Neodymium Iron Boron Magnets

Neodymium Iron Boron Magnets

Neodymium iron boron (NdFeB), or “neo” magnets offer the highest energy product of any material today and are available in a wide range of shapes, sizes and grades. Neo magnets can be found in a variety of applications including high-performance motors, brushless DC motors, magnetic separation, magnetic resonance imaging, sensors, switches and loudspeakers.

Arnold is now able to supply NdFeB that is fully compliant with the US Defense Federal Acquisition Regulation Supplement (DFARS 225.7018 Restriction on acquisition of certain magnets and tungsten, ‘The John S. McCain National Defense Authorization Act – NDAA 2019’).

Magnetic properties will differ depending upon alignment direction during compaction and upon size and shape. Download individual spec. sheets from the table below, or get the full neodymium iron boron catalogue for specific grades and their magnetic properties, including the trade-off in Br (and energy product) for HcJ (intrinsic coercivity, resistance to demagnetisation). For GBD Neodymium Iron Boron Grades, see below.


MAXIMUM USE TEMPERATURE AND CORROSION

Determining whether or not to use neo magnets instead of our RECOMA® SmCo magnets, for example, is a function of the maximum temperature of the application, required magnetic output at typical use temperature and total cost of the system.

Neo magnets have some limitations due to their corrosive behaviour. In humid applications, a protective coating is highly recommended. Coatings which have been used successfully include epoxy coating, nickel plating and combinations of these coatings. Arnold also has the capability to apply Parylene coating to neo magnets. Effectiveness of coating is dependent upon the quality of the base material. Arnold has evaluated multiple manufacturers for corrosion resistance of the base material and only supplies licensed, highly corrosion-resistant materials produced under tight control.


