Ferrite Ring Magnet

$0.10 | 1 piece (Min.Order)

Ferrite rings are toroidal (doughnut) shaped, or cylindrical shaped pieces of ferrite (a ceramic compound).What do they do?Ferrite rings help to protect against EMI (electromagnetic interference) and RFI (radio frequency interference). They prevent interference moving to a device or from a...
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Description

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/

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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