Product description
Neodymium Loudspeakers have several advantages over traditional ceramic magnet designs. Typically they are much lighter and more powerful than conventional speakers which use ferrite, AlNiCo or Samarium Cobalt magnets. Neodymium speakers often have motors that use a small cylindrical slug or ring magnet that is encased in a low carbon steel pot structure. The magnetic flux which is already more than 10 times higher than any other material is concentrated across the "gap" where the voice coil moves back and forth. The strength of the motor (BxL) increases so efficiency goes up and the whole magnetic structure becomes more compact. Typically Neo speakers have the additional benifit of not causing any (EMI) interference from stray magnetic flux so by definition they are video shielded. Neodymium magnets are part of the material science of the future with applications growing everyday. One example is the fast growing earbud market. Neo has made it possible to essentially shrink down headphones to sizes that will fit inside your ears. In addition they are also efficient enough to produce high volume sound from small battery powered devices with low amplifier output such as walkmans, MP3 players, tablets, laptops and cell phones.
Ring NdFeB Magnets Production process:
Raw Materials-->Mixture--->Vacuum Melting--- > Powder Production--- >Molding ---> Vacuum Sintering--- > Testing--- >Mechanical Processing--- > Surface Coating--- >Magnetized--- > Inspecting--- > Packing and Shipping.
Ring NdFeB Magnets Directions of Magnetization:
A. Thickness Magnetized
B. Axially Magnetized
C. Diametrally Magnetized
D. Multi-poles magnetized
E. Radial Magnetized
F. Customized specific requirements magnetized
The competitive advantages are as follows:
1. Wide product range, covering all grades from N series to AH series.
2. Samples and small quantity are available.
3. Stock raw metal materials for shorter lead time.
4. Comparatively low price.
5. Reliable quality and technology innovation.
If you have any question plese contant me: Candy
High Performance Sinterated NdFeB Magnet Item
Grade
Remanence;Br
Coercive Force;bHc
Intrisic Coercive Force;iHc
Max Energy Product;(BH)max
Working
Temp.
Â
kGs
T
kOe
KA/m
kOe
KA/m
MGOe
KJ/m3
Max.
Min.
Max.
Min.
Max.
Min.
Max.
Min.
N
N54
15.1Â
14.5Â
1.51Â
1.45Â
≥10.5
≥836
≥11
≥876
55
51
438
406
≤80
N52
14.8Â
14.2Â
1.48Â
1.42Â
≥10.5
≥836
≥11
≥876
53
49
422
390
≤80
N50
14.5Â
14.0Â
1.45Â
1.40Â
≥11.0
≥876
≥12
≥955
51
47
406
374
≤80
N48
14.3Â
13.7Â
1.43Â
1.37Â
≥11.0
≥876
≥12
≥955
49
45
390
358
≤80
N45
13.8Â
13.2Â
1.38Â
1.32Â
≥11.0
≥876
≥12
≥955
46
42
366
334
≤80
N42
13.5Â
12.9Â
1.35Â
1.29Â
≥11.0
≥876
≥12
≥955
44
40
350
318
≤80
N40
13.2Â
12.6Â
1.32Â
1.26Â
≥11.0
≥876
≥12
≥955