AVAILABLE NEODYMIUM IRON BORON GRADES

Edit Properties:BrBrHcBHcBHcJHcJBHmaxBHmaxRev. Temp. Coef.Rev. Temp. Coef.Temp.
Grade
Typical mT
Typical gauss
min kA/m
min oersteds
min kA/m
min oersteds
Typical kJ/m3
Typical MGOe
Br %/°C
HcJ %/°C
max °C
N35
1,210
12,100
860
10,800
955
12,000
283
35
-0.12
-0.618
80
N38
1,260
12,600
860
10,800
955
12,000
306
38
-0.12
-0.75
80
N40
1,285
12,850
923
11,600
955
12,000
318
40
-0.12
-0.75
80
N42
1,315
13,150
860
10,800
955
12,000
334
42
-0.12
-0.75
80
N45
1,350
13,500
860
10,800
955
12,000
350
44
-0.12
-0.75
80
N48
1,400
14,000
836
10,500
955
12,000
390
49
-0.12
-0.75
80
N50
1,425
14,250
836
10,500
955
12,000
390
49
-0.12
-0.75
80
N52
1,450
14,500
836
10,500
876
11,000
406
51
-0.12
-0.75
60
N55
1,490
14,900
716
9,000
876
11,000
430
54
-0.12
-0.75
60
1,175
11,750
836
10,500
1,114
14,000
267
34
-0.12
-0.675
100
1,210
12,100
868
10,900
1,114
14,000
283
35
-0.12
-0.675
100
1,260
12,600
899
11,300
1,114
14,000
307
39
-0.12
-0.675
100
1,285
12,850
923
11,600
1,114
14,000
322
40
-0.12
-0.675
100
1,315
13,150
955
12,000
1,114
14,000
338
42
-0.12
-0.675
100
1,350
13,500
971
12,200
1,114
14,000
354
44
-0.12
-0.675
100
1,395
13,950
995
12,500
1,114
14,000
378
48
-0.12
-0.675
100
1,105
11,050
796
10,000
1,353
17,000
235
30
-0.12
-0.605
120
1,175
11,750
836
10,500
1,353
17,000
267
34
-0.12
-0.605
120
1,210
12,100
868
10,900
1,353
17,000
283
35
-0.12
-0.605
120
1,260
12,600
899
11,300
1,353
17,000
307
39
-0.12
-0.605
120
1,285
12,850
923
11,600
1,353
17,000
322
40
-0.12
-0.605
120
1,300
13,000
955
12,000
1,353
17,000
330
41
-0.12
-0.605
120
1,350
13,500
971
12,200
1,353
17,000
354
44
-0.12
-0.605
120
1,390
13,900
1,011
12,700
1,353
17,000
378
48
-0.12
-0.605
120
1,415
14,150
1,035
13,000
1,274
16,000
390
49
-0.12
-0.605
120
1,125
11,250
811
10,200
1,592
20,000
243
31
-0.12
-0.535
150
1,175
11,750
844
10,600
1,592
20,000
267
34
-0.12
-0.535
150
1,210
12,100
876
11,000
1,592
20,000
283
35
-0.12
-0.535
150
1,260
12,600
907
11,400
1,592
20,000
307
39
-0.12
-0.535
150
1,285
12,850
939
11,800
1,592
20,000
322
40
-0.12
-0.535
150
1,310
13,100
955
12,000
1,592
20,000
330
41
-0.12
-0.535
150
1,350
13,500
979
12,300
1,592
20,000
354
44
-0.12
-0.535
150
1,390
13,900
995
12,500
1,512
19,000
374
47
-0.12
-0.535
150
1,075
10,750
764
9,600
1,990
25,000
227
29
-0.12
-0.465
180
1,125
11,250
812
10,200
1,990
25,000
243
31
-0.12
-0.465
180
1,175
11,750
852
10,700
1,990
25,000
267
34
-0.12
-0.465
180
1,210
12,100
860
10,080
1,990
25,000
283
35
-0.12
-0.465
180
1,260
12,600
876
11,000
1,990
25,000
307
39
-0.12
-0.465
180
1,285
12,850
915
11,500
1,990
25,000
318
40
-0.12
-0.465
180
1,310
13,100
955
12,000
1,990
25,000
330
41
-0.12
-0.465
180
1,350
13,500
955
12,500
1,910
24,000
358
45
-0.12
-0.465
180
1,085
10,850
780
9,800
2,388
30,000
227
29
-0.12
-0.42
200
1,125
11,250
812
10,200
2,388
30,000
243
31
-0.12
-0.42
200
1,165
11,650
820
10,300
2,388
30,000
267
34
-0.12
-0.42
200
1,200
12,000
836
10,500
2,388
30,000
279
35
-0.12
-0.42
200
1,235
12,350
899
11,300
2,388
30,000
303
38
-0.12
-0.42
200
1,270
12,700
915
11,500
2,388
30,000
314
39
-0.12
-0.42
200
1,075
10,750
780
9,800
2,706
34,000
223
28
-0.12
-0.393
220
1,120
11,200
812
10,200
2,706
34,000
239
30
-0.12
-0.393
220
1,195
11,950
883
11,100
2,706
34,000
275
35
-0.12
-0.393
220

Grain Boundary Diffusion (GBD)

“GBD Neo” magnets offer a combination of high energy density and temperature stability at a moderate cost by reducing the amount of Dysprosium (Dy) (GBDD) and Terbium (Tb) (GBDT) used. This process enhances coercivity while limiting the adverse effects on remanence, when compared to traditional neo manufacturing methods. This process favours smaller magnets with a thickness of less than 6mm or laminated materials. For high frequency applications at working temperatures approaching 180°C, consider using this product. Get the full GBD Neo Catalogue for specific grades and their magnetic properties.

