250-280 | ≧3140 | 27.0-30.0 | ≧3.4 | 4.9 |
Y28H-2 | 360-380 | ≧3600 | 271-295 | ≧3400 | 382-405 | ≧4800 | 26.0-30.0 | ≧3.3 | 4.9 |
Y30 | 370-400 | ≧3700 | 175-210 | ≧2200 | 180-220 | ≧2260 | 26.0-30.0 | ≧3.3 | 4.9 |
Y30BH | 380-390 | ≧3800 | 223-235 | ≧2800 | 231-245 | ≧2900 | 27.0-30.0 | ≧3.4 | 4.9 |
Y30H-1 | 380-400 | ≧3800 | 230-275 | ≧2890 | 235-290 | ≧2950 | 27.0-32.5 | ≧3.4 | 4.9 |
Y30H-2 | 395-415 | ≧3950 | 275-300 | ≧3460 | 310-335 | ≧3900 | 27.0-32.0 | ≧3.4 | 4.9 |
Y32 | 400-420 | ≧4000 | 160-190 | ≧2010 | 165-195 | ≧2070 | 30.0-33.5 | ≧3.8 | 4.9 |
Y32H-1 | 400-420 | ≧4000 | 190-230 | ≧2390 | 230-250 | ≧2890 | 31.0-35.0 | ≧3.9 | 4.9 |
Y32H-2 | 400-440 | ≧4000 | 224-240 | ≧2810 | 230-250 | ≧2890 | 31.0-34.0 | ≧3.9 | 4.9 |
Y33 | 410-430 | ≧4100 | 220-250 | ≧2760 | 225-255 | ≧2830 | 31.5-35.0 | ≧4 | 4.9 |
Y33H | 410-430 | ≧4100 | 250-270 | ≧3140 | 250-275 | ≧3140 | 31.5-35.0 | ≧4 | 4.9 |
Y34 | 420-440 | ≧4200 | 200-230 | ≧2510 | 205-235 | ≧2580 | 32.5-36.0 | ≧4.1 | 4.9 |
Y35 | 430-450 | ≧4300 | 215-239 | ≧2700 | 217-241 | ≧2730 | 33.1-33.2 | ≧4.2 | 4.9 |
Y36 | 440-450 | ≧4400 | 247-271 | ≧3100 | 250-374 | ≧3140 | 35.1-38.3 | ≧4.4 | 4.9 |
Y38 | 440-460 | ≧4400 | 285-305 | ≧3580 | 294-310 | ≧3690 | 36.6-40.6 | ≧4.6 | 4.9 |
Y40 | 450-460 | ≧4500 | 330-354 | ≧4150 | 340-360 | ≧4270 | 37.6-41.8 | ≧4.7 | 4.9 |
Physical property of Hard Ferrite magnets
Curie Temperature (°C) | 450 |
Maximum Operating Temperature (°C) | 250 |
Hardness (Hv) | 480-580 |
Density (g/cm3) | 4.8 - 4.9 |
Relative Recoil Permeability (μrec) | 1.05 - 1.20 |
Saturation Field Strength, kOe (KA/m) | 10 (800) |
Temperature Coefficient of Br (%/°C) | -0.2 |
Temperature Coefficient of iHc (%/°C) | 0.3 |
Tensile Strength (N/mm) | <100 |
Transverse Rupture Strength (N/mm) | 300 |
USA Standard - Permanent Ferrite / Ceramic magnet
Grade | Remanence | Coercive Force | Intrinsic Coercive | Max Energy | Density | Tw Max | Remark | ||||
Br | Hcb | Hcj | BHmax | ||||||||
KGs | mT | KOe | KA/m | KOe | KA/m | KJ/m3 | MGOe | g/cm3 | ℃ | ||
C1 | 2.3 | 230 | 1.86 | 150 | 3.5 | 258 | 8.36 | 1.05 | 4.8 | 250 | Isotropic |
C5 | 3.8 | 380 | 2.4 | 190 | 2.5 | 200 | 27.1 | 3.4 | 4.9 | 250 | |
C7 | 3.4 | 340 | 3.23 | 258 | 4.0 | 318 | 21.9 | 2.75 | 4.9 | 250 | |