41
38
334
302
≤80
N38
13.0Â
12.2Â
1.30Â
1.22Â
≥11.0
≥876
≥12
≥955
40
36
318
287
≤80
N35
12.2Â
11.7Â
1.22Â
1.17Â
≥10.9
≥868
≥12
≥955
36
33
287
263
≤80
M
N52M
14.8Â
14.2Â
1.48Â
1.42Â
≥13.3
≥1059
≥14
≥1114
43
49
422
390
≤100
N50M
14.5Â
14.0Â
1.45Â
1.40Â
≥13.1
≥1043
≥14
≥1114
41
47
406
374
≤100
N48M
14.3Â
13.7Â
1.43Â
1.37Â
≥12.8
≥1019
≥14
≥1114
49
45
390
358
≤100
N45M
13.8Â
13.2Â
1.38Â
1.32Â
≥12.4
≥987
≥14
≥1114
46
42
366
334
≤100
N42M
13.5Â
12.9Â
1.35Â
1.29Â
≥12.1
≥963
≥14
≥1114
44
40
350
318
≤100
N40M
13.2Â
12.6Â
1.32Â
1.26Â
≥11.8
≥939
≥14
≥1114
41
38
334
302
≤100
N38M
13.0Â
12.2Â
1.30Â
1.22Â
≥11.7
≥915
≥14
≥1114
40
36
318
287
≤100
N35MÂ
12.2Â
11.7Â
1.22Â
1.17Â
≥10.9
≥868
≥14
≥1114
36
33
287
263
≤100
H
N50H
14.5Â
14.0Â
1.45Â
1.40Â
≥12.9
≥1027
≥16
≥1274
51
47
406
374
≤120
N48H
14.3Â
13.7Â
1.43Â
1.37Â
≥12.7
≥1011
≥16
≥1274
49
45
390
358
≤120
N46H
14.0Â
13.4Â
1.40Â
1.34Â
≥12.5
≥995
≥17
≥1353
47
43
374
342
≤120
N44H
13.7Â
13.1Â
1.37Â
1.31Â
≥12.3
≥979
≥17
≥1353
45
41
358
326
≤120
N42H
13.5Â
12.9Â
1.35Â
1.29Â
≥12.1
≥963
≥17
≥1353
44
40
350
318
≤120
N40H
13.2Â
12.6Â
1.32Â
1.26Â
≥11.8
≥939
≥17
≥1353
42
38
334
302
≤120
N38H
13.0Â
12.2Â
1.30Â
1.22Â
≥11.5
≥915
≥17
≥1353
40
36
318
287
≤120
N35H
12.4Â
11.7Â
1.24Â
1.17Â
≥11.0
≥876
≥17
≥1353
37
33
295
263
≤120
N33H
11.7Â
11.3Â
1.17Â
1.13Â
≥10.5
≥836
≥17
≥1353
34
31
271
247
≤120
SH
N45SH
14.0Â
13.4Â
1.40Â
1.34Â
≥12.5
≥995
≥20
≥1592
47
43
374
342
≤150
N44SH
13.7Â
13.1Â
1.37Â
1.31Â
≥12.3
≥979
≥20
≥1592
45
41
358
326
≤150
N42SH
13.5Â
12.9Â
1.35Â
1.29Â
≥12.1
≥963
≥20
≥1592
44
40
350
318
≤150
N40SH
13.2Â
12.6Â
1.32Â
1.26Â
≥11.8
≥939
≥20
≥1592
42
38
334
302
≤150
N38SH
12.9Â
12.2Â
1.29Â
1.22Â
≥11.5
≥915
≥20
≥1592
40
36
318
287
≤150
N35SH
12.4Â
11.7Â
1.24Â
1.17Â
≥11.0
≥876
≥20
≥1592
37
33
295
263
≤150
N33SH
12.1Â
11.4Â
1.21Â
1.14Â
≥10.7
≥852
≥20
≥1592
35
31
279
247
≤150
UH
N42UH
13.5Â
12.9Â
1.35Â
1.29Â
≥12.1
≥963
≥25
≥1990
44
40
350
318
≤180
N40UH
13.2Â
12.6Â
1.32Â
1.26Â
≥11.8
≥939
≥25
≥1990
42
38
334
302
≤180
N38UH
12.9Â
12.2Â
1.29Â
1.22Â
≥11.5
≥915
≥25
≥1990
40
36
318
287
≤180
N35UH
12.4Â
11.7Â
1.24Â
1.17Â
≥11.0
≥876
≥25
≥1990
37
33
295
263
≤180
N33UH
12.1Â
11.4Â
1.21Â
1.14Â
≥10.7
≥852
≥25
≥1990
35
31
279
247
≤180
N30UH
11.6Â
10.8Â
1.16Â
1.08Â
≥10.2
≥812
≥25
≥1990
32
28
255
223
≤180
EH
N38EH
12.9Â
12.2Â
1.29Â
1.22Â
≥11.5
≥915
≥30
≥2388
40
36
318
287
≤200
N35EH
12.4Â
11.7Â
1.24Â
1.17Â
≥11.0
≥876
≥30
≥2388
37
33
295
263
≤200
N33EH
12.1Â
11.4Â
1.21Â
1.14Â
≥10.7
≥851
≥30
≥2388
35
31
279
247
≤200
N30EH
11.5Â
10.8Â
1.15Â
1.08Â
≥10.2
≥812
≥30
≥2388
32
28
255
223
≤200
AH
N33AH
12.1Â
11.4Â
1.21Â
1.14Â
≥10.7
≥852
≥35
≥2786
35
31
279
247
≤230
N30AH
11.5Â
10.8Â
1.15Â
1.08Â
≥10.2
≥812
≥35
≥2786
32
28
255
223
≤230
N28AH
11.2Â
10.4Â
1.12Â
1.04Â
≥9.70
≥772
≥35
≥2786
30
26
239
207
≤230