Available Grain Boundary Diffused Neo Grades

Properties:BrBrHcBHcBHcJHcJBHmaxBHmaxRev. Temp. Coef.Rev. Temp. Coef.Temp.
Grade
Typical mT
Typical gauss
min kA/m
min oersteds
min kA/m
min oersteds
Typical kJ/m3
Typical MGOe
Br %/°C
HcJ %/°C
max °C
1,350
13,500
979
12,300
1,592
20,000
354
44
-0.12
-0.549
150
1,390
13,900
1,011
12,700
1,592
20,000
374
47
-0.12
-0.549
150
1,425
14,250
836
10,500
1,592
20,000
390
49
-0.12
-0.549
150
1,440
14,400
1,067
13,400
1,592
20,000
402
51
-0.12
-0.549
150
1,460
14,600
1,083
13,600
1,512
19,000
418
53
-0.12
-0.549
150
1,480
14,800
1,098
13,800
1,512
19,000
426
54
-0.12
-0.549
150
1,390
13,900
1,011
12,700
1,512
22,000
374
47
-0.12
-0.549
150
1,425
14,250
836
10,500
1,751
22,000
390
49
-0.12
-0.549
150
1,440
14,400
1,067
13,400
1,751
22,000
402
51
-0.12
-0.549
150
1,460
14,600
1,083
13,600
1,751
21,000
418
53
-0.12
-0.549
150
1,260
12,600
876
11,000
1,990
25,000
306.5
39
-0.12
-0.51
180
1,270
12,700
915
11,500
1,990
25,000
318
40
-0.12
-0.51
180
1,310
13,100
955
12,000
1,990
25,000
330
41
-0.12
-0.465
180
1,350
13,500
979
12,300
1,990
25,000
354
44
-0.12
-0.465
180
1,390
13,900
1,011
12,700
1,990
25,000
374
47
-0.12
-0.465
180
1,410
14,100
1,051
13,200
1,990
25,000
386
49
-0.12
-0.465
180
1,430
14,300
1,067
13,400
1,990
25,000
394
50
-0.12
-0.51
180
1,450
14,500
1,075
13,500
1,910
24,000
418
53
-0.12
-0.51
180
1,310
13,100
955
12,000
2,149
27,000
330
41
-0.12
-0.465
180
1,350
13,500
979
12,300
2,149
27,000
354
44
-0.12
-0.465
180
1,390
13,900
1,011
12,700
2,419
27,000
374
47
-0.12
-0.465
180
1,410
14,100
1,051
13,200
2,449
27,000
386
49
-0.12
-0.465
180
1,430
14,300
1,067
13,400
1,990
25,000
394
50
-0.12
-0.51
180
1,125
11,250
812
10,200
2,388
30,000
243
31
-0.12
-0.472
200
1,165
11,650
820
10,300
2,388
30,000
267
34
-0.12
-0.472
200
1,200
12,000
836
10,500
2,388
30,000
279
35
-0.12
-0.472
200
1,260
12,600
876
11,000
2,388
30,000
306.5
39
-0.12
-0.472
200
1,270
12,700
915
11,500
2,388
30,000
318
40
-0.12
-0.472
200
1,310
13,100
955
12,000
2,388
30,000
330
41
-0.12
-0.472
200
1,310
13,100
971
12,200
2,388
30,000
338
43
-0.12
-0.472
200
1,360
13,600
1,011
12,700
2,388
30,000
362
46
-0.12
-0.472
200
1,385
13,850
1,027
12,900
2,388
30,000
370
47
-0.12
-0.472
200
1,260
12,600
876
11,000
2,547
32,000
306.5
40
-0.12
-0.472
200
1,285
12,850
915
11,500
2,547
32,000
318
40
-0.12
-0.472
200
1,310
13,100
971
12,200
2,547
32,000
338
42
-0.12
-0.472
200
1,360
13,600
1,011
12,700
2,547
32,000
362
45
-0.12
-0.472
200
1,125
11,250
812
10,200
2,706
34,000
243
31
-0.12
-0.449
220
1,165
11,650
820
10,300
2,706
34,000
267
34
-0.12
-0.449
220
1,200
12,000
836
10,500
2,706
34,000
279
35
-0.12
-0.449
220
1,260
12,600
876
11,000
2,706
34,000
306.5
39
-0.12
-0.449
220
1,270
12,700
915
11,500
2,706
34,000
318
40
-0.12
-0.449
220
1,250
12,500
923
11,600
2,786
35,000
298.5
38
-0.12
-0.472
200
1,275
12,750
955
12,000
2,786
35,000
322
40
-0.12
-0.472
200
1,320
13,200
979
12,300
2,786
35,000
346
43
-0.12
-0.472
200
1,235
12,350
915
11,500
2,945
37,000
306.5
39
-0.12
-0.472
200
1,275
12,750
955
12,000
2,945
37,000
323.5
41
-0.12
-0.472
200
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