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Industrial Round Ring Magnets N35-N52 Rare Earth Strong Magnets
Product Details:
| Place of Origin: | China |
| Brand Name: | Monte Bianco |
| Certification: | ISO9001, ISO14001, TS16949 |
| Model Number: | N35-N52 (M.H.SH.UH.EH.AH) |
Payment & Shipping Terms:
| Minimum Order Quantity: | 500PCS |
|---|---|
| Price: | Negotiation |
| Packaging Details: | Standard Package |
| Delivery Time: | 15-30 working days after received your payment |
| Payment Terms: | T/T |
| Supply Ability: | 1000k pcs/month |
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Detail Information |
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| Name: | Industrial Ndfeb Magnet | Grade: | N35-N52 (M.H.SH.UH.EH.AH) |
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| Max Operating Temperature: | 80-220℃（176-428℉） | Tolerance: | International Standard |
| Composite: | Neodymium Magnet, NdFeB Magnet, Rubber Magnet, Rare Earth Magnet, Neodymium-Iron-Boron | Coating: | Ni Cu Ni, Zn, Cr, Gold, Silver, Epoxy, Phosphating |
| Type: | Permanent, Round Block, Ring, NdFeB Magnet | Packing: | Foam Board+carton Box Or Customized |
| Highlight: | Industrial Round Ring Magnets,Ring Rare Earth Magnets N35,N52 Rare Earth Strong Magnets |
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Product Description
Round Ring Industrial Ndfeb Magnet Materials Rare Earth Strong Magnet
Neodymium magnet is a general term for strong magnets, with a chemical formula of Nd2Fe14B. It is an artificial permanent magnet with the strongest magnetic force to date, with a material grade of N35-N52. It can be processed into magnets of different shapes according to different requirements, such as tiles, blocks, punches, magnets, magnetic rods, protrusions, ladders, etc
Please see the following our neo magnet grade
| grade | Br | Hcb | Hcj | (BH)max | temperature coefficient | Max working temperature | |||||
| α Br | β Hcj | ||||||||||
| T | kGs | kA/m | kOe | kA/m | kOe | kJ/m3 | MGOe | %/℃ | %/℃ | ℃ | |
| N54 | 1.45-1.48 | 14.5-14.8 | ≥836 | ≥10.5 | ≥876 | ≥11 | 415-461 | 52-58 | -0.12 | -0.65 | 80 |
| N52 | 1.42-1.45 | 14.2-14.8 | ≥836 | ≥10.5 | ≥876 | ≥11 | 398-415 | 50-52 | -0.12 | -0.65 | 80 |
| N50 | 1.40-1.42 | 14.0-14.5 | ≥836 | ≥10.5 | ≥955 | ≥12 | 374-398 | 47-50 | -0.12 | -0.65 | 80 |
| N48 | 1.37-1.40 | 13.7-14.2 | ≥836 | ≥10.5 | ≥955 | ≥12 | 358-374 | 45-48 | -0.12 | -0.65 | 80 |
| N45 | 1.32-1.37 | 13.2-13.7 | ≥836 | ≥10.5 | ≥955 | ≥12 | 342-358 | 43-45 | -0.12 | -0.65 | 80 |
| N42 | 1.29-1.32 | 12.9-13.2 | ≥836 | ≥10.5 | ≥955 | ≥12 | 318-334 | 40-42 | -0.12 | -0.65 | 80 |
| N40 | 1.26-1.29 | 12.6-12.9 | ≥836 | ≥10.5 | ≥955 | ≥12 | 303-318 | 38-40 | -0.12 | -0.65 | 80 |
| N38 | 1.22-1.26 | 12.2-12.6 | ≥859 | ≥10.8 | ≥955 | ≥12 | 287-303 | 36-38 | -0.12 | -0.65 | 80 |
| N35 | 1.17-1.21 | 11.7-12.1 | ≥859 | ≥10.8 | ≥955 | ≥12 | 263-279 | 33-35 | -0.12 | -0.65 | 80 |
| N33 | 1.14-1.17 | 11.4-11.7 | ≥836 | ≥10.5 | ≥955 | ≥12 | 247-263 | 31-33 | -0.12 | -0.65 | 80 |
| N30 | 1.08-1.12 | 10.8-11.2 | ≥796 | ≥10.0 | ≥955 | ≥12 | 223-239 | 28-30 | -0.12 | -0.65 | 80 |
| N52M | 1.42-1.45 | 14.2-14.5 | ≥995 | 12.5 | ≥1114 | ≥14 | 389-422 | 49-53 | -0.12 | -0.65 | 100 |
| N50M | 1.39-1.45 | 13.9-14.5 | ≥1050 | ≥13.2 | ≥1114 | ≥14 | 374-406 | 47-51 | -0.12 | -0.65 | 100 |
| N48M | 1.37-1.42 | 13.7-14.2 | ≥1018 | ≥12.8 | ≥1114 | ≥14 | 366-390 | 46-49 | -0.12 | -0.65 | 100 |
| N45M | 1.32-1.38 | 13.2-13.8 | ≥987 | ≥12.4 | ≥1114 | ≥14 | 334-366 | 42-46 | -0.12 | -0.65 | 100 |
| N42M | 1.29-1.32 | 12.9-13.2 | ≥955 | ≥12.0 | ≥1114 | ≥14 | 318-334 | 40-42 | -0.12 | -0.65 | 100 |
| N40M | 1.26-1.29 | 12.6-12.9 | ≥939 | ≥11.8 | ≥1114 | ≥14 | 303-318 | 38-40 | -0.12 | -0.65 | 100 |
| N38M | 1.22-1.26 | 12.2-12.6 | ≥916 | ≥11.5 | ≥1114 | ≥14 | 287-303 | 36-38 | -0.12 | -0.65 | 100 |
| N35M | 1.17-1.21 | 11.7-12.1 | ≥876 | ≥11.0 | ≥1114 | ≥14 | 263-279 | 33-35 | -0.12 | -0.65 | 100 |
| N33M | 1.14-1.17 | 11.4-11.7 | ≥852 | ≥10.7 | ≥1114 | ≥14 | 247-263 | 31-33 | -0.12 | -0.65 | 100 |
| N30M | 1.08-1.12 | 10.8-11.2 | ≥812 | ≥10.2 | ≥1114 | ≥14 | 223-239 | 28-30 | -0.12 | -0.65 | 100 |
| N52H | 1.42-1.45 | 14.2-14.5 | ≥1035 | ≥13.0 | ≥1353 | ≥16.5 | 398-422 | 50-53 | -0.11 | -0.58 | 120 |
| N50H | 1.39-1.42 | 13.9-14.2 | ≥1035 | ≥13.0 | ≥1353 | ≥17 | 374-398 | 47-50 | -0.11 | -0.58 | 120 |
| N48H | 1.36-1.42 | 13.6-14.2 | ≥1026 | ≥12.9 | ≥1353 | ≥17 | 358-374 | 45-49 | -0.11 | -0.58 | 120 |
| N45H | 1.32-1.38 | 13.2-13.8 | ≥987 | ≥12.4 | ≥1353 | ≥17 | 334-366 | 42-46 | -0.11 | -0.58 | 120 |
| N42H | 1.29-1.32 | 12.9-13.2 | ≥955 | ≥12.0 | ≥1353 | ≥17 | 318-334 | 40-42 | -0.11 | -0.58 | 120 |
| N40H | 1.26-1.29 | 12.6-12.9 | ≥939 | ≥11.8 | ≥1353 | ≥17 | 303-318 | 38-40 | -0.11 | -0.62 | 120 |
| N38H | 1.22-1.26 | 12.2-12.6 | ≥916 | ≥11.6 | ≥1353 | ≥17 | 287-303 | 36-38 | -0.11 | -0.62 | 120 |
| N35H | 1.17-1.21 | 11.7-12.1 | ≥875 | ≥11.0 | ≥1353 | ≥17 | 263-279 | 33-35 | -0.11 | -0.62 | 120 |
| N33H | 1.14-1.17 | 11.4-11.7 | ≥851 | ≥10.7 | ≥1353 | ≥17 | 247-263 | 31-33 | -0.11 | -0.62 | 120 |
| N30H | 1.08-1.12 | 10.8-11.2 | ≥812 | ≥10.2 | ≥1353 | ≥17 | 223-239 | 28-30 | -0.11 | -0.62 | 120 |
| N50SH | 1.39-1.42 | 13.9-14.2 | ≥1035 | ≥13.0 | ≥1500 | ≥19 | 398-415 | 47-50 | -0.11 | -0.6 | 150 |
| N48SH | 1.36-1.42 | 13.6-14.2 | ≥1026 | ≥12.9 | ≥1592 | ≥20 | 358-398 | 45-49 | -0.11 | -0.6 | 150 |
| N45SH | 1.32-1.36 | 13.2-13.6 | ≥987 | ≥12.4 | ≥1592 | ≥20 | 334-366 | 42-46 | -0.11 | -0.6 | 150 |
| N42SH | 1.29-1.32 | 12.9-13.2 | ≥963 | ≥12.1 | ≥1592 | ≥20 | 318-334 | 40-42 | -0.11 | -0.6 | 150 |
| N40SH | 1.26-1.29 | 12.6-12.9 | ≥931 | ≥11.7 | ≥1592 | ≥20 | 303-318 | 38-40 | -0.11 | -0.6 | 150 |
| N38SH | 1.22-1.26 | 12.2-12.6 | ≥899 | ≥11.3 | ≥1592 | ≥20 | 287-303 | 36-38 | -0.11 | -0.6 | 150 |
| N35SH | 1.17-1.21 | 11.7-12.1 | ≥876 | ≥11.0 | ≥1592 | ≥20 | 263-279 | 33-35 | -0.11 | -0.6 | 150 |
| N33SH | 1.14-1.17 | 11.4-11.7 | ≥851 | ≥10.7 | ≥1592 | ≥20 | 247-263 | 31-33 | -0.11 | -0.6 | 150 |
| N30SH | 1.08-1.12 | 10.8-11.2 | ≥812 | ≥10.2 | ≥1592 | ≥20 | 223-239 | 28-30 | -0.11 | -0.6 | 150 |
| N45UH | 1.32-1.36 | 13.2-13.6 | ≥987 | ≥12.4 | ≥1990 | ≥25 | 334-366 | 42-46 | -0.1 | -0.55 | 180 |
| N42UH | 1.29-1.32 | 12.9-13.2 | ≥963 | ≥12.1 | ≥1990 | ≥25 | 318-334 | 40-42 | -0.1 | -0.55 | 180 |
| N40UH | 1.26-1.32 | 12.6-13.2 | ≥939 | ≥11.8 | ≥1990 | ≥25 | 303-318 | 38-40 | -0.1 | -0.55 | 180 |
| N38UH | 1.22-1.26 | 12.2-12.6 | ≥915 | ≥11.5 | ≥1990 | ≥25 | 287-303 | 36-38 | -0.1 | -0.55 | 180 |
| N35UH | 1.17-1.21 | 11.7-12.1 | ≥875 | ≥11.0 | ≥1990 | ≥25 | 263-279 | 33-35 | -0.1 | -0.55 | 180 |
| N33UH | 1.14-1.17 | 11.4-11.7 | ≥851 | ≥10.7 | ≥1990 | ≥25 | 247-263 | 31-33 | -0.1 | -0.55 | 180 |
| N30UH | 1.08-1.12 | 10.8-11.2 | ≥812 | ≥10.2 | ≥1990 | ≥25 | 223-239 | 28-30 | -0.1 | -0.55 | 180 |
| N38EH | 1.22-1.29 | 12.2-12.9 | ≥907 | ≥11.4 | ≥2388 | ≥30 | 287-318 | 36-40 | -0.09 | -0.5 | 200 |
| N35EH | 1.18-1.25 | 11.8-12.5 | ≥875 | ≥11.0 | ≥2388 | ≥30 | 263-295 | 33-37 | -0.09 | -0.5 | 200 |
| N33EH | 1.14-1.17 | 11.4-11.7 | ≥851 | ≥10.7 | ≥2388 | ≥30 | 247-263 | 31-33 | -0.09 | -0.5 | 200 |
| N30EH | 1.08-1.12 | 10.8-11.2 | ≥812 | ≥10.2 | ≥2388 | ≥30 | 223-239 | 28-30 | -0.09 | -0.5 | 200 |
| N32AH | 1.12-1.20 | 10.8-12.0 | ≥860 | ≥10.8 | ≥2626 | ≥33 | 247-279 | 31-35 | -0.09 | -0.44 | 220 |
The unit of coercivity is either Oe or A/m, with 1A/m=79.6Oe. Coercivity is divided into magnetic induced coercivity (Hcb) and intrinsic coercivity (Hcj).
1. Magnetically induced coercivity
When an electromagnetic field is magnetized in the opposite direction, the value of the magnetic induction intensity in the opposite direction required to reduce the magnetic induction intensity to zero is called magnetic coercivity. But at this time, the magnetization of the electromagnetic field is not zero, but the strength of the applied reverse magnetic field and the magnetization of the electromagnetic field complement each other. When the external magnetic induction intensity is zero, if the external electromagnetic field is removed, the electromagnetic field still has certain magnetic properties.
2. Intrinsic coercivity
The reverse magnetic induction required to reduce the magnetization of the magnet to zero is called intrinsic coercivity. The intrinsic coercivity is a physical quantity that measures the ability of electromagnetic field to resist demagnetization, and it is the coercivity that indicates that the magnetization M in the raw material recedes to zero. In the use of electromagnetic fields, the greater the coercive force of the electromagnetic field, the better the environmental temperature stability.
