Ferrite Block Magnet

$0.68 | 5000 piece (Min.Order)

The molding of Hard Ferrite magnet is mostly by a press machine equipped with coil what can generate an external magnetic field for getting anisotropic magnet. The material for making anisotropic Hard Ferrite magnet is usually at wet slurry status so that molecules can be perfectly aligned in molding process. So we call magnets made by such kind process as wet anisotropic Hard Ferrite magnets what only can be magnetized along pre-orientation. The (BH)max of anisotropic Hard Ferrite is several times stronger than of isotropic Hard Ferrite magnet...
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Description

Wet Anisotropic, Dry Isotropic & Dry Anisotropic Hard Ferrite magnet

The molding of Ferrite Block Magnet is mostly by a press machine equipped with coil what can generate an external magnetic field for getting anisotropic magnet. The material for making anisotropic Hard Ferrite magnet is usually at wet slurry status so that molecules can be perfectly aligned in molding process. So we call magnets made by such kind process as wet anisotropic Hard Ferrite magnets what only can be magnetized along pre-orientation. The (BH)max of anisotropic Hard Ferrite is several times stronger than of isotropic Hard Ferrite magnet.

The raw material for making isotropic Ferrite Block Magnet is generally at dry powder status. The molding is by a punch machine what could not apply an external magnetic field on magnet. Thus the subsequently attained magnets are called dry isotropic Hard Ferrite magnets. Magnetization on isotropic Ferrite Block Magnet could be done with any preferred orientation and pattern depending on magnetizing yoke.

There is also one type Ferrite Block Magnet called dry anisotropic Hard Ferrite magnet. It is made of dry material powder but being oriented by an external magnetic field. The magnetic property of dry anisotropic Hard Ferrite magnet is lower than wet anisotropic one. Usually the dry and anisotropic process is used to mold magnet with complex structure but higher property than isotropic one.


Shape and Dimensional Tolerance

Ferrite Block Magnet can be economically molded with ring, arc segment, rectangular, disc, cylinder, trapezium or 2 combined geometries in one piece. Depending on these basic geometries, sphere, olivary shape, and other irregular geometry are available by further machining process. Slotting in Hard Ferrite magnet is practicable by pre-design in tooling or diamond grinding process. Hard Ferrite magnets with 3S (super-small, super-big and super-thin) structure are also producible by wet molding process.

The dimensional deviation of Hard Ferrite magnet is controlled within +/-2% before being machined, and could be controlled within +/-0.10mm after being simply ground by diamond tool. Customs tolerance or precise control even +/-0.015mm is achievable, but should be negotiated. In most circumstance, wet anisotropic Ferrite Block Magnet is supplied with surfaces which parallel to anisotropic orientation un-ground and other surfaces ground. Definitions on tolerance of concentricity, roundness, squareness, perpendicularity and others please refer to MMPA standard No. 0100-00 or DIN17410 or ISO2768.


Tooling of Hard Ferrite Magnet

The economic process for manufacturing Ferrite Block Magnet at big quantity is by molding with tooling. The tooling for making anisotropic Hard Ferrite magnet is considerably expensive, but for making isotropic Hard Ferrite magnet it is cheap. If the required magnet is with same diameter, or same length and width when it is block type, as the current tooling, then we can utilize the ready tooling to mold different thickness/height magnets within permissible range.

In practice, sometimes we slice big block, grind bigger diameter ring/disc and machine arc segment type of close dimension into the required one. This process is helpful to get precise dimension, to save tooling cost when the order quantity is not so big (particularly at prototype phase), and to homogenize weight and flux of each piece product. The shortage of making magnet by machine is very expensive cost.

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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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