C8(C8A) | 3.85 | 385 | 2.95 | 235 | 3.0 | 240 | 27.8 | 3.5 | 4.9 | 250 | Anisotropic |
C8B | 4.2 | 420 | 2.9 | 232 | 2.96 | 236 | 32.8 | 4.1 | 4.9 | 250 | |
C9 | 3.8 | 380 | 3.5 | 280 | 4.0 | 320 | 26.4 | 3.3 | 4.9 | 250 | |
C10 | 4.0 | 400 | 3.6 | 288 | 3.5 | 280 | 30.4 | 3.8 | 4.9 | 250 | |
C11 | 4.3 | 430 | 2.5 | 200 | 2.55 | 204 | 34.4 | 4.3 | 4.9 | 250 | |
The Standard of International Electronics Committee (IEC404-8-1)
Grade | Remanence | Coercive Force | Intrinsic Coercive | Max Energy | Density | ||||
Br | Hcb | Hcj | (BH)max | ||||||
KGs | mT | KOe | KA/m | KOe | KA/m | KJ/m3 | MGOe | g/cm3 | |
HF8/22 | 2.00-2.20 | 200-220 | 1.57-1.76 | 125-140 | 2.76-2.89 | 220-230 | 6.5-6.8 | 0.8-1.1 | 4.8 |
HF20/19 | 3.20-3.33 | 320-333 | 2.14-2.39 | 170-190 | 2.39-2.51 | 190-200 | 20.0-21.0 | 2.5-2.7 | 4.9 |
HF20/28 | 3.10-3.25 | 310-325 | 2.76-2.89 | 220-230 | 3.52-3.64 | 280-290 | 20.0-21.0 | 2.5-2.7 | 4.9 |
HF22/30 | 3.50-3.65 | 350-365 | 3.20-3.33 | 255-265 | 3.64-3.77 | 290-300 | 22.0-23.5 | 2.8-3.0 | 4.9 |
HF24/16 | 3.50-3.65 | 350-365 | 1.95-2.20 | 155-175 | 2.01-2.26 | 160-180 | 24.0-25.5 | 3.0-3.2 | 4.9 |
HF24/23 | 3.50-3.65 | 350-365 | 2.76-2.89 | 220-230 | 2.89-3.01 | 230-240 | 24.0-25.5 | 3.0-3.2 | 4.9 |
HF24/35 | 3.60-3.70 | 360-370 | 3.27-3.39 | 260-270 | 4.40-4.52 | 350-360 | 24.0-25.5 | 3.0-3.2 | 4.9 |
HF26/16 | 3.70-3.80 | 370-380 | 1.95-2.20 | 155-175 | 2.01-2.26 | 160-180 | 26.0-27.0 | 3.2-3.4 | 4.9 |
HF26/18 | 3.70-3.80 | 370-380 | 2.20-2.39 | 175-190 | 2.26-2.39 | 180-190 | 26.0-27.0 | 3.3-3.4 | 4.9 |
HF26/24 | 3.70-3.80 | 370-380 | 2.89-3.01 | 230-240 | 3.01-3.14 | 240-250 | 26.0-27.0 | 3.3-3.4 | 4.9 |
HF26/26 | 3.70-3.80 | 370-380 | 2.89-3.01 | 230-240 | 3.27-3.39 | 260-270 | 26.0-27.0 | 3.3-3.4 | 4.9 |
HF26/30 | 3.85-3.95 | 385-395 | 3.27-3.39 | 260-270 | 3.77-3.89 | 300-310 | 26.0-27.0 | 3.3-3.4 | 4.9 |
HF28/26 | 3.85-3.95 | 385-395 | 3.14-3.33 | 250-265 | 3.27-3.45 | 260-275 | 28.0-30.0 | 3.5-3.8 | 4.9 |
HF28/28 | 3.85-3.95 | 385-395 | 3.27-3.39 | 260-270 | 3.50-3.60 | 280-290 | 28.0-30.0 | 3.5-3.8 | 4.9 |
HF30/26 | 3.95-4.05 | 395-405 | 3.14-3.33 | 250-260 | 3.27-3.39 | 260-270 | 30.0-31.5 | 3.8-3.9 | 4.9 |